Add files using upload-large-folder tool

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/datasets/__init__.py

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+"""
+================================
+Datasets (:mod:`scipy.datasets`)
+================================
+
+.. currentmodule:: scipy.datasets
+
+Dataset Methods
+===============
+
+.. autosummary::
+   :toctree: generated/
+
+   ascent
+   face
+   electrocardiogram
+
+Utility Methods
+===============
+
+.. autosummary::
+   :toctree: generated/
+
+   download_all    -- Download all the dataset files to specified path.
+   clear_cache     -- Clear cached dataset directory.
+
+
+Usage of Datasets
+=================
+
+SciPy dataset methods can be simply called as follows: ``'<dataset-name>()'``
+This downloads the dataset files over the network once, and saves the cache,
+before returning a `numpy.ndarray` object representing the dataset.
+
+Note that the return data structure and data type might be different for
+different dataset methods. For a more detailed example on usage, please look
+into the particular dataset method documentation above.
+
+
+How dataset retrieval and storage works
+=======================================
+
+SciPy dataset files are stored within individual GitHub repositories under the
+SciPy GitHub organization, following a naming convention as
+``'dataset-<name>'``, for example `scipy.datasets.face` files live at
+https://github.com/scipy/dataset-face.  The `scipy.datasets` submodule utilizes
+and depends on `Pooch <https://www.fatiando.org/pooch/latest/>`_, a Python
+package built to simplify fetching data files. Pooch uses these repos to
+retrieve the respective dataset files when calling the dataset function.
+
+A registry of all the datasets, essentially a mapping of filenames with their
+SHA256 hash and repo urls are maintained, which Pooch uses to handle and verify
+the downloads on function call. After downloading the dataset once, the files
+are saved in the system cache directory under ``'scipy-data'``.
+
+Dataset cache locations may vary on different platforms.
+
+For macOS::
+
+    '~/Library/Caches/scipy-data'
+
+For Linux and other Unix-like platforms::
+
+    '~/.cache/scipy-data'  # or the value of the XDG_CACHE_HOME env var, if defined
+
+For Windows::
+
+    'C:\\Users\\<user>\\AppData\\Local\\<AppAuthor>\\scipy-data\\Cache'
+
+
+In environments with constrained network connectivity for various security
+reasons or on systems without continuous internet connections, one may manually
+load the cache of the datasets by placing the contents of the dataset repo in
+the above mentioned cache directory to avoid fetching dataset errors without
+the internet connectivity.
+
+"""
+
+
+from ._fetchers import face, ascent, electrocardiogram
+from ._download_all import download_all
+from ._utils import clear_cache
+
+__all__ = ['ascent', 'electrocardiogram', 'face',
+           'download_all', 'clear_cache']
+
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/datasets/_download_all.py

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+"""
+Platform independent script to download all the
+`scipy.datasets` module data files.
+This doesn't require a full scipy build.
+
+Run: python _download_all.py <download_dir>
+"""
+
+from scipy._lib._array_api import xp_capabilities
+
+import argparse
+try:
+    import pooch
+except ImportError:
+    pooch = None
+
+
+if __package__ is None or __package__ == '':
+    # Running as python script, use absolute import
+    import _registry  # type: ignore
+else:
+    # Running as python module, use relative import
+    from . import _registry
+
+
+@xp_capabilities(out_of_scope=True)
+def download_all(path=None):
+    """
+    Utility method to download all the dataset files
+    for `scipy.datasets` module.
+
+    Parameters
+    ----------
+    path : str, optional
+        Directory path to download all the dataset files.
+        If None, default to the system cache_dir detected by pooch.
+
+    Examples
+    --------
+    Download the datasets to the default cache location:
+
+    >>> from scipy import datasets
+    >>> datasets.download_all()
+
+    Download the datasets to the current directory:
+
+    >>> datasets.download_all(".")
+
+    """
+    if pooch is None:
+        raise ImportError("Missing optional dependency 'pooch' required "
+                          "for scipy.datasets module. Please use pip or "
+                          "conda to install 'pooch'.")
+    if path is None:
+        path = pooch.os_cache('scipy-data')
+    # https://github.com/scipy/scipy/issues/21879
+    downloader = pooch.HTTPDownloader(headers={"User-Agent": "SciPy"})
+    for dataset_name, dataset_hash in _registry.registry.items():
+        pooch.retrieve(url=_registry.registry_urls[dataset_name],
+                       known_hash=dataset_hash,
+                       fname=dataset_name, path=path, downloader=downloader)
+
+
+def main():
+    parser = argparse.ArgumentParser(description='Download SciPy data files.')
+    parser.add_argument("path", nargs='?', type=str,
+                        default=pooch.os_cache('scipy-data'),
+                        help="Directory path to download all the data files.")
+    args = parser.parse_args()
+    download_all(args.path)
+
+
+if __name__ == "__main__":
+    main()

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/datasets/_fetchers.py

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+import sys
+
+from numpy import array, frombuffer, load
+from ._registry import registry, registry_urls
+
+from scipy._lib._array_api import xp_capabilities
+
+try:
+    import pooch
+except ImportError:
+    pooch = None
+    data_fetcher = None
+else:
+    data_fetcher = pooch.create(
+        # Use the default cache folder for the operating system
+        # Pooch uses appdirs (https://github.com/ActiveState/appdirs) to
+        # select an appropriate directory for the cache on each platform.
+        path=pooch.os_cache("scipy-data"),
+
+        # The remote data is on Github
+        # base_url is a required param, even though we override this
+        # using individual urls in the registry.
+        base_url="https://github.com/scipy/",
+        registry=registry,
+        urls=registry_urls
+    )
+
+
+def fetch_data(dataset_name, data_fetcher=data_fetcher):
+    if data_fetcher is None:
+        raise ImportError("Missing optional dependency 'pooch' required "
+                          "for scipy.datasets module. Please use pip or "
+                          "conda to install 'pooch'.")
+    # https://github.com/scipy/scipy/issues/21879
+    downloader = pooch.HTTPDownloader(
+        headers={"User-Agent": f"SciPy {sys.modules['scipy'].__version__}"}
+    )
+    # The "fetch" method returns the full path to the downloaded data file.
+    return data_fetcher.fetch(dataset_name, downloader=downloader)
+
+
+@xp_capabilities(out_of_scope=True)
+def ascent():
+    """
+    Get an 8-bit grayscale bit-depth, 512 x 512 derived image for easy
+    use in demos.
+
+    The image is derived from
+    https://pixnio.com/people/accent-to-the-top
+
+    Parameters
+    ----------
+    None
+
+    Returns
+    -------
+    ascent : ndarray
+       convenient image to use for testing and demonstration
+
+    Examples
+    --------
+    >>> import scipy.datasets
+    >>> ascent = scipy.datasets.ascent()
+    >>> ascent.shape
+    (512, 512)
+    >>> ascent.max()
+    np.uint8(255)
+
+    >>> import matplotlib.pyplot as plt
+    >>> plt.gray()
+    >>> plt.imshow(ascent)
+    >>> plt.show()
+
+    """
+    import pickle
+
+    # The file will be downloaded automatically the first time this is run,
+    # returning the path to the downloaded file. Afterwards, Pooch finds
+    # it in the local cache and doesn't repeat the download.
+    fname = fetch_data("ascent.dat")
+    # Now we just need to load it with our standard Python tools.
+    with open(fname, 'rb') as f:
+        ascent = array(pickle.load(f))
+    return ascent
+
+
+@xp_capabilities(out_of_scope=True)
+def electrocardiogram():
+    """
+    Load an electrocardiogram as an example for a 1-D signal.
+
+    The returned signal is a 5 minute long electrocardiogram (ECG), a medical
+    recording of the heart's electrical activity, sampled at 360 Hz.
+
+    Returns
+    -------
+    ecg : ndarray
+        The electrocardiogram in millivolt (mV) sampled at 360 Hz.
+
+    Notes
+    -----
+    The provided signal is an excerpt (19:35 to 24:35) from the `record 208`_
+    (lead MLII) provided by the MIT-BIH Arrhythmia Database [1]_ on
+    PhysioNet [2]_. The excerpt includes noise induced artifacts, typical
+    heartbeats as well as pathological changes.
+
+    .. _record 208: https://physionet.org/physiobank/database/html/mitdbdir/records.htm#208
+
+    .. versionadded:: 1.1.0
+
+    References
+    ----------
+    .. [1] Moody GB, Mark RG. The impact of the MIT-BIH Arrhythmia Database.
+           IEEE Eng in Med and Biol 20(3):45-50 (May-June 2001).
+           (PMID: 11446209); :doi:`10.13026/C2F305`
+    .. [2] Goldberger AL, Amaral LAN, Glass L, Hausdorff JM, Ivanov PCh,
+           Mark RG, Mietus JE, Moody GB, Peng C-K, Stanley HE. PhysioBank,
+           PhysioToolkit, and PhysioNet: Components of a New Research Resource
+           for Complex Physiologic Signals. Circulation 101(23):e215-e220;
+           :doi:`10.1161/01.CIR.101.23.e215`
+
+    Examples
+    --------
+    >>> from scipy.datasets import electrocardiogram
+    >>> ecg = electrocardiogram()
+    >>> ecg
+    array([-0.245, -0.215, -0.185, ..., -0.405, -0.395, -0.385], shape=(108000,))
+    >>> ecg.shape, ecg.mean(), ecg.std()
+    ((108000,), -0.16510875, 0.5992473991177294)
+
+    As stated the signal features several areas with a different morphology.
+    E.g., the first few seconds show the electrical activity of a heart in
+    normal sinus rhythm as seen below.
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> fs = 360
+    >>> time = np.arange(ecg.size) / fs
+    >>> plt.plot(time, ecg)
+    >>> plt.xlabel("time in s")
+    >>> plt.ylabel("ECG in mV")
+    >>> plt.xlim(9, 10.2)
+    >>> plt.ylim(-1, 1.5)
+    >>> plt.show()
+
+    After second 16, however, the first premature ventricular contractions,
+    also called extrasystoles, appear. These have a different morphology
+    compared to typical heartbeats. The difference can easily be observed
+    in the following plot.
+
+    >>> plt.plot(time, ecg)
+    >>> plt.xlabel("time in s")
+    >>> plt.ylabel("ECG in mV")
+    >>> plt.xlim(46.5, 50)
+    >>> plt.ylim(-2, 1.5)
+    >>> plt.show()
+
+    At several points large artifacts disturb the recording, e.g.:
+
+    >>> plt.plot(time, ecg)
+    >>> plt.xlabel("time in s")
+    >>> plt.ylabel("ECG in mV")
+    >>> plt.xlim(207, 215)
+    >>> plt.ylim(-2, 3.5)
+    >>> plt.show()
+
+    Finally, examining the power spectrum reveals that most of the biosignal is
+    made up of lower frequencies. At 60 Hz the noise induced by the mains
+    electricity can be clearly observed.
+
+    >>> from scipy.signal import welch
+    >>> f, Pxx = welch(ecg, fs=fs, nperseg=2048, scaling="spectrum")
+    >>> plt.semilogy(f, Pxx)
+    >>> plt.xlabel("Frequency in Hz")
+    >>> plt.ylabel("Power spectrum of the ECG in mV**2")
+    >>> plt.xlim(f[[0, -1]])
+    >>> plt.show()
+    """
+    fname = fetch_data("ecg.dat")
+    with load(fname) as file:
+        ecg = file["ecg"].astype(int)  # np.uint16 -> int
+    # Convert raw output of ADC to mV: (ecg - adc_zero) / adc_gain
+    ecg = (ecg - 1024) / 200.0
+    return ecg
+
+
+@xp_capabilities(out_of_scope=True)
+def face(gray=False):
+    """
+    Get a 1024 x 768, color image of a raccoon face.
+
+    The image is derived from
+    https://pixnio.com/fauna-animals/raccoons/raccoon-procyon-lotor
+
+    Parameters
+    ----------
+    gray : bool, optional
+        If True return 8-bit grey-scale image, otherwise return a color image
+
+    Returns
+    -------
+    face : ndarray
+        image of a raccoon face
+
+    Examples
+    --------
+    >>> import scipy.datasets
+    >>> face = scipy.datasets.face()
+    >>> face.shape
+    (768, 1024, 3)
+    >>> face.max()
+    np.uint8(255)
+
+    >>> import matplotlib.pyplot as plt
+    >>> plt.gray()
+    >>> plt.imshow(face)
+    >>> plt.show()
+
+    """
+    import bz2
+    fname = fetch_data("face.dat")
+    with open(fname, 'rb') as f:
+        rawdata = f.read()
+    face_data = bz2.decompress(rawdata)
+    face = frombuffer(face_data, dtype='uint8').reshape((768, 1024, 3))
+    if gray is True:
+        face = (0.21 * face[:, :, 0] + 0.71 * face[:, :, 1] +
+                0.07 * face[:, :, 2]).astype('uint8')
+    return face

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/datasets/_registry.py

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+##########################################################################
+# This file serves as the dataset registry for SciPy Datasets SubModule.
+##########################################################################
+
+
+# To generate the SHA256 hash, use the command
+# openssl sha256 <filename>
+registry = {
+    "ascent.dat": "03ce124c1afc880f87b55f6b061110e2e1e939679184f5614e38dacc6c1957e2",
+    "ecg.dat": "f20ad3365fb9b7f845d0e5c48b6fe67081377ee466c3a220b7f69f35c8958baf",
+    "face.dat": "9d8b0b4d081313e2b485748c770472e5a95ed1738146883d84c7030493e82886"
+}
+
+registry_urls = {
+    "ascent.dat": "https://raw.githubusercontent.com/scipy/dataset-ascent/main/ascent.dat",
+    "ecg.dat": "https://raw.githubusercontent.com/scipy/dataset-ecg/main/ecg.dat",
+    "face.dat": "https://raw.githubusercontent.com/scipy/dataset-face/main/face.dat"
+}
+
+# dataset method mapping with their associated filenames
+# <method_name> : ["filename1", "filename2", ...]
+method_files_map = {
+    "ascent": ["ascent.dat"],
+    "electrocardiogram": ["ecg.dat"],
+    "face": ["face.dat"]
+}

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/datasets/_utils.py

@@ -0,0 +1,84 @@
+import os
+import shutil
+from ._registry import method_files_map
+
+from scipy._lib._array_api import xp_capabilities
+
+try:
+    import platformdirs
+except ImportError:
+    platformdirs = None  # type: ignore[assignment]
+
+
+def _clear_cache(datasets, cache_dir=None, method_map=None):
+    if method_map is None:
+        # Use SciPy Datasets method map
+        method_map = method_files_map
+    if cache_dir is None:
+        # Use default cache_dir path
+        if platformdirs is None:
+            # platformdirs is pooch dependency
+            raise ImportError("Missing optional dependency 'pooch' required "
+                              "for scipy.datasets module. Please use pip or "
+                              "conda to install 'pooch'.")
+        cache_dir = platformdirs.user_cache_dir("scipy-data")
+
+    if not os.path.exists(cache_dir):
+        print(f"Cache Directory {cache_dir} doesn't exist. Nothing to clear.")
+        return
+
+    if datasets is None:
+        print(f"Cleaning the cache directory {cache_dir}!")
+        shutil.rmtree(cache_dir)
+    else:
+        if not isinstance(datasets, list | tuple):
+            # single dataset method passed should be converted to list
+            datasets = [datasets, ]
+        for dataset in datasets:
+            assert callable(dataset)
+            dataset_name = dataset.__name__  # Name of the dataset method
+            if dataset_name not in method_map:
+                raise ValueError(f"Dataset method {dataset_name} doesn't "
+                                 "exist. Please check if the passed dataset "
+                                 "is a subset of the following dataset "
+                                 f"methods: {list(method_map.keys())}")
+
+            data_files = method_map[dataset_name]
+            data_filepaths = [os.path.join(cache_dir, file)
+                              for file in data_files]
+            for data_filepath in data_filepaths:
+                if os.path.exists(data_filepath):
+                    print("Cleaning the file "
+                          f"{os.path.split(data_filepath)[1]} "
+                          f"for dataset {dataset_name}")
+                    os.remove(data_filepath)
+                else:
+                    print(f"Path {data_filepath} doesn't exist. "
+                          "Nothing to clear.")
+
+
+@xp_capabilities(out_of_scope=True)
+def clear_cache(datasets=None):
+    """
+    Cleans the scipy datasets cache directory.
+
+    If a scipy.datasets method or a list/tuple of the same is
+    provided, then clear_cache removes all the data files
+    associated to the passed dataset method callable(s).
+
+    By default, it removes all the cached data files.
+
+    Parameters
+    ----------
+    datasets : callable or list/tuple of callable or None
+
+    Examples
+    --------
+    >>> from scipy import datasets
+    >>> ascent_array = datasets.ascent()
+    >>> ascent_array.shape
+    (512, 512)
+    >>> datasets.clear_cache([datasets.ascent])
+    Cleaning the file ascent.dat for dataset ascent
+    """
+    _clear_cache(datasets)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/differentiate/__init__.py

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+"""
+==============================================================
+Finite Difference Differentiation (:mod:`scipy.differentiate`)
+==============================================================
+
+.. currentmodule:: scipy.differentiate
+
+SciPy ``differentiate`` provides functions for performing finite difference
+numerical differentiation of black-box functions.
+
+.. autosummary::
+   :toctree: generated/
+
+   derivative
+   jacobian
+   hessian
+
+"""
+
+
+from ._differentiate import *
+
+__all__ = ['derivative', 'jacobian', 'hessian']
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/differentiate/_differentiate.py

@@ -0,0 +1,1140 @@
+# mypy: disable-error-code="attr-defined"
+import warnings
+import numpy as np
+import scipy._lib._elementwise_iterative_method as eim
+from scipy._lib._util import _RichResult
+from scipy._lib._array_api import array_namespace, xp_copy, xp_promote, xp_capabilities
+import scipy._lib.array_api_extra as xpx
+
+_EERRORINCREASE = -1  # used in derivative
+
+def _derivative_iv(f, x, args, tolerances, maxiter, order, initial_step,
+                   step_factor, step_direction, preserve_shape, callback):
+    # Input validation for `derivative`
+    xp = array_namespace(x)
+
+    if not callable(f):
+        raise ValueError('`f` must be callable.')
+
+    if not np.iterable(args):
+        args = (args,)
+
+    tolerances = {} if tolerances is None else tolerances
+    atol = tolerances.get('atol', None)
+    rtol = tolerances.get('rtol', None)
+
+    # tolerances are floats, not arrays; OK to use NumPy
+    message = 'Tolerances and step parameters must be non-negative scalars.'
+    tols = np.asarray([atol if atol is not None else 1,
+                       rtol if rtol is not None else 1,
+                       step_factor])
+    if (not np.issubdtype(tols.dtype, np.number) or np.any(tols < 0)
+            or np.any(np.isnan(tols)) or tols.shape != (3,)):
+        raise ValueError(message)
+    step_factor = float(tols[2])
+
+    maxiter_int = int(maxiter)
+    if maxiter != maxiter_int or maxiter <= 0:
+        raise ValueError('`maxiter` must be a positive integer.')
+
+    order_int = int(order)
+    if order_int != order or order <= 0:
+        raise ValueError('`order` must be a positive integer.')
+
+    step_direction = xp.asarray(step_direction)
+    initial_step = xp.asarray(initial_step)
+    temp = xp.broadcast_arrays(x, step_direction, initial_step)
+    x, step_direction, initial_step = temp
+
+    message = '`preserve_shape` must be True or False.'
+    if preserve_shape not in {True, False}:
+        raise ValueError(message)
+
+    if callback is not None and not callable(callback):
+        raise ValueError('`callback` must be callable.')
+
+    return (f, x, args, atol, rtol, maxiter_int, order_int, initial_step,
+            step_factor, step_direction, preserve_shape, callback)
+
+
+
+_array_api_strict_skip_reason = 'Array API does not support fancy indexing assignment.'
+_dask_reason = 'boolean indexing assignment'
+
+
+@xp_capabilities(skip_backends=[('array_api_strict', _array_api_strict_skip_reason),
+                                ('dask.array', _dask_reason)], jax_jit=False)
+def derivative(f, x, *, args=(), tolerances=None, maxiter=10,
+               order=8, initial_step=0.5, step_factor=2.0,
+               step_direction=0, preserve_shape=False, callback=None):
+    """Evaluate the derivative of an elementwise, real scalar function numerically.
+
+    For each element of the output of `f`, `derivative` approximates the first
+    derivative of `f` at the corresponding element of `x` using finite difference
+    differentiation.
+
+    This function works elementwise when `x`, `step_direction`, and `args` contain
+    (broadcastable) arrays.
+
+    Parameters
+    ----------
+    f : callable
+        The function whose derivative is desired. The signature must be::
+
+            f(xi: ndarray, *argsi) -> ndarray
+
+        where each element of ``xi`` is a finite real number and ``argsi`` is a tuple,
+        which may contain an arbitrary number of arrays that are broadcastable with
+        ``xi``. `f` must be an elementwise function: each scalar element ``f(xi)[j]``
+        must equal ``f(xi[j])`` for valid indices ``j``. It must not mutate the array
+        ``xi`` or the arrays in ``argsi``.
+    x : float array_like
+        Abscissae at which to evaluate the derivative. Must be broadcastable with
+        `args` and `step_direction`.
+    args : tuple of array_like, optional
+        Additional positional array arguments to be passed to `f`. Arrays
+        must be broadcastable with one another and the arrays of `init`.
+        If the callable for which the root is desired requires arguments that are
+        not broadcastable with `x`, wrap that callable with `f` such that `f`
+        accepts only `x` and broadcastable ``*args``.
+    tolerances : dictionary of floats, optional
+        Absolute and relative tolerances. Valid keys of the dictionary are:
+
+        - ``atol`` - absolute tolerance on the derivative
+        - ``rtol`` - relative tolerance on the derivative
+
+        Iteration will stop when ``res.error < atol + rtol * abs(res.df)``. The default
+        `atol` is the smallest normal number of the appropriate dtype, and
+        the default `rtol` is the square root of the precision of the
+        appropriate dtype.
+    order : int, default: 8
+        The (positive integer) order of the finite difference formula to be
+        used. Odd integers will be rounded up to the next even integer.
+    initial_step : float array_like, default: 0.5
+        The (absolute) initial step size for the finite difference derivative
+        approximation.
+    step_factor : float, default: 2.0
+        The factor by which the step size is *reduced* in each iteration; i.e.
+        the step size in iteration 1 is ``initial_step/step_factor``. If
+        ``step_factor < 1``, subsequent steps will be greater than the initial
+        step; this may be useful if steps smaller than some threshold are
+        undesirable (e.g. due to subtractive cancellation error).
+    maxiter : int, default: 10
+        The maximum number of iterations of the algorithm to perform. See
+        Notes.
+    step_direction : integer array_like
+        An array representing the direction of the finite difference steps (for
+        use when `x` lies near to the boundary of the domain of the function.)
+        Must be broadcastable with `x` and all `args`.
+        Where 0 (default), central differences are used; where negative (e.g.
+        -1), steps are non-positive; and where positive (e.g. 1), all steps are
+        non-negative.
+    preserve_shape : bool, default: False
+        In the following, "arguments of `f`" refers to the array ``xi`` and
+        any arrays within ``argsi``. Let ``shape`` be the broadcasted shape
+        of `x` and all elements of `args` (which is conceptually
+        distinct from ``xi` and ``argsi`` passed into `f`).
+
+        - When ``preserve_shape=False`` (default), `f` must accept arguments
+          of *any* broadcastable shapes.
+
+        - When ``preserve_shape=True``, `f` must accept arguments of shape
+          ``shape`` *or* ``shape + (n,)``, where ``(n,)`` is the number of
+          abscissae at which the function is being evaluated.
+
+        In either case, for each scalar element ``xi[j]`` within ``xi``, the array
+        returned by `f` must include the scalar ``f(xi[j])`` at the same index.
+        Consequently, the shape of the output is always the shape of the input
+        ``xi``.
+
+        See Examples.
+    callback : callable, optional
+        An optional user-supplied function to be called before the first
+        iteration and after each iteration.
+        Called as ``callback(res)``, where ``res`` is a ``_RichResult``
+        similar to that returned by `derivative` (but containing the current
+        iterate's values of all variables). If `callback` raises a
+        ``StopIteration``, the algorithm will terminate immediately and
+        `derivative` will return a result. `callback` must not mutate
+        `res` or its attributes.
+
+    Returns
+    -------
+    res : _RichResult
+        An object similar to an instance of `scipy.optimize.OptimizeResult` with the
+        following attributes. The descriptions are written as though the values will
+        be scalars; however, if `f` returns an array, the outputs will be
+        arrays of the same shape.
+
+        success : bool array
+            ``True`` where the algorithm terminated successfully (status ``0``);
+            ``False`` otherwise.
+        status : int array
+            An integer representing the exit status of the algorithm.
+
+            - ``0`` : The algorithm converged to the specified tolerances.
+            - ``-1`` : The error estimate increased, so iteration was terminated.
+            - ``-2`` : The maximum number of iterations was reached.
+            - ``-3`` : A non-finite value was encountered.
+            - ``-4`` : Iteration was terminated by `callback`.
+            - ``1`` : The algorithm is proceeding normally (in `callback` only).
+
+        df : float array
+            The derivative of `f` at `x`, if the algorithm terminated
+            successfully.
+        error : float array
+            An estimate of the error: the magnitude of the difference between
+            the current estimate of the derivative and the estimate in the
+            previous iteration.
+        nit : int array
+            The number of iterations of the algorithm that were performed.
+        nfev : int array
+            The number of points at which `f` was evaluated.
+        x : float array
+            The value at which the derivative of `f` was evaluated
+            (after broadcasting with `args` and `step_direction`).
+
+    See Also
+    --------
+    jacobian, hessian
+
+    Notes
+    -----
+    The implementation was inspired by jacobi [1]_, numdifftools [2]_, and
+    DERIVEST [3]_, but the implementation follows the theory of Taylor series
+    more straightforwardly (and arguably naively so).
+    In the first iteration, the derivative is estimated using a finite
+    difference formula of order `order` with maximum step size `initial_step`.
+    Each subsequent iteration, the maximum step size is reduced by
+    `step_factor`, and the derivative is estimated again until a termination
+    condition is reached. The error estimate is the magnitude of the difference
+    between the current derivative approximation and that of the previous
+    iteration.
+
+    The stencils of the finite difference formulae are designed such that
+    abscissae are "nested": after `f` is evaluated at ``order + 1``
+    points in the first iteration, `f` is evaluated at only two new points
+    in each subsequent iteration; ``order - 1`` previously evaluated function
+    values required by the finite difference formula are reused, and two
+    function values (evaluations at the points furthest from `x`) are unused.
+
+    Step sizes are absolute. When the step size is small relative to the
+    magnitude of `x`, precision is lost; for example, if `x` is ``1e20``, the
+    default initial step size of ``0.5`` cannot be resolved. Accordingly,
+    consider using larger initial step sizes for large magnitudes of `x`.
+
+    The default tolerances are challenging to satisfy at points where the
+    true derivative is exactly zero. If the derivative may be exactly zero,
+    consider specifying an absolute tolerance (e.g. ``atol=1e-12``) to
+    improve convergence.
+
+    References
+    ----------
+    .. [1] Hans Dembinski (@HDembinski). jacobi.
+           https://github.com/HDembinski/jacobi
+    .. [2] Per A. Brodtkorb and John D'Errico. numdifftools.
+           https://numdifftools.readthedocs.io/en/latest/
+    .. [3] John D'Errico. DERIVEST: Adaptive Robust Numerical Differentiation.
+           https://www.mathworks.com/matlabcentral/fileexchange/13490-adaptive-robust-numerical-differentiation
+    .. [4] Numerical Differentition. Wikipedia.
+           https://en.wikipedia.org/wiki/Numerical_differentiation
+
+    Examples
+    --------
+    Evaluate the derivative of ``np.exp`` at several points ``x``.
+
+    >>> import numpy as np
+    >>> from scipy.differentiate import derivative
+    >>> f = np.exp
+    >>> df = np.exp  # true derivative
+    >>> x = np.linspace(1, 2, 5)
+    >>> res = derivative(f, x)
+    >>> res.df  # approximation of the derivative
+    array([2.71828183, 3.49034296, 4.48168907, 5.75460268, 7.3890561 ])
+    >>> res.error  # estimate of the error
+    array([7.13740178e-12, 9.16600129e-12, 1.17594823e-11, 1.51061386e-11,
+           1.94262384e-11])
+    >>> abs(res.df - df(x))  # true error
+    array([2.53130850e-14, 3.55271368e-14, 5.77315973e-14, 5.59552404e-14,
+           6.92779167e-14])
+
+    Show the convergence of the approximation as the step size is reduced.
+    Each iteration, the step size is reduced by `step_factor`, so for
+    sufficiently small initial step, each iteration reduces the error by a
+    factor of ``1/step_factor**order`` until finite precision arithmetic
+    inhibits further improvement.
+
+    >>> import matplotlib.pyplot as plt
+    >>> iter = list(range(1, 12))  # maximum iterations
+    >>> hfac = 2  # step size reduction per iteration
+    >>> hdir = [-1, 0, 1]  # compare left-, central-, and right- steps
+    >>> order = 4  # order of differentiation formula
+    >>> x = 1
+    >>> ref = df(x)
+    >>> errors = []  # true error
+    >>> for i in iter:
+    ...     res = derivative(f, x, maxiter=i, step_factor=hfac,
+    ...                      step_direction=hdir, order=order,
+    ...                      # prevent early termination
+    ...                      tolerances=dict(atol=0, rtol=0))
+    ...     errors.append(abs(res.df - ref))
+    >>> errors = np.array(errors)
+    >>> plt.semilogy(iter, errors[:, 0], label='left differences')
+    >>> plt.semilogy(iter, errors[:, 1], label='central differences')
+    >>> plt.semilogy(iter, errors[:, 2], label='right differences')
+    >>> plt.xlabel('iteration')
+    >>> plt.ylabel('error')
+    >>> plt.legend()
+    >>> plt.show()
+    >>> (errors[1, 1] / errors[0, 1], 1 / hfac**order)
+    (0.06215223140159822, 0.0625)
+
+    The implementation is vectorized over `x`, `step_direction`, and `args`.
+    The function is evaluated once before the first iteration to perform input
+    validation and standardization, and once per iteration thereafter.
+
+    >>> def f(x, p):
+    ...     f.nit += 1
+    ...     return x**p
+    >>> f.nit = 0
+    >>> def df(x, p):
+    ...     return p*x**(p-1)
+    >>> x = np.arange(1, 5)
+    >>> p = np.arange(1, 6).reshape((-1, 1))
+    >>> hdir = np.arange(-1, 2).reshape((-1, 1, 1))
+    >>> res = derivative(f, x, args=(p,), step_direction=hdir, maxiter=1)
+    >>> np.allclose(res.df, df(x, p))
+    True
+    >>> res.df.shape
+    (3, 5, 4)
+    >>> f.nit
+    2
+
+    By default, `preserve_shape` is False, and therefore the callable
+    `f` may be called with arrays of any broadcastable shapes.
+    For example:
+
+    >>> shapes = []
+    >>> def f(x, c):
+    ...    shape = np.broadcast_shapes(x.shape, c.shape)
+    ...    shapes.append(shape)
+    ...    return np.sin(c*x)
+    >>>
+    >>> c = [1, 5, 10, 20]
+    >>> res = derivative(f, 0, args=(c,))
+    >>> shapes
+    [(4,), (4, 8), (4, 2), (3, 2), (2, 2), (1, 2)]
+
+    To understand where these shapes are coming from - and to better
+    understand how `derivative` computes accurate results - note that
+    higher values of ``c`` correspond with higher frequency sinusoids.
+    The higher frequency sinusoids make the function's derivative change
+    faster, so more function evaluations are required to achieve the target
+    accuracy:
+
+    >>> res.nfev
+    array([11, 13, 15, 17], dtype=int32)
+
+    The initial ``shape``, ``(4,)``, corresponds with evaluating the
+    function at a single abscissa and all four frequencies; this is used
+    for input validation and to determine the size and dtype of the arrays
+    that store results. The next shape corresponds with evaluating the
+    function at an initial grid of abscissae and all four frequencies.
+    Successive calls to the function evaluate the function at two more
+    abscissae, increasing the effective order of the approximation by two.
+    However, in later function evaluations, the function is evaluated at
+    fewer frequencies because the corresponding derivative has already
+    converged to the required tolerance. This saves function evaluations to
+    improve performance, but it requires the function to accept arguments of
+    any shape.
+
+    "Vector-valued" functions are unlikely to satisfy this requirement.
+    For example, consider
+
+    >>> def f(x):
+    ...    return [x, np.sin(3*x), x+np.sin(10*x), np.sin(20*x)*(x-1)**2]
+
+    This integrand is not compatible with `derivative` as written; for instance,
+    the shape of the output will not be the same as the shape of ``x``. Such a
+    function *could* be converted to a compatible form with the introduction of
+    additional parameters, but this would be inconvenient. In such cases,
+    a simpler solution would be to use `preserve_shape`.
+
+    >>> shapes = []
+    >>> def f(x):
+    ...     shapes.append(x.shape)
+    ...     x0, x1, x2, x3 = x
+    ...     return [x0, np.sin(3*x1), x2+np.sin(10*x2), np.sin(20*x3)*(x3-1)**2]
+    >>>
+    >>> x = np.zeros(4)
+    >>> res = derivative(f, x, preserve_shape=True)
+    >>> shapes
+    [(4,), (4, 8), (4, 2), (4, 2), (4, 2), (4, 2)]
+
+    Here, the shape of ``x`` is ``(4,)``. With ``preserve_shape=True``, the
+    function may be called with argument ``x`` of shape ``(4,)`` or ``(4, n)``,
+    and this is what we observe.
+
+    """
+    # TODO (followup):
+    #  - investigate behavior at saddle points
+    #  - multivariate functions?
+    #  - relative steps?
+    #  - show example of `np.vectorize`
+
+    res = _derivative_iv(f, x, args, tolerances, maxiter, order, initial_step,
+                            step_factor, step_direction, preserve_shape, callback)
+    (func, x, args, atol, rtol, maxiter, order,
+     h0, fac, hdir, preserve_shape, callback) = res
+
+    # Initialization
+    # Since f(x) (no step) is not needed for central differences, it may be
+    # possible to eliminate this function evaluation. However, it's useful for
+    # input validation and standardization, and everything else is designed to
+    # reduce function calls, so let's keep it simple.
+    temp = eim._initialize(func, (x,), args, preserve_shape=preserve_shape)
+    func, xs, fs, args, shape, dtype, xp = temp
+
+    finfo = xp.finfo(dtype)
+    atol = finfo.smallest_normal if atol is None else atol
+    rtol = finfo.eps**0.5 if rtol is None else rtol  # keep same as `hessian`
+
+    x, f = xs[0], fs[0]
+    df = xp.full_like(f, xp.nan)
+
+    # Ideally we'd broadcast the shape of `hdir` in `_elementwise_algo_init`, but
+    # it's simpler to do it here than to generalize `_elementwise_algo_init` further.
+    # `hdir` and `x` are already broadcasted in `_derivative_iv`, so we know
+    # that `hdir` can be broadcasted to the final shape. Same with `h0`.
+    hdir = xp.broadcast_to(hdir, shape)
+    hdir = xp.reshape(hdir, (-1,))
+    hdir = xp.astype(xp.sign(hdir), dtype)
+    h0 = xp.broadcast_to(h0, shape)
+    h0 = xp.reshape(h0, (-1,))
+    h0 = xp.astype(h0, dtype)
+    h0 = xpx.at(h0)[h0 <= 0].set(xp.nan)
+
+    status = xp.full_like(x, eim._EINPROGRESS, dtype=xp.int32)  # in progress
+    nit, nfev = 0, 1  # one function evaluations performed above
+    # Boolean indices of left, central, right, and (all) one-sided steps
+    il = hdir < 0
+    ic = hdir == 0
+    ir = hdir > 0
+    io = il | ir
+
+    # Most of these attributes are reasonably obvious, but:
+    # - `fs` holds all the function values of all active `x`. The zeroth
+    #   axis corresponds with active points `x`, the first axis corresponds
+    #   with the different steps (in the order described in
+    #   `_derivative_weights`).
+    # - `terms` (which could probably use a better name) is half the `order`,
+    #   which is always even.
+    work = _RichResult(x=x, df=df, fs=f[:, xp.newaxis], error=xp.nan, h=h0,
+                       df_last=xp.nan, error_last=xp.nan, fac=fac,
+                       atol=atol, rtol=rtol, nit=nit, nfev=nfev,
+                       status=status, dtype=dtype, terms=(order+1)//2,
+                       hdir=hdir, il=il, ic=ic, ir=ir, io=io,
+                       # Store the weights in an object so they can't get compressed
+                       # Using RichResult to allow dot notation, but a dict would work
+                       diff_state=_RichResult(central=[], right=[], fac=None))
+
+    # This is the correspondence between terms in the `work` object and the
+    # final result. In this case, the mapping is trivial. Note that `success`
+    # is prepended automatically.
+    res_work_pairs = [('status', 'status'), ('df', 'df'), ('error', 'error'),
+                      ('nit', 'nit'), ('nfev', 'nfev'), ('x', 'x')]
+
+    def pre_func_eval(work):
+        """Determine the abscissae at which the function needs to be evaluated.
+
+        See `_derivative_weights` for a description of the stencil (pattern
+        of the abscissae).
+
+        In the first iteration, there is only one stored function value in
+        `work.fs`, `f(x)`, so we need to evaluate at `order` new points. In
+        subsequent iterations, we evaluate at two new points. Note that
+        `work.x` is always flattened into a 1D array after broadcasting with
+        all `args`, so we add a new axis at the end and evaluate all point
+        in one call to the function.
+
+        For improvement:
+        - Consider measuring the step size actually taken, since ``(x + h) - x``
+          is not identically equal to `h` with floating point arithmetic.
+        - Adjust the step size automatically if `x` is too big to resolve the
+          step.
+        - We could probably save some work if there are no central difference
+          steps or no one-sided steps.
+        """
+        n = work.terms  # half the order
+        h = work.h[:, xp.newaxis]  # step size
+        c = work.fac  # step reduction factor
+        d = c**0.5  # square root of step reduction factor (one-sided stencil)
+        # Note - no need to be careful about dtypes until we allocate `x_eval`
+
+        if work.nit == 0:
+            hc = h / c**xp.arange(n, dtype=work.dtype)
+            hc = xp.concat((-xp.flip(hc, axis=-1), hc), axis=-1)
+        else:
+            hc = xp.concat((-h, h), axis=-1) / c**(n-1)
+
+        if work.nit == 0:
+            hr = h / d**xp.arange(2*n, dtype=work.dtype)
+        else:
+            hr = xp.concat((h, h/d), axis=-1) / c**(n-1)
+
+        n_new = 2*n if work.nit == 0 else 2  # number of new abscissae
+        x_eval = xp.zeros((work.hdir.shape[0], n_new), dtype=work.dtype)
+        il, ic, ir = work.il, work.ic, work.ir
+        x_eval = xpx.at(x_eval)[ir].set(work.x[ir][:, xp.newaxis] + hr[ir])
+        x_eval = xpx.at(x_eval)[ic].set(work.x[ic][:, xp.newaxis] + hc[ic])
+        x_eval = xpx.at(x_eval)[il].set(work.x[il][:, xp.newaxis] - hr[il])
+        return x_eval
+
+    def post_func_eval(x, f, work):
+        """ Estimate the derivative and error from the function evaluations
+
+        As in `pre_func_eval`: in the first iteration, there is only one stored
+        function value in `work.fs`, `f(x)`, so we need to add the `order` new
+        points. In subsequent iterations, we add two new points. The tricky
+        part is getting the order to match that of the weights, which is
+        described in `_derivative_weights`.
+
+        For improvement:
+        - Change the order of the weights (and steps in `pre_func_eval`) to
+          simplify `work_fc` concatenation and eliminate `fc` concatenation.
+        - It would be simple to do one-step Richardson extrapolation with `df`
+          and `df_last` to increase the order of the estimate and/or improve
+          the error estimate.
+        - Process the function evaluations in a more numerically favorable
+          way. For instance, combining the pairs of central difference evals
+          into a second-order approximation and using Richardson extrapolation
+          to produce a higher order approximation seemed to retain accuracy up
+          to very high order.
+        - Alternatively, we could use `polyfit` like Jacobi. An advantage of
+          fitting polynomial to more points than necessary is improved noise
+          tolerance.
+        """
+        n = work.terms
+        n_new = n if work.nit == 0 else 1
+        il, ic, io = work.il, work.ic, work.io
+
+        # Central difference
+        # `work_fc` is *all* the points at which the function has been evaluated
+        # `fc` is the points we're using *this iteration* to produce the estimate
+        work_fc = (f[ic][:, :n_new], work.fs[ic], f[ic][:, -n_new:])
+        work_fc = xp.concat(work_fc, axis=-1)
+        if work.nit == 0:
+            fc = work_fc
+        else:
+            fc = (work_fc[:, :n], work_fc[:, n:n+1], work_fc[:, -n:])
+            fc = xp.concat(fc, axis=-1)
+
+        # One-sided difference
+        work_fo = xp.concat((work.fs[io], f[io]), axis=-1)
+        if work.nit == 0:
+            fo = work_fo
+        else:
+            fo = xp.concat((work_fo[:, 0:1], work_fo[:, -2*n:]), axis=-1)
+
+        work.fs = xp.zeros((ic.shape[0], work.fs.shape[-1] + 2*n_new), dtype=work.dtype)
+        work.fs = xpx.at(work.fs)[ic].set(work_fc)
+        work.fs = xpx.at(work.fs)[io].set(work_fo)
+
+        wc, wo = _derivative_weights(work, n, xp)
+        work.df_last = xp.asarray(work.df, copy=True)
+        work.df = xpx.at(work.df)[ic].set(fc @ wc / work.h[ic])
+        work.df = xpx.at(work.df)[io].set(fo @ wo / work.h[io])
+        work.df = xpx.at(work.df)[il].multiply(-1)
+
+        work.h /= work.fac
+        work.error_last = work.error
+        # Simple error estimate - the difference in derivative estimates between
+        # this iteration and the last. This is typically conservative because if
+        # convergence has begin, the true error is much closer to the difference
+        # between the current estimate and the *next* error estimate. However,
+        # we could use Richarson extrapolation to produce an error estimate that
+        # is one order higher, and take the difference between that and
+        # `work.df` (which would just be constant factor that depends on `fac`.)
+        work.error = xp.abs(work.df - work.df_last)
+
+    def check_termination(work):
+        """Terminate due to convergence, non-finite values, or error increase"""
+        stop = xp.astype(xp.zeros_like(work.df), xp.bool)
+
+        i = work.error < work.atol + work.rtol*abs(work.df)
+        work.status = xpx.at(work.status)[i].set(eim._ECONVERGED)
+        stop = xpx.at(stop)[i].set(True)
+
+        if work.nit > 0:
+            i = ~((xp.isfinite(work.x) & xp.isfinite(work.df)) | stop)
+            work.df = xpx.at(work.df)[i].set(xp.nan)
+            work.status = xpx.at(work.status)[i].set(eim._EVALUEERR)
+            stop = xpx.at(stop)[i].set(True)
+
+        # With infinite precision, there is a step size below which
+        # all smaller step sizes will reduce the error. But in floating point
+        # arithmetic, catastrophic cancellation will begin to cause the error
+        # to increase again. This heuristic tries to avoid step sizes that are
+        # too small. There may be more theoretically sound approaches for
+        # detecting a step size that minimizes the total error, but this
+        # heuristic seems simple and effective.
+        i = (work.error > work.error_last*10) & ~stop
+        work.status = xpx.at(work.status)[i].set(_EERRORINCREASE)
+        stop = xpx.at(stop)[i].set(True)
+
+        return stop
+
+    def post_termination_check(work):
+        return
+
+    def customize_result(res, shape):
+        return shape
+
+    return eim._loop(work, callback, shape, maxiter, func, args, dtype,
+                     pre_func_eval, post_func_eval, check_termination,
+                     post_termination_check, customize_result, res_work_pairs,
+                     xp, preserve_shape)
+
+
+def _derivative_weights(work, n, xp):
+    # This produces the weights of the finite difference formula for a given
+    # stencil. In experiments, use of a second-order central difference formula
+    # with Richardson extrapolation was more accurate numerically, but it was
+    # more complicated, and it would have become even more complicated when
+    # adding support for one-sided differences. However, now that all the
+    # function evaluation values are stored, they can be processed in whatever
+    # way is desired to produce the derivative estimate. We leave alternative
+    # approaches to future work. To be more self-contained, here is the theory
+    # for deriving the weights below.
+    #
+    # Recall that the Taylor expansion of a univariate, scalar-values function
+    # about a point `x` may be expressed as:
+    #      f(x + h)  =     f(x) + f'(x)*h + f''(x)/2!*h**2  + O(h**3)
+    # Suppose we evaluate f(x), f(x+h), and f(x-h).  We have:
+    #      f(x)      =     f(x)
+    #      f(x + h)  =     f(x) + f'(x)*h + f''(x)/2!*h**2  + O(h**3)
+    #      f(x - h)  =     f(x) - f'(x)*h + f''(x)/2!*h**2  + O(h**3)
+    # We can solve for weights `wi` such that:
+    #   w1*f(x)      = w1*(f(x))
+    # + w2*f(x + h)  = w2*(f(x) + f'(x)*h + f''(x)/2!*h**2) + O(h**3)
+    # + w3*f(x - h)  = w3*(f(x) - f'(x)*h + f''(x)/2!*h**2) + O(h**3)
+    #                =     0    + f'(x)*h + 0               + O(h**3)
+    # Then
+    #     f'(x) ~ (w1*f(x) + w2*f(x+h) + w3*f(x-h))/h
+    # is a finite difference derivative approximation with error O(h**2),
+    # and so it is said to be a "second-order" approximation. Under certain
+    # conditions (e.g. well-behaved function, `h` sufficiently small), the
+    # error in the approximation will decrease with h**2; that is, if `h` is
+    # reduced by a factor of 2, the error is reduced by a factor of 4.
+    #
+    # By default, we use eighth-order formulae. Our central-difference formula
+    # uses abscissae:
+    #   x-h/c**3, x-h/c**2, x-h/c, x-h, x, x+h, x+h/c, x+h/c**2, x+h/c**3
+    # where `c` is the step factor. (Typically, the step factor is greater than
+    # one, so the outermost points - as written above - are actually closest to
+    # `x`.) This "stencil" is chosen so that each iteration, the step can be
+    # reduced by the factor `c`, and most of the function evaluations can be
+    # reused with the new step size. For example, in the next iteration, we
+    # will have:
+    #   x-h/c**4, x-h/c**3, x-h/c**2, x-h/c, x, x+h/c, x+h/c**2, x+h/c**3, x+h/c**4
+    # We do not reuse `x-h` and `x+h` for the new derivative estimate.
+    # While this would increase the order of the formula and thus the
+    # theoretical convergence rate, it is also less stable numerically.
+    # (As noted above, there are other ways of processing the values that are
+    # more stable. Thus, even now we store `f(x-h)` and `f(x+h)` in `work.fs`
+    # to simplify future development of this sort of improvement.)
+    #
+    # The (right) one-sided formula is produced similarly using abscissae
+    #   x, x+h, x+h/d, x+h/d**2, ..., x+h/d**6, x+h/d**7, x+h/d**7
+    # where `d` is the square root of `c`. (The left one-sided formula simply
+    # uses -h.) When the step size is reduced by factor `c = d**2`, we have
+    # abscissae:
+    #   x, x+h/d**2, x+h/d**3..., x+h/d**8, x+h/d**9, x+h/d**9
+    # `d` is chosen as the square root of `c` so that the rate of the step-size
+    # reduction is the same per iteration as in the central difference case.
+    # Note that because the central difference formulas are inherently of even
+    # order, for simplicity, we use only even-order formulas for one-sided
+    # differences, too.
+
+    # It's possible for the user to specify `fac` in, say, double precision but
+    # `x` and `args` in single precision. `fac` gets converted to single
+    # precision, but we should always use double precision for the intermediate
+    # calculations here to avoid additional error in the weights.
+    fac = float(work.fac)
+
+    # Note that if the user switches back to floating point precision with
+    # `x` and `args`, then `fac` will not necessarily equal the (lower
+    # precision) cached `_derivative_weights.fac`, and the weights will
+    # need to be recalculated. This could be fixed, but it's late, and of
+    # low consequence.
+
+    diff_state = work.diff_state
+    if fac != diff_state.fac:
+        diff_state.central = []
+        diff_state.right = []
+        diff_state.fac = fac
+
+    if len(diff_state.central) != 2*n + 1:
+        # Central difference weights. Consider refactoring this; it could
+        # probably be more compact.
+        # Note: Using NumPy here is OK; we convert to xp-type at the end
+        i = np.arange(-n, n + 1)
+        p = np.abs(i) - 1.  # center point has power `p` -1, but sign `s` is 0
+        s = np.sign(i)
+
+        h = s / fac ** p
+        A = np.vander(h, increasing=True).T
+        b = np.zeros(2*n + 1)
+        b[1] = 1
+        weights = np.linalg.solve(A, b)
+
+        # Enforce identities to improve accuracy
+        weights[n] = 0
+        for i in range(n):
+            weights[-i-1] = -weights[i]
+
+        # Cache the weights. We only need to calculate them once unless
+        # the step factor changes.
+        diff_state.central = weights
+
+        # One-sided difference weights. The left one-sided weights (with
+        # negative steps) are simply the negative of the right one-sided
+        # weights, so no need to compute them separately.
+        i = np.arange(2*n + 1)
+        p = i - 1.
+        s = np.sign(i)
+
+        h = s / np.sqrt(fac) ** p
+        A = np.vander(h, increasing=True).T
+        b = np.zeros(2 * n + 1)
+        b[1] = 1
+        weights = np.linalg.solve(A, b)
+
+        diff_state.right = weights
+
+    return (xp.asarray(diff_state.central, dtype=work.dtype),
+            xp.asarray(diff_state.right, dtype=work.dtype))
+
+
+@xp_capabilities(skip_backends=[('array_api_strict', _array_api_strict_skip_reason),
+                                ('dask.array', _dask_reason)], jax_jit=False)
+def jacobian(f, x, *, tolerances=None, maxiter=10, order=8, initial_step=0.5,
+             step_factor=2.0, step_direction=0):
+    r"""Evaluate the Jacobian of a function numerically.
+
+    Parameters
+    ----------
+    f : callable
+        The function whose Jacobian is desired. The signature must be::
+
+            f(xi: ndarray) -> ndarray
+
+        where each element of ``xi`` is a finite real. If the function to be
+        differentiated accepts additional arguments, wrap it (e.g. using
+        `functools.partial` or ``lambda``) and pass the wrapped callable
+        into `jacobian`. `f` must not mutate the array ``xi``. See Notes
+        regarding vectorization and the dimensionality of the input and output.
+    x : float array_like
+        Points at which to evaluate the Jacobian. Must have at least one dimension.
+        See Notes regarding the dimensionality and vectorization.
+    tolerances : dictionary of floats, optional
+        Absolute and relative tolerances. Valid keys of the dictionary are:
+
+        - ``atol`` - absolute tolerance on the derivative
+        - ``rtol`` - relative tolerance on the derivative
+
+        Iteration will stop when ``res.error < atol + rtol * abs(res.df)``. The default
+        `atol` is the smallest normal number of the appropriate dtype, and
+        the default `rtol` is the square root of the precision of the
+        appropriate dtype.
+    maxiter : int, default: 10
+        The maximum number of iterations of the algorithm to perform. See
+        Notes.
+    order : int, default: 8
+        The (positive integer) order of the finite difference formula to be
+        used. Odd integers will be rounded up to the next even integer.
+    initial_step : float array_like, default: 0.5
+        The (absolute) initial step size for the finite difference derivative
+        approximation. Must be broadcastable with `x` and `step_direction`.
+    step_factor : float, default: 2.0
+        The factor by which the step size is *reduced* in each iteration; i.e.
+        the step size in iteration 1 is ``initial_step/step_factor``. If
+        ``step_factor < 1``, subsequent steps will be greater than the initial
+        step; this may be useful if steps smaller than some threshold are
+        undesirable (e.g. due to subtractive cancellation error).
+    step_direction : integer array_like
+        An array representing the direction of the finite difference steps (e.g.
+        for use when `x` lies near to the boundary of the domain of the function.)
+        Must be broadcastable with `x` and `initial_step`.
+        Where 0 (default), central differences are used; where negative (e.g.
+        -1), steps are non-positive; and where positive (e.g. 1), all steps are
+        non-negative.
+
+    Returns
+    -------
+    res : _RichResult
+        An object similar to an instance of `scipy.optimize.OptimizeResult` with the
+        following attributes. The descriptions are written as though the values will
+        be scalars; however, if `f` returns an array, the outputs will be
+        arrays of the same shape.
+
+        success : bool array
+            ``True`` where the algorithm terminated successfully (status ``0``);
+            ``False`` otherwise.
+        status : int array
+            An integer representing the exit status of the algorithm.
+
+            - ``0`` : The algorithm converged to the specified tolerances.
+            - ``-1`` : The error estimate increased, so iteration was terminated.
+            - ``-2`` : The maximum number of iterations was reached.
+            - ``-3`` : A non-finite value was encountered.
+
+        df : float array
+            The Jacobian of `f` at `x`, if the algorithm terminated
+            successfully.
+        error : float array
+            An estimate of the error: the magnitude of the difference between
+            the current estimate of the Jacobian and the estimate in the
+            previous iteration.
+        nit : int array
+            The number of iterations of the algorithm that were performed.
+        nfev : int array
+            The number of points at which `f` was evaluated.
+
+        Each element of an attribute is associated with the corresponding
+        element of `df`. For instance, element ``i`` of `nfev` is the
+        number of points at which `f` was evaluated for the sake of
+        computing element ``i`` of `df`.
+
+    See Also
+    --------
+    derivative, hessian
+
+    Notes
+    -----
+    Suppose we wish to evaluate the Jacobian of a function
+    :math:`f: \mathbf{R}^m \rightarrow \mathbf{R}^n`. Assign to variables
+    ``m`` and ``n`` the positive integer values of :math:`m` and :math:`n`,
+    respectively, and let ``...`` represent an arbitrary tuple of integers.
+    If we wish to evaluate the Jacobian at a single point, then:
+
+    - argument `x` must be an array of shape ``(m,)``
+    - argument `f` must be vectorized to accept an array of shape ``(m, ...)``.
+      The first axis represents the :math:`m` inputs of :math:`f`; the remainder
+      are for evaluating the function at multiple points in a single call.
+    - argument `f` must return an array of shape ``(n, ...)``. The first
+      axis represents the :math:`n` outputs of :math:`f`; the remainder
+      are for the result of evaluating the function at multiple points.
+    - attribute ``df`` of the result object will be an array of shape ``(n, m)``,
+      the Jacobian.
+
+    This function is also vectorized in the sense that the Jacobian can be
+    evaluated at ``k`` points in a single call. In this case, `x` would be an
+    array of shape ``(m, k)``, `f` would accept an array of shape
+    ``(m, k, ...)`` and return an array of shape ``(n, k, ...)``, and the ``df``
+    attribute of the result would have shape ``(n, m, k)``.
+
+    Suppose the desired callable ``f_not_vectorized`` is not vectorized; it can
+    only accept an array of shape ``(m,)``. A simple solution to satisfy the required
+    interface is to wrap ``f_not_vectorized`` as follows::
+
+        def f(x):
+            return np.apply_along_axis(f_not_vectorized, axis=0, arr=x)
+
+    Alternatively, suppose the desired callable ``f_vec_q`` is vectorized, but
+    only for 2-D arrays of shape ``(m, q)``. To satisfy the required interface,
+    consider::
+
+        def f(x):
+            m, batch = x.shape[0], x.shape[1:]  # x.shape is (m, ...)
+            x = np.reshape(x, (m, -1))  # `-1` is short for q = prod(batch)
+            res = f_vec_q(x)  # pass shape (m, q) to function
+            n = res.shape[0]
+            return np.reshape(res, (n,) + batch)  # return shape (n, ...)
+
+    Then pass the wrapped callable ``f`` as the first argument of `jacobian`.
+
+    References
+    ----------
+    .. [1] Jacobian matrix and determinant, *Wikipedia*,
+           https://en.wikipedia.org/wiki/Jacobian_matrix_and_determinant
+
+    Examples
+    --------
+    The Rosenbrock function maps from :math:`\mathbf{R}^m \rightarrow \mathbf{R}`;
+    the SciPy implementation `scipy.optimize.rosen` is vectorized to accept an
+    array of shape ``(m, p)`` and return an array of shape ``p``. Suppose we wish
+    to evaluate the Jacobian (AKA the gradient because the function returns a scalar)
+    at ``[0.5, 0.5, 0.5]``.
+
+    >>> import numpy as np
+    >>> from scipy.differentiate import jacobian
+    >>> from scipy.optimize import rosen, rosen_der
+    >>> m = 3
+    >>> x = np.full(m, 0.5)
+    >>> res = jacobian(rosen, x)
+    >>> ref = rosen_der(x)  # reference value of the gradient
+    >>> res.df, ref
+    (array([-51.,  -1.,  50.]), array([-51.,  -1.,  50.]))
+
+    As an example of a function with multiple outputs, consider Example 4
+    from [1]_.
+
+    >>> def f(x):
+    ...     x1, x2, x3 = x
+    ...     return [x1, 5*x3, 4*x2**2 - 2*x3, x3*np.sin(x1)]
+
+    The true Jacobian is given by:
+
+    >>> def df(x):
+    ...         x1, x2, x3 = x
+    ...         one = np.ones_like(x1)
+    ...         return [[one, 0*one, 0*one],
+    ...                 [0*one, 0*one, 5*one],
+    ...                 [0*one, 8*x2, -2*one],
+    ...                 [x3*np.cos(x1), 0*one, np.sin(x1)]]
+
+    Evaluate the Jacobian at an arbitrary point.
+
+    >>> rng = np.random.default_rng(389252938452)
+    >>> x = rng.random(size=3)
+    >>> res = jacobian(f, x)
+    >>> ref = df(x)
+    >>> res.df.shape == (4, 3)
+    True
+    >>> np.allclose(res.df, ref)
+    True
+
+    Evaluate the Jacobian at 10 arbitrary points in a single call.
+
+    >>> x = rng.random(size=(3, 10))
+    >>> res = jacobian(f, x)
+    >>> ref = df(x)
+    >>> res.df.shape == (4, 3, 10)
+    True
+    >>> np.allclose(res.df, ref)
+    True
+
+    """
+    xp = array_namespace(x)
+    x0 = xp_promote(x, force_floating=True, xp=xp)
+
+    if x0.ndim < 1:
+        message = "Argument `x` must be at least 1-D."
+        raise ValueError(message)
+
+    m = x0.shape[0]
+    i = xp.arange(m)
+
+    def wrapped(x):
+        p = () if x.ndim == x0.ndim else (x.shape[-1],)  # number of abscissae
+
+        new_shape = (m, m) + x0.shape[1:] + p
+        xph = xp.expand_dims(x0, axis=1)
+        if x.ndim != x0.ndim:
+            xph = xp.expand_dims(xph, axis=-1)
+        xph = xp_copy(xp.broadcast_to(xph, new_shape), xp=xp)
+        xph = xpx.at(xph)[i, i].set(x)
+        return f(xph)
+
+    res = derivative(wrapped, x, tolerances=tolerances,
+                     maxiter=maxiter, order=order, initial_step=initial_step,
+                     step_factor=step_factor, preserve_shape=True,
+                     step_direction=step_direction)
+
+    del res.x  # the user knows `x`, and the way it gets broadcasted is meaningless here
+    return res
+
+
+@xp_capabilities(skip_backends=[('array_api_strict', _array_api_strict_skip_reason),
+                                ('dask.array', _dask_reason)], jax_jit=False)
+def hessian(f, x, *, tolerances=None, maxiter=10,
+            order=8, initial_step=0.5, step_factor=2.0):
+    r"""Evaluate the Hessian of a function numerically.
+
+    Parameters
+    ----------
+    f : callable
+        The function whose Hessian is desired. The signature must be::
+
+            f(xi: ndarray) -> ndarray
+
+        where each element of ``xi`` is a finite real. If the function to be
+        differentiated accepts additional arguments, wrap it (e.g. using
+        `functools.partial` or ``lambda``) and pass the wrapped callable
+        into `hessian`. `f` must not mutate the array ``xi``. See Notes
+        regarding vectorization and the dimensionality of the input and output.
+    x : float array_like
+        Points at which to evaluate the Hessian. Must have at least one dimension.
+        See Notes regarding the dimensionality and vectorization.
+    tolerances : dictionary of floats, optional
+        Absolute and relative tolerances. Valid keys of the dictionary are:
+
+        - ``atol`` - absolute tolerance on the derivative
+        - ``rtol`` - relative tolerance on the derivative
+
+        Iteration will stop when ``res.error < atol + rtol * abs(res.df)``. The default
+        `atol` is the smallest normal number of the appropriate dtype, and
+        the default `rtol` is the square root of the precision of the
+        appropriate dtype.
+    order : int, default: 8
+        The (positive integer) order of the finite difference formula to be
+        used. Odd integers will be rounded up to the next even integer.
+    initial_step : float, default: 0.5
+        The (absolute) initial step size for the finite difference derivative
+        approximation.
+    step_factor : float, default: 2.0
+        The factor by which the step size is *reduced* in each iteration; i.e.
+        the step size in iteration 1 is ``initial_step/step_factor``. If
+        ``step_factor < 1``, subsequent steps will be greater than the initial
+        step; this may be useful if steps smaller than some threshold are
+        undesirable (e.g. due to subtractive cancellation error).
+    maxiter : int, default: 10
+        The maximum number of iterations of the algorithm to perform. See
+        Notes.
+
+    Returns
+    -------
+    res : _RichResult
+        An object similar to an instance of `scipy.optimize.OptimizeResult` with the
+        following attributes. The descriptions are written as though the values will
+        be scalars; however, if `f` returns an array, the outputs will be
+        arrays of the same shape.
+
+        success : bool array
+            ``True`` where the algorithm terminated successfully (status ``0``);
+            ``False`` otherwise.
+        status : int array
+            An integer representing the exit status of the algorithm.
+
+            - ``0`` : The algorithm converged to the specified tolerances.
+            - ``-1`` : The error estimate increased, so iteration was terminated.
+            - ``-2`` : The maximum number of iterations was reached.
+            - ``-3`` : A non-finite value was encountered.
+
+        ddf : float array
+            The Hessian of `f` at `x`, if the algorithm terminated
+            successfully.
+        error : float array
+            An estimate of the error: the magnitude of the difference between
+            the current estimate of the Hessian and the estimate in the
+            previous iteration.
+        nfev : int array
+            The number of points at which `f` was evaluated.
+
+        Each element of an attribute is associated with the corresponding
+        element of `ddf`. For instance, element ``[i, j]`` of `nfev` is the
+        number of points at which `f` was evaluated for the sake of
+        computing element ``[i, j]`` of `ddf`.
+
+    See Also
+    --------
+    derivative, jacobian
+
+    Notes
+    -----
+    Suppose we wish to evaluate the Hessian of a function
+    :math:`f: \mathbf{R}^m \rightarrow \mathbf{R}`, and we assign to variable
+    ``m`` the positive integer value of :math:`m`. If we wish to evaluate
+    the Hessian at a single point, then:
+
+    - argument `x` must be an array of shape ``(m,)``
+    - argument `f` must be vectorized to accept an array of shape
+      ``(m, ...)``. The first axis represents the :math:`m` inputs of
+      :math:`f`; the remaining axes indicated by ellipses are for evaluating
+      the function at several abscissae in a single call.
+    - argument `f` must return an array of shape ``(...)``.
+    - attribute ``dff`` of the result object will be an array of shape ``(m, m)``,
+      the Hessian.
+
+    This function is also vectorized in the sense that the Hessian can be
+    evaluated at ``k`` points in a single call. In this case, `x` would be an
+    array of shape ``(m, k)``, `f` would accept an array of shape
+    ``(m, ...)`` and return an array of shape ``(...)``, and the ``ddf``
+    attribute of the result would have shape ``(m, m, k)``. Note that the
+    axis associated with the ``k`` points is included within the axes
+    denoted by ``(...)``.
+
+    Currently, `hessian` is implemented by nesting calls to `jacobian`.
+    All options passed to `hessian` are used for both the inner and outer
+    calls with one exception: the `rtol` used in the inner `jacobian` call
+    is tightened by a factor of 100 with the expectation that the inner
+    error can be ignored. A consequence is that `rtol` should not be set
+    less than 100 times the precision of the dtype of `x`; a warning is
+    emitted otherwise.
+
+    References
+    ----------
+    .. [1] Hessian matrix, *Wikipedia*,
+           https://en.wikipedia.org/wiki/Hessian_matrix
+
+    Examples
+    --------
+    The Rosenbrock function maps from :math:`\mathbf{R}^m \rightarrow \mathbf{R}`;
+    the SciPy implementation `scipy.optimize.rosen` is vectorized to accept an
+    array of shape ``(m, ...)`` and return an array of shape ``...``. Suppose we
+    wish to evaluate the Hessian at ``[0.5, 0.5, 0.5]``.
+
+    >>> import numpy as np
+    >>> from scipy.differentiate import hessian
+    >>> from scipy.optimize import rosen, rosen_hess
+    >>> m = 3
+    >>> x = np.full(m, 0.5)
+    >>> res = hessian(rosen, x)
+    >>> ref = rosen_hess(x)  # reference value of the Hessian
+    >>> np.allclose(res.ddf, ref)
+    True
+
+    `hessian` is vectorized to evaluate the Hessian at multiple points
+    in a single call.
+
+    >>> rng = np.random.default_rng(4589245925010)
+    >>> x = rng.random((m, 10))
+    >>> res = hessian(rosen, x)
+    >>> ref = [rosen_hess(xi) for xi in x.T]
+    >>> ref = np.moveaxis(ref, 0, -1)
+    >>> np.allclose(res.ddf, ref)
+    True
+
+    """
+    # todo:
+    # - add ability to vectorize over additional parameters (*args?)
+    # - error estimate stack with inner jacobian (or use legit 2D stencil)
+
+    kwargs = dict(maxiter=maxiter, order=order, initial_step=initial_step,
+                  step_factor=step_factor)
+    tolerances = {} if tolerances is None else tolerances
+    atol = tolerances.get('atol', None)
+    rtol = tolerances.get('rtol', None)
+
+    xp = array_namespace(x)
+    x0 = xp_promote(x, force_floating=True, xp=xp)
+
+    finfo = xp.finfo(x0.dtype)
+    rtol = finfo.eps**0.5 if rtol is None else rtol  # keep same as `derivative`
+
+    # tighten the inner tolerance to make the inner error negligible
+    rtol_min = finfo.eps * 100
+    message = (f"The specified `{rtol=}`, but error estimates are likely to be "
+               f"unreliable when `rtol < {rtol_min}`.")
+    if 0 < rtol < rtol_min:  # rtol <= 0 is an error
+        warnings.warn(message, RuntimeWarning, stacklevel=2)
+        rtol = rtol_min
+
+    def df(x):
+        tolerances = dict(rtol=rtol/100, atol=atol)
+        temp = jacobian(f, x, tolerances=tolerances, **kwargs)
+        nfev.append(temp.nfev if len(nfev) == 0 else temp.nfev.sum(axis=-1))
+        return temp.df
+
+    nfev = []  # track inner function evaluations
+    res = jacobian(df, x, tolerances=tolerances, **kwargs)  # jacobian of jacobian
+
+    nfev = xp.cumulative_sum(xp.stack(nfev), axis=0)
+    res_nit = xp.astype(res.nit[xp.newaxis, ...], xp.int64)  # appease torch
+    res.nfev = xp.take_along_axis(nfev, res_nit, axis=0)[0]
+    res.ddf = res.df
+    del res.df  # this is renamed to ddf
+    del res.nit  # this is only the outer-jacobian nit
+
+    return res

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/__init__.py

@@ -0,0 +1,103 @@
+"""
+=========================================================
+Legacy discrete Fourier transforms (:mod:`scipy.fftpack`)
+=========================================================
+
+.. legacy::
+
+   New code should use :mod:`scipy.fft`.
+
+Fast Fourier Transforms (FFTs)
+==============================
+
+.. autosummary::
+   :toctree: generated/
+
+   fft - Fast (discrete) Fourier Transform (FFT)
+   ifft - Inverse FFT
+   fft2 - 2-D FFT
+   ifft2 - 2-D inverse FFT
+   fftn - N-D FFT
+   ifftn - N-D inverse FFT
+   rfft - FFT of strictly real-valued sequence
+   irfft - Inverse of rfft
+   dct - Discrete cosine transform
+   idct - Inverse discrete cosine transform
+   dctn - N-D Discrete cosine transform
+   idctn - N-D Inverse discrete cosine transform
+   dst - Discrete sine transform
+   idst - Inverse discrete sine transform
+   dstn - N-D Discrete sine transform
+   idstn - N-D Inverse discrete sine transform
+
+Differential and pseudo-differential operators
+==============================================
+
+.. autosummary::
+   :toctree: generated/
+
+   diff - Differentiation and integration of periodic sequences
+   tilbert - Tilbert transform:         cs_diff(x,h,h)
+   itilbert - Inverse Tilbert transform: sc_diff(x,h,h)
+   hilbert - Hilbert transform:         cs_diff(x,inf,inf)
+   ihilbert - Inverse Hilbert transform: sc_diff(x,inf,inf)
+   cs_diff - cosh/sinh pseudo-derivative of periodic sequences
+   sc_diff - sinh/cosh pseudo-derivative of periodic sequences
+   ss_diff - sinh/sinh pseudo-derivative of periodic sequences
+   cc_diff - cosh/cosh pseudo-derivative of periodic sequences
+   shift - Shift periodic sequences
+
+Helper functions
+================
+
+.. autosummary::
+   :toctree: generated/
+
+   fftshift - Shift the zero-frequency component to the center of the spectrum
+   ifftshift - The inverse of `fftshift`
+   fftfreq - Return the Discrete Fourier Transform sample frequencies
+   rfftfreq - DFT sample frequencies (for usage with rfft, irfft)
+   next_fast_len - Find the optimal length to zero-pad an FFT for speed
+
+Note that ``fftshift``, ``ifftshift`` and ``fftfreq`` are numpy functions
+exposed by ``fftpack``; importing them from ``numpy`` should be preferred.
+
+Convolutions (:mod:`scipy.fftpack.convolve`)
+============================================
+
+.. module:: scipy.fftpack.convolve
+
+.. autosummary::
+   :toctree: generated/
+
+   convolve
+   convolve_z
+   init_convolution_kernel
+   destroy_convolve_cache
+
+"""
+
+
+__all__ = ['fft','ifft','fftn','ifftn','rfft','irfft',
+           'fft2','ifft2',
+           'diff',
+           'tilbert','itilbert','hilbert','ihilbert',
+           'sc_diff','cs_diff','cc_diff','ss_diff',
+           'shift',
+           'fftfreq', 'rfftfreq',
+           'fftshift', 'ifftshift',
+           'next_fast_len',
+           'dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn'
+           ]
+
+from ._basic import *
+from ._pseudo_diffs import *
+from ._helper import *
+from ._realtransforms import *
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import basic, helper, pseudo_diffs, realtransforms
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/_basic.py

@@ -0,0 +1,428 @@
+"""
+Discrete Fourier Transforms - _basic.py
+"""
+# Created by Pearu Peterson, August,September 2002
+__all__ = ['fft','ifft','fftn','ifftn','rfft','irfft',
+           'fft2','ifft2']
+
+from scipy.fft import _pocketfft
+from ._helper import _good_shape
+
+
+def fft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return discrete Fourier transform of real or complex sequence.
+
+    The returned complex array contains ``y(0), y(1),..., y(n-1)``, where
+
+    ``y(j) = (x * exp(-2*pi*sqrt(-1)*j*np.arange(n)/n)).sum()``.
+
+    Parameters
+    ----------
+    x : array_like
+        Array to Fourier transform.
+    n : int, optional
+        Length of the Fourier transform. If ``n < x.shape[axis]``, `x` is
+        truncated. If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the fft's are computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    z : complex ndarray
+        with the elements::
+
+            [y(0),y(1),..,y(n/2),y(1-n/2),...,y(-1)]        if n is even
+            [y(0),y(1),..,y((n-1)/2),y(-(n-1)/2),...,y(-1)]  if n is odd
+
+        where::
+
+            y(j) = sum[k=0..n-1] x[k] * exp(-sqrt(-1)*j*k* 2*pi/n), j = 0..n-1
+
+    See Also
+    --------
+    ifft : Inverse FFT
+    rfft : FFT of a real sequence
+
+    Notes
+    -----
+    The packing of the result is "standard": If ``A = fft(a, n)``, then
+    ``A[0]`` contains the zero-frequency term, ``A[1:n/2]`` contains the
+    positive-frequency terms, and ``A[n/2:]`` contains the negative-frequency
+    terms, in order of decreasingly negative frequency. So ,for an 8-point
+    transform, the frequencies of the result are [0, 1, 2, 3, -4, -3, -2, -1].
+    To rearrange the fft output so that the zero-frequency component is
+    centered, like [-4, -3, -2, -1,  0,  1,  2,  3], use `fftshift`.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    This function is most efficient when `n` is a power of two, and least
+    efficient when `n` is prime.
+
+    Note that if ``x`` is real-valued, then ``A[j] == A[n-j].conjugate()``.
+    If ``x`` is real-valued and ``n`` is even, then ``A[n/2]`` is real.
+
+    If the data type of `x` is real, a "real FFT" algorithm is automatically
+    used, which roughly halves the computation time. To increase efficiency
+    a little further, use `rfft`, which does the same calculation, but only
+    outputs half of the symmetrical spectrum. If the data is both real and
+    symmetrical, the `dct` can again double the efficiency by generating
+    half of the spectrum from half of the signal.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft, ifft
+    >>> x = np.arange(5)
+    >>> np.allclose(fft(ifft(x)), x, atol=1e-15)  # within numerical accuracy.
+    True
+
+    """
+    return _pocketfft.fft(x, n, axis, None, overwrite_x)
+
+
+def ifft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return discrete inverse Fourier transform of real or complex sequence.
+
+    The returned complex array contains ``y(0), y(1),..., y(n-1)``, where
+
+    ``y(j) = (x * exp(2*pi*sqrt(-1)*j*np.arange(n)/n)).mean()``.
+
+    Parameters
+    ----------
+    x : array_like
+        Transformed data to invert.
+    n : int, optional
+        Length of the inverse Fourier transform.  If ``n < x.shape[axis]``,
+        `x` is truncated. If ``n > x.shape[axis]``, `x` is zero-padded.
+        The default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the ifft's are computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    ifft : ndarray of floats
+        The inverse discrete Fourier transform.
+
+    See Also
+    --------
+    fft : Forward FFT
+
+    Notes
+    -----
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    This function is most efficient when `n` is a power of two, and least
+    efficient when `n` is prime.
+
+    If the data type of `x` is real, a "real IFFT" algorithm is automatically
+    used, which roughly halves the computation time.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fft, ifft
+    >>> import numpy as np
+    >>> x = np.arange(5)
+    >>> np.allclose(ifft(fft(x)), x, atol=1e-15)  # within numerical accuracy.
+    True
+
+    """
+    return _pocketfft.ifft(x, n, axis, None, overwrite_x)
+
+
+def rfft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Discrete Fourier transform of a real sequence.
+
+    Parameters
+    ----------
+    x : array_like, real-valued
+        The data to transform.
+    n : int, optional
+        Defines the length of the Fourier transform. If `n` is not specified
+        (the default) then ``n = x.shape[axis]``. If ``n < x.shape[axis]``,
+        `x` is truncated, if ``n > x.shape[axis]``, `x` is zero-padded.
+    axis : int, optional
+        The axis along which the transform is applied. The default is the
+        last axis.
+    overwrite_x : bool, optional
+        If set to true, the contents of `x` can be overwritten. Default is
+        False.
+
+    Returns
+    -------
+    z : real ndarray
+        The returned real array contains::
+
+          [y(0),Re(y(1)),Im(y(1)),...,Re(y(n/2))]              if n is even
+          [y(0),Re(y(1)),Im(y(1)),...,Re(y(n/2)),Im(y(n/2))]   if n is odd
+
+        where::
+
+          y(j) = sum[k=0..n-1] x[k] * exp(-sqrt(-1)*j*k*2*pi/n)
+          j = 0..n-1
+
+    See Also
+    --------
+    fft, irfft, scipy.fft.rfft
+
+    Notes
+    -----
+    Within numerical accuracy, ``y == rfft(irfft(y))``.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    To get an output with a complex datatype, consider using the newer
+    function `scipy.fft.rfft`.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fft, rfft
+    >>> a = [9, -9, 1, 3]
+    >>> fft(a)
+    array([  4. +0.j,   8.+12.j,  16. +0.j,   8.-12.j])
+    >>> rfft(a)
+    array([  4.,   8.,  12.,  16.])
+
+    """
+    return _pocketfft.rfft_fftpack(x, n, axis, None, overwrite_x)
+
+
+def irfft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return inverse discrete Fourier transform of real sequence x.
+
+    The contents of `x` are interpreted as the output of the `rfft`
+    function.
+
+    Parameters
+    ----------
+    x : array_like
+        Transformed data to invert.
+    n : int, optional
+        Length of the inverse Fourier transform.
+        If n < x.shape[axis], x is truncated.
+        If n > x.shape[axis], x is zero-padded.
+        The default results in n = x.shape[axis].
+    axis : int, optional
+        Axis along which the ifft's are computed; the default is over
+        the last axis (i.e., axis=-1).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    irfft : ndarray of floats
+        The inverse discrete Fourier transform.
+
+    See Also
+    --------
+    rfft, ifft, scipy.fft.irfft
+
+    Notes
+    -----
+    The returned real array contains::
+
+        [y(0),y(1),...,y(n-1)]
+
+    where for n is even::
+
+        y(j) = 1/n (sum[k=1..n/2-1] (x[2*k-1]+sqrt(-1)*x[2*k])
+                                     * exp(sqrt(-1)*j*k* 2*pi/n)
+                    + c.c. + x[0] + (-1)**(j) x[n-1])
+
+    and for n is odd::
+
+        y(j) = 1/n (sum[k=1..(n-1)/2] (x[2*k-1]+sqrt(-1)*x[2*k])
+                                     * exp(sqrt(-1)*j*k* 2*pi/n)
+                    + c.c. + x[0])
+
+    c.c. denotes complex conjugate of preceding expression.
+
+    For details on input parameters, see `rfft`.
+
+    To process (conjugate-symmetric) frequency-domain data with a complex
+    datatype, consider using the newer function `scipy.fft.irfft`.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import rfft, irfft
+    >>> a = [1.0, 2.0, 3.0, 4.0, 5.0]
+    >>> irfft(a)
+    array([ 2.6       , -3.16405192,  1.24398433, -1.14955713,  1.46962473])
+    >>> irfft(rfft(a))
+    array([1., 2., 3., 4., 5.])
+
+    """
+    return _pocketfft.irfft_fftpack(x, n, axis, None, overwrite_x)
+
+
+def fftn(x, shape=None, axes=None, overwrite_x=False):
+    """
+    Return multidimensional discrete Fourier transform.
+
+    The returned array contains::
+
+      y[j_1,..,j_d] = sum[k_1=0..n_1-1, ..., k_d=0..n_d-1]
+         x[k_1,..,k_d] * prod[i=1..d] exp(-sqrt(-1)*2*pi/n_i * j_i * k_i)
+
+    where d = len(x.shape) and n = x.shape.
+
+    Parameters
+    ----------
+    x : array_like
+        The (N-D) array to transform.
+    shape : int or array_like of ints or None, optional
+        The shape of the result. If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        The axes of `x` (`y` if `shape` is not None) along which the
+        transform is applied.
+        The default is over all axes.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed. Default is False.
+
+    Returns
+    -------
+    y : complex-valued N-D NumPy array
+        The (N-D) DFT of the input array.
+
+    See Also
+    --------
+    ifftn
+
+    Notes
+    -----
+    If ``x`` is real-valued, then
+    ``y[..., j_i, ...] == y[..., n_i-j_i, ...].conjugate()``.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fftn, ifftn
+    >>> y = (-np.arange(16), 8 - np.arange(16), np.arange(16))
+    >>> np.allclose(y, fftn(ifftn(y)))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.fftn(x, shape, axes, None, overwrite_x)
+
+
+def ifftn(x, shape=None, axes=None, overwrite_x=False):
+    """
+    Return inverse multidimensional discrete Fourier transform.
+
+    The sequence can be of an arbitrary type.
+
+    The returned array contains::
+
+      y[j_1,..,j_d] = 1/p * sum[k_1=0..n_1-1, ..., k_d=0..n_d-1]
+         x[k_1,..,k_d] * prod[i=1..d] exp(sqrt(-1)*2*pi/n_i * j_i * k_i)
+
+    where ``d = len(x.shape)``, ``n = x.shape``, and ``p = prod[i=1..d] n_i``.
+
+    For description of parameters see `fftn`.
+
+    See Also
+    --------
+    fftn : for detailed information.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fftn, ifftn
+    >>> import numpy as np
+    >>> y = (-np.arange(16), 8 - np.arange(16), np.arange(16))
+    >>> np.allclose(y, ifftn(fftn(y)))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.ifftn(x, shape, axes, None, overwrite_x)
+
+
+def fft2(x, shape=None, axes=(-2,-1), overwrite_x=False):
+    """
+    2-D discrete Fourier transform.
+
+    Return the 2-D discrete Fourier transform of the 2-D argument
+    `x`.
+
+    See Also
+    --------
+    fftn : for detailed information.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft2, ifft2
+    >>> y = np.mgrid[:5, :5][0]
+    >>> y
+    array([[0, 0, 0, 0, 0],
+           [1, 1, 1, 1, 1],
+           [2, 2, 2, 2, 2],
+           [3, 3, 3, 3, 3],
+           [4, 4, 4, 4, 4]])
+    >>> np.allclose(y, ifft2(fft2(y)))
+    True
+    """
+    return fftn(x,shape,axes,overwrite_x)
+
+
+def ifft2(x, shape=None, axes=(-2,-1), overwrite_x=False):
+    """
+    2-D discrete inverse Fourier transform of real or complex sequence.
+
+    Return inverse 2-D discrete Fourier transform of
+    arbitrary type sequence x.
+
+    See `ifft` for more information.
+
+    See Also
+    --------
+    fft2, ifft
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft2, ifft2
+    >>> y = np.mgrid[:5, :5][0]
+    >>> y
+    array([[0, 0, 0, 0, 0],
+           [1, 1, 1, 1, 1],
+           [2, 2, 2, 2, 2],
+           [3, 3, 3, 3, 3],
+           [4, 4, 4, 4, 4]])
+    >>> np.allclose(y, fft2(ifft2(y)))
+    True
+
+    """
+    return ifftn(x,shape,axes,overwrite_x)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/_helper.py

@@ -0,0 +1,115 @@
+import operator
+
+import numpy as np
+from numpy.fft import fftshift, ifftshift, fftfreq
+
+import scipy.fft._pocketfft.helper as _helper
+
+__all__ = ['fftshift', 'ifftshift', 'fftfreq', 'rfftfreq', 'next_fast_len']
+
+
+def rfftfreq(n, d=1.0):
+    """DFT sample frequencies (for usage with rfft, irfft).
+
+    The returned float array contains the frequency bins in
+    cycles/unit (with zero at the start) given a window length `n` and a
+    sample spacing `d`::
+
+      f = [0,1,1,2,2,...,n/2-1,n/2-1,n/2]/(d*n)   if n is even
+      f = [0,1,1,2,2,...,n/2-1,n/2-1,n/2,n/2]/(d*n)   if n is odd
+
+    Parameters
+    ----------
+    n : int
+        Window length.
+    d : scalar, optional
+        Sample spacing. Default is 1.
+
+    Returns
+    -------
+    out : ndarray
+        The array of length `n`, containing the sample frequencies.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy import fftpack
+    >>> sig = np.array([-2, 8, 6, 4, 1, 0, 3, 5], dtype=float)
+    >>> sig_fft = fftpack.rfft(sig)
+    >>> n = sig_fft.size
+    >>> timestep = 0.1
+    >>> freq = fftpack.rfftfreq(n, d=timestep)
+    >>> freq
+    array([ 0.  ,  1.25,  1.25,  2.5 ,  2.5 ,  3.75,  3.75,  5.  ])
+
+    """
+    n = operator.index(n)
+    if n < 0:
+        raise ValueError(f"n = {n} is not valid. "
+                         "n must be a nonnegative integer.")
+
+    return (np.arange(1, n + 1, dtype=int) // 2) / float(n * d)
+
+
+def next_fast_len(target):
+    """
+    Find the next fast size of input data to `fft`, for zero-padding, etc.
+
+    SciPy's FFTPACK has efficient functions for radix {2, 3, 4, 5}, so this
+    returns the next composite of the prime factors 2, 3, and 5 which is
+    greater than or equal to `target`. (These are also known as 5-smooth
+    numbers, regular numbers, or Hamming numbers.)
+
+    Parameters
+    ----------
+    target : int
+        Length to start searching from. Must be a positive integer.
+
+    Returns
+    -------
+    out : int
+        The first 5-smooth number greater than or equal to `target`.
+
+    Notes
+    -----
+    .. versionadded:: 0.18.0
+
+    Examples
+    --------
+    On a particular machine, an FFT of prime length takes 133 ms:
+
+    >>> from scipy import fftpack
+    >>> import numpy as np
+    >>> rng = np.random.default_rng()
+    >>> min_len = 10007  # prime length is worst case for speed
+    >>> a = rng.standard_normal(min_len)
+    >>> b = fftpack.fft(a)
+
+    Zero-padding to the next 5-smooth length reduces computation time to
+    211 us, a speedup of 630 times:
+
+    >>> fftpack.next_fast_len(min_len)
+    10125
+    >>> b = fftpack.fft(a, 10125)
+
+    Rounding up to the next power of 2 is not optimal, taking 367 us to
+    compute, 1.7 times as long as the 5-smooth size:
+
+    >>> b = fftpack.fft(a, 16384)
+
+    """
+    # Real transforms use regular sizes so this is backwards compatible
+    return _helper.good_size(target, True)
+
+
+def _good_shape(x, shape, axes):
+    """Ensure that shape argument is valid for scipy.fftpack
+
+    scipy.fftpack does not support len(shape) < x.ndim when axes is not given.
+    """
+    if shape is not None and axes is None:
+        shape = _helper._iterable_of_int(shape, 'shape')
+        if len(shape) != np.ndim(x):
+            raise ValueError("when given, axes and shape arguments"
+                             " have to be of the same length")
+    return shape

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/_pseudo_diffs.py

@@ -0,0 +1,554 @@
+"""
+Differential and pseudo-differential operators.
+"""
+# Created by Pearu Peterson, September 2002
+
+__all__ = ['diff',
+           'tilbert','itilbert','hilbert','ihilbert',
+           'cs_diff','cc_diff','sc_diff','ss_diff',
+           'shift']
+
+import threading
+
+from numpy import pi, asarray, sin, cos, sinh, cosh, tanh, iscomplexobj
+from . import convolve
+
+from scipy.fft._pocketfft.helper import _datacopied
+
+
+_cache = threading.local()
+
+
+def diff(x,order=1,period=None, _cache=_cache):
+    """
+    Return kth derivative (or integral) of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = pow(sqrt(-1)*j*2*pi/period, order) * x_j
+      y_0 = 0 if order is not 0.
+
+    Parameters
+    ----------
+    x : array_like
+        Input array.
+    order : int, optional
+        The order of differentiation. Default order is 1. If order is
+        negative, then integration is carried out under the assumption
+        that ``x_0 == 0``.
+    period : float, optional
+        The assumed period of the sequence. Default is ``2*pi``.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) = 0`` then ``diff(diff(x, k), -k) == x`` (within
+    numerical accuracy).
+
+    For odd order and even ``len(x)``, the Nyquist mode is taken zero.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'diff_cache'):
+            _cache.diff_cache = {}
+        _cache = _cache.diff_cache
+
+    tmp = asarray(x)
+    if order == 0:
+        return tmp
+    if iscomplexobj(tmp):
+        return diff(tmp.real, order, period, _cache)+1j*diff(
+            tmp.imag, order, period, _cache)
+    if period is not None:
+        c = 2*pi/period
+    else:
+        c = 1.0
+    n = len(x)
+    omega = _cache.get((n,order,c))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,order=order,c=c):
+            if k:
+                return pow(c*k,order)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=order,
+                                                 zero_nyquist=1)
+        _cache[(n,order,c)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=order % 2,
+                             overwrite_x=overwrite_x)
+
+
+def tilbert(x, h, period=None, _cache=_cache):
+    """
+    Return h-Tilbert transform of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+        y_j = sqrt(-1)*coth(j*h*2*pi/period) * x_j
+        y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The input array to transform.
+    h : float
+        Defines the parameter of the Tilbert transform.
+    period : float, optional
+        The assumed period of the sequence. Default period is ``2*pi``.
+
+    Returns
+    -------
+    tilbert : ndarray
+        The result of the transform.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) == 0`` and ``n = len(x)`` is odd, then
+    ``tilbert(itilbert(x)) == x``.
+
+    If ``2 * pi * h / period`` is approximately 10 or larger, then
+    numerically ``tilbert == hilbert``
+    (theoretically oo-Tilbert == Hilbert).
+
+    For even ``len(x)``, the Nyquist mode of ``x`` is taken zero.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'tilbert_cache'):
+            _cache.tilbert_cache = {}
+        _cache = _cache.tilbert_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return tilbert(tmp.real, h, period, _cache) + \
+               1j * tilbert(tmp.imag, h, period, _cache)
+
+    if period is not None:
+        h = h * 2 * pi / period
+
+    n = len(x)
+    omega = _cache.get((n, h))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k, h=h):
+            if k:
+                return 1.0/tanh(h*k)
+
+            return 0
+
+        omega = convolve.init_convolution_kernel(n, kernel, d=1)
+        _cache[(n,h)] = omega
+
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+def itilbert(x,h,period=None, _cache=_cache):
+    """
+    Return inverse h-Tilbert transform of a periodic sequence x.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*tanh(j*h*2*pi/period) * x_j
+      y_0 = 0
+
+    For more details, see `tilbert`.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'itilbert_cache'):
+            _cache.itilbert_cache = {}
+        _cache = _cache.itilbert_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return itilbert(tmp.real, h, period, _cache) + \
+               1j*itilbert(tmp.imag, h, period, _cache)
+    if period is not None:
+        h = h*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,h))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,h=h):
+            if k:
+                return -tanh(h*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,h)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+def hilbert(x, _cache=_cache):
+    """
+    Return Hilbert transform of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sqrt(-1)*sign(j) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The input array, should be periodic.
+    _cache : dict, optional
+        Dictionary that contains the kernel used to do a convolution with.
+
+    Returns
+    -------
+    y : ndarray
+        The transformed input.
+
+    See Also
+    --------
+    scipy.signal.hilbert : Compute the analytic signal, using the Hilbert
+                           transform.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) == 0`` then ``hilbert(ihilbert(x)) == x``.
+
+    For even len(x), the Nyquist mode of x is taken zero.
+
+    The sign of the returned transform does not have a factor -1 that is more
+    often than not found in the definition of the Hilbert transform. Note also
+    that `scipy.signal.hilbert` does have an extra -1 factor compared to this
+    function.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'hilbert_cache'):
+            _cache.hilbert_cache = {}
+        _cache = _cache.hilbert_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return hilbert(tmp.real, _cache) + 1j * hilbert(tmp.imag, _cache)
+    n = len(x)
+    omega = _cache.get(n)
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k):
+            if k > 0:
+                return 1.0
+            elif k < 0:
+                return -1.0
+            return 0.0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[n] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+def ihilbert(x, _cache=_cache):
+    """
+    Return inverse Hilbert transform of a periodic sequence x.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*sign(j) * x_j
+      y_0 = 0
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'ihilbert_cache'):
+            _cache.ihilbert_cache = {}
+        _cache = _cache.ihilbert_cache
+    return -hilbert(x, _cache)
+
+
+def cs_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-cosh/sinh pseudo-derivative of a periodic sequence.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*cosh(j*a*2*pi/period)/sinh(j*b*2*pi/period) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a, b : float
+        Defines the parameters of the cosh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence. Default period is ``2*pi``.
+
+    Returns
+    -------
+    cs_diff : ndarray
+        Pseudo-derivative of periodic sequence `x`.
+
+    Notes
+    -----
+    For even len(`x`), the Nyquist mode of `x` is taken as zero.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'cs_diff_cache'):
+            _cache.cs_diff_cache = {}
+        _cache = _cache.cs_diff_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return cs_diff(tmp.real, a, b, period, _cache) + \
+               1j*cs_diff(tmp.imag, a, b, period, _cache)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return -cosh(a*k)/sinh(b*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+def sc_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-sinh/cosh pseudo-derivative of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sqrt(-1)*sinh(j*a*2*pi/period)/cosh(j*b*2*pi/period) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        Input array.
+    a,b : float
+        Defines the parameters of the sinh/cosh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is 2*pi.
+
+    Notes
+    -----
+    ``sc_diff(cs_diff(x,a,b),b,a) == x``
+    For even ``len(x)``, the Nyquist mode of x is taken as zero.
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'sc_diff_cache'):
+            _cache.sc_diff_cache = {}
+        _cache = _cache.sc_diff_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return sc_diff(tmp.real, a, b, period, _cache) + \
+               1j * sc_diff(tmp.imag, a, b, period, _cache)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return sinh(a*k)/cosh(b*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+def ss_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-sinh/sinh pseudo-derivative of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sinh(j*a*2*pi/period)/sinh(j*b*2*pi/period) * x_j
+      y_0 = a/b * x_0
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a,b
+        Defines the parameters of the sinh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is ``2*pi``.
+
+    Notes
+    -----
+    ``ss_diff(ss_diff(x,a,b),b,a) == x``
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'ss_diff_cache'):
+            _cache.ss_diff_cache = {}
+        _cache = _cache.ss_diff_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return ss_diff(tmp.real, a, b, period, _cache) + \
+               1j*ss_diff(tmp.imag, a, b, period, _cache)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return sinh(a*k)/sinh(b*k)
+            return float(a)/b
+        omega = convolve.init_convolution_kernel(n,kernel)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,overwrite_x=overwrite_x)
+
+
+def cc_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-cosh/cosh pseudo-derivative of a periodic sequence.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = cosh(j*a*2*pi/period)/cosh(j*b*2*pi/period) * x_j
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a,b : float
+        Defines the parameters of the sinh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is ``2*pi``.
+
+    Returns
+    -------
+    cc_diff : ndarray
+        Pseudo-derivative of periodic sequence `x`.
+
+    Notes
+    -----
+    ``cc_diff(cc_diff(x,a,b),b,a) == x``
+
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'cc_diff_cache'):
+            _cache.cc_diff_cache = {}
+        _cache = _cache.cc_diff_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return cc_diff(tmp.real, a, b, period, _cache) + \
+               1j * cc_diff(tmp.imag, a, b, period, _cache)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            return cosh(a*k)/cosh(b*k)
+        omega = convolve.init_convolution_kernel(n,kernel)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,overwrite_x=overwrite_x)
+
+
+def shift(x, a, period=None, _cache=_cache):
+    """
+    Shift periodic sequence x by a: y(u) = x(u+a).
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+          y_j = exp(j*a*2*pi/period*sqrt(-1)) * x_f
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a : float
+        Defines the parameters of the sinh/sinh pseudo-differential
+    period : float, optional
+        The period of the sequences x and y. Default period is ``2*pi``.
+    """
+    if isinstance(_cache, threading.local):
+        if not hasattr(_cache, 'shift_cache'):
+            _cache.shift_cache = {}
+        _cache = _cache.shift_cache
+
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return shift(tmp.real, a, period, _cache) + 1j * shift(
+            tmp.imag, a, period, _cache)
+    if period is not None:
+        a = a*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel_real(k,a=a):
+            return cos(a*k)
+
+        def kernel_imag(k,a=a):
+            return sin(a*k)
+        omega_real = convolve.init_convolution_kernel(n,kernel_real,d=0,
+                                                      zero_nyquist=0)
+        omega_imag = convolve.init_convolution_kernel(n,kernel_imag,d=1,
+                                                      zero_nyquist=0)
+        _cache[(n,a)] = omega_real,omega_imag
+    else:
+        omega_real,omega_imag = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve_z(tmp,omega_real,omega_imag,
+                               overwrite_x=overwrite_x)
+

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/_realtransforms.py

@@ -0,0 +1,598 @@
+"""
+Real spectrum transforms (DCT, DST, MDCT)
+"""
+
+__all__ = ['dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn']
+
+from scipy.fft import _pocketfft
+from ._helper import _good_shape
+
+_inverse_typemap = {1: 1, 2: 3, 3: 2, 4: 4}
+
+
+def dctn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Cosine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result. If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the DCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idctn : Inverse multidimensional DCT
+
+    Notes
+    -----
+    For full details of the DCT types and normalization modes, as well as
+    references, see `dct`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dctn, idctn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idctn(dctn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dctn(x, type, shape, axes, norm, overwrite_x)
+
+
+def idctn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Cosine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the IDCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dctn : multidimensional DCT
+
+    Notes
+    -----
+    For full details of the IDCT types and normalization modes, as well as
+    references, see `idct`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dctn, idctn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idctn(dctn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    type = _inverse_typemap[type]
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dctn(x, type, shape, axes, norm, overwrite_x)
+
+
+def dstn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Sine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the DCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idstn : Inverse multidimensional DST
+
+    Notes
+    -----
+    For full details of the DST types and normalization modes, as well as
+    references, see `dst`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dstn, idstn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idstn(dstn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dstn(x, type, shape, axes, norm, overwrite_x)
+
+
+def idstn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Sine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the IDST is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dstn : multidimensional DST
+
+    Notes
+    -----
+    For full details of the IDST types and normalization modes, as well as
+    references, see `idst`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dstn, idstn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idstn(dstn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    type = _inverse_typemap[type]
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dstn(x, type, shape, axes, norm, overwrite_x)
+
+
+def dct(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    r"""
+    Return the Discrete Cosine Transform of arbitrary type sequence x.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the dct is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idct : Inverse DCT
+
+    Notes
+    -----
+    For a single dimension array ``x``, ``dct(x, norm='ortho')`` is equal to
+    MATLAB ``dct(x)``.
+
+    There are, theoretically, 8 types of the DCT, only the first 4 types are
+    implemented in scipy. 'The' DCT generally refers to DCT type 2, and 'the'
+    Inverse DCT generally refers to DCT type 3.
+
+    **Type I**
+
+    There are several definitions of the DCT-I; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = x_0 + (-1)^k x_{N-1} + 2 \sum_{n=1}^{N-2} x_n \cos\left(
+       \frac{\pi k n}{N-1} \right)
+
+    If ``norm='ortho'``, ``x[0]`` and ``x[N-1]`` are multiplied by a scaling
+    factor of :math:`\sqrt{2}`, and ``y[k]`` is multiplied by a scaling factor
+    ``f``
+
+    .. math::
+
+        f = \begin{cases}
+         \frac{1}{2}\sqrt{\frac{1}{N-1}} & \text{if }k=0\text{ or }N-1, \\
+         \frac{1}{2}\sqrt{\frac{2}{N-1}} & \text{otherwise} \end{cases}
+
+    .. versionadded:: 1.2.0
+       Orthonormalization in DCT-I.
+
+    .. note::
+       The DCT-I is only supported for input size > 1.
+
+    **Type II**
+
+    There are several definitions of the DCT-II; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = 2 \sum_{n=0}^{N-1} x_n \cos\left(\frac{\pi k(2n+1)}{2N} \right)
+
+    If ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+       f = \begin{cases}
+       \sqrt{\frac{1}{4N}} & \text{if }k=0, \\
+       \sqrt{\frac{1}{2N}} & \text{otherwise} \end{cases}
+
+    which makes the corresponding matrix of coefficients orthonormal
+    (``O @ O.T = np.eye(N)``).
+
+    **Type III**
+
+    There are several definitions, we use the following (for ``norm=None``)
+
+    .. math::
+
+       y_k = x_0 + 2 \sum_{n=1}^{N-1} x_n \cos\left(\frac{\pi(2k+1)n}{2N}\right)
+
+    or, for ``norm='ortho'``
+
+    .. math::
+
+       y_k = \frac{x_0}{\sqrt{N}} + \sqrt{\frac{2}{N}} \sum_{n=1}^{N-1} x_n
+       \cos\left(\frac{\pi(2k+1)n}{2N}\right)
+
+    The (unnormalized) DCT-III is the inverse of the (unnormalized) DCT-II, up
+    to a factor ``2N``. The orthonormalized DCT-III is exactly the inverse of
+    the orthonormalized DCT-II.
+
+    **Type IV**
+
+    There are several definitions of the DCT-IV; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = 2 \sum_{n=0}^{N-1} x_n \cos\left(\frac{\pi(2k+1)(2n+1)}{4N} \right)
+
+    If ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+
+        f = \frac{1}{\sqrt{2N}}
+
+    .. versionadded:: 1.2.0
+       Support for DCT-IV.
+
+    References
+    ----------
+    .. [1] 'A Fast Cosine Transform in One and Two Dimensions', by J.
+           Makhoul, `IEEE Transactions on acoustics, speech and signal
+           processing` vol. 28(1), pp. 27-34,
+           :doi:`10.1109/TASSP.1980.1163351` (1980).
+    .. [2] Wikipedia, "Discrete cosine transform",
+           https://en.wikipedia.org/wiki/Discrete_cosine_transform
+
+    Examples
+    --------
+    The Type 1 DCT is equivalent to the FFT (though faster) for real,
+    even-symmetrical inputs. The output is also real and even-symmetrical.
+    Half of the FFT input is used to generate half of the FFT output:
+
+    >>> from scipy.fftpack import fft, dct
+    >>> import numpy as np
+    >>> fft(np.array([4., 3., 5., 10., 5., 3.])).real
+    array([ 30.,  -8.,   6.,  -2.,   6.,  -8.])
+    >>> dct(np.array([4., 3., 5., 10.]), 1)
+    array([ 30.,  -8.,   6.,  -2.])
+
+    """
+    return _pocketfft.dct(x, type, n, axis, norm, overwrite_x)
+
+
+def idct(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    """
+    Return the Inverse Discrete Cosine Transform of an arbitrary type sequence.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the idct is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    idct : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dct : Forward DCT
+
+    Notes
+    -----
+    For a single dimension array `x`, ``idct(x, norm='ortho')`` is equal to
+    MATLAB ``idct(x)``.
+
+    'The' IDCT is the IDCT of type 2, which is the same as DCT of type 3.
+
+    IDCT of type 1 is the DCT of type 1, IDCT of type 2 is the DCT of type
+    3, and IDCT of type 3 is the DCT of type 2. IDCT of type 4 is the DCT
+    of type 4. For the definition of these types, see `dct`.
+
+    Examples
+    --------
+    The Type 1 DCT is equivalent to the DFT for real, even-symmetrical
+    inputs. The output is also real and even-symmetrical. Half of the IFFT
+    input is used to generate half of the IFFT output:
+
+    >>> from scipy.fftpack import ifft, idct
+    >>> import numpy as np
+    >>> ifft(np.array([ 30.,  -8.,   6.,  -2.,   6.,  -8.])).real
+    array([  4.,   3.,   5.,  10.,   5.,   3.])
+    >>> idct(np.array([ 30.,  -8.,   6.,  -2.]), 1) / 6
+    array([  4.,   3.,   5.,  10.])
+
+    """
+    type = _inverse_typemap[type]
+    return _pocketfft.dct(x, type, n, axis, norm, overwrite_x)
+
+
+def dst(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    r"""
+    Return the Discrete Sine Transform of arbitrary type sequence x.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the dst is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    dst : ndarray of reals
+        The transformed input array.
+
+    See Also
+    --------
+    idst : Inverse DST
+
+    Notes
+    -----
+    For a single dimension array ``x``.
+
+    There are, theoretically, 8 types of the DST for different combinations of
+    even/odd boundary conditions and boundary off sets [1]_, only the first
+    4 types are implemented in scipy.
+
+    **Type I**
+
+    There are several definitions of the DST-I; we use the following
+    for ``norm=None``. DST-I assumes the input is odd around `n=-1` and `n=N`.
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(k+1)(n+1)}{N+1}\right)
+
+    Note that the DST-I is only supported for input size > 1.
+    The (unnormalized) DST-I is its own inverse, up to a factor ``2(N+1)``.
+    The orthonormalized DST-I is exactly its own inverse.
+
+    **Type II**
+
+    There are several definitions of the DST-II; we use the following for
+    ``norm=None``. DST-II assumes the input is odd around `n=-1/2` and
+    `n=N-1/2`; the output is odd around :math:`k=-1` and even around `k=N-1`
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(k+1)(2n+1)}{2N}\right)
+
+    if ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+
+        f = \begin{cases}
+        \sqrt{\frac{1}{4N}} & \text{if }k = 0, \\
+        \sqrt{\frac{1}{2N}} & \text{otherwise} \end{cases}
+
+    **Type III**
+
+    There are several definitions of the DST-III, we use the following (for
+    ``norm=None``). DST-III assumes the input is odd around `n=-1` and even
+    around `n=N-1`
+
+    .. math::
+
+        y_k = (-1)^k x_{N-1} + 2 \sum_{n=0}^{N-2} x_n \sin\left(
+        \frac{\pi(2k+1)(n+1)}{2N}\right)
+
+    The (unnormalized) DST-III is the inverse of the (unnormalized) DST-II, up
+    to a factor ``2N``. The orthonormalized DST-III is exactly the inverse of the
+    orthonormalized DST-II.
+
+    .. versionadded:: 0.11.0
+
+    **Type IV**
+
+    There are several definitions of the DST-IV, we use the following (for
+    ``norm=None``). DST-IV assumes the input is odd around `n=-0.5` and even
+    around `n=N-0.5`
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(2k+1)(2n+1)}{4N}\right)
+
+    The (unnormalized) DST-IV is its own inverse, up to a factor ``2N``. The
+    orthonormalized DST-IV is exactly its own inverse.
+
+    .. versionadded:: 1.2.0
+       Support for DST-IV.
+
+    References
+    ----------
+    .. [1] Wikipedia, "Discrete sine transform",
+           https://en.wikipedia.org/wiki/Discrete_sine_transform
+
+    """
+    return _pocketfft.dst(x, type, n, axis, norm, overwrite_x)
+
+
+def idst(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    """
+    Return the Inverse Discrete Sine Transform of an arbitrary type sequence.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated. If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the idst is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    idst : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dst : Forward DST
+
+    Notes
+    -----
+    'The' IDST is the IDST of type 2, which is the same as DST of type 3.
+
+    IDST of type 1 is the DST of type 1, IDST of type 2 is the DST of type
+    3, and IDST of type 3 is the DST of type 2. For the definition of these
+    types, see `dst`.
+
+    .. versionadded:: 0.11.0
+
+    """
+    type = _inverse_typemap[type]
+    return _pocketfft.dst(x, type, n, axis, norm, overwrite_x)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/basic.py

@@ -0,0 +1,20 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'fft','ifft','fftn','ifftn','rfft','irfft',
+    'fft2','ifft2'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="basic",
+                                   private_modules=["_basic"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/helper.py

@@ -0,0 +1,19 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'fftshift', 'ifftshift', 'fftfreq', 'rfftfreq', 'next_fast_len'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="helper",
+                                   private_modules=["_helper"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/pseudo_diffs.py

@@ -0,0 +1,22 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'diff',
+    'tilbert', 'itilbert', 'hilbert', 'ihilbert',
+    'cs_diff', 'cc_diff', 'sc_diff', 'ss_diff',
+    'shift', 'convolve'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="pseudo_diffs",
+                                   private_modules=["_pseudo_diffs"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/fftpack/realtransforms.py

@@ -0,0 +1,19 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="realtransforms",
+                                   private_modules=["_realtransforms"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_bsplines.py

@@ -0,0 +1,2614 @@
+import operator
+from math import prod
+from types import GenericAlias
+
+import numpy as np
+from scipy._lib._util import normalize_axis_index
+from scipy.linalg import (get_lapack_funcs, LinAlgError,
+                          cholesky_banded, cho_solve_banded,
+                          solve, solve_banded)
+from scipy.optimize import minimize_scalar
+from . import _dierckx
+from . import _fitpack_impl
+from scipy.sparse import csr_array
+from scipy.special import poch
+from itertools import combinations
+
+from scipy._lib._array_api import array_namespace, concat_1d, xp_capabilities
+
+__all__ = ["BSpline", "make_interp_spline", "make_lsq_spline",
+           "make_smoothing_spline"]
+
+
+def _get_dtype(dtype):
+    """Return np.complex128 for complex dtypes, np.float64 otherwise."""
+    if np.issubdtype(dtype, np.complexfloating):
+        return np.complex128
+    else:
+        return np.float64
+
+
+def _as_float_array(x, check_finite=False):
+    """Convert the input into a C contiguous float array.
+
+    NB: Upcasts half- and single-precision floats to double precision.
+    """
+    x = np.ascontiguousarray(x)
+    dtyp = _get_dtype(x.dtype)
+    x = x.astype(dtyp, copy=False)
+    if check_finite and not np.isfinite(x).all():
+        raise ValueError("Array must not contain infs or nans.")
+    return x
+
+
+def _dual_poly(j, k, t, y):
+    """
+    Dual polynomial of the B-spline B_{j,k,t} -
+    polynomial which is associated with B_{j,k,t}:
+    $p_{j,k}(y) = (y - t_{j+1})(y - t_{j+2})...(y - t_{j+k})$
+    """
+    if k == 0:
+        return 1
+    return np.prod([(y - t[j + i]) for i in range(1, k + 1)])
+
+
+def _diff_dual_poly(j, k, y, d, t):
+    """
+    d-th derivative of the dual polynomial $p_{j,k}(y)$
+    """
+    if d == 0:
+        return _dual_poly(j, k, t, y)
+    if d == k:
+        return poch(1, k)
+    comb = list(combinations(range(j + 1, j + k + 1), d))
+    res = 0
+    for i in range(len(comb) * len(comb[0])):
+        res += np.prod([(y - t[j + p]) for p in range(1, k + 1)
+                        if (j + p) not in comb[i//d]])
+    return res
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class BSpline:
+    r"""Univariate spline in the B-spline basis.
+
+    .. math::
+
+        S(x) = \sum_{j=0}^{n-1} c_j  B_{j, k; t}(x)
+
+    where :math:`B_{j, k; t}` are B-spline basis functions of degree `k`
+    and knots `t`.
+
+    Parameters
+    ----------
+    t : ndarray, shape (n+k+1,)
+        knots
+    c : ndarray, shape (>=n, ...)
+        spline coefficients
+    k : int
+        B-spline degree
+    extrapolate : bool or 'periodic', optional
+        whether to extrapolate beyond the base interval, ``t[k] .. t[n]``,
+        or to return nans.
+        If True, extrapolates the first and last polynomial pieces of b-spline
+        functions active on the base interval.
+        If 'periodic', periodic extrapolation is used.
+        Default is True.
+    axis : int, optional
+        Interpolation axis. Default is zero.
+
+    Attributes
+    ----------
+    t : ndarray
+        knot vector
+    c : ndarray
+        spline coefficients
+    k : int
+        spline degree
+    extrapolate : bool
+        If True, extrapolates the first and last polynomial pieces of b-spline
+        functions active on the base interval.
+    axis : int
+        Interpolation axis.
+    tck : tuple
+        A read-only equivalent of ``(self.t, self.c, self.k)``
+
+    Methods
+    -------
+    __call__
+    basis_element
+    derivative
+    antiderivative
+    integrate
+    insert_knot
+    construct_fast
+    design_matrix
+    from_power_basis
+
+    Notes
+    -----
+    B-spline basis elements are defined via
+
+    .. math::
+
+        B_{i, 0}(x) = 1, \textrm{if $t_i \le x < t_{i+1}$, otherwise $0$,}
+
+        B_{i, k}(x) = \frac{x - t_i}{t_{i+k} - t_i} B_{i, k-1}(x)
+                 + \frac{t_{i+k+1} - x}{t_{i+k+1} - t_{i+1}} B_{i+1, k-1}(x)
+
+    **Implementation details**
+
+    - At least ``k+1`` coefficients are required for a spline of degree `k`,
+      so that ``n >= k+1``. Additional coefficients, ``c[j]`` with
+      ``j > n``, are ignored.
+
+    - B-spline basis elements of degree `k` form a partition of unity on the
+      *base interval*, ``t[k] <= x <= t[n]``.
+
+
+    Examples
+    --------
+    Translating the recursive definition of B-splines into Python code, we have:
+
+    >>> def B(x, k, i, t):
+    ...    if k == 0:
+    ...       return 1.0 if t[i] <= x < t[i+1] else 0.0
+    ...    if t[i+k] == t[i]:
+    ...       c1 = 0.0
+    ...    else:
+    ...       c1 = (x - t[i])/(t[i+k] - t[i]) * B(x, k-1, i, t)
+    ...    if t[i+k+1] == t[i+1]:
+    ...       c2 = 0.0
+    ...    else:
+    ...       c2 = (t[i+k+1] - x)/(t[i+k+1] - t[i+1]) * B(x, k-1, i+1, t)
+    ...    return c1 + c2
+
+    >>> def bspline(x, t, c, k):
+    ...    n = len(t) - k - 1
+    ...    assert (n >= k+1) and (len(c) >= n)
+    ...    return sum(c[i] * B(x, k, i, t) for i in range(n))
+
+    Note that this is an inefficient (if straightforward) way to
+    evaluate B-splines --- this spline class does it in an equivalent,
+    but much more efficient way.
+
+    Here we construct a quadratic spline function on the base interval
+    ``2 <= x <= 4`` and compare with the naive way of evaluating the spline:
+
+    >>> from scipy.interpolate import BSpline
+    >>> k = 2
+    >>> t = [0, 1, 2, 3, 4, 5, 6]
+    >>> c = [-1, 2, 0, -1]
+    >>> spl = BSpline(t, c, k)
+    >>> spl(2.5)
+    array(1.375)
+    >>> bspline(2.5, t, c, k)
+    1.375
+
+    Note that outside of the base interval results differ. This is because
+    `BSpline` extrapolates the first and last polynomial pieces of B-spline
+    functions active on the base interval.
+
+    >>> import matplotlib.pyplot as plt
+    >>> import numpy as np
+    >>> fig, ax = plt.subplots()
+    >>> xx = np.linspace(1.5, 4.5, 50)
+    >>> ax.plot(xx, [bspline(x, t, c ,k) for x in xx], 'r-', lw=3, label='naive')
+    >>> ax.plot(xx, spl(xx), 'b-', lw=4, alpha=0.7, label='BSpline')
+    >>> ax.grid(True)
+    >>> ax.legend(loc='best')
+    >>> plt.show()
+
+
+    References
+    ----------
+    .. [1] Tom Lyche and Knut Morken, Spline methods,
+        http://www.uio.no/studier/emner/matnat/ifi/INF-MAT5340/v05/undervisningsmateriale/
+    .. [2] Carl de Boor, A practical guide to splines, Springer, 2001.
+
+    """
+
+    # generic type compatibility with scipy-stubs
+    __class_getitem__ = classmethod(GenericAlias)
+
+
+    def __init__(self, t, c, k, extrapolate=True, axis=0):
+        super().__init__()
+
+        self._asarray = array_namespace(c, t).asarray
+
+        self.k = operator.index(k)
+        self._c = np.asarray(c)
+        self._t = np.ascontiguousarray(t, dtype=np.float64)
+
+        if extrapolate == 'periodic':
+            self.extrapolate = extrapolate
+        else:
+            self.extrapolate = bool(extrapolate)
+
+        n = self._t.shape[0] - self.k - 1
+
+        axis = normalize_axis_index(axis, self._c.ndim)
+
+        # Note that the normalized axis is stored in the object.
+        self.axis = axis
+        if axis != 0:
+            # roll the interpolation axis to be the first one in self.c
+            # More specifically, the target shape for self.c is (n, ...),
+            # and axis !=0 means that we have c.shape (..., n, ...)
+            #                                               ^
+            #                                              axis
+            self._c = np.moveaxis(self._c, axis, 0)
+
+        if k < 0:
+            raise ValueError("Spline order cannot be negative.")
+        if self._t.ndim != 1:
+            raise ValueError("Knot vector must be one-dimensional.")
+        if n < self.k + 1:
+            raise ValueError(f"Need at least {2*k + 2} knots for degree {k}")
+        if (np.diff(self._t) < 0).any():
+            raise ValueError("Knots must be in a non-decreasing order.")
+        if len(np.unique(self._t[k:n+1])) < 2:
+            raise ValueError("Need at least two internal knots.")
+        if not np.isfinite(self._t).all():
+            raise ValueError("Knots should not have nans or infs.")
+        if self._c.ndim < 1:
+            raise ValueError("Coefficients must be at least 1-dimensional.")
+        if self._c.shape[0] < n:
+            raise ValueError("Knots, coefficients and degree are inconsistent.")
+
+        dt = _get_dtype(self._c.dtype)
+
+        self._c = np.ascontiguousarray(self._c, dtype=dt)
+
+    @classmethod
+    def construct_fast(cls, t, c, k, extrapolate=True, axis=0):
+        """Construct a spline without making checks.
+
+        Accepts same parameters as the regular constructor. Input arrays
+        `t` and `c` must of correct shape and dtype.
+        """
+        self = object.__new__(cls)
+        self._t, self._c, self.k = np.asarray(t), np.asarray(c), k
+        self.extrapolate = extrapolate
+        self.axis = axis
+        self._asarray = array_namespace(t, c).asarray
+        return self
+
+    @property
+    def tck(self):
+        """Equivalent to ``(self.t, self.c, self.k)`` (read-only).
+        """
+        return self.t, self.c, self.k
+
+    # Under the hood, self._c and self._t are always saved as numpy array
+    # because they are used in a C extension expecting numpy arrays.
+    @property
+    def t(self):
+        return self._asarray(self._t)
+
+    @t.setter
+    def t(self, t):
+        self._t = np.asarray(t)
+
+    @property
+    def c(self):
+        return self._asarray(self._c)
+
+    @c.setter
+    def c(self, c):
+        self._c = np.asarray(c)
+
+    @classmethod
+    def basis_element(cls, t, extrapolate=True):
+        """Return a B-spline basis element ``B(x | t[0], ..., t[k+1])``.
+
+        Parameters
+        ----------
+        t : ndarray, shape (k+2,)
+            internal knots
+        extrapolate : bool or 'periodic', optional
+            whether to extrapolate beyond the base interval, ``t[0] .. t[k+1]``,
+            or to return nans.
+            If 'periodic', periodic extrapolation is used.
+            Default is True.
+
+        Returns
+        -------
+        basis_element : callable
+            A callable representing a B-spline basis element for the knot
+            vector `t`.
+
+        Notes
+        -----
+        The degree of the B-spline, `k`, is inferred from the length of `t` as
+        ``len(t)-2``. The knot vector is constructed by appending and prepending
+        ``k+1`` elements to internal knots `t`.
+
+        Examples
+        --------
+        Construct a cubic B-spline:
+
+        >>> import numpy as np
+        >>> from scipy.interpolate import BSpline
+        >>> b = BSpline.basis_element([0, 1, 2, 3, 4])
+        >>> k = b.k
+        >>> b.t[k:-k]
+        array([ 0.,  1.,  2.,  3.,  4.])
+        >>> k
+        3
+
+        Construct a quadratic B-spline on ``[0, 1, 1, 2]``, and compare
+        to its explicit form:
+
+        >>> t = [0, 1, 1, 2]
+        >>> b = BSpline.basis_element(t)
+        >>> def f(x):
+        ...     return np.where(x < 1, x*x, (2. - x)**2)
+
+        >>> import matplotlib.pyplot as plt
+        >>> fig, ax = plt.subplots()
+        >>> x = np.linspace(0, 2, 51)
+        >>> ax.plot(x, b(x), 'g', lw=3)
+        >>> ax.plot(x, f(x), 'r', lw=8, alpha=0.4)
+        >>> ax.grid(True)
+        >>> plt.show()
+
+        """
+        xp = array_namespace(t)
+        t = np.asarray(t)
+        k = t.shape[0] - 2
+        t = _as_float_array(t)  # TODO: use concat_1d instead of np.r_
+        t = np.r_[(t[0]-1,) * k, t, (t[-1]+1,) * k]
+        c = np.zeros_like(t)
+        c[k] = 1.
+
+        t, c = xp.asarray(t), xp.asarray(c)
+        return cls.construct_fast(t, c, k, extrapolate)
+
+    @classmethod
+    def design_matrix(cls, x, t, k, extrapolate=False):
+        """
+        Returns a design matrix as a CSR format sparse array.
+
+        Parameters
+        ----------
+        x : array_like, shape (n,)
+            Points to evaluate the spline at.
+        t : array_like, shape (nt,)
+            Sorted 1D array of knots.
+        k : int
+            B-spline degree.
+        extrapolate : bool or 'periodic', optional
+            Whether to extrapolate based on the first and last intervals
+            or raise an error. If 'periodic', periodic extrapolation is used.
+            Default is False.
+
+            .. versionadded:: 1.10.0
+
+        Returns
+        -------
+        design_matrix : `csr_array` object
+            Sparse matrix in CSR format where each row contains all the basis
+            elements of the input row (first row = basis elements of x[0],
+            ..., last row = basis elements x[-1]).
+
+        Examples
+        --------
+        Construct a design matrix for a B-spline
+
+        >>> from scipy.interpolate import make_interp_spline, BSpline
+        >>> import numpy as np
+        >>> x = np.linspace(0, np.pi * 2, 4)
+        >>> y = np.sin(x)
+        >>> k = 3
+        >>> bspl = make_interp_spline(x, y, k=k)
+        >>> design_matrix = bspl.design_matrix(x, bspl.t, k)
+        >>> design_matrix.toarray()
+        [[1.        , 0.        , 0.        , 0.        ],
+        [0.2962963 , 0.44444444, 0.22222222, 0.03703704],
+        [0.03703704, 0.22222222, 0.44444444, 0.2962963 ],
+        [0.        , 0.        , 0.        , 1.        ]]
+
+        Construct a design matrix for some vector of knots
+
+        >>> k = 2
+        >>> t = [-1, 0, 1, 2, 3, 4, 5, 6]
+        >>> x = [1, 2, 3, 4]
+        >>> design_matrix = BSpline.design_matrix(x, t, k).toarray()
+        >>> design_matrix
+        [[0.5, 0.5, 0. , 0. , 0. ],
+        [0. , 0.5, 0.5, 0. , 0. ],
+        [0. , 0. , 0.5, 0.5, 0. ],
+        [0. , 0. , 0. , 0.5, 0.5]]
+
+        This result is equivalent to the one created in the sparse format
+
+        >>> c = np.eye(len(t) - k - 1)
+        >>> design_matrix_gh = BSpline(t, c, k)(x)
+        >>> np.allclose(design_matrix, design_matrix_gh, atol=1e-14)
+        True
+
+        Notes
+        -----
+        .. versionadded:: 1.8.0
+
+        In each row of the design matrix all the basis elements are evaluated
+        at the certain point (first row - x[0], ..., last row - x[-1]).
+
+        `nt` is a length of the vector of knots: as far as there are
+        `nt - k - 1` basis elements, `nt` should be not less than `2 * k + 2`
+        to have at least `k + 1` basis element.
+
+        Out of bounds `x` raises a ValueError.
+        """
+        x = _as_float_array(x, True)
+        t = _as_float_array(t, True)
+
+        if extrapolate != 'periodic':
+            extrapolate = bool(extrapolate)
+
+        if k < 0:
+            raise ValueError("Spline order cannot be negative.")
+        if t.ndim != 1 or np.any(t[1:] < t[:-1]):
+            raise ValueError(f"Expect t to be a 1-D sorted array_like, but "
+                             f"got t={t}.")
+        # There are `nt - k - 1` basis elements in a BSpline built on the
+        # vector of knots with length `nt`, so to have at least `k + 1` basis
+        # elements we need to have at least `2 * k + 2` elements in the vector
+        # of knots.
+        if len(t) < 2 * k + 2:
+            raise ValueError(f"Length t is not enough for k={k}.")
+
+        if extrapolate == 'periodic':
+            # With periodic extrapolation we map x to the segment
+            # [t[k], t[n]].
+            n = t.size - k - 1
+            x = t[k] + (x - t[k]) % (t[n] - t[k])
+            extrapolate = False
+        elif not extrapolate and (
+            (min(x) < t[k]) or (max(x) > t[t.shape[0] - k - 1])
+        ):
+            # Checks from `find_interval` function
+            raise ValueError(f'Out of bounds w/ x = {x}.')
+
+        # Compute number of non-zeros of final CSR array in order to determine
+        # the dtype of indices and indptr of the CSR array.
+        n = x.shape[0]
+        nnz = n * (k + 1)
+        if nnz < np.iinfo(np.int32).max:
+            int_dtype = np.int32
+        else:
+            int_dtype = np.int64
+
+        # Get the non-zero elements of the design matrix and per-row `offsets`:
+        # In row `i`, k+1 nonzero elements are consecutive, and start from `offset[i]`
+        data, offsets, _ = _dierckx.data_matrix(x, t, k, np.ones_like(x), extrapolate)
+        data = data.ravel()
+
+        if offsets.dtype != int_dtype:
+            offsets = offsets.astype(int_dtype)
+
+        # Convert from per-row offsets to the CSR indices/indptr format
+        indices = np.repeat(offsets, k+1).reshape(-1, k+1)
+        indices = indices + np.arange(k+1, dtype=int_dtype)
+        indices = indices.ravel()
+
+        indptr = np.arange(0, (n + 1) * (k + 1), k + 1, dtype=int_dtype)
+
+        return csr_array(
+            (data, indices, indptr),
+            shape=(x.shape[0], t.shape[0] - k - 1)
+        )
+
+    def __call__(self, x, nu=0, extrapolate=None):
+        """
+        Evaluate a spline function.
+
+        Parameters
+        ----------
+        x : array_like
+            points to evaluate the spline at.
+        nu : int, optional
+            derivative to evaluate (default is 0).
+        extrapolate : bool or 'periodic', optional
+            whether to extrapolate based on the first and last intervals
+            or return nans. If 'periodic', periodic extrapolation is used.
+            Default is `self.extrapolate`.
+
+        Returns
+        -------
+        y : array_like
+            Shape is determined by replacing the interpolation axis
+            in the coefficient array with the shape of `x`.
+
+        """
+        if extrapolate is None:
+            extrapolate = self.extrapolate
+        x = np.asarray(x)
+        x_shape, x_ndim = x.shape, x.ndim
+        x = np.ascontiguousarray(x.ravel(), dtype=np.float64)
+
+        # With periodic extrapolation we map x to the segment
+        # [self.t[k], self.t[n]].
+        if extrapolate == 'periodic':
+            n = self._t.size - self.k - 1
+            x = self._t[self.k] + (x - self._t[self.k]) % (self._t[n] - self._t[self.k])
+            extrapolate = False
+
+        self._ensure_c_contiguous()
+
+        # if self.c is complex: the C code in _dierckxmodule.cc expects
+        # floats, so make a view---this expands the last axis, and
+        # the view is C contiguous if the original is.
+        # if c.dtype is complex of shape (n,), c.view(float).shape == (2*n,)
+        # if c.dtype is complex of shape (n, m), c.view(float).shape == (n, 2*m)
+
+        is_complex = self._c.dtype.kind == 'c'
+        if is_complex:
+            cc = self._c.view(float)
+            if self._c.ndim == 1:
+                cc = cc.reshape(self._c.shape[0], 2)
+        else:
+            cc = self._c
+
+        # flatten the trailing dims
+        cc = cc.reshape(cc.shape[0], -1)
+
+        # heavy lifting: actually perform the evaluations
+        out = _dierckx.evaluate_spline(self._t, cc, self.k, x, nu, extrapolate)
+
+        if is_complex:
+            out = out.view(complex)
+
+        out = out.reshape(x_shape + self._c.shape[1:])
+        if self.axis != 0:
+            # transpose to move the calculated values to the interpolation axis
+            l = list(range(out.ndim))
+            l = l[x_ndim:x_ndim+self.axis] + l[:x_ndim] + l[x_ndim+self.axis:]
+            out = out.transpose(l)
+        return self._asarray(out)
+
+    def _ensure_c_contiguous(self):
+        """
+        c and t may be modified by the user. The Cython code expects
+        that they are C contiguous.
+
+        """
+        if not self._t.flags.c_contiguous:
+            self._t = self._t.copy()
+        if not self._c.flags.c_contiguous:
+            self._c = self._c.copy()
+
+    def derivative(self, nu=1):
+        """Return a B-spline representing the derivative.
+
+        Parameters
+        ----------
+        nu : int, optional
+            Derivative order.
+            Default is 1.
+
+        Returns
+        -------
+        b : `BSpline` object
+            A new instance representing the derivative.
+
+        See Also
+        --------
+        splder, splantider
+
+        """
+        c = self._asarray(self.c, copy=True)
+        t = self.t
+        xp = array_namespace(t, c)
+
+        # pad the c array if needed
+        ct = t.shape[0] - c.shape[0]
+        if ct > 0:
+            c = concat_1d(xp, c, xp.zeros((ct,) + c.shape[1:]))
+        tck = _fitpack_impl.splder((t, c, self.k), nu)
+        return self.construct_fast(*tck, extrapolate=self.extrapolate,
+                                   axis=self.axis)
+
+    def antiderivative(self, nu=1):
+        """Return a B-spline representing the antiderivative.
+
+        Parameters
+        ----------
+        nu : int, optional
+            Antiderivative order. Default is 1.
+
+        Returns
+        -------
+        b : `BSpline` object
+            A new instance representing the antiderivative.
+
+        Notes
+        -----
+        If antiderivative is computed and ``self.extrapolate='periodic'``,
+        it will be set to False for the returned instance. This is done because
+        the antiderivative is no longer periodic and its correct evaluation
+        outside of the initially given x interval is difficult.
+
+        See Also
+        --------
+        splder, splantider
+
+        """
+        c = self._asarray(self.c, copy=True)
+        t = self.t
+        xp = array_namespace(t, c)
+
+        # pad the c array if needed
+        ct = t.shape[0] - c.shape[0]
+        if ct > 0:
+            c = concat_1d(xp, c, xp.zeros((ct,) + c.shape[1:]))
+        tck = _fitpack_impl.splantider((t, c, self.k), nu)
+
+        if self.extrapolate == 'periodic':
+            extrapolate = False
+        else:
+            extrapolate = self.extrapolate
+
+        return self.construct_fast(*tck, extrapolate=extrapolate,
+                                   axis=self.axis)
+
+    def integrate(self, a, b, extrapolate=None):
+        """Compute a definite integral of the spline.
+
+        Parameters
+        ----------
+        a : float
+            Lower limit of integration.
+        b : float
+            Upper limit of integration.
+        extrapolate : bool or 'periodic', optional
+            whether to extrapolate beyond the base interval,
+            ``t[k] .. t[-k-1]``, or take the spline to be zero outside of the
+            base interval. If 'periodic', periodic extrapolation is used.
+            If None (default), use `self.extrapolate`.
+
+        Returns
+        -------
+        I : array_like
+            Definite integral of the spline over the interval ``[a, b]``.
+
+        Examples
+        --------
+        Construct the linear spline ``x if x < 1 else 2 - x`` on the base
+        interval :math:`[0, 2]`, and integrate it
+
+        >>> from scipy.interpolate import BSpline
+        >>> b = BSpline.basis_element([0, 1, 2])
+        >>> b.integrate(0, 1)
+        array(0.5)
+
+        If the integration limits are outside of the base interval, the result
+        is controlled by the `extrapolate` parameter
+
+        >>> b.integrate(-1, 1)
+        array(0.0)
+        >>> b.integrate(-1, 1, extrapolate=False)
+        array(0.5)
+
+        >>> import matplotlib.pyplot as plt
+        >>> fig, ax = plt.subplots()
+        >>> ax.grid(True)
+        >>> ax.axvline(0, c='r', lw=5, alpha=0.5)  # base interval
+        >>> ax.axvline(2, c='r', lw=5, alpha=0.5)
+        >>> xx = [-1, 1, 2]
+        >>> ax.plot(xx, b(xx))
+        >>> plt.show()
+
+        """
+        if extrapolate is None:
+            extrapolate = self.extrapolate
+
+        # Prepare self.t and self.c.
+        self._ensure_c_contiguous()
+
+        # Swap integration bounds if needed.
+        sign = 1
+        if b < a:
+            a, b = b, a
+            sign = -1
+        n = self._t.size - self.k - 1
+
+        if extrapolate != "periodic" and not extrapolate:
+            # Shrink the integration interval, if needed.
+            a = max(a, self._t[self.k])
+            b = min(b, self._t[n])
+
+            if self._c.ndim == 1:
+                # Fast path: use FITPACK's routine
+                # (cf _fitpack_impl.splint).
+                integral = _fitpack_impl.splint(a, b, (self._t, self._c, self.k))
+                return self._asarray(integral * sign)
+
+        # Compute the antiderivative.
+        c = self._c
+        ct = len(self._t) - len(c)
+        if ct > 0:
+            c = np.r_[c, np.zeros((ct,) + c.shape[1:])]
+        ta, ca, ka = _fitpack_impl.splantider((self._t, c, self.k), 1)
+
+        if extrapolate == 'periodic':
+            # Split the integral into the part over period (can be several
+            # of them) and the remaining part.
+
+            ts, te = self._t[self.k], self._t[n]
+            period = te - ts
+            interval = b - a
+            n_periods, left = divmod(interval, period)
+
+            if n_periods > 0:
+                # Evaluate the difference of antiderivatives.
+                x = np.asarray([ts, te], dtype=np.float64)
+                out = _dierckx.evaluate_spline(ta, ca.reshape(ca.shape[0], -1),
+                                      ka, x, 0, False)
+                integral = out[1] - out[0]
+                integral *= n_periods
+            else:
+                integral = np.zeros((1, prod(self._c.shape[1:])),
+                                    dtype=self._c.dtype)
+
+            # Map a to [ts, te], b is always a + left.
+            a = ts + (a - ts) % period
+            b = a + left
+
+            # If b <= te then we need to integrate over [a, b], otherwise
+            # over [a, te] and from xs to what is remained.
+            if b <= te:
+                x = np.asarray([a, b], dtype=np.float64)
+                out = _dierckx.evaluate_spline(ta, ca.reshape(ca.shape[0], -1),
+                                      ka, x, 0, False)
+                integral += out[1] - out[0]
+            else:
+                x = np.asarray([a, te], dtype=np.float64)
+                out = _dierckx.evaluate_spline(ta, ca.reshape(ca.shape[0], -1),
+                                      ka, x, 0, False)
+                integral += out[1] - out[0]
+
+                x = np.asarray([ts, ts + b - te], dtype=np.float64)
+                out = _dierckx.evaluate_spline(ta, ca.reshape(ca.shape[0], -1),
+                                      ka, x, 0, False)
+                integral += out[1] - out[0]
+        else:
+            # Evaluate the difference of antiderivatives.
+            x = np.asarray([a, b], dtype=np.float64)
+            out = _dierckx.evaluate_spline(ta, ca.reshape(ca.shape[0], -1),
+                                  ka, x, 0, extrapolate)
+            integral = out[1] - out[0]
+
+        integral *= sign
+        return self._asarray(integral.reshape(ca.shape[1:]))
+
+    @classmethod
+    def from_power_basis(cls, pp, bc_type='not-a-knot'):
+        r"""
+        Construct a polynomial in the B-spline basis
+        from a piecewise polynomial in the power basis.
+
+        For now, accepts ``CubicSpline`` instances only.
+
+        Parameters
+        ----------
+        pp : CubicSpline
+            A piecewise polynomial in the power basis, as created
+            by ``CubicSpline``
+        bc_type : string, optional
+            Boundary condition type as in ``CubicSpline``: one of the
+            ``not-a-knot``, ``natural``, ``clamped``, or ``periodic``.
+            Necessary for construction an instance of ``BSpline`` class.
+            Default is ``not-a-knot``.
+
+        Returns
+        -------
+        b : `BSpline` object
+            A new instance representing the initial polynomial
+            in the B-spline basis.
+
+        Notes
+        -----
+        .. versionadded:: 1.8.0
+
+        Accepts only ``CubicSpline`` instances for now.
+
+        The algorithm follows from differentiation
+        the Marsden's identity [1]: each of coefficients of spline
+        interpolation function in the B-spline basis is computed as follows:
+
+        .. math::
+
+            c_j = \sum_{m=0}^{k} \frac{(k-m)!}{k!}
+                       c_{m,i} (-1)^{k-m} D^m p_{j,k}(x_i)
+
+        :math:`c_{m, i}` - a coefficient of CubicSpline,
+        :math:`D^m p_{j, k}(x_i)` - an m-th defivative of a dual polynomial
+        in :math:`x_i`.
+
+        ``k`` always equals 3 for now.
+
+        First ``n - 2`` coefficients are computed in :math:`x_i = x_j`, e.g.
+
+        .. math::
+
+            c_1 = \sum_{m=0}^{k} \frac{(k-1)!}{k!} c_{m,1} D^m p_{j,3}(x_1)
+
+        Last ``nod + 2`` coefficients are computed in ``x[-2]``,
+        ``nod`` - number of derivatives at the ends.
+
+        For example, consider :math:`x = [0, 1, 2, 3, 4]`,
+        :math:`y = [1, 1, 1, 1, 1]` and bc_type = ``natural``
+
+        The coefficients of CubicSpline in the power basis:
+
+        :math:`[[0, 0, 0, 0, 0], [0, 0, 0, 0, 0],
+        [0, 0, 0, 0, 0], [1, 1, 1, 1, 1]]`
+
+        The knot vector: :math:`t = [0, 0, 0, 0, 1, 2, 3, 4, 4, 4, 4]`
+
+        In this case
+
+        .. math::
+
+            c_j = \frac{0!}{k!} c_{3, i} k! = c_{3, i} = 1,~j = 0, ..., 6
+
+        References
+        ----------
+        .. [1] Tom Lyche and Knut Morken, Spline Methods, 2005, Section 3.1.2
+
+        """
+        from ._cubic import CubicSpline
+        if not isinstance(pp, CubicSpline):
+            raise NotImplementedError(f"Only CubicSpline objects are accepted "
+                                      f"for now. Got {type(pp)} instead.")
+        x = pp.x
+        coef = pp.c
+        k = pp.c.shape[0] - 1
+        n = x.shape[0]
+
+        if bc_type == 'not-a-knot':
+            t = _not_a_knot(x, k)
+        elif bc_type == 'natural' or bc_type == 'clamped':
+            t = _augknt(x, k)
+        elif bc_type == 'periodic':
+            t = _periodic_knots(x, k)
+        else:
+            raise TypeError(f'Unknown boundary condition: {bc_type}')
+
+        nod = t.shape[0] - (n + k + 1)  # number of derivatives at the ends
+        c = np.zeros(n + nod, dtype=pp.c.dtype)
+        for m in range(k + 1):
+            for i in range(n - 2):
+                c[i] += poch(k + 1, -m) * coef[m, i]\
+                        * np.power(-1, k - m)\
+                        * _diff_dual_poly(i, k, x[i], m, t)
+            for j in range(n - 2, n + nod):
+                c[j] += poch(k + 1, -m) * coef[m, n - 2]\
+                        * np.power(-1, k - m)\
+                        * _diff_dual_poly(j, k, x[n - 2], m, t)
+        return cls.construct_fast(t, c, k, pp.extrapolate, pp.axis)
+
+    def insert_knot(self, x, m=1):
+        """Insert a new knot at `x` of multiplicity `m`.
+
+        Given the knots and coefficients of a B-spline representation, create a
+        new B-spline with a knot inserted `m` times at point `x`.
+
+        Parameters
+        ----------
+        x : float
+            The position of the new knot
+        m : int, optional
+            The number of times to insert the given knot (its multiplicity).
+            Default is 1.
+
+        Returns
+        -------
+        spl : `BSpline` object
+            A new `BSpline` object with the new knot inserted.
+
+        Notes
+        -----
+        Based on algorithms from [1]_ and [2]_.
+
+        In case of a periodic spline (``self.extrapolate == "periodic"``)
+        there must be either at least k interior knots t(j) satisfying
+        ``t(k+1)<t(j)<=x`` or at least k interior knots t(j) satisfying
+        ``x<=t(j)<t(n-k)``.
+
+        This routine is functionally equivalent to `scipy.interpolate.insert`.
+
+        .. versionadded:: 1.13
+
+        References
+        ----------
+        .. [1] W. Boehm, "Inserting new knots into b-spline curves.",
+            Computer Aided Design, 12, p.199-201, 1980.
+            :doi:`10.1016/0010-4485(80)90154-2`.
+        .. [2] P. Dierckx, "Curve and surface fitting with splines, Monographs on
+            Numerical Analysis", Oxford University Press, 1993.
+
+        See Also
+        --------
+        scipy.interpolate.insert
+
+        Examples
+        --------
+        You can insert knots into a B-spline:
+
+        >>> import numpy as np
+        >>> from scipy.interpolate import BSpline, make_interp_spline
+        >>> x = np.linspace(0, 10, 5)
+        >>> y = np.sin(x)
+        >>> spl = make_interp_spline(x, y, k=3)
+        >>> spl.t
+        array([ 0.,  0.,  0.,  0.,  5., 10., 10., 10., 10.])
+
+        Insert a single knot
+
+        >>> spl_1 = spl.insert_knot(3)
+        >>> spl_1.t
+        array([ 0.,  0.,  0.,  0.,  3.,  5., 10., 10., 10., 10.])
+
+        Insert a multiple knot
+
+        >>> spl_2 = spl.insert_knot(8, m=3)
+        >>> spl_2.t
+        array([ 0.,  0.,  0.,  0.,  5.,  8.,  8.,  8., 10., 10., 10., 10.])
+
+        """
+        x = float(x)
+
+        if x < self._t[self.k] or x > self._t[-self.k-1]:
+            raise ValueError(f"Cannot insert a knot at {x}.")
+        if m <= 0:
+            raise ValueError(f"`m` must be positive, got {m = }.")
+
+        tt = self._t.copy()
+        cc = self._c.copy()
+
+        for _ in range(m):
+            tt, cc = _insert(x, tt, cc, self.k, self.extrapolate == "periodic")
+        tt, cc = self._asarray(tt), self._asarray(cc)
+        return self.construct_fast(tt, cc, self.k, self.extrapolate, self.axis)
+
+
+def _insert(xval, t, c, k, periodic=False):
+    """Insert a single knot at `xval`."""
+    #
+    # This is a port of the FORTRAN `insert` routine by P. Dierckx,
+    # https://github.com/scipy/scipy/blob/maintenance/1.11.x/scipy/interpolate/fitpack/insert.f
+    # which carries the following comment:
+    #
+    # subroutine insert inserts a new knot x into a spline function s(x)
+    # of degree k and calculates the b-spline representation of s(x) with
+    # respect to the new set of knots. in addition, if iopt.ne.0, s(x)
+    # will be considered as a periodic spline with period per=t(n-k)-t(k+1)
+    # satisfying the boundary constraints
+    #      t(i+n-2*k-1) = t(i)+per  ,i=1,2,...,2*k+1
+    #      c(i+n-2*k-1) = c(i)      ,i=1,2,...,k
+    # in that case, the knots and b-spline coefficients returned will also
+    # satisfy these boundary constraints, i.e.
+    #      tt(i+nn-2*k-1) = tt(i)+per  ,i=1,2,...,2*k+1
+    #      cc(i+nn-2*k-1) = cc(i)      ,i=1,2,...,k
+    interval = _dierckx.find_interval(t, k, float(xval), k, False)
+    if interval < 0:
+        # extrapolated values are guarded for in BSpline.insert_knot
+        raise ValueError(f"Cannot insert the knot at {xval}.")
+
+    # super edge case: a knot with multiplicity > k+1
+    # see https://github.com/scipy/scipy/commit/037204c3e91
+    if t[interval] == t[interval + k + 1]:
+        interval -= 1
+
+    if periodic:
+        if (interval + 1 <= 2*k) and (interval + 1 >= t.shape[0] - 2*k):
+            # in case of a periodic spline (iopt.ne.0) there must be
+            # either at least k interior knots t(j) satisfying t(k+1)<t(j)<=x
+            # or at least k interior knots t(j) satisfying x<=t(j)<t(n-k)
+            raise ValueError("Not enough internal knots.")
+
+    # knots
+    tt = np.r_[t[:interval+1], xval, t[interval+1:]]
+
+    newshape = (c.shape[0] + 1,) + c.shape[1:]
+    cc = np.zeros(newshape, dtype=c.dtype)
+
+    # coefficients
+    cc[interval+1:, ...] = c[interval:, ...]
+
+    for i in range(interval, interval-k, -1):
+        fac = (xval - tt[i]) / (tt[i+k+1] - tt[i])
+        cc[i, ...] = fac*c[i, ...] + (1. - fac)*c[i-1, ...]
+
+    cc[:interval - k+1, ...] = c[:interval - k+1, ...]
+
+    if periodic:
+        # c   incorporate the boundary conditions for a periodic spline.
+        n = tt.shape[0]
+        nk = n - k - 1
+        n2k = n - 2*k - 1
+        T = tt[nk] - tt[k]   # period
+
+        if interval >= nk - k:
+            # adjust the left-hand boundary knots & coefs
+            tt[:k] = tt[nk - k:nk] - T
+            cc[:k, ...] = cc[n2k:n2k + k, ...]
+
+        if interval <= 2*k-1:
+            # adjust the right-hand boundary knots & coefs
+            tt[n-k:] = tt[k+1:k+1+k] + T
+            cc[n2k:n2k + k, ...] = cc[:k, ...]
+
+    return tt, cc
+
+
+#################################
+#  Interpolating spline helpers #
+#################################
+
+def _not_a_knot(x, k):
+    """Given data x, construct the knot vector w/ not-a-knot BC.
+    cf de Boor, XIII(12).
+
+    For even k, it's a bit ad hoc: Greville sites + omit 2nd and 2nd-to-last
+    data points, a la not-a-knot.
+    This seems to match what Dierckx does, too:
+    https://github.com/scipy/scipy/blob/maintenance/1.11.x/scipy/interpolate/fitpack/fpcurf.f#L63-L80
+    """
+    x = np.asarray(x)
+    if k % 2 == 1:
+        k2 = (k + 1) // 2
+        t = x.copy()
+    else:
+        k2 = k // 2
+        t = (x[1:] + x[:-1]) / 2
+
+    t = t[k2:-k2]
+    t = np.r_[(x[0],)*(k+1), t, (x[-1],)*(k+1)]
+    return t
+
+
+def _augknt(x, k):
+    """Construct a knot vector appropriate for the order-k interpolation."""
+    return np.r_[(x[0],)*k, x, (x[-1],)*k]
+
+
+def _convert_string_aliases(deriv, target_shape):
+    if isinstance(deriv, str):
+        if deriv == "clamped":
+            deriv = [(1, np.zeros(target_shape))]
+        elif deriv == "natural":
+            deriv = [(2, np.zeros(target_shape))]
+        else:
+            raise ValueError(f"Unknown boundary condition : {deriv}")
+    return deriv
+
+
+def _process_deriv_spec(deriv):
+    if deriv is not None:
+        try:
+            ords, vals = zip(*deriv)
+        except TypeError as e:
+            msg = ("Derivatives, `bc_type`, should be specified as a pair of "
+                   "iterables of pairs of (order, value).")
+            raise ValueError(msg) from e
+    else:
+        ords, vals = [], []
+    return np.atleast_1d(ords, vals)
+
+
+def _woodbury_algorithm(A, ur, ll, b, k):
+    '''
+    Solve a cyclic banded linear system with upper right
+    and lower blocks of size ``(k-1) / 2`` using
+    the Woodbury formula
+
+    Parameters
+    ----------
+    A : 2-D array, shape(k, n)
+        Matrix of diagonals of original matrix (see
+        ``solve_banded`` documentation).
+    ur : 2-D array, shape(bs, bs)
+        Upper right block matrix.
+    ll : 2-D array, shape(bs, bs)
+        Lower left block matrix.
+    b : 1-D array, shape(n,)
+        Vector of constant terms of the system of linear equations.
+    k : int
+        B-spline degree.
+
+    Returns
+    -------
+    c : 1-D array, shape(n,)
+        Solution of the original system of linear equations.
+
+    Notes
+    -----
+    This algorithm works only for systems with banded matrix A plus
+    a correction term U @ V.T, where the matrix U @ V.T gives upper right
+    and lower left block of A
+    The system is solved with the following steps:
+        1.  New systems of linear equations are constructed:
+            A @ z_i = u_i,
+            u_i - column vector of U,
+            i = 1, ..., k - 1
+        2.  Matrix Z is formed from vectors z_i:
+            Z = [ z_1 | z_2 | ... | z_{k - 1} ]
+        3.  Matrix H = (1 + V.T @ Z)^{-1}
+        4.  The system A' @ y = b is solved
+        5.  x = y - Z @ (H @ V.T @ y)
+    Also, ``n`` should be greater than ``k``, otherwise corner block
+    elements will intersect with diagonals.
+
+    Examples
+    --------
+    Consider the case of n = 8, k = 5 (size of blocks - 2 x 2).
+    The matrix of a system:       U:          V:
+      x  x  x  *  *  a  b         a b 0 0     0 0 1 0
+      x  x  x  x  *  *  c         0 c 0 0     0 0 0 1
+      x  x  x  x  x  *  *         0 0 0 0     0 0 0 0
+      *  x  x  x  x  x  *         0 0 0 0     0 0 0 0
+      *  *  x  x  x  x  x         0 0 0 0     0 0 0 0
+      d  *  *  x  x  x  x         0 0 d 0     1 0 0 0
+      e  f  *  *  x  x  x         0 0 e f     0 1 0 0
+
+    References
+    ----------
+    .. [1] William H. Press, Saul A. Teukolsky, William T. Vetterling
+           and Brian P. Flannery, Numerical Recipes, 2007, Section 2.7.3
+
+    '''
+    k_mod = k - k % 2
+    bs = int((k - 1) / 2) + (k + 1) % 2
+
+    n = A.shape[1] + 1
+    U = np.zeros((n - 1, k_mod))
+    VT = np.zeros((k_mod, n - 1))  # V transpose
+
+    # upper right block
+    U[:bs, :bs] = ur
+    VT[np.arange(bs), np.arange(bs) - bs] = 1
+
+    # lower left block
+    U[-bs:, -bs:] = ll
+    VT[np.arange(bs) - bs, np.arange(bs)] = 1
+
+    Z = solve_banded((bs, bs), A, U)
+
+    H = solve(np.identity(k_mod) + VT @ Z, np.identity(k_mod))
+
+    y = solve_banded((bs, bs), A, b)
+    c = y - Z @ (H @ (VT @ y))
+
+    return c
+
+
+def _periodic_knots(x, k):
+    '''
+    returns vector of nodes on circle
+    '''
+    xc = np.copy(x)
+    n = len(xc)
+    if k % 2 == 0:
+        dx = np.diff(xc)
+        xc[1: -1] -= dx[:-1] / 2
+    dx = np.diff(xc)
+    t = np.zeros(n + 2 * k)
+    t[k: -k] = xc
+    for i in range(0, k):
+        # filling first `k` elements in descending order
+        t[k - i - 1] = t[k - i] - dx[-(i % (n - 1)) - 1]
+        # filling last `k` elements in ascending order
+        t[-k + i] = t[-k + i - 1] + dx[i % (n - 1)]
+    return t
+
+
+def _make_interp_per_full_matr(x, y, t, k):
+    '''
+    Returns a solution of a system for B-spline interpolation with periodic
+    boundary conditions. First ``k - 1`` rows of matrix are conditions of
+    periodicity (continuity of ``k - 1`` derivatives at the boundary points).
+    Last ``n`` rows are interpolation conditions.
+    RHS is ``k - 1`` zeros and ``n`` ordinates in this case.
+
+    Parameters
+    ----------
+    x : 1-D array, shape (n,)
+        Values of x - coordinate of a given set of points.
+    y : 1-D array, shape (n,)
+        Values of y - coordinate of a given set of points.
+    t : 1-D array, shape(n+2*k,)
+        Vector of knots.
+    k : int
+        The maximum degree of spline
+
+    Returns
+    -------
+    c : 1-D array, shape (n+k-1,)
+        B-spline coefficients
+
+    Notes
+    -----
+    ``t`` is supposed to be taken on circle.
+
+    '''
+
+    x, y, t = map(np.asarray, (x, y, t))
+
+    n = x.size
+    # LHS: the colocation matrix + derivatives at edges
+    matr = np.zeros((n + k - 1, n + k - 1))
+
+    # derivatives at x[0] and x[-1]:
+    for i in range(k - 1):
+        bb = _dierckx.evaluate_all_bspl(t, k, x[0], k, i + 1)
+        matr[i, : k + 1] += bb
+        bb = _dierckx.evaluate_all_bspl(t, k, x[-1], n + k - 1, i + 1)[:-1]
+        matr[i, -k:] -= bb
+
+    # colocation matrix
+    for i in range(n):
+        xval = x[i]
+        # find interval
+        if xval == t[k]:
+            left = k
+        else:
+            left = np.searchsorted(t, xval) - 1
+
+        # fill a row
+        bb = _dierckx.evaluate_all_bspl(t, k, xval, left)
+        matr[i + k - 1, left-k:left+1] = bb
+
+    # RHS
+    b = np.r_[[0] * (k - 1), y]
+
+    c = solve(matr, b)
+    return c
+
+
+def _handle_lhs_derivatives(t, k, xval, ab, kl, ku, deriv_ords, offset=0):
+    """ Fill in the entries of the colocation matrix corresponding to known
+    derivatives at `xval`.
+
+    The colocation matrix is in the banded storage, as prepared by _coloc.
+    No error checking.
+
+    Parameters
+    ----------
+    t : ndarray, shape (nt + k + 1,)
+        knots
+    k : integer
+        B-spline order
+    xval : float
+        The value at which to evaluate the derivatives at.
+    ab : ndarray, shape(2*kl + ku + 1, nt), Fortran order
+        B-spline colocation matrix.
+        This argument is modified *in-place*.
+    kl : integer
+        Number of lower diagonals of ab.
+    ku : integer
+        Number of upper diagonals of ab.
+    deriv_ords : 1D ndarray
+        Orders of derivatives known at xval
+    offset : integer, optional
+        Skip this many rows of the matrix ab.
+
+    """
+    # find where `xval` is in the knot vector, `t`
+    left = _dierckx.find_interval(t, k, float(xval), k, False)
+
+    # compute and fill in the derivatives @ xval
+    for row in range(deriv_ords.shape[0]):
+        nu = deriv_ords[row]
+        wrk = _dierckx.evaluate_all_bspl(t, k, xval, left, nu)
+
+        # if A were a full matrix, it would be just
+        # ``A[row + offset, left-k:left+1] = bb``.
+        for a in range(k+1):
+            clmn = left - k + a
+            ab[kl + ku + offset + row - clmn, clmn] = wrk[a]
+
+
+def _make_periodic_spline(x, y, t, k, axis, *, xp):
+    '''
+    Compute the (coefficients of) interpolating B-spline with periodic
+    boundary conditions.
+
+    Parameters
+    ----------
+    x : array_like, shape (n,)
+        Abscissas.
+    y : array_like, shape (n,)
+        Ordinates.
+    k : int
+        B-spline degree.
+    t : array_like, shape (n + 2 * k,).
+        Knots taken on a circle, ``k`` on the left and ``k`` on the right
+        of the vector ``x``.
+
+    Returns
+    -------
+    b : `BSpline` object
+        A `BSpline` object of the degree ``k`` and with knots ``t``.
+
+    Notes
+    -----
+    The original system is formed by ``n + k - 1`` equations where the first
+    ``k - 1`` of them stand for the ``k - 1`` derivatives continuity on the
+    edges while the other equations correspond to an interpolating case
+    (matching all the input points). Due to a special form of knot vector, it
+    can be proved that in the original system the first and last ``k``
+    coefficients of a spline function are the same, respectively. It follows
+    from the fact that all ``k - 1`` derivatives are equal term by term at ends
+    and that the matrix of the original system of linear equations is
+    non-degenerate. So, we can reduce the number of equations to ``n - 1``
+    (first ``k - 1`` equations could be reduced). Another trick of this
+    implementation is cyclic shift of values of B-splines due to equality of
+    ``k`` unknown coefficients. With this we can receive matrix of the system
+    with upper right and lower left blocks, and ``k`` diagonals.  It allows
+    to use Woodbury formula to optimize the computations.
+
+    '''
+    n = y.shape[0]
+
+    extradim = prod(y.shape[1:])
+    y_new = y.reshape(n, extradim)
+    c = np.zeros((n + k - 1, extradim))
+
+    # n <= k case is solved with full matrix
+    if n <= k:
+        for i in range(extradim):
+            c[:, i] = _make_interp_per_full_matr(x, y_new[:, i], t, k)
+        c = np.ascontiguousarray(c.reshape((n + k - 1,) + y.shape[1:]))
+        t, c = xp.asarray(t), xp.asarray(c)
+        return BSpline.construct_fast(t, c, k, extrapolate='periodic', axis=axis)
+
+    nt = len(t) - k - 1
+
+    # size of block elements
+    kul = int(k / 2)
+
+    # kl = ku = k
+    ab = np.zeros((3 * k + 1, nt), dtype=np.float64, order='F')
+
+    # upper right and lower left blocks
+    ur = np.zeros((kul, kul))
+    ll = np.zeros_like(ur)
+
+    # `offset` is made to shift all the non-zero elements to the end of the
+    # matrix
+    # NB: 1. drop the last element of `x` because `x[0] = x[-1] + T` & `y[0] == y[-1]`
+    #     2. pass ab.T to _coloc to make it C-ordered; below it'll be fed to banded
+    #        LAPACK, which needs F-ordered arrays
+    _dierckx._coloc(x[:-1], t, k, ab.T, k)
+
+    # remove zeros before the matrix
+    ab = ab[-k - (k + 1) % 2:, :]
+
+    # The least elements in rows (except repetitions) are diagonals
+    # of block matrices. Upper right matrix is an upper triangular
+    # matrix while lower left is a lower triangular one.
+    for i in range(kul):
+        ur += np.diag(ab[-i - 1, i: kul], k=i)
+        ll += np.diag(ab[i, -kul - (k % 2): n - 1 + 2 * kul - i], k=-i)
+
+    # remove elements that occur in the last point
+    # (first and last points are equivalent)
+    A = ab[:, kul: -k + kul]
+
+    for i in range(extradim):
+        cc = _woodbury_algorithm(A, ur, ll, y_new[:, i][:-1], k)
+        c[:, i] = np.concatenate((cc[-kul:], cc, cc[:kul + k % 2]))
+    c = np.ascontiguousarray(c.reshape((n + k - 1,) + y.shape[1:]))
+    t, c = xp.asarray(t), xp.asarray(c)
+    return BSpline.construct_fast(t, c, k, extrapolate='periodic', axis=axis)
+
+
+@xp_capabilities(cpu_only=True, jax_jit=False, allow_dask_compute=True)
+def make_interp_spline(x, y, k=3, t=None, bc_type=None, axis=0,
+                       check_finite=True):
+    """Create an interpolating B-spline with specified degree and boundary conditions.
+
+    Parameters
+    ----------
+    x : array_like, shape (n,)
+        Abscissas.
+    y : array_like, shape (n, ...)
+        Ordinates.
+    k : int, optional
+        B-spline degree. Default is cubic, ``k = 3``.
+    t : array_like, shape (nt + k + 1,), optional.
+        Knots.
+        The number of knots needs to agree with the number of data points and
+        the number of derivatives at the edges. Specifically, ``nt - n`` must
+        equal ``len(deriv_l) + len(deriv_r)``.
+    bc_type : 2-tuple or None
+        Boundary conditions.
+        Default is None, which means choosing the boundary conditions
+        automatically. Otherwise, it must be a length-two tuple where the first
+        element (``deriv_l``) sets the boundary conditions at ``x[0]`` and
+        the second element (``deriv_r``) sets the boundary conditions at
+        ``x[-1]``. Each of these must be an iterable of pairs
+        ``(order, value)`` which gives the values of derivatives of specified
+        orders at the given edge of the interpolation interval.
+        Alternatively, the following string aliases are recognized:
+
+        * ``"clamped"``: The first derivatives at the ends are zero. This is
+          equivalent to ``bc_type=([(1, 0.0)], [(1, 0.0)])``.
+        * ``"natural"``: The second derivatives at ends are zero. This is
+          equivalent to ``bc_type=([(2, 0.0)], [(2, 0.0)])``.
+        * ``"not-a-knot"`` (default): The first and second segments are the
+          same polynomial. This is equivalent to having ``bc_type=None``.
+        * ``"periodic"``: The values and the first ``k-1`` derivatives at the
+          ends are equivalent.
+
+    axis : int, optional
+        Interpolation axis. Default is 0.
+    check_finite : bool, optional
+        Whether to check that the input arrays contain only finite numbers.
+        Disabling may give a performance gain, but may result in problems
+        (crashes, non-termination) if the inputs do contain infinities or NaNs.
+        Default is True.
+
+    Returns
+    -------
+    b : `BSpline` object
+        A `BSpline` object of the degree ``k`` and with knots ``t``.
+
+    See Also
+    --------
+    BSpline : base class representing the B-spline objects
+    CubicSpline : a cubic spline in the polynomial basis
+    make_lsq_spline : a similar factory function for spline fitting
+    UnivariateSpline : a wrapper over FITPACK spline fitting routines
+    splrep : a wrapper over FITPACK spline fitting routines
+
+    Examples
+    --------
+    Use cubic interpolation on Chebyshev nodes:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> def cheb_nodes(N):
+    ...     jj = 2.*np.arange(N) + 1
+    ...     x = np.cos(np.pi * jj / 2 / N)[::-1]
+    ...     return x
+
+    >>> x = cheb_nodes(20)
+    >>> y = np.sqrt(1 - x**2)
+
+    >>> from scipy.interpolate import BSpline, make_interp_spline
+    >>> b = make_interp_spline(x, y)
+    >>> np.allclose(b(x), y)
+    True
+
+    Note that the default is a cubic spline with a not-a-knot boundary condition
+
+    >>> b.k
+    3
+
+    Here we use a 'natural' spline, with zero 2nd derivatives at edges:
+
+    >>> l, r = [(2, 0.0)], [(2, 0.0)]
+    >>> b_n = make_interp_spline(x, y, bc_type=(l, r))  # or, bc_type="natural"
+    >>> np.allclose(b_n(x), y)
+    True
+    >>> x0, x1 = x[0], x[-1]
+    >>> np.allclose([b_n(x0, 2), b_n(x1, 2)], [0, 0])
+    True
+
+    Interpolation of parametric curves is also supported. As an example, we
+    compute a discretization of a snail curve in polar coordinates
+
+    >>> phi = np.linspace(0, 2.*np.pi, 40)
+    >>> r = 0.3 + np.cos(phi)
+    >>> x, y = r*np.cos(phi), r*np.sin(phi)  # convert to Cartesian coordinates
+
+    Build an interpolating curve, parameterizing it by the angle
+
+    >>> spl = make_interp_spline(phi, np.c_[x, y])
+
+    Evaluate the interpolant on a finer grid (note that we transpose the result
+    to unpack it into a pair of x- and y-arrays)
+
+    >>> phi_new = np.linspace(0, 2.*np.pi, 100)
+    >>> x_new, y_new = spl(phi_new).T
+
+    Plot the result
+
+    >>> plt.plot(x, y, 'o')
+    >>> plt.plot(x_new, y_new, '-')
+    >>> plt.show()
+
+    Build a B-spline curve with 2 dimensional y
+
+    >>> x = np.linspace(0, 2*np.pi, 10)
+    >>> y = np.array([np.sin(x), np.cos(x)])
+
+    Periodic condition is satisfied because y coordinates of points on the ends
+    are equivalent
+
+    >>> ax = plt.axes(projection='3d')
+    >>> xx = np.linspace(0, 2*np.pi, 100)
+    >>> bspl = make_interp_spline(x, y, k=5, bc_type='periodic', axis=1)
+    >>> ax.plot3D(xx, *bspl(xx))
+    >>> ax.scatter3D(x, *y, color='red')
+    >>> plt.show()
+
+    """
+    # convert string aliases for the boundary conditions
+    if bc_type is None or bc_type == 'not-a-knot' or bc_type == 'periodic':
+        deriv_l, deriv_r = None, None
+    elif isinstance(bc_type, str):
+        deriv_l, deriv_r = bc_type, bc_type
+    else:
+        try:
+            deriv_l, deriv_r = bc_type
+        except TypeError as e:
+            raise ValueError(f"Unknown boundary condition: {bc_type}") from e
+
+    xp = array_namespace(x, y, t)
+    x = _as_float_array(x, check_finite)
+    y = _as_float_array(y, check_finite)
+
+    axis = normalize_axis_index(axis, y.ndim)
+    y = np.moveaxis(y, axis, 0)    # now internally interp axis is zero
+
+    # sanity check the input
+    if bc_type == 'periodic' and not np.allclose(y[0], y[-1], atol=1e-15):
+        raise ValueError("First and last points does not match while "
+                         "periodic case expected")
+    if x.size != y.shape[0]:
+        raise ValueError(f'Shapes of x {x.shape} and y {y.shape} are incompatible')
+    if np.any(x[1:] == x[:-1]):
+        raise ValueError("Expect x to not have duplicates")
+    if x.ndim != 1 or np.any(x[1:] < x[:-1]):
+        raise ValueError("Expect x to be a 1D strictly increasing sequence.")
+
+    # special-case k=0 right away
+    if k == 0:
+        if any(_ is not None for _ in (t, deriv_l, deriv_r)):
+            raise ValueError("Too much info for k=0: t and bc_type can only "
+                             "be None.")
+        t = np.r_[x, x[-1]]
+        c = np.asarray(y)
+        c = np.ascontiguousarray(c, dtype=_get_dtype(c.dtype))
+        t, c = xp.asarray(t), xp.asarray(c)
+        return BSpline.construct_fast(t, c, k, axis=axis)
+
+    # special-case k=1 (e.g., Lyche and Morken, Eq.(2.16))
+    if k == 1 and t is None:
+        if not (deriv_l is None and deriv_r is None):
+            raise ValueError("Too much info for k=1: bc_type can only be None.")
+        t = np.r_[x[0], x, x[-1]]
+        c = np.asarray(y)
+        c = np.ascontiguousarray(c, dtype=_get_dtype(c.dtype))
+        t, c = xp.asarray(t), xp.asarray(c)
+        return BSpline.construct_fast(t, c, k, axis=axis)
+
+    k = operator.index(k)
+
+    if bc_type == 'periodic' and t is not None:
+        raise NotImplementedError("For periodic case t is constructed "
+                                  "automatically and can not be passed "
+                                  "manually")
+
+    # come up with a sensible knot vector, if needed
+    if t is None:
+        if deriv_l is None and deriv_r is None:
+            if bc_type == 'periodic':
+                t = _periodic_knots(x, k)
+            else:
+                t = _not_a_knot(x, k)
+        else:
+            t = _augknt(x, k)
+
+    t = _as_float_array(t, check_finite)
+
+    if k < 0:
+        raise ValueError("Expect non-negative k.")
+    if t.ndim != 1 or np.any(t[1:] < t[:-1]):
+        raise ValueError("Expect t to be a 1-D sorted array_like.")
+    if t.size < x.size + k + 1:
+        raise ValueError(f"Got {t.size} knots, need at least {x.size + k + 1}.")
+    if (x[0] < t[k]) or (x[-1] > t[-k]):
+        raise ValueError(f'Out of bounds w/ x = {x}.')
+
+    if bc_type == 'periodic':
+        return _make_periodic_spline(x, y, t, k, axis, xp=xp)
+
+    # Here : deriv_l, r = [(nu, value), ...]
+    deriv_l = _convert_string_aliases(deriv_l, y.shape[1:])
+    deriv_l_ords, deriv_l_vals = _process_deriv_spec(deriv_l)
+    nleft = deriv_l_ords.shape[0]
+
+    deriv_r = _convert_string_aliases(deriv_r, y.shape[1:])
+    deriv_r_ords, deriv_r_vals = _process_deriv_spec(deriv_r)
+    nright = deriv_r_ords.shape[0]
+
+    if not all(0 <= i <= k for i in deriv_l_ords):
+        raise ValueError(f"Bad boundary conditions at {x[0]}.")
+
+    if not all(0 <= i <= k for i in deriv_r_ords):
+        raise ValueError(f"Bad boundary conditions at {x[-1]}.")
+
+    # have `n` conditions for `nt` coefficients; need nt-n derivatives
+    n = x.size
+    nt = t.size - k - 1
+
+    if nt - n != nleft + nright:
+        raise ValueError("The number of derivatives at boundaries does not "
+                         f"match: expected {nt-n}, got {nleft}+{nright}")
+
+    # bail out if the `y` array is zero-sized
+    if y.size == 0:
+        c = np.zeros((nt,) + y.shape[1:], dtype=float)
+        return BSpline.construct_fast(t, c, k, axis=axis)
+
+    # set up the LHS: the colocation matrix + derivatives at boundaries
+    # NB: ab is in F order for banded LAPACK; _coloc needs C-ordered arrays,
+    #     this pass ab.T into _coloc
+    kl = ku = k
+    ab = np.zeros((2*kl + ku + 1, nt), dtype=np.float64, order='F')
+    _dierckx._coloc(x, t, k, ab.T, nleft)
+    if nleft > 0:
+        _handle_lhs_derivatives(t, k, x[0], ab, kl, ku, deriv_l_ords)
+    if nright > 0:
+        _handle_lhs_derivatives(t, k, x[-1], ab, kl, ku, deriv_r_ords,
+                                offset=nt-nright)
+
+    # set up the RHS: values to interpolate (+ derivative values, if any)
+    extradim = prod(y.shape[1:])
+    rhs = np.empty((nt, extradim), dtype=y.dtype)
+    if nleft > 0:
+        rhs[:nleft] = deriv_l_vals.reshape(-1, extradim)
+    rhs[nleft:nt - nright] = y.reshape(-1, extradim)
+    if nright > 0:
+        rhs[nt - nright:] = deriv_r_vals.reshape(-1, extradim)
+
+    # solve Ab @ x = rhs; this is the relevant part of linalg.solve_banded
+    if check_finite:
+        ab, rhs = map(np.asarray_chkfinite, (ab, rhs))
+    gbsv, = get_lapack_funcs(('gbsv',), (ab, rhs))
+    lu, piv, c, info = gbsv(kl, ku, ab, rhs,
+                            overwrite_ab=True, overwrite_b=True)
+
+    if info > 0:
+        raise LinAlgError("Colocation matrix is singular.")
+    elif info < 0:
+        raise ValueError(f'illegal value in {-info}-th argument of internal gbsv')
+    c = np.ascontiguousarray(c.reshape((nt,) + y.shape[1:]))
+    t, c = xp.asarray(t), xp.asarray(c)
+    return BSpline.construct_fast(t, c, k, axis=axis)
+
+
+@xp_capabilities(cpu_only=True, jax_jit=False, allow_dask_compute=True)
+def make_lsq_spline(x, y, t, k=3, w=None, axis=0, check_finite=True, *, method="qr"):
+    r"""Create a smoothing B-spline satisfying the Least SQuares (LSQ) criterion.
+
+    The result is a linear combination
+
+    .. math::
+
+            S(x) = \sum_j c_j B_j(x; t)
+
+    of the B-spline basis elements, :math:`B_j(x; t)`, which minimizes
+
+    .. math::
+
+        \sum_{j} \left( w_j \times (S(x_j) - y_j) \right)^2
+
+    Parameters
+    ----------
+    x : array_like, shape (m,)
+        Abscissas.
+    y : array_like, shape (m, ...)
+        Ordinates.
+    t : array_like, shape (n + k + 1,).
+        Knots.
+        Knots and data points must satisfy Schoenberg-Whitney conditions.
+    k : int, optional
+        B-spline degree. Default is cubic, ``k = 3``.
+    w : array_like, shape (m,), optional
+        Weights for spline fitting. Must be positive. If ``None``,
+        then weights are all equal.
+        Default is ``None``.
+    axis : int, optional
+        Interpolation axis. Default is zero.
+    check_finite : bool, optional
+        Whether to check that the input arrays contain only finite numbers.
+        Disabling may give a performance gain, but may result in problems
+        (crashes, non-termination) if the inputs do contain infinities or NaNs.
+        Default is True.
+    method : str, optional
+        Method for solving the linear LSQ problem. Allowed values are "norm-eq"
+        (Explicitly construct and solve the normal system of equations), and
+        "qr" (Use the QR factorization of the design matrix).
+        Default is "qr".
+
+    Returns
+    -------
+    b : `BSpline` object
+        A `BSpline` object of the degree ``k`` with knots ``t``.
+
+    See Also
+    --------
+    BSpline : base class representing the B-spline objects
+    make_interp_spline : a similar factory function for interpolating splines
+    LSQUnivariateSpline : a FITPACK-based spline fitting routine
+    splrep : a FITPACK-based fitting routine
+
+    Notes
+    -----
+    The number of data points must be larger than the spline degree ``k``.
+
+    Knots ``t`` must satisfy the Schoenberg-Whitney conditions,
+    i.e., there must be a subset of data points ``x[j]`` such that
+    ``t[j] < x[j] < t[j+k+1]``, for ``j=0, 1,...,n-k-2``.
+
+    Examples
+    --------
+    Generate some noisy data:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> rng = np.random.default_rng()
+    >>> x = np.linspace(-3, 3, 50)
+    >>> y = np.exp(-x**2) + 0.1 * rng.standard_normal(50)
+
+    Now fit a smoothing cubic spline with a pre-defined internal knots.
+    Here we make the knot vector (k+1)-regular by adding boundary knots:
+
+    >>> from scipy.interpolate import make_lsq_spline, BSpline
+    >>> t = [-1, 0, 1]
+    >>> k = 3
+    >>> t = np.r_[(x[0],)*(k+1),
+    ...           t,
+    ...           (x[-1],)*(k+1)]
+    >>> spl = make_lsq_spline(x, y, t, k)
+
+    For comparison, we also construct an interpolating spline for the same
+    set of data:
+
+    >>> from scipy.interpolate import make_interp_spline
+    >>> spl_i = make_interp_spline(x, y)
+
+    Plot both:
+
+    >>> xs = np.linspace(-3, 3, 100)
+    >>> plt.plot(x, y, 'ro', ms=5)
+    >>> plt.plot(xs, spl(xs), 'g-', lw=3, label='LSQ spline')
+    >>> plt.plot(xs, spl_i(xs), 'b-', lw=3, alpha=0.7, label='interp spline')
+    >>> plt.legend(loc='best')
+    >>> plt.show()
+
+    **NaN handling**: If the input arrays contain ``nan`` values, the result is
+    not useful since the underlying spline fitting routines cannot deal with
+    ``nan``. A workaround is to use zero weights for not-a-number data points:
+
+    >>> y[8] = np.nan
+    >>> w = np.isnan(y)
+    >>> y[w] = 0.
+    >>> tck = make_lsq_spline(x, y, t, w=~w)
+
+    Notice the need to replace a ``nan`` by a numerical value (precise value
+    does not matter as long as the corresponding weight is zero.)
+
+    """
+    xp = array_namespace(x, y, t, w)
+
+    x = _as_float_array(x, check_finite)
+    y = _as_float_array(y, check_finite)
+    t = _as_float_array(t, check_finite)
+    if w is not None:
+        w = _as_float_array(w, check_finite)
+    else:
+        w = np.ones_like(x)
+    k = operator.index(k)
+
+    axis = normalize_axis_index(axis, y.ndim)
+
+    y = np.moveaxis(y, axis, 0)    # now internally interp axis is zero
+    if not y.flags.c_contiguous:
+        # C routines in _dierckx currently require C contiguity
+        y = y.copy(order='C')
+
+    if x.ndim != 1:
+        raise ValueError("Expect x to be a 1-D sequence.")
+    if x.shape[0] < k+1:
+        raise ValueError("Need more x points.")
+    if k < 0:
+        raise ValueError("Expect non-negative k.")
+    if t.ndim != 1 or np.any(t[1:] - t[:-1] < 0):
+        raise ValueError("Expect t to be a 1D strictly increasing sequence.")
+    if x.size != y.shape[0]:
+        raise ValueError(f'Shapes of x {x.shape} and y {y.shape} are incompatible')
+    if k > 0 and np.any((x < t[k]) | (x > t[-k])):
+        raise ValueError(f'Out of bounds w/ x = {x}.')
+    if x.size != w.size:
+        raise ValueError(f'Shapes of x {x.shape} and w {w.shape} are incompatible')
+    if method == "norm-eq" and np.any(x[1:] - x[:-1] <= 0):
+        raise ValueError("Expect x to be a 1D strictly increasing sequence.")
+    if method == "qr" and any(x[1:] - x[:-1] < 0):
+        raise ValueError("Expect x to be a 1D non-decreasing sequence.")
+
+    # number of coefficients
+    n = t.size - k - 1
+
+    # complex y: view as float, preserve the length
+    was_complex =  y.dtype.kind == 'c'
+    yy = y.view(float)
+    if was_complex and y.ndim == 1:
+        yy = yy.reshape(y.shape[0], 2)
+
+    # multiple r.h.s
+    extradim = prod(yy.shape[1:])
+    yy = yy.reshape(-1, extradim)
+
+    # complex y: view as float, preserve the length
+    was_complex =  y.dtype.kind == 'c'
+    yy = y.view(float)
+    if was_complex and y.ndim == 1:
+        yy = yy.reshape(y.shape[0], 2)
+
+    # multiple r.h.s
+    extradim = prod(yy.shape[1:])
+    yy = yy.reshape(-1, extradim)
+
+    if method == "norm-eq":
+        # construct A.T @ A and rhs with A the colocation matrix, and
+        # rhs = A.T @ y for solving the LSQ problem  ``A.T @ A @ c = A.T @ y``
+        lower = True
+        ab = np.zeros((k+1, n), dtype=np.float64, order='F')
+        rhs = np.zeros((n, extradim), dtype=np.float64)
+        _dierckx._norm_eq_lsq(x, t, k,
+                              yy,
+                              w,
+                              ab.T, rhs)
+
+        # undo complex -> float and flattening the trailing dims
+        if was_complex:
+            rhs = rhs.view(complex)
+
+        rhs = rhs.reshape((n,) + y.shape[1:])
+
+        # have observation matrix & rhs, can solve the LSQ problem
+        cho_decomp = cholesky_banded(ab, overwrite_ab=True, lower=lower,
+                                     check_finite=check_finite)
+        m = rhs.shape[0]
+        c = cho_solve_banded((cho_decomp, lower), rhs.reshape(m, -1), overwrite_b=True,
+                             check_finite=check_finite).reshape(rhs.shape)
+    elif method == "qr":
+        _, _, c, _, _ = _lsq_solve_qr(x, yy, t, k, w)
+
+        if was_complex:
+            c = c.view(complex)
+
+    else:
+        raise ValueError(f"Unknown {method =}.")
+
+
+    # restore the shape of `c` for both single and multiple r.h.s.
+    c = c.reshape((n,) + y.shape[1:])
+    c = np.ascontiguousarray(c)
+    t, c = xp.asarray(t), xp.asarray(c)
+    return BSpline.construct_fast(t, c, k, axis=axis)
+
+
+######################
+# LSQ spline helpers #
+######################
+
+def _lsq_solve_qr_for_root_rati_periodic(x, y, t, k, w):
+    """Solve for the LSQ spline coeffs given x, y and knots.
+
+    `y` is always 2D: for 1D data, the shape is ``(m, 1)``.
+    `w` is always 1D: one weight value per `x` value.
+
+    """
+    y_w = y * w[:, None]
+    # Ref: https://github.com/scipy/scipy/blob/maintenance/1.16.x/scipy/interpolate/fitpack/fpperi.f#L221-L238
+    R, H1, H2, offset, nc = _dierckx.data_matrix_periodic(x, t, k, w, False)
+    # Ref: https://github.com/scipy/scipy/blob/maintenance/1.16.x/scipy/interpolate/fitpack/fpperi.f#L239-L314
+    A1, A2, Z, p, _ = _dierckx.qr_reduce_periodic(
+        R, H1, H2, offset, nc, y_w, k,
+        len(t), True
+    )         # modifies arguments in-place
+    # Ref: https://github.com/scipy/scipy/blob/main/scipy/interpolate/fitpack/fpbacp.f
+    c, residuals, _ = _dierckx.fpbacp(A1, A2, Z, k, k, x, y, t, w)
+    return R, A1, A2, Z, y_w, c, p, residuals
+
+
+def _lsq_solve_qr(x, y, t, k, w, periodic=False):
+    """Solve for the LSQ spline coeffs given x, y and knots.
+
+    `y` is always 2D: for 1D data, the shape is ``(m, 1)``.
+    `w` is always 1D: one weight value per `x` value.
+
+    """
+    y_w = y * w[:, None]
+    if not periodic:
+        A, offset, nc = _dierckx.data_matrix(x, t, k, w)
+        _dierckx.qr_reduce(A, offset, nc, y_w)         # modifies arguments in-place
+        c, residuals, fp = _dierckx.fpback(A, nc, x, y, t, k, w, y_w)
+        return A, y_w, c, fp, residuals
+    else:
+        # Ref: https://github.com/scipy/scipy/blob/maintenance/1.16.x/scipy/interpolate/fitpack/fpperi.f#L221-L238
+        R, H1, H2, offset, nc = _dierckx.data_matrix_periodic(x, t, k, w, False)
+        # Ref: https://github.com/scipy/scipy/blob/maintenance/1.16.x/scipy/interpolate/fitpack/fpperi.f#L239-L314
+        A1, A2, Z, fp = _dierckx.qr_reduce_periodic(
+            R, H1, H2, offset, nc, y_w, k,
+            len(t), False)         # modifies arguments in-place
+        # Ref: https://github.com/scipy/scipy/blob/main/scipy/interpolate/fitpack/fpbacp.f
+        c, residuals, _ = _dierckx.fpbacp(A1, A2, Z, k, k, x, y, t, w)
+        return R, y_w, c, fp, residuals
+
+
+
+
+#############################
+#  Smoothing spline helpers #
+#############################
+
+def _compute_optimal_gcv_parameter(X, wE, y, w):
+    """
+    Returns an optimal regularization parameter from the GCV criteria [1].
+
+    Parameters
+    ----------
+    X : array, shape (5, n)
+        5 bands of the design matrix ``X`` stored in LAPACK banded storage.
+    wE : array, shape (5, n)
+        5 bands of the penalty matrix :math:`W^{-1} E` stored in LAPACK banded
+        storage.
+    y : array, shape (n,)
+        Ordinates.
+    w : array, shape (n,)
+        Vector of weights.
+
+    Returns
+    -------
+    lam : float
+        An optimal from the GCV criteria point of view regularization
+        parameter.
+
+    Notes
+    -----
+    No checks are performed.
+
+    References
+    ----------
+    .. [1] G. Wahba, "Estimating the smoothing parameter" in Spline models
+        for observational data, Philadelphia, Pennsylvania: Society for
+        Industrial and Applied Mathematics, 1990, pp. 45-65.
+        :doi:`10.1137/1.9781611970128`
+
+    """
+
+    def compute_banded_symmetric_XT_W_Y(X, w, Y):
+        """
+        Assuming that the product :math:`X^T W Y` is symmetric and both ``X``
+        and ``Y`` are 5-banded, compute the unique bands of the product.
+
+        Parameters
+        ----------
+        X : array, shape (5, n)
+            5 bands of the matrix ``X`` stored in LAPACK banded storage.
+        w : array, shape (n,)
+            Array of weights
+        Y : array, shape (5, n)
+            5 bands of the matrix ``Y`` stored in LAPACK banded storage.
+
+        Returns
+        -------
+        res : array, shape (4, n)
+            The result of the product :math:`X^T Y` stored in the banded way.
+
+        Notes
+        -----
+        As far as the matrices ``X`` and ``Y`` are 5-banded, their product
+        :math:`X^T W Y` is 7-banded. It is also symmetric, so we can store only
+        unique diagonals.
+
+        """
+        # compute W Y
+        W_Y = np.copy(Y)
+
+        W_Y[2] *= w
+        for i in range(2):
+            W_Y[i, 2 - i:] *= w[:-2 + i]
+            W_Y[3 + i, :-1 - i] *= w[1 + i:]
+
+        n = X.shape[1]
+        res = np.zeros((4, n))
+        for i in range(n):
+            for j in range(min(n-i, 4)):
+                res[-j-1, i + j] = sum(X[j:, i] * W_Y[:5-j, i + j])
+        return res
+
+    def compute_b_inv(A):
+        """
+        Inverse 3 central bands of matrix :math:`A=U^T D^{-1} U` assuming that
+        ``U`` is a unit upper triangular banded matrix using an algorithm
+        proposed in [1].
+
+        Parameters
+        ----------
+        A : array, shape (4, n)
+            Matrix to inverse, stored in LAPACK banded storage.
+
+        Returns
+        -------
+        B : array, shape (4, n)
+            3 unique bands of the symmetric matrix that is an inverse to ``A``.
+            The first row is filled with zeros.
+
+        Notes
+        -----
+        The algorithm is based on the cholesky decomposition and, therefore,
+        in case matrix ``A`` is close to not positive defined, the function
+        raises LinalgError.
+
+        Both matrices ``A`` and ``B`` are stored in LAPACK banded storage.
+
+        References
+        ----------
+        .. [1] M. F. Hutchinson and F. R. de Hoog, "Smoothing noisy data with
+            spline functions," Numerische Mathematik, vol. 47, no. 1,
+            pp. 99-106, 1985.
+            :doi:`10.1007/BF01389878`
+
+        """
+
+        def find_b_inv_elem(i, j, U, D, B):
+            rng = min(3, n - i - 1)
+            rng_sum = 0.
+            if j == 0:
+                # use 2-nd formula from [1]
+                for k in range(1, rng + 1):
+                    rng_sum -= U[-k - 1, i + k] * B[-k - 1, i + k]
+                rng_sum += D[i]
+                B[-1, i] = rng_sum
+            else:
+                # use 1-st formula from [1]
+                for k in range(1, rng + 1):
+                    diag = abs(k - j)
+                    ind = i + min(k, j)
+                    rng_sum -= U[-k - 1, i + k] * B[-diag - 1, ind + diag]
+                B[-j - 1, i + j] = rng_sum
+
+        U = cholesky_banded(A)
+        for i in range(2, 5):
+            U[-i, i-1:] /= U[-1, :-i+1]
+        D = 1. / (U[-1])**2
+        U[-1] /= U[-1]
+
+        n = U.shape[1]
+
+        B = np.zeros(shape=(4, n))
+        for i in range(n - 1, -1, -1):
+            for j in range(min(3, n - i - 1), -1, -1):
+                find_b_inv_elem(i, j, U, D, B)
+        # the first row contains garbage and should be removed
+        B[0] = [0.] * n
+        return B
+
+    def _gcv(lam, X, XtWX, wE, XtE, y):
+        r"""
+        Computes the generalized cross-validation criteria [1].
+
+        Parameters
+        ----------
+        lam : float, (:math:`\lambda \geq 0`)
+            Regularization parameter.
+        X : array, shape (5, n)
+            Matrix is stored in LAPACK banded storage.
+        XtWX : array, shape (4, n)
+            Product :math:`X^T W X` stored in LAPACK banded storage.
+        wE : array, shape (5, n)
+            Matrix :math:`W^{-1} E` stored in LAPACK banded storage.
+        XtE : array, shape (4, n)
+            Product :math:`X^T E` stored in LAPACK banded storage.
+
+        Returns
+        -------
+        res : float
+            Value of the GCV criteria with the regularization parameter
+            :math:`\lambda`.
+
+        Notes
+        -----
+        Criteria is computed from the formula (1.3.2) [3]:
+
+        .. math:
+
+        GCV(\lambda) = \dfrac{1}{n} \sum\limits_{k = 1}^{n} \dfrac{ \left(
+        y_k - f_{\lambda}(x_k) \right)^2}{\left( 1 - \Tr{A}/n\right)^2}$.
+        The criteria is discussed in section 1.3 [3].
+
+        The numerator is computed using (2.2.4) [3] and the denominator is
+        computed using an algorithm from [2] (see in the ``compute_b_inv``
+        function).
+
+        References
+        ----------
+        .. [1] G. Wahba, "Estimating the smoothing parameter" in Spline models
+            for observational data, Philadelphia, Pennsylvania: Society for
+            Industrial and Applied Mathematics, 1990, pp. 45-65.
+            :doi:`10.1137/1.9781611970128`
+        .. [2] M. F. Hutchinson and F. R. de Hoog, "Smoothing noisy data with
+            spline functions," Numerische Mathematik, vol. 47, no. 1,
+            pp. 99-106, 1985.
+            :doi:`10.1007/BF01389878`
+        .. [3] E. Zemlyanoy, "Generalized cross-validation smoothing splines",
+            BSc thesis, 2022. Might be available (in Russian)
+            `here <https://www.hse.ru/ba/am/students/diplomas/620910604>`_
+
+        """
+        # Compute the numerator from (2.2.4) [3]
+        n = X.shape[1]
+        c = solve_banded((2, 2), X + lam * wE, y)
+        res = np.zeros(n)
+        # compute ``W^{-1} E c`` with respect to banded-storage of ``E``
+        tmp = wE * c
+        for i in range(n):
+            for j in range(max(0, i - n + 3), min(5, i + 3)):
+                res[i] += tmp[j, i + 2 - j]
+        numer = np.linalg.norm(lam * res)**2 / n
+
+        # compute the denominator
+        lhs = XtWX + lam * XtE
+        try:
+            b_banded = compute_b_inv(lhs)
+            # compute the trace of the product b_banded @ XtX
+            tr = b_banded * XtWX
+            tr[:-1] *= 2
+            # find the denominator
+            denom = (1 - sum(sum(tr)) / n)**2
+        except LinAlgError:
+            # cholesky decomposition cannot be performed
+            raise ValueError('Seems like the problem is ill-posed')
+
+        res = numer / denom
+
+        return res
+
+    n = X.shape[1]
+
+    XtWX = compute_banded_symmetric_XT_W_Y(X, w, X)
+    XtE = compute_banded_symmetric_XT_W_Y(X, w, wE)
+
+    if y.ndim == 1:
+        gcv_est = minimize_scalar(
+            _gcv, bounds=(0, n), method='Bounded', args=(X, XtWX, wE, XtE, y)
+        )
+        if gcv_est.success:
+            return gcv_est.x
+        raise ValueError(f"Unable to find minimum of the GCV "
+                         f"function: {gcv_est.message}")
+    elif y.ndim == 2:
+        gcv_est = np.empty(y.shape[1])
+        for i in range(y.shape[1]):
+            est = minimize_scalar(
+                _gcv, bounds=(0, n), method='Bounded', args=(X, XtWX, wE, XtE, y[:, i])
+            )
+            if est.success:
+               gcv_est[i] = est.x
+            else:
+                raise ValueError(f"Unable to find minimum of the GCV "
+                                 f"function: {gcv_est.message}")
+        return gcv_est
+    else:
+        # trailing dims must have been flattened already.
+        raise RuntimeError("Internal error. Please report it to scipy developers.")
+
+
+def _coeff_of_divided_diff(x):
+    """
+    Returns the coefficients of the divided difference.
+
+    Parameters
+    ----------
+    x : array, shape (n,)
+        Array which is used for the computation of divided difference.
+
+    Returns
+    -------
+    res : array_like, shape (n,)
+        Coefficients of the divided difference.
+
+    Notes
+    -----
+    Vector ``x`` should have unique elements, otherwise an error division by
+    zero might be raised.
+
+    No checks are performed.
+
+    """
+    n = x.shape[0]
+    res = np.zeros(n)
+    for i in range(n):
+        pp = 1.
+        for k in range(n):
+            if k != i:
+                pp *= (x[i] - x[k])
+        res[i] = 1. / pp
+    return res
+
+
+@xp_capabilities(cpu_only=True, jax_jit=False, allow_dask_compute=True)
+def make_smoothing_spline(x, y, w=None, lam=None, *, axis=0):
+    r"""
+    Create a smoothing B-spline satisfying the Generalized Cross Validation (GCV) criterion.
+
+    Compute the (coefficients of) smoothing cubic spline function using
+    ``lam`` to control the tradeoff between the amount of smoothness of the
+    curve and its proximity to the data. In case ``lam`` is None, using the
+    GCV criteria [1] to find it.
+
+    A smoothing spline is found as a solution to the regularized weighted
+    linear regression problem:
+
+    .. math::
+
+        \sum\limits_{i=1}^n w_i\lvert y_i - f(x_i) \rvert^2 +
+        \lambda\int\limits_{x_1}^{x_n} (f^{(2)}(u))^2 d u
+
+    where :math:`f` is a spline function, :math:`w` is a vector of weights and
+    :math:`\lambda` is a regularization parameter.
+
+    If ``lam`` is None, we use the GCV criteria to find an optimal
+    regularization parameter, otherwise we solve the regularized weighted
+    linear regression problem with given parameter. The parameter controls
+    the tradeoff in the following way: the larger the parameter becomes, the
+    smoother the function gets.
+
+    Parameters
+    ----------
+    x : array_like, shape (n,)
+        Abscissas. `n` must be at least 5.
+    y : array_like, shape (n, ...)
+        Ordinates. `n` must be at least 5.
+    w : array_like, shape (n,), optional
+        Vector of weights. Default is ``np.ones_like(x)``.
+    lam : float, (:math:`\lambda \geq 0`), optional
+        Regularization parameter. If ``lam`` is None, then it is found from
+        the GCV criteria. Default is None.
+    axis : int, optional
+        The data axis. Default is zero.
+        The assumption is that ``y.shape[axis] == n``, and all other axes of ``y``
+        are batching axes.
+
+    Returns
+    -------
+    func : `BSpline` object
+        An object representing a spline in the B-spline basis
+        as a solution of the problem of smoothing splines using
+        the GCV criteria [1] in case ``lam`` is None, otherwise using the
+        given parameter ``lam``.
+
+    Notes
+    -----
+    This algorithm is a clean room reimplementation of the algorithm
+    introduced by Woltring in FORTRAN [2]. The original version cannot be used
+    in SciPy source code because of the license issues. The details of the
+    reimplementation are discussed here (available only in Russian) [4].
+
+    If the vector of weights ``w`` is None, we assume that all the points are
+    equal in terms of weights, and vector of weights is vector of ones.
+
+    Note that in weighted residual sum of squares, weights are not squared:
+    :math:`\sum\limits_{i=1}^n w_i\lvert y_i - f(x_i) \rvert^2` while in
+    ``splrep`` the sum is built from the squared weights.
+
+    In cases when the initial problem is ill-posed (for example, the product
+    :math:`X^T W X` where :math:`X` is a design matrix is not a positive
+    defined matrix) a ValueError is raised.
+
+    References
+    ----------
+    .. [1] G. Wahba, "Estimating the smoothing parameter" in Spline models for
+        observational data, Philadelphia, Pennsylvania: Society for Industrial
+        and Applied Mathematics, 1990, pp. 45-65.
+        :doi:`10.1137/1.9781611970128`
+    .. [2] H. J. Woltring, A Fortran package for generalized, cross-validatory
+        spline smoothing and differentiation, Advances in Engineering
+        Software, vol. 8, no. 2, pp. 104-113, 1986.
+        :doi:`10.1016/0141-1195(86)90098-7`
+    .. [3] T. Hastie, J. Friedman, and R. Tisbshirani, "Smoothing Splines" in
+        The elements of Statistical Learning: Data Mining, Inference, and
+        prediction, New York: Springer, 2017, pp. 241-249.
+        :doi:`10.1007/978-0-387-84858-7`
+    .. [4] E. Zemlyanoy, "Generalized cross-validation smoothing splines",
+        BSc thesis, 2022.
+        `<https://www.hse.ru/ba/am/students/diplomas/620910604>`_ (in
+        Russian)
+
+    Examples
+    --------
+    Generate some noisy data
+
+    >>> import numpy as np
+    >>> np.random.seed(1234)
+    >>> n = 200
+    >>> def func(x):
+    ...    return x**3 + x**2 * np.sin(4 * x)
+    >>> x = np.sort(np.random.random_sample(n) * 4 - 2)
+    >>> y = func(x) + np.random.normal(scale=1.5, size=n)
+
+    Make a smoothing spline function
+
+    >>> from scipy.interpolate import make_smoothing_spline
+    >>> spl = make_smoothing_spline(x, y)
+
+    Plot both
+
+    >>> import matplotlib.pyplot as plt
+    >>> grid = np.linspace(x[0], x[-1], 400)
+    >>> plt.plot(x, y, '.')
+    >>> plt.plot(grid, spl(grid), label='Spline')
+    >>> plt.plot(grid, func(grid), label='Original function')
+    >>> plt.legend(loc='best')
+    >>> plt.show()
+
+    """  # noqa:E501
+    xp = array_namespace(x, y)
+
+    x = np.ascontiguousarray(x, dtype=float)
+    y = np.ascontiguousarray(y, dtype=float)
+
+    if any(x[1:] - x[:-1] <= 0):
+        raise ValueError('``x`` should be an ascending array')
+
+    if x.ndim != 1 or x.shape[0] != y.shape[axis]:
+        raise ValueError(f'``x`` should be 1D and {x.shape = } == {y.shape = }')
+
+    if w is None:
+        w = np.ones(len(x))
+    else:
+        w = np.ascontiguousarray(w)
+        if any(w <= 0):
+            raise ValueError('Invalid vector of weights')
+
+    t = np.r_[[x[0]] * 3, x, [x[-1]] * 3]
+    n = x.shape[0]
+
+    if n <= 4:
+        raise ValueError('``x`` and ``y`` length must be at least 5')
+
+    # Internals assume that the data axis is the zero-th axis
+    axis = normalize_axis_index(axis, y.ndim)
+    y = np.moveaxis(y, axis, 0)
+
+    # flatten the trailing axes of y to simplify further manipulations
+    y_shape1 = y.shape[1:]
+    if y_shape1 != ():
+        y = y.reshape((n, -1))
+
+    # It is known that the solution to the stated minimization problem exists
+    # and is a natural cubic spline with vector of knots equal to the unique
+    # elements of ``x`` [3], so we will solve the problem in the basis of
+    # natural splines.
+
+    # create design matrix in the B-spline basis
+    X_bspl = BSpline.design_matrix(x, t, 3)
+    # move from B-spline basis to the basis of natural splines using equations
+    # (2.1.7) [4]
+    # central elements
+    X = np.zeros((5, n))
+    for i in range(1, 4):
+        X[i, 2: -2] = X_bspl[i: i - 4, 3: -3][np.diag_indices(n - 4)]
+
+    # first elements
+    X[1, 1] = X_bspl[0, 0]
+    X[2, :2] = ((x[2] + x[1] - 2 * x[0]) * X_bspl[0, 0],
+                X_bspl[1, 1] + X_bspl[1, 2])
+    X[3, :2] = ((x[2] - x[0]) * X_bspl[1, 1], X_bspl[2, 2])
+
+    # last elements
+    X[1, -2:] = (X_bspl[-3, -3], (x[-1] - x[-3]) * X_bspl[-2, -2])
+    X[2, -2:] = (X_bspl[-2, -3] + X_bspl[-2, -2],
+                 (2 * x[-1] - x[-2] - x[-3]) * X_bspl[-1, -1])
+    X[3, -2] = X_bspl[-1, -1]
+
+    # create penalty matrix and divide it by vector of weights: W^{-1} E
+    wE = np.zeros((5, n))
+    wE[2:, 0] = _coeff_of_divided_diff(x[:3]) / w[:3]
+    wE[1:, 1] = _coeff_of_divided_diff(x[:4]) / w[:4]
+    for j in range(2, n - 2):
+        wE[:, j] = (x[j+2] - x[j-2]) * _coeff_of_divided_diff(x[j-2:j+3])\
+                   / w[j-2: j+3]
+
+    wE[:-1, -2] = -_coeff_of_divided_diff(x[-4:]) / w[-4:]
+    wE[:-2, -1] = _coeff_of_divided_diff(x[-3:]) / w[-3:]
+    wE *= 6
+
+    if lam is None:
+        lam = _compute_optimal_gcv_parameter(X, wE, y, w)
+    elif lam < 0.:
+        raise ValueError('Regularization parameter should be non-negative')
+
+    # solve the initial problem in the basis of natural splines
+    if np.ndim(lam) == 0:
+        c = solve_banded((2, 2), X + lam * wE, y)
+    elif np.ndim(lam) == 1:
+        # XXX: solve_banded does not suppport batched `ab` matrices; loop manually
+        c = np.empty((n, lam.shape[0]))
+        for i in range(lam.shape[0]):
+            c[:, i] = solve_banded((2, 2), X + lam[i] * wE, y[:, i])
+    else:
+        # this should not happen, ever
+        raise RuntimeError("Internal error, please report it to SciPy developers.")
+    c = c.reshape((c.shape[0], *y_shape1))
+
+    # hack: these are c[0], c[1] etc, shape-compatible with np.r_ below
+    c0, c1 = c[0:1, ...], c[1:2, ...]     # c[0], c[1]
+    cm0, cm1 = c[-1:-2:-1, ...], c[-2:-3:-1, ...]    # c[-1], c[-2]
+
+    # move back to B-spline basis using equations (2.2.10) [4]
+    c_ = np.r_[c0 * (t[5] + t[4] - 2 * t[3]) + c1,
+               c0 * (t[5] - t[3]) + c1,
+               c[1: -1, ...],
+               cm0 * (t[-4] - t[-6]) + cm1,
+               cm0 * (2 * t[-4] - t[-5] - t[-6]) + cm1]
+
+    t, c_ = xp.asarray(t), xp.asarray(c_)
+    return BSpline.construct_fast(t, c_, 3, axis=axis)
+
+
+########################
+#  FITPACK look-alikes #
+########################
+
+def fpcheck(x, t, k, periodic=False):
+    """Check consistency of data vector `x` and knot vector `t`.
+
+    Parameters
+    ----------
+    x : array_like, shape (m,)
+        1D sorted array of data points.
+    t : array_like, shape (n,)
+        1D non-decreasing knot vector.
+    k : int
+        Degree of the spline.
+    periodic : bool, optional
+        Whether the spline is periodic. Default is False.
+
+    Raises
+    ------
+    ValueError
+        If the configuration of `x`, `t`, and `k` violates any required condition.
+    """
+    # This routine is a unified clone of the FITPACK Fortran routines `fpchec.f`
+    # and `fpchep.f`:
+    # - https://github.com/scipy/scipy/blob/main/scipy/interpolate/fitpack/fpchec.f
+    # - https://github.com/scipy/scipy/blob/main/scipy/interpolate/fitpack/fpchep.f
+    #
+    # These routines verify the number and position of the knots t(j), j=1,...,n,
+    # of a spline of degree k, relative to the number and distribution of data points
+    # x(i), i=1,...,m. If all of the following conditions are fulfilled,
+    # validation passes.
+    #
+    # For non-periodic splines:
+    #   1) k+1 <= n-k-1 <= m
+    #   2) t(1) <= t(2) <= ... <= t(k+1)
+    #      t(n-k) <= t(n-k+1) <= ... <= t(n)
+    #   3) t(k+1) < t(k+2) < ... < t(n-k)
+    #   4) t(k+1) <= x(i) <= t(n-k)
+    #   5) Schoenberg-Whitney conditions hold: there exists a subset y(j) such that
+    #        t(j) < y(j) < t(j+k+1), for j = 1, ..., n-k-1
+    #
+    # For periodic splines:
+    #   1) k+1 <= n-k-1 <= m + k - 1
+    #   2) Same boundary knot monotonicity as above
+    #   3) Same strict interior knot increase as above
+    #   4) t(k+1) <= x(i) <= t(n-k)
+    #   5) Schoenberg-Whitney conditions must hold for *some periodic shift*
+    #        of the data sequence; i.e. wrapped data points x(i) must satisfy
+    #        t(j) < y(j) < t(j+k+1), j = k+1, ..., n-k-1
+    x = np.asarray(x)
+    t = np.asarray(t)
+
+    if x.ndim != 1 or t.ndim != 1:
+        raise ValueError(f"Expect `x` and `t` be 1D sequences. Got {x = } and {t = }")
+
+    m = x.shape[0]
+    n = t.shape[0]
+    nk1 = n - k - 1
+
+    # check condition no 1
+    if periodic:
+        # c      1) k+1 <= nk1 <= m+k-1
+        if not (k + 1 <= nk1 <= m + k - 1):
+            raise ValueError(f"Need k+1 <= n-k-1 <= m+k-1. Got {m = }, {n = }, {k = }")
+    else:
+        # c      1) k+1 <= n-k-1 <= m
+        if not (k + 1 <= nk1 <= m):
+            raise ValueError(f"Need k+1 <= n-k-1 <= m. Got {m = }, {n = } and {k = }.")
+
+    # check condition no 2
+    # c      2) t(1) <= t(2) <= ... <= t(k+1)
+    # c         t(n-k) <= t(n-k+1) <= ... <= t(n)
+    if (t[:k+1] > t[1:k+2]).any():
+        raise ValueError(f"First k knots must be ordered; got {t = }.")
+
+    if (t[nk1:] < t[nk1-1:-1]).any():
+        raise ValueError(f"Last k knots must be ordered; got {t = }.")
+
+    # c  check condition no 3
+    # c      3) t(k+1) < t(k+2) < ... < t(n-k)
+    if (t[k+1:n-k] <= t[k:n-k-1]).any():
+        raise ValueError(f"Internal knots must be distinct. Got {t = }.")
+
+    # c  check condition no 4
+    # c      4) t(k+1) <= x(i) <= t(n-k)
+    # NB: FITPACK's fpchec only checks x[0] & x[-1], so we follow.
+    if (x[0] < t[k]) or (x[-1] > t[n-k-1]):
+        raise ValueError(f"Out of bounds: {x = } and {t = }.")
+
+    # c  check condition no 5
+    # c      5) the conditions specified by Schoenberg and Whitney must hold
+    # c         for at least one subset of data points y(j) such that
+    # c             t(j) < y(j) < t(j+k+1)
+    # c
+    # c         For non-periodic splines:
+    # c             j = 1, 2, ..., n-k-1 (i.e., j in [1, n-k-1])
+    # c             The data points must lie strictly inside some B-spline supports.
+    # c
+    # c         For periodic splines:
+    # c             j = k+1, ..., n-k-1
+    # c             The condition must hold for a wrapped subset of the data points,
+    # c             i.e., there exists a cyclic shift of the data such that
+    # c                 t(j) < x(i) < t(j+k+1)
+    # c             holds for all j in that range. The test must account for the
+    # c             periodic domain length: per = t(n-k) - t(k+1), and wrap around x(i)
+    # c             as x(i) + per if needed.
+    mesg = f"Schoenberg-Whitney condition is violated with {t = } and {x =}."
+
+    if periodic:
+        per = t[n - k - 1] - t[k]
+        m1 = m - 1
+        for shift in range(1, m):
+            for j in range(k, nk1):
+                tj = t[j]
+                tl = t[j + k + 1]
+                found = False
+                for i in range(shift, shift + m1 + 1):
+                    idx = i if i < m else i - m
+                    xi = x[idx] + (0 if i < m else per)
+                    if tj < xi < tl:
+                        found = True
+                        break
+                if not found:
+                    break
+            else:
+                return
+        raise ValueError(mesg)
+    else:
+        if (x[0] >= t[k+1]) or (x[-1] <= t[n-k-2]):
+            raise ValueError(mesg)
+
+        m = x.shape[0]
+        l = k+1
+        nk3 = n - k - 3
+        if nk3 < 2:
+            return
+        for j in range(1, nk3+1):
+            tj = t[j]
+            l += 1
+            tl = t[l]
+            i = np.argmax(x > tj)
+            if i >= m-1:
+                raise ValueError(mesg)
+            if x[i] >= tl:
+                raise ValueError(mesg)
+        return

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_cubic.py

@@ -0,0 +1,1029 @@
+"""Interpolation algorithms using piecewise cubic polynomials."""
+
+from typing import Literal
+
+import numpy as np
+
+from scipy.linalg import solve, solve_banded
+from scipy._lib._array_api import array_namespace, xp_size, xp_capabilities
+from scipy._lib.array_api_compat import numpy as np_compat
+
+from . import PPoly
+from ._polyint import _isscalar
+
+__all__ = ["CubicHermiteSpline", "PchipInterpolator", "pchip_interpolate",
+           "Akima1DInterpolator", "CubicSpline"]
+
+
+def prepare_input(x, y, axis, dydx=None, xp=None):
+    """Prepare input for cubic spline interpolators.
+
+    All data are converted to numpy arrays and checked for correctness.
+    Axes equal to `axis` of arrays `y` and `dydx` are moved to be the 0th
+    axis. The value of `axis` is converted to lie in
+    [0, number of dimensions of `y`).
+    """
+
+    x, y = map(xp.asarray, (x, y))
+    if xp.isdtype(x.dtype, "complex floating"):
+        raise ValueError("`x` must contain real values.")
+    x = xp.astype(x, xp.float64)
+
+    if xp.isdtype(y.dtype, "complex floating"):
+        dtype = xp.complex128
+    else:
+        dtype = xp.float64
+
+    if dydx is not None:
+        dydx = xp.asarray(dydx)
+        if y.shape != dydx.shape:
+            raise ValueError("The shapes of `y` and `dydx` must be identical.")
+        if xp.isdtype(dydx.dtype, "complex floating"):
+            dtype = xp.complex128
+        dydx = xp.astype(dydx, dtype, copy=False)
+
+    y = xp.astype(y, dtype, copy=False)
+    axis = axis % y.ndim
+    if x.ndim != 1:
+        raise ValueError("`x` must be 1-dimensional.")
+    if x.shape[0] < 2:
+        raise ValueError("`x` must contain at least 2 elements.")
+    if x.shape[0] != y.shape[axis]:
+        raise ValueError(f"The length of `y` along `axis`={axis} doesn't "
+                         "match the length of `x`")
+
+    if not xp.all(xp.isfinite(x)):
+        raise ValueError("`x` must contain only finite values.")
+    if not xp.all(xp.isfinite(y)):
+        raise ValueError("`y` must contain only finite values.")
+
+    if dydx is not None and not xp.all(xp.isfinite(dydx)):
+        raise ValueError("`dydx` must contain only finite values.")
+
+    dx = xp.diff(x)
+    if xp.any(dx <= 0):
+        raise ValueError("`x` must be strictly increasing sequence.")
+
+    y = xp.moveaxis(y, axis, 0)
+    if dydx is not None:
+        dydx = xp.moveaxis(dydx, axis, 0)
+
+    return x, dx, y, axis, dydx
+
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class CubicHermiteSpline(PPoly):
+    """Piecewise cubic interpolator to fit values and first derivatives (C1 smooth).
+
+    The result is represented as a `PPoly` instance.
+
+    Parameters
+    ----------
+    x : array_like, shape (n,)
+        1-D array containing values of the independent variable.
+        Values must be real, finite and in strictly increasing order.
+    y : array_like
+        Array containing values of the dependent variable. It can have
+        arbitrary number of dimensions, but the length along ``axis``
+        (see below) must match the length of ``x``. Values must be finite.
+    dydx : array_like
+        Array containing derivatives of the dependent variable. It can have
+        arbitrary number of dimensions, but the length along ``axis``
+        (see below) must match the length of ``x``. Values must be finite.
+    axis : int, optional
+        Axis along which `y` is assumed to be varying. Meaning that for
+        ``x[i]`` the corresponding values are ``np.take(y, i, axis=axis)``.
+        Default is 0.
+    extrapolate : {bool, 'periodic', None}, optional
+        If bool, determines whether to extrapolate to out-of-bounds points
+        based on first and last intervals, or to return NaNs. If 'periodic',
+        periodic extrapolation is used. If None (default), it is set to True.
+
+    Attributes
+    ----------
+    x : ndarray, shape (n,)
+        Breakpoints. The same ``x`` which was passed to the constructor.
+    c : ndarray, shape (4, n-1, ...)
+        Coefficients of the polynomials on each segment. The trailing
+        dimensions match the dimensions of `y`, excluding ``axis``.
+        For example, if `y` is 1-D, then ``c[k, i]`` is a coefficient for
+        ``(x-x[i])**(3-k)`` on the segment between ``x[i]`` and ``x[i+1]``.
+    axis : int
+        Interpolation axis. The same axis which was passed to the
+        constructor.
+
+    Methods
+    -------
+    __call__
+    derivative
+    antiderivative
+    integrate
+    solve
+    roots
+
+    See Also
+    --------
+    Akima1DInterpolator : Akima 1D interpolator.
+    PchipInterpolator : PCHIP 1-D monotonic cubic interpolator.
+    CubicSpline : Cubic spline data interpolator.
+    PPoly : Piecewise polynomial in terms of coefficients and breakpoints
+
+    Notes
+    -----
+    If you want to create a higher-order spline matching higher-order
+    derivatives, use `BPoly.from_derivatives`.
+
+    References
+    ----------
+    .. [1] `Cubic Hermite spline
+            <https://en.wikipedia.org/wiki/Cubic_Hermite_spline>`_
+            on Wikipedia.
+    """
+
+    def __init__(self, x, y, dydx, axis=0, extrapolate=None):
+        xp = array_namespace(x, y, dydx)
+
+        if extrapolate is None:
+            extrapolate = True
+
+        x, dx, y, axis, dydx = prepare_input(x, y, axis, dydx, xp=xp)
+
+        dxr = xp.reshape(dx, (dx.shape[0], ) + (1, ) * (y.ndim - 1))
+        slope = xp.diff(y, axis=0) / dxr
+        t = (dydx[:-1, ...] + dydx[1:, ...] - 2 * slope) / dxr
+
+        c = xp.stack((
+           t / dxr,
+           (slope - dydx[:-1, ...]) / dxr - t,
+           dydx[:-1, ...],
+           y[:-1, ...]
+        ))
+
+        super().__init__(c, x, extrapolate=extrapolate)
+        self.axis = axis
+
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class PchipInterpolator(CubicHermiteSpline):
+    r"""PCHIP shape-preserving interpolator (C1 smooth).
+
+    ``x`` and ``y`` are arrays of values used to approximate some function f,
+    with ``y = f(x)``. The interpolant uses monotonic cubic splines
+    to find the value of new points. (PCHIP stands for Piecewise Cubic
+    Hermite Interpolating Polynomial).
+
+    Parameters
+    ----------
+    x : ndarray, shape (npoints, )
+        A 1-D array of monotonically increasing real values. ``x`` cannot
+        include duplicate values (otherwise f is overspecified)
+    y : ndarray, shape (..., npoints, ...)
+        An N-D array of real values. ``y``'s length along the interpolation
+        axis must be equal to the length of ``x``. Use the ``axis``
+        parameter to select the interpolation axis.
+    axis : int, optional
+        Axis in the ``y`` array corresponding to the x-coordinate values. Defaults
+        to ``axis=0``.
+    extrapolate : bool, optional
+        Whether to extrapolate to out-of-bounds points based on first
+        and last intervals, or to return NaNs.
+
+    Methods
+    -------
+    __call__
+    derivative
+    antiderivative
+    integrate
+    solve
+    roots
+
+
+    See Also
+    --------
+    CubicHermiteSpline : Piecewise-cubic interpolator.
+    Akima1DInterpolator : Akima 1D interpolator.
+    CubicSpline : Cubic spline data interpolator.
+    PPoly : Piecewise polynomial in terms of coefficients and breakpoints.
+
+    Notes
+    -----
+    The interpolator preserves monotonicity in the interpolation data and does
+    not overshoot if the data is not smooth.
+
+    The first derivatives are guaranteed to be continuous, but the second
+    derivatives may jump at :math:`x_k`.
+
+    Determines the derivatives at the points :math:`x_k`, :math:`f'_k`,
+    by using PCHIP algorithm [1]_.
+
+    Let :math:`h_k = x_{k+1} - x_k`, and  :math:`d_k = (y_{k+1} - y_k) / h_k`
+    are the slopes at internal points :math:`x_k`.
+    If the signs of :math:`d_k` and :math:`d_{k-1}` are different or either of
+    them equals zero, then :math:`f'_k = 0`. Otherwise, it is given by the
+    weighted harmonic mean
+
+    .. math::
+
+        \frac{w_1 + w_2}{f'_k} = \frac{w_1}{d_{k-1}} + \frac{w_2}{d_k}
+
+    where :math:`w_1 = 2 h_k + h_{k-1}` and :math:`w_2 = h_k + 2 h_{k-1}`.
+
+    The end slopes are set using a one-sided scheme [2]_.
+
+
+    References
+    ----------
+    .. [1] F. N. Fritsch and J. Butland,
+           A method for constructing local
+           monotone piecewise cubic interpolants,
+           SIAM J. Sci. Comput., 5(2), 300-304 (1984).
+           :doi:`10.1137/0905021`.
+    .. [2] C. Moler, Numerical Computing with Matlab, 2004.
+           :doi:`10.1137/1.9780898717952`
+
+    """
+
+    # PchipInterpolator is not generic in scipy-stubs
+    __class_getitem__ = None
+
+    def __init__(self, x, y, axis=0, extrapolate=None):
+        xp = array_namespace(x, y)
+        x, _, y, axis, _ = prepare_input(x, y, axis, xp=xp)
+        if xp.isdtype(y.dtype, "complex floating"):
+            msg = ("`PchipInterpolator` only works with real values for `y`. "
+                   "If you are trying to use the real components of the passed array, "
+                   "use `np.real` on the array before passing to `PchipInterpolator`.")
+            raise ValueError(msg)
+        xv = xp.reshape(x, (x.shape[0],) + (1,)*(y.ndim-1))
+        dk = self._find_derivatives(xv, y, xp=xp)
+        super().__init__(x, y, dk, axis=0, extrapolate=extrapolate)
+        self.axis = axis
+
+    @staticmethod
+    def _edge_case(h0, h1, m0, m1, xp):
+        # one-sided three-point estimate for the derivative
+        d = ((2*h0 + h1)*m0 - h0*m1) / (h0 + h1)
+
+        # try to preserve shape
+        mask = xp.sign(d) != xp.sign(m0)
+        mask2 = (xp.sign(m0) != xp.sign(m1)) & (xp.abs(d) > 3.*xp.abs(m0))
+        mmm = (~mask) & mask2
+
+        d[mask] = 0.
+        d[mmm] = 3.*m0[mmm]
+
+        return d
+
+    @staticmethod
+    def _find_derivatives(x, y, xp):
+        # Determine the derivatives at the points y_k, d_k, by using
+        #  PCHIP algorithm is:
+        # We choose the derivatives at the point x_k by
+        # Let m_k be the slope of the kth segment (between k and k+1)
+        # If m_k=0 or m_{k-1}=0 or sgn(m_k) != sgn(m_{k-1}) then d_k == 0
+        # else use weighted harmonic mean:
+        #   w_1 = 2h_k + h_{k-1}, w_2 = h_k + 2h_{k-1}
+        #   1/d_k = 1/(w_1 + w_2)*(w_1 / m_k + w_2 / m_{k-1})
+        #   where h_k is the spacing between x_k and x_{k+1}
+        y_shape = y.shape
+        if y.ndim == 1:
+            # So that _edge_case doesn't end up assigning to scalars
+            x = x[:, None]
+            y = y[:, None]
+
+        hk = x[1:] - x[:-1]
+        mk = (y[1:] - y[:-1]) / hk
+
+        if y.shape[0] == 2:
+            # edge case: only have two points, use linear interpolation
+            dk = xp.zeros_like(y)
+            dk[0] = mk
+            dk[1] = mk
+            return xp.reshape(dk, y_shape)
+
+        smk = xp.sign(mk)
+        condition = (smk[1:] != smk[:-1]) | (mk[1:] == 0) | (mk[:-1] == 0)
+
+        w1 = 2*hk[1:] + hk[:-1]
+        w2 = hk[1:] + 2*hk[:-1]
+
+        # values where division by zero occurs will be excluded
+        # by 'condition' afterwards
+        with np.errstate(divide='ignore', invalid='ignore'):
+            whmean = (w1/mk[:-1] + w2/mk[1:]) / (w1 + w2)
+
+        dk = np.zeros_like(y)
+        dk[1:-1][condition] = 0.0
+        dk[1:-1][~condition] = 1.0 / whmean[~condition]
+
+        # special case endpoints, as suggested in
+        # Cleve Moler, Numerical Computing with MATLAB, Chap 3.6 (pchiptx.m)
+        dk[0] = PchipInterpolator._edge_case(hk[0], hk[1], mk[0], mk[1], xp=xp)
+        dk[-1] = PchipInterpolator._edge_case(hk[-1], hk[-2], mk[-1], mk[-2], xp=xp)
+
+        return xp.reshape(dk, y_shape)
+
+
+def pchip_interpolate(xi, yi, x, der=0, axis=0):
+    """
+    Convenience function for pchip interpolation.
+
+    xi and yi are arrays of values used to approximate some function f,
+    with ``yi = f(xi)``. The interpolant uses monotonic cubic splines
+    to find the value of new points x and the derivatives there.
+
+    See `scipy.interpolate.PchipInterpolator` for details.
+
+    Parameters
+    ----------
+    xi : array_like
+        A sorted list of x-coordinates, of length N.
+    yi : array_like
+        A 1-D array of real values. `yi`'s length along the interpolation
+        axis must be equal to the length of `xi`. If N-D array, use axis
+        parameter to select correct axis.
+    x : scalar or array_like
+        Of length M.
+    der : int or list, optional
+        Derivatives to extract. The 0th derivative can be included to
+        return the function value.
+    axis : int, optional
+        Axis in the yi array corresponding to the x-coordinate values.
+
+    Returns
+    -------
+    y : scalar or array_like
+        The result, of length R or length M or M by R.
+
+    See Also
+    --------
+    PchipInterpolator : PCHIP 1-D monotonic cubic interpolator.
+
+    Examples
+    --------
+    We can interpolate 2D observed data using pchip interpolation:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> from scipy.interpolate import pchip_interpolate
+    >>> x_observed = np.linspace(0.0, 10.0, 11)
+    >>> y_observed = np.sin(x_observed)
+    >>> x = np.linspace(min(x_observed), max(x_observed), num=100)
+    >>> y = pchip_interpolate(x_observed, y_observed, x)
+    >>> plt.plot(x_observed, y_observed, "o", label="observation")
+    >>> plt.plot(x, y, label="pchip interpolation")
+    >>> plt.legend()
+    >>> plt.show()
+
+    """
+    P = PchipInterpolator(xi, yi, axis=axis)
+
+    if der == 0:
+        return P(x)
+    elif _isscalar(der):
+        return P.derivative(der)(x)
+    else:
+        return [P.derivative(nu)(x) for nu in der]
+
+
+@xp_capabilities(cpu_only=True, xfail_backends=[
+    ("dask.array", "lacks nd fancy indexing"),
+    ("jax.numpy", "immutable arrays"),
+    ("array_api_strict", "fancy indexing __setitem__"),
+])
+class Akima1DInterpolator(CubicHermiteSpline):
+    r"""Akima "visually pleasing" interpolator (C1 smooth).
+
+    Fit piecewise cubic polynomials, given vectors x and y. The interpolation
+    method by Akima uses a continuously differentiable sub-spline built from
+    piecewise cubic polynomials. The resultant curve passes through the given
+    data points and will appear smooth and natural.
+
+    Parameters
+    ----------
+    x : ndarray, shape (npoints, )
+        1-D array of monotonically increasing real values.
+    y : ndarray, shape (..., npoints, ...)
+        N-D array of real values. The length of ``y`` along the interpolation axis
+        must be equal to the length of ``x``. Use the ``axis`` parameter to
+        select the interpolation axis.
+    axis : int, optional
+        Axis in the ``y`` array corresponding to the x-coordinate values. Defaults
+        to ``axis=0``.
+    method : {'akima', 'makima'}, optional
+        If ``"makima"``, use the modified Akima interpolation [2]_.
+        Defaults to ``"akima"``, use the Akima interpolation [1]_.
+
+        .. versionadded:: 1.13.0
+
+    extrapolate : {bool, None}, optional
+        If bool, determines whether to extrapolate to out-of-bounds points
+        based on first and last intervals, or to return NaNs. If None,
+        ``extrapolate`` is set to False.
+
+    Methods
+    -------
+    __call__
+    derivative
+    antiderivative
+    integrate
+    solve
+    roots
+
+    See Also
+    --------
+    PchipInterpolator : PCHIP 1-D monotonic cubic interpolator.
+    CubicSpline : Cubic spline data interpolator.
+    PPoly : Piecewise polynomial in terms of coefficients and breakpoints
+
+    Notes
+    -----
+    .. versionadded:: 0.14
+
+    Use only for precise data, as the fitted curve passes through the given
+    points exactly. This routine is useful for plotting a pleasingly smooth
+    curve through a few given points for purposes of plotting.
+
+    Let :math:`\delta_i = (y_{i+1} - y_i) / (x_{i+1} - x_i)` be the slopes of
+    the interval :math:`\left[x_i, x_{i+1}\right)`. Akima's derivative at
+    :math:`x_i` is defined as:
+
+    .. math::
+
+        d_i = \frac{w_1}{w_1 + w_2}\delta_{i-1} + \frac{w_2}{w_1 + w_2}\delta_i
+
+    In the Akima interpolation [1]_ (``method="akima"``), the weights are:
+
+    .. math::
+
+        \begin{aligned}
+        w_1 &= |\delta_{i+1} - \delta_i| \\
+        w_2 &= |\delta_{i-1} - \delta_{i-2}|
+        \end{aligned}
+
+    In the modified Akima interpolation [2]_ (``method="makima"``),
+    to eliminate overshoot and avoid edge cases of both numerator and
+    denominator being equal to 0, the weights are modified as follows:
+
+    .. math::
+
+        \begin{align*}
+        w_1 &= |\delta_{i+1} - \delta_i| + |\delta_{i+1} + \delta_i| / 2 \\
+        w_2 &= |\delta_{i-1} - \delta_{i-2}| + |\delta_{i-1} + \delta_{i-2}| / 2
+        \end{align*}
+
+    Examples
+    --------
+    Comparison of ``method="akima"`` and ``method="makima"``:
+
+    >>> import numpy as np
+    >>> from scipy.interpolate import Akima1DInterpolator
+    >>> import matplotlib.pyplot as plt
+    >>> x = np.linspace(1, 7, 7)
+    >>> y = np.array([-1, -1, -1, 0, 1, 1, 1])
+    >>> xs = np.linspace(min(x), max(x), num=100)
+    >>> y_akima = Akima1DInterpolator(x, y, method="akima")(xs)
+    >>> y_makima = Akima1DInterpolator(x, y, method="makima")(xs)
+
+    >>> fig, ax = plt.subplots()
+    >>> ax.plot(x, y, "o", label="data")
+    >>> ax.plot(xs, y_akima, label="akima")
+    >>> ax.plot(xs, y_makima, label="makima")
+    >>> ax.legend()
+    >>> fig.show()
+
+    The overshoot that occurred in ``"akima"`` has been avoided in ``"makima"``.
+
+    References
+    ----------
+    .. [1] A new method of interpolation and smooth curve fitting based
+           on local procedures. Hiroshi Akima, J. ACM, October 1970, 17(4),
+           589-602. :doi:`10.1145/321607.321609`
+    .. [2] Makima Piecewise Cubic Interpolation. Cleve Moler and Cosmin Ionita, 2019.
+           https://blogs.mathworks.com/cleve/2019/04/29/makima-piecewise-cubic-interpolation/
+
+    """
+
+    # PchipInterpolator is not generic in scipy-stubs
+    __class_getitem__ = None
+
+    def __init__(self, x, y, axis=0, *, method: Literal["akima", "makima"]="akima",
+                 extrapolate:bool | None = None):
+        if method not in {"akima", "makima"}:
+            raise NotImplementedError(f"`method`={method} is unsupported.")
+        # Original implementation in MATLAB by N. Shamsundar (BSD licensed), see
+        # https://www.mathworks.com/matlabcentral/fileexchange/1814-akima-interpolation
+
+        xp = array_namespace(x, y)
+        x, dx, y, axis, _ = prepare_input(x, y, axis, xp=xp)
+
+        if xp.isdtype(y.dtype, "complex floating"):
+            msg = ("`Akima1DInterpolator` only works with real values for `y`. "
+                   "If you are trying to use the real components of the passed array, "
+                   "use `np.real` on the array before passing to "
+                   "`Akima1DInterpolator`.")
+            raise ValueError(msg)
+
+        # Akima extrapolation historically False; parent class defaults to True.
+        extrapolate = False if extrapolate is None else extrapolate
+
+        if y.shape[0] == 2:
+            # edge case: only have two points, use linear interpolation
+            xv = xp.reshape(x, (x.shape[0],) + (1,)*(y.ndim-1))
+            hk = xv[1:, ...] - xv[:-1, ...]
+            mk = (y[1:, ...] - y[:-1, ...]) / hk
+            t = xp.zeros_like(y)
+            t[...] = mk
+        else:
+            # determine slopes between breakpoints
+            m = xp.empty((x.shape[0] + 3, ) + y.shape[1:])
+            dx = dx[(slice(None), ) + (None, ) * (y.ndim - 1)]
+            m[2:-2, ...] = xp.diff(y, axis=0) / dx
+
+            # add two additional points on the left ...
+            m[1, ...] = 2. * m[2, ...] - m[3, ...]
+            m[0, ...] = 2. * m[1, ...] - m[2, ...]
+            # ... and on the right
+            m[-2, ...] = 2. * m[-3, ...] - m[-4, ...]
+            m[-1, ...] = 2. * m[-2, ...] - m[-3, ...]
+
+            # if m1 == m2 != m3 == m4, the slope at the breakpoint is not
+            # defined. This is the fill value:
+            t = .5 * (m[3:, ...] + m[:-3, ...])
+            # get the denominator of the slope t
+            dm = xp.abs(xp.diff(m, axis=0))
+            if method == "makima":
+                pm = xp.abs(m[1:, ...] + m[:-1, ...])
+                f1 = dm[2:, ...] + 0.5 * pm[2:, ...]
+                f2 = dm[:-2, ...] + 0.5 * pm[:-2, ...]
+            else:
+                f1 = dm[2:, ...]
+                f2 = dm[:-2, ...]
+
+            # makima is more numerically stable for small f12,
+            # so a finite cutoff should not improve any behavior
+            # however, akima has a qualitative discontinuity near f12=0
+            # a finite cutoff moves it, but cannot remove it.
+            # the cutoff break_mult could be made a keyword argument
+            # method='akima' also benefits from a check for m2=m3
+            break_mult = 1.e-9
+
+            f12 = f1 + f2
+
+            # These are the mask of where the slope at breakpoint is defined:
+            mmax = xp.max(f12) if xp_size(f12) > 0 else -xp.inf
+            ind = xp.nonzero(f12 > break_mult * mmax)
+
+            x_ind, y_ind = ind[0], ind[1:]
+            # Set the slope at breakpoint
+            t[ind] = m[(x_ind + 1,) + y_ind] + (
+                (f2[ind] / f12[ind])
+                * (m[(x_ind + 2,) + y_ind] - m[(x_ind + 1,) + y_ind])
+            )
+
+        super().__init__(x, y, t, axis=0, extrapolate=extrapolate)
+        self.axis = axis
+
+    def extend(self, c, x, right=True):
+        raise NotImplementedError("Extending a 1-D Akima interpolator is not "
+                                  "yet implemented")
+
+    # These are inherited from PPoly, but they do not produce an Akima
+    # interpolator. Hence stub them out.
+    @classmethod
+    def from_spline(cls, tck, extrapolate=None):
+        raise NotImplementedError("This method does not make sense for "
+                                  "an Akima interpolator.")
+
+    @classmethod
+    def from_bernstein_basis(cls, bp, extrapolate=None):
+        raise NotImplementedError("This method does not make sense for "
+                                  "an Akima interpolator.")
+
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class CubicSpline(CubicHermiteSpline):
+    """Piecewise cubic interpolator to fit values (C2 smooth).
+
+    Interpolate data with a piecewise cubic polynomial which is twice
+    continuously differentiable [1]_. The result is represented as a `PPoly`
+    instance with breakpoints matching the given data.
+
+    Parameters
+    ----------
+    x : array_like, shape (n,)
+        1-D array containing values of the independent variable.
+        Values must be real, finite and in strictly increasing order.
+    y : array_like
+        Array containing values of the dependent variable. It can have
+        arbitrary number of dimensions, but the length along ``axis``
+        (see below) must match the length of ``x``. Values must be finite.
+    axis : int, optional
+        Axis along which `y` is assumed to be varying. Meaning that for
+        ``x[i]`` the corresponding values are ``np.take(y, i, axis=axis)``.
+        Default is 0.
+    bc_type : string or 2-tuple, optional
+        Boundary condition type. Two additional equations, given by the
+        boundary conditions, are required to determine all coefficients of
+        polynomials on each segment [2]_.
+
+        If `bc_type` is a string, then the specified condition will be applied
+        at both ends of a spline. Available conditions are:
+
+        * 'not-a-knot' (default): The first and second segment at a curve end
+          are the same polynomial. It is a good default when there is no
+          information on boundary conditions.
+        * 'periodic': The interpolated functions is assumed to be periodic
+          of period ``x[-1] - x[0]``. The first and last value of `y` must be
+          identical: ``y[0] == y[-1]``. This boundary condition will result in
+          ``y'[0] == y'[-1]`` and ``y''[0] == y''[-1]``.
+        * 'clamped': The first derivative at curves ends are zero. Assuming
+          a 1D `y`, ``bc_type=((1, 0.0), (1, 0.0))`` is the same condition.
+        * 'natural': The second derivative at curve ends are zero. Assuming
+          a 1D `y`, ``bc_type=((2, 0.0), (2, 0.0))`` is the same condition.
+
+        If `bc_type` is a 2-tuple, the first and the second value will be
+        applied at the curve start and end respectively. The tuple values can
+        be one of the previously mentioned strings (except 'periodic') or a
+        tuple ``(order, deriv_values)`` allowing to specify arbitrary
+        derivatives at curve ends:
+
+        * `order`: the derivative order, 1 or 2.
+        * `deriv_value`: array_like containing derivative values, shape must
+          be the same as `y`, excluding ``axis`` dimension. For example, if
+          `y` is 1-D, then `deriv_value` must be a scalar. If `y` is 3-D with
+          the shape (n0, n1, n2) and axis=2, then `deriv_value` must be 2-D
+          and have the shape (n0, n1).
+    extrapolate : {bool, 'periodic', None}, optional
+        If bool, determines whether to extrapolate to out-of-bounds points
+        based on first and last intervals, or to return NaNs. If 'periodic',
+        periodic extrapolation is used. If None (default), ``extrapolate`` is
+        set to 'periodic' for ``bc_type='periodic'`` and to True otherwise.
+
+    Attributes
+    ----------
+    x : ndarray, shape (n,)
+        Breakpoints. The same ``x`` which was passed to the constructor.
+    c : ndarray, shape (4, n-1, ...)
+        Coefficients of the polynomials on each segment. The trailing
+        dimensions match the dimensions of `y`, excluding ``axis``.
+        For example, if `y` is 1-d, then ``c[k, i]`` is a coefficient for
+        ``(x-x[i])**(3-k)`` on the segment between ``x[i]`` and ``x[i+1]``.
+    axis : int
+        Interpolation axis. The same axis which was passed to the
+        constructor.
+
+    Methods
+    -------
+    __call__
+    derivative
+    antiderivative
+    integrate
+    solve
+    roots
+
+    See Also
+    --------
+    Akima1DInterpolator : Akima 1D interpolator.
+    PchipInterpolator : PCHIP 1-D monotonic cubic interpolator.
+    PPoly : Piecewise polynomial in terms of coefficients and breakpoints.
+
+    Notes
+    -----
+    Parameters `bc_type` and ``extrapolate`` work independently, i.e. the
+    former controls only construction of a spline, and the latter only
+    evaluation.
+
+    When a boundary condition is 'not-a-knot' and n = 2, it is replaced by
+    a condition that the first derivative is equal to the linear interpolant
+    slope. When both boundary conditions are 'not-a-knot' and n = 3, the
+    solution is sought as a parabola passing through given points.
+
+    When 'not-a-knot' boundary conditions is applied to both ends, the
+    resulting spline will be the same as returned by `splrep` (with ``s=0``)
+    and `InterpolatedUnivariateSpline`, but these two methods use a
+    representation in B-spline basis.
+
+    .. versionadded:: 0.18.0
+
+    Examples
+    --------
+    In this example the cubic spline is used to interpolate a sampled sinusoid.
+    You can see that the spline continuity property holds for the first and
+    second derivatives and violates only for the third derivative.
+
+    >>> import numpy as np
+    >>> from scipy.interpolate import CubicSpline
+    >>> import matplotlib.pyplot as plt
+    >>> x = np.arange(10)
+    >>> y = np.sin(x)
+    >>> cs = CubicSpline(x, y)
+    >>> xs = np.arange(-0.5, 9.6, 0.1)
+    >>> fig, ax = plt.subplots(figsize=(6.5, 4))
+    >>> ax.plot(x, y, 'o', label='data')
+    >>> ax.plot(xs, np.sin(xs), label='true')
+    >>> ax.plot(xs, cs(xs), label="S")
+    >>> ax.plot(xs, cs(xs, 1), label="S'")
+    >>> ax.plot(xs, cs(xs, 2), label="S''")
+    >>> ax.plot(xs, cs(xs, 3), label="S'''")
+    >>> ax.set_xlim(-0.5, 9.5)
+    >>> ax.legend(loc='lower left', ncol=2)
+    >>> plt.show()
+
+    In the second example, the unit circle is interpolated with a spline. A
+    periodic boundary condition is used. You can see that the first derivative
+    values, ds/dx=0, ds/dy=1 at the periodic point (1, 0) are correctly
+    computed. Note that a circle cannot be exactly represented by a cubic
+    spline. To increase precision, more breakpoints would be required.
+
+    >>> theta = 2 * np.pi * np.linspace(0, 1, 5)
+    >>> y = np.c_[np.cos(theta), np.sin(theta)]
+    >>> cs = CubicSpline(theta, y, bc_type='periodic')
+    >>> print("ds/dx={:.1f} ds/dy={:.1f}".format(cs(0, 1)[0], cs(0, 1)[1]))
+    ds/dx=0.0 ds/dy=1.0
+    >>> xs = 2 * np.pi * np.linspace(0, 1, 100)
+    >>> fig, ax = plt.subplots(figsize=(6.5, 4))
+    >>> ax.plot(y[:, 0], y[:, 1], 'o', label='data')
+    >>> ax.plot(np.cos(xs), np.sin(xs), label='true')
+    >>> ax.plot(cs(xs)[:, 0], cs(xs)[:, 1], label='spline')
+    >>> ax.axes.set_aspect('equal')
+    >>> ax.legend(loc='center')
+    >>> plt.show()
+
+    The third example is the interpolation of a polynomial y = x**3 on the
+    interval 0 <= x<= 1. A cubic spline can represent this function exactly.
+    To achieve that we need to specify values and first derivatives at
+    endpoints of the interval. Note that y' = 3 * x**2 and thus y'(0) = 0 and
+    y'(1) = 3.
+
+    >>> cs = CubicSpline([0, 1], [0, 1], bc_type=((1, 0), (1, 3)))
+    >>> x = np.linspace(0, 1)
+    >>> np.allclose(x**3, cs(x))
+    True
+
+    References
+    ----------
+    .. [1] `Cubic Spline Interpolation
+            <https://en.wikiversity.org/wiki/Cubic_Spline_Interpolation>`_
+            on Wikiversity.
+    .. [2] Carl de Boor, "A Practical Guide to Splines", Springer-Verlag, 1978.
+    """
+
+    def __init__(self, x, y, axis=0, bc_type='not-a-knot', extrapolate=None):
+        xp = array_namespace(x, y)
+        x, dx, y, axis, _ = prepare_input(x, y, axis, xp=np_compat)
+        n = len(x)
+
+        bc, y = self._validate_bc(bc_type, y, y.shape[1:], axis)
+
+        if extrapolate is None:
+            if bc[0] == 'periodic':
+                extrapolate = 'periodic'
+            else:
+                extrapolate = True
+
+        if y.size == 0:
+            # bail out early for zero-sized arrays
+            s = np.zeros_like(y)
+        else:
+            dxr = dx.reshape([dx.shape[0]] + [1] * (y.ndim - 1))
+            slope = np.diff(y, axis=0) / dxr
+
+            # If bc is 'not-a-knot' this change is just a convention.
+            # If bc is 'periodic' then we already checked that y[0] == y[-1],
+            # and the spline is just a constant, we handle this case in the
+            # same way by setting the first derivatives to slope, which is 0.
+            if n == 2:
+                if bc[0] in ['not-a-knot', 'periodic']:
+                    bc[0] = (1, slope[0])
+                if bc[1] in ['not-a-knot', 'periodic']:
+                    bc[1] = (1, slope[0])
+
+            # This is a special case, when both conditions are 'not-a-knot'
+            # and n == 3. In this case 'not-a-knot' can't be handled regularly
+            # as the both conditions are identical. We handle this case by
+            # constructing a parabola passing through given points.
+            if n == 3 and bc[0] == 'not-a-knot' and bc[1] == 'not-a-knot':
+                A = np.zeros((3, 3))  # This is a standard matrix.
+                b = np.empty((3,) + y.shape[1:], dtype=y.dtype)
+
+                A[0, 0] = 1
+                A[0, 1] = 1
+                A[1, 0] = dx[1]
+                A[1, 1] = 2 * (dx[0] + dx[1])
+                A[1, 2] = dx[0]
+                A[2, 1] = 1
+                A[2, 2] = 1
+
+                b[0] = 2 * slope[0]
+                b[1] = 3 * (dxr[0] * slope[1] + dxr[1] * slope[0])
+                b[2] = 2 * slope[1]
+
+                m = b.shape[0]
+                s = solve(A, b.reshape(m, -1), overwrite_a=True, overwrite_b=True,
+                          check_finite=False).reshape(b.shape)
+            elif n == 3 and bc[0] == 'periodic':
+                # In case when number of points is 3 we compute the derivatives
+                # manually
+                t = (slope / dxr).sum(0) / (1. / dxr).sum(0)
+                s = np.broadcast_to(t, (n,) + y.shape[1:])
+            else:
+                # Find derivative values at each x[i] by solving a tridiagonal
+                # system.
+                A = np.zeros((3, n))  # This is a banded matrix representation.
+                b = np.empty((n,) + y.shape[1:], dtype=y.dtype)
+
+                # Filling the system for i=1..n-2
+                #                         (x[i-1] - x[i]) * s[i-1] +\
+                # 2 * ((x[i] - x[i-1]) + (x[i+1] - x[i])) * s[i]   +\
+                #                         (x[i] - x[i-1]) * s[i+1] =\
+                #       3 * ((x[i+1] - x[i])*(y[i] - y[i-1])/(x[i] - x[i-1]) +\
+                #           (x[i] - x[i-1])*(y[i+1] - y[i])/(x[i+1] - x[i]))
+
+                A[1, 1:-1] = 2 * (dx[:-1] + dx[1:])  # The diagonal
+                A[0, 2:] = dx[:-1]                   # The upper diagonal
+                A[-1, :-2] = dx[1:]                  # The lower diagonal
+
+                b[1:-1] = 3 * (dxr[1:] * slope[:-1] + dxr[:-1] * slope[1:])
+
+                bc_start, bc_end = bc
+
+                if bc_start == 'periodic':
+                    # Due to the periodicity, and because y[-1] = y[0], the
+                    # linear system has (n-1) unknowns/equations instead of n:
+                    A = A[:, 0:-1]
+                    A[1, 0] = 2 * (dx[-1] + dx[0])
+                    A[0, 1] = dx[-1]
+
+                    b = b[:-1]
+
+                    # Also, due to the periodicity, the system is not tri-diagonal.
+                    # We need to compute a "condensed" matrix of shape (n-2, n-2).
+                    # See https://web.archive.org/web/20151220180652/http://www.cfm.brown.edu/people/gk/chap6/node14.html
+                    # for more explanations.
+                    # The condensed matrix is obtained by removing the last column
+                    # and last row of the (n-1, n-1) system matrix. The removed
+                    # values are saved in scalar variables with the (n-1, n-1)
+                    # system matrix indices forming their names:
+                    a_m1_0 = dx[-2]  # lower left corner value: A[-1, 0]
+                    a_m1_m2 = dx[-1]
+                    a_m1_m1 = 2 * (dx[-1] + dx[-2])
+                    a_m2_m1 = dx[-3]
+                    a_0_m1 = dx[0]
+
+                    b[0] = 3 * (dxr[0] * slope[-1] + dxr[-1] * slope[0])
+                    b[-1] = 3 * (dxr[-1] * slope[-2] + dxr[-2] * slope[-1])
+
+                    Ac = A[:, :-1]
+                    b1 = b[:-1]
+                    b2 = np.zeros_like(b1)
+                    b2[0] = -a_0_m1
+                    b2[-1] = -a_m2_m1
+
+                    # s1 and s2 are the solutions of (n-2, n-2) system
+                    m = b1.shape[0]
+                    s1 = solve_banded((1, 1), Ac, b1.reshape(m, -1), overwrite_ab=False,
+                                      overwrite_b=False, check_finite=False)
+                    s1 = s1.reshape(b1.shape)
+
+                    m = b2.shape[0]
+                    s2 = solve_banded((1, 1), Ac, b2.reshape(m, -1), overwrite_ab=False,
+                                      overwrite_b=False, check_finite=False)
+                    s2 = s2.reshape(b2.shape)
+
+                    # computing the s[n-2] solution:
+                    s_m1 = ((b[-1] - a_m1_0 * s1[0] - a_m1_m2 * s1[-1]) /
+                            (a_m1_m1 + a_m1_0 * s2[0] + a_m1_m2 * s2[-1]))
+
+                    # s is the solution of the (n, n) system:
+                    s = np.empty((n,) + y.shape[1:], dtype=y.dtype)
+                    s[:-2] = s1 + s_m1 * s2
+                    s[-2] = s_m1
+                    s[-1] = s[0]
+                else:
+                    if bc_start == 'not-a-knot':
+                        A[1, 0] = dx[1]
+                        A[0, 1] = x[2] - x[0]
+                        d = x[2] - x[0]
+                        b[0] = ((dxr[0] + 2*d) * dxr[1] * slope[0] +
+                                dxr[0]**2 * slope[1]) / d
+                    elif bc_start[0] == 1:
+                        A[1, 0] = 1
+                        A[0, 1] = 0
+                        b[0] = bc_start[1]
+                    elif bc_start[0] == 2:
+                        A[1, 0] = 2 * dx[0]
+                        A[0, 1] = dx[0]
+                        b[0] = -0.5 * bc_start[1] * dx[0]**2 + 3 * (y[1] - y[0])
+
+                    if bc_end == 'not-a-knot':
+                        A[1, -1] = dx[-2]
+                        A[-1, -2] = x[-1] - x[-3]
+                        d = x[-1] - x[-3]
+                        b[-1] = ((dxr[-1]**2*slope[-2] +
+                                 (2*d + dxr[-1])*dxr[-2]*slope[-1]) / d)
+                    elif bc_end[0] == 1:
+                        A[1, -1] = 1
+                        A[-1, -2] = 0
+                        b[-1] = bc_end[1]
+                    elif bc_end[0] == 2:
+                        A[1, -1] = 2 * dx[-1]
+                        A[-1, -2] = dx[-1]
+                        b[-1] = 0.5 * bc_end[1] * dx[-1]**2 + 3 * (y[-1] - y[-2])
+
+                    m = b.shape[0]
+                    s = solve_banded((1, 1), A, b.reshape(m, -1), overwrite_ab=True,
+                                     overwrite_b=True, check_finite=False)
+                    s = s.reshape(b.shape)
+
+        x, y, s = map(xp.asarray, (x, y, s))
+        super().__init__(x, y, s, axis=0, extrapolate=extrapolate)
+        self.axis = axis
+
+    @staticmethod
+    def _validate_bc(bc_type, y, expected_deriv_shape, axis):
+        """Validate and prepare boundary conditions.
+
+        Returns
+        -------
+        validated_bc : 2-tuple
+            Boundary conditions for a curve start and end.
+        y : ndarray
+            y casted to complex dtype if one of the boundary conditions has
+            complex dtype.
+        """
+        if isinstance(bc_type, str):
+            if bc_type == 'periodic':
+                if not np.allclose(y[0], y[-1], rtol=1e-15, atol=1e-15):
+                    raise ValueError(
+                        f"The first and last `y` point along axis {axis} must "
+                        "be identical (within machine precision) when "
+                        "bc_type='periodic'.")
+
+            bc_type = (bc_type, bc_type)
+
+        else:
+            if len(bc_type) != 2:
+                raise ValueError("`bc_type` must contain 2 elements to "
+                                 "specify start and end conditions.")
+
+            if 'periodic' in bc_type:
+                raise ValueError("'periodic' `bc_type` is defined for both "
+                                 "curve ends and cannot be used with other "
+                                 "boundary conditions.")
+
+        validated_bc = []
+        for bc in bc_type:
+            if isinstance(bc, str):
+                if bc == 'clamped':
+                    validated_bc.append((1, np.zeros(expected_deriv_shape)))
+                elif bc == 'natural':
+                    validated_bc.append((2, np.zeros(expected_deriv_shape)))
+                elif bc in ['not-a-knot', 'periodic']:
+                    validated_bc.append(bc)
+                else:
+                    raise ValueError(f"bc_type={bc} is not allowed.")
+            else:
+                try:
+                    deriv_order, deriv_value = bc
+                except Exception as e:
+                    raise ValueError(
+                        "A specified derivative value must be "
+                        "given in the form (order, value)."
+                    ) from e
+
+                if deriv_order not in [1, 2]:
+                    raise ValueError("The specified derivative order must "
+                                     "be 1 or 2.")
+
+                deriv_value = np.asarray(deriv_value)
+                if deriv_value.shape != expected_deriv_shape:
+                    raise ValueError(
+                        f"`deriv_value` shape {deriv_value.shape} is not "
+                        f"the expected one {expected_deriv_shape}."
+                    )
+
+                if np.issubdtype(deriv_value.dtype, np.complexfloating):
+                    y = y.astype(complex, copy=False)
+
+                validated_bc.append((deriv_order, deriv_value))
+
+        return validated_bc, y

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_ndbspline.py

@@ -0,0 +1,518 @@
+import itertools
+import functools
+import operator
+import numpy as np
+
+from math import prod
+from types import GenericAlias
+
+from . import _dierckx  # type: ignore[attr-defined]
+
+import scipy.sparse.linalg as ssl
+from scipy.sparse import csr_array
+from scipy._lib._array_api import array_namespace, xp_capabilities
+
+from ._bsplines import _not_a_knot, BSpline
+
+__all__ = ["NdBSpline"]
+
+
+def _get_dtype(dtype):
+    """Return np.complex128 for complex dtypes, np.float64 otherwise."""
+    if np.issubdtype(dtype, np.complexfloating):
+        return np.complex128
+    else:
+        return np.float64
+
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class NdBSpline:
+    """Tensor product spline object.
+
+    The value at point ``xp = (x1, x2, ..., xN)`` is evaluated as a linear
+    combination of products of one-dimensional b-splines in each of the ``N``
+    dimensions::
+
+       c[i1, i2, ..., iN] * B(x1; i1, t1) * B(x2; i2, t2) * ... * B(xN; iN, tN)
+
+
+    Here ``B(x; i, t)`` is the ``i``-th b-spline defined by the knot vector
+    ``t`` evaluated at ``x``.
+
+    Parameters
+    ----------
+    t : tuple of 1D ndarrays
+        knot vectors in directions 1, 2, ... N,
+        ``len(t[i]) == n[i] + k + 1``
+    c : ndarray, shape (n1, n2, ..., nN, ...)
+        b-spline coefficients
+    k : int or length-d tuple of integers
+        spline degrees.
+        A single integer is interpreted as having this degree for
+        all dimensions.
+    extrapolate : bool, optional
+        Whether to extrapolate out-of-bounds inputs, or return `nan`.
+        Default is to extrapolate.
+
+    Attributes
+    ----------
+    t : tuple of ndarrays
+        Knots vectors.
+    c : ndarray
+        Coefficients of the tensor-product spline.
+    k : tuple of integers
+        Degrees for each dimension.
+    extrapolate : bool, optional
+        Whether to extrapolate or return nans for out-of-bounds inputs.
+        Defaults to true.
+
+    Methods
+    -------
+    __call__
+    derivative
+    design_matrix
+
+    See Also
+    --------
+    BSpline : a one-dimensional B-spline object
+    NdPPoly : an N-dimensional piecewise tensor product polynomial
+
+    """
+
+    # generic type compatibility with scipy-stubs
+    __class_getitem__ = classmethod(GenericAlias)
+
+    def __init__(self, t, c, k, *, extrapolate=None):
+        self._k, self._indices_k1d, (self._t, self._len_t) = _preprocess_inputs(k, t)
+
+        self._asarray = array_namespace(c, *t).asarray
+
+        if extrapolate is None:
+            extrapolate = True
+        self.extrapolate = bool(extrapolate)
+
+        self._c = np.asarray(c)
+
+        ndim = self._t.shape[0]   # == len(self.t)
+        if self._c.ndim < ndim:
+            raise ValueError(f"Coefficients must be at least {ndim}-dimensional.")
+
+        for d in range(ndim):
+            td = self.t[d]
+            kd = self.k[d]
+            n = td.shape[0] - kd - 1
+
+            if self._c.shape[d] != n:
+                raise ValueError(f"Knots, coefficients and degree in dimension"
+                                 f" {d} are inconsistent:"
+                                 f" got {self._c.shape[d]} coefficients for"
+                                 f" {len(td)} knots, need at least {n} for"
+                                 f" k={k}.")
+
+        dt = _get_dtype(self._c.dtype)
+        self._c = np.ascontiguousarray(self._c, dtype=dt)
+
+    @property
+    def k(self):
+        return tuple(self._k)
+
+    @property
+    def t(self):
+        # repack the knots into a tuple
+        return tuple(
+            self._asarray(self._t[d, :self._len_t[d]]) for d in range(self._t.shape[0])
+        )
+
+    @property
+    def c(self):
+        return self._asarray(self._c)
+
+    def __call__(self, xi, *, nu=None, extrapolate=None):
+        """Evaluate the tensor product b-spline at ``xi``.
+
+        Parameters
+        ----------
+        xi : array_like, shape(..., ndim)
+            The coordinates to evaluate the interpolator at.
+            This can be a list or tuple of ndim-dimensional points
+            or an array with the shape (num_points, ndim).
+        nu : sequence of length ``ndim``, optional
+            Orders of derivatives to evaluate. Each must be non-negative.
+            Defaults to the zeroth derivivative.
+        extrapolate : bool, optional
+            Whether to exrapolate based on first and last intervals in each
+            dimension, or return `nan`. Default is to ``self.extrapolate``.
+
+        Returns
+        -------
+        values : ndarray, shape ``xi.shape[:-1] + self.c.shape[ndim:]``
+            Interpolated values at ``xi``
+        """
+        ndim = self._t.shape[0]  # == len(self.t)
+
+        if extrapolate is None:
+            extrapolate = self.extrapolate
+        extrapolate = bool(extrapolate)
+
+        if nu is None:
+            nu = np.zeros((ndim,), dtype=np.int64)
+        else:
+            nu = np.asarray(nu, dtype=np.int64)
+            if nu.ndim != 1 or nu.shape[0] != ndim:
+                raise ValueError(
+                    f"invalid number of derivative orders {nu = } for "
+                    f"ndim = {len(self.t)}.")
+            if any(nu < 0):
+                raise ValueError(f"derivatives must be positive, got {nu = }")
+
+        # prepare xi : shape (..., m1, ..., md) -> (1, m1, ..., md)
+        xi = np.asarray(xi, dtype=float)
+        xi_shape = xi.shape
+        xi = xi.reshape(-1, xi_shape[-1])
+        xi = np.ascontiguousarray(xi)
+
+        if xi_shape[-1] != ndim:
+            raise ValueError(f"Shapes: xi.shape={xi_shape} and ndim={ndim}")
+
+        # complex -> double
+        was_complex = self._c.dtype.kind == 'c'
+        cc = self._c
+        if was_complex and self._c.ndim == ndim:
+            # make sure that core dimensions are intact, and complex->float
+            # size doubling only adds a trailing dimension
+            cc = self._c[..., None]
+        cc = cc.view(float)
+
+        # prepare the coefficients: flatten the trailing dimensions
+        c1 = cc.reshape(cc.shape[:ndim] + (-1,))
+        c1r = c1.ravel()
+
+        # replacement for np.ravel_multi_index for indexing of `c1`:
+        _strides_c1 = np.asarray([s // c1.dtype.itemsize
+                                  for s in c1.strides], dtype=np.int64)
+
+        num_c_tr = c1.shape[-1]  # # of trailing coefficients
+        out = _dierckx.evaluate_ndbspline(xi,
+                                 self._t,
+                                 self._len_t,
+                                 self._k,
+                                 nu,
+                                 extrapolate,
+                                 c1r,
+                                 num_c_tr,
+                                 _strides_c1,
+                                 self._indices_k1d,
+        )
+        out = out.view(self._c.dtype)
+        out = out.reshape(xi_shape[:-1] + self._c.shape[ndim:])
+        return self._asarray(out)
+
+    @classmethod
+    def design_matrix(cls, xvals, t, k, extrapolate=True):
+        """Construct the design matrix as a CSR format sparse array.
+
+        Parameters
+        ----------
+        xvals :  ndarray, shape(npts, ndim)
+            Data points. ``xvals[j, :]`` gives the ``j``-th data point as an
+            ``ndim``-dimensional array.
+        t : tuple of 1D ndarrays, length-ndim
+            Knot vectors in directions 1, 2, ... ndim,
+        k : int
+            B-spline degree.
+        extrapolate : bool, optional
+            Whether to extrapolate out-of-bounds values of raise a `ValueError`
+
+        Returns
+        -------
+        design_matrix : a CSR array
+            Each row of the design matrix corresponds to a value in `xvals` and
+            contains values of b-spline basis elements which are non-zero
+            at this value.
+
+        """
+        xvals = np.asarray(xvals, dtype=float)
+        ndim = xvals.shape[-1]
+        if len(t) != ndim:
+            raise ValueError(
+                f"Data and knots are inconsistent: len(t) = {len(t)} for "
+                f" {ndim = }."
+            )
+
+        # tabulate the flat indices for iterating over the (k+1)**ndim subarray
+        k, _indices_k1d, (_t, len_t) = _preprocess_inputs(k, t)
+
+        # Precompute the shape and strides of the 'coefficients array'.
+        # This would have been the NdBSpline coefficients; in the present context
+        # this is a helper to compute the indices into the colocation matrix.
+        c_shape = tuple(len_t[d] - k[d] - 1 for d in range(ndim))
+
+        # The strides of the coeffs array: the computation is equivalent to
+        # >>> cstrides = [s // 8 for s in np.empty(c_shape).strides]
+        cs = c_shape[1:] + (1,)
+        cstrides = np.cumprod(cs[::-1], dtype=np.int64)[::-1].copy()
+
+        # heavy lifting happens here
+        data, indices, indptr = _dierckx._coloc_nd(xvals,
+                _t, len_t, k, _indices_k1d, cstrides)
+
+        return csr_array((data, indices, indptr))
+
+    def _bspline_derivative_along_axis(self, c, t, k, axis, nu=1):
+        # Move the selected axis to front
+        c = np.moveaxis(c, axis, 0)
+        n = c.shape[0]
+        trailing_shape = c.shape[1:]
+        c_flat = c.reshape(n, -1)
+
+        new_c_list = []
+        new_t = None
+
+        for i in range(c_flat.shape[1]):
+            if k >= nu:
+                b = BSpline.construct_fast(t, c_flat[:, i], k)
+                db = b.derivative(nu)
+                # truncate coefficients to match new knot/degree size
+                db.c = db.c[:len(db.t) - db.k - 1]
+            else:
+                db = BSpline.construct_fast(t, np.zeros(len(t) - 1), 0)
+
+            if new_t is None:
+                new_t = db.t
+
+            new_c_list.append(db.c)
+
+        new_c = np.stack(new_c_list, axis=1).reshape(
+            (len(new_c_list[0]),) + trailing_shape)
+        new_c = np.moveaxis(new_c, 0, axis)
+
+        return new_c, new_t
+
+    def derivative(self, nu):
+        """
+        Construct a new NdBSpline representing the partial derivative.
+
+        Parameters
+        ----------
+        nu : array_like of shape (ndim,)
+            Orders of the partial derivatives to compute along each dimension.
+
+        Returns
+        -------
+        NdBSpline
+            A new NdBSpline representing the partial derivative of the original spline.
+
+        """
+        nu_arr = np.asarray(nu, dtype=np.int64)
+        ndim = len(self.t)
+
+        if nu_arr.ndim != 1 or nu_arr.shape[0] != ndim:
+            raise ValueError(
+                f"invalid number of derivative orders {nu = } for "
+                f"ndim = {len(self.t)}.")
+
+        if any(nu_arr < 0):
+            raise ValueError(f"derivative orders must be positive, got {nu = }")
+
+        # extract t and c as numpy arrays
+        t_new = [self._t[d, :self._len_t[d]] for d in range(self._t.shape[0])]
+        k_new = list(self.k)
+        c_new = self._c.copy()
+
+        for axis, n in enumerate(nu_arr):
+            if n == 0:
+                continue
+
+            c_new, t_new[axis] = self._bspline_derivative_along_axis(
+                c_new, t_new[axis], k_new[axis], axis, nu=n
+            )
+            k_new[axis] = max(k_new[axis] - n, 0)
+
+        return NdBSpline(tuple(self._asarray(t) for t in t_new),
+                         self._asarray(c_new),
+                         tuple(k_new),
+                         extrapolate=self.extrapolate
+        )
+
+def _preprocess_inputs(k, t_tpl):
+    """Helpers: validate and preprocess NdBSpline inputs.
+
+       Parameters
+       ----------
+       k : int or tuple
+          Spline orders
+       t_tpl : tuple or array-likes
+          Knots.
+    """
+    # 1. Make sure t_tpl is a tuple
+    if not isinstance(t_tpl, tuple):
+        raise ValueError(f"Expect `t` to be a tuple of array-likes. "
+                         f"Got {t_tpl} instead."
+        )
+
+    # 2. Make ``k`` a tuple of integers
+    ndim = len(t_tpl)
+    try:
+        len(k)
+    except TypeError:
+        # make k a tuple
+        k = (k,)*ndim
+
+    k = np.asarray([operator.index(ki) for ki in k], dtype=np.int64)
+
+    if len(k) != ndim:
+        raise ValueError(f"len(t) = {len(t_tpl)} != {len(k) = }.")
+
+    # 3. Validate inputs
+    ndim = len(t_tpl)
+    for d in range(ndim):
+        td = np.asarray(t_tpl[d])
+        kd = k[d]
+        n = td.shape[0] - kd - 1
+        if kd < 0:
+            raise ValueError(f"Spline degree in dimension {d} cannot be"
+                             f" negative.")
+        if td.ndim != 1:
+            raise ValueError(f"Knot vector in dimension {d} must be"
+                             f" one-dimensional.")
+        if n < kd + 1:
+            raise ValueError(f"Need at least {2*kd + 2} knots for degree"
+                             f" {kd} in dimension {d}.")
+        if (np.diff(td) < 0).any():
+            raise ValueError(f"Knots in dimension {d} must be in a"
+                             f" non-decreasing order.")
+        if len(np.unique(td[kd:n + 1])) < 2:
+            raise ValueError(f"Need at least two internal knots in"
+                             f" dimension {d}.")
+        if not np.isfinite(td).all():
+            raise ValueError(f"Knots in dimension {d} should not have"
+                             f" nans or infs.")
+
+    # 4. tabulate the flat indices for iterating over the (k+1)**ndim subarray
+    # non-zero b-spline elements
+    shape = tuple(kd + 1 for kd in k)
+    indices = np.unravel_index(np.arange(prod(shape)), shape)
+    _indices_k1d = np.asarray(indices, dtype=np.int64).T.copy()
+
+    # 5. pack the knots into a single array:
+    #    ([1, 2, 3, 4], [5, 6], (7, 8, 9)) -->
+    #    array([[1, 2, 3, 4],
+    #           [5, 6, nan, nan],
+    #           [7, 8, 9, nan]])
+    t_tpl = [np.asarray(t) for t in t_tpl]
+    ndim = len(t_tpl)
+    len_t = [len(ti) for ti in t_tpl]
+    _t = np.empty((ndim, max(len_t)), dtype=float)
+    _t.fill(np.nan)
+    for d in range(ndim):
+        _t[d, :len(t_tpl[d])] = t_tpl[d]
+    len_t = np.asarray(len_t, dtype=np.int64)
+
+    return k, _indices_k1d, (_t, len_t)
+
+
+def _iter_solve(a, b, solver=ssl.gcrotmk, **solver_args):
+    # work around iterative solvers not accepting multiple r.h.s.
+
+    # also work around a.dtype == float64 and b.dtype == complex128
+    # cf https://github.com/scipy/scipy/issues/19644
+    if np.issubdtype(b.dtype, np.complexfloating):
+        real = _iter_solve(a, b.real, solver, **solver_args)
+        imag = _iter_solve(a, b.imag, solver, **solver_args)
+        return real + 1j*imag
+
+    if b.ndim == 2 and b.shape[1] !=1:
+        res = np.empty_like(b)
+        for j in range(b.shape[1]):
+            res[:, j], info = solver(a, b[:, j], **solver_args)
+            if info != 0:
+                raise ValueError(f"{solver = } returns {info =} for column {j}.")
+        return res
+    else:
+        res, info = solver(a, b, **solver_args)
+        if info != 0:
+            raise ValueError(f"{solver = } returns {info = }.")
+        return res
+
+
+def make_ndbspl(points, values, k=3, *, solver=ssl.gcrotmk, **solver_args):
+    """Construct an interpolating NdBspline.
+
+    Parameters
+    ----------
+    points : tuple of ndarrays of float, with shapes (m1,), ... (mN,)
+        The points defining the regular grid in N dimensions. The points in
+        each dimension (i.e. every element of the `points` tuple) must be
+        strictly ascending or descending.
+    values : ndarray of float, shape (m1, ..., mN, ...)
+        The data on the regular grid in n dimensions.
+    k : int, optional
+        The spline degree. Must be odd. Default is cubic, k=3
+    solver : a `scipy.sparse.linalg` solver (iterative or direct), optional.
+        An iterative solver from `scipy.sparse.linalg` or a direct one,
+        `sparse.sparse.linalg.spsolve`.
+        Used to solve the sparse linear system
+        ``design_matrix @ coefficients = rhs`` for the coefficients.
+        Default is `scipy.sparse.linalg.gcrotmk`
+    solver_args : dict, optional
+        Additional arguments for the solver. The call signature is
+        ``solver(csr_array, rhs_vector, **solver_args)``
+
+    Returns
+    -------
+    spl : NdBSpline object
+
+    Notes
+    -----
+    Boundary conditions are not-a-knot in all dimensions.
+    """
+    ndim = len(points)
+    xi_shape = tuple(len(x) for x in points)
+
+    try:
+        len(k)
+    except TypeError:
+        # make k a tuple
+        k = (k,)*ndim
+
+    for d, point in enumerate(points):
+        numpts = len(np.atleast_1d(point))
+        if numpts <= k[d]:
+            raise ValueError(f"There are {numpts} points in dimension {d},"
+                             f" but order {k[d]} requires at least "
+                             f" {k[d]+1} points per dimension.")
+
+    t = tuple(_not_a_knot(np.asarray(points[d], dtype=float), k[d])
+              for d in range(ndim))
+    xvals = np.asarray([xv for xv in itertools.product(*points)], dtype=float)
+
+    # construct the colocation matrix
+    matr = NdBSpline.design_matrix(xvals, t, k)
+
+    # Remove zeros from the sparse matrix
+    # If k=1, then solve() doesn't take long enough for this to help
+    if k[0] >= 3:
+        matr.eliminate_zeros()
+
+    # Solve for the coefficients given `values`.
+    # Trailing dimensions: first ndim dimensions are data, the rest are batch
+    # dimensions, so stack `values` into a 2D array for `spsolve` to undestand.
+    v_shape = values.shape
+    vals_shape = (prod(v_shape[:ndim]), prod(v_shape[ndim:]))
+    vals = values.reshape(vals_shape)
+
+    if solver != ssl.spsolve:
+        solver = functools.partial(_iter_solve, solver=solver)
+        if "atol" not in solver_args:
+            # avoid a DeprecationWarning, grumble grumble
+            solver_args["atol"] = 1e-6
+
+    coef = solver(matr, vals, **solver_args)
+    coef = coef.reshape(xi_shape + v_shape[ndim:])
+    return NdBSpline(t, coef, k)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_ndgriddata.py

@@ -0,0 +1,330 @@
+"""
+Convenience interface to N-D interpolation
+
+.. versionadded:: 0.9
+
+"""
+import numpy as np
+from ._interpnd import (LinearNDInterpolator, NDInterpolatorBase,
+     CloughTocher2DInterpolator, _ndim_coords_from_arrays)
+from scipy.spatial import cKDTree
+
+__all__ = ['griddata', 'NearestNDInterpolator', 'LinearNDInterpolator',
+           'CloughTocher2DInterpolator']
+
+#------------------------------------------------------------------------------
+# Nearest-neighbor interpolation
+#------------------------------------------------------------------------------
+
+
+class NearestNDInterpolator(NDInterpolatorBase):
+    """Nearest-neighbor interpolator in N > 1 dimensions.
+
+    Methods
+    -------
+    __call__
+
+    Parameters
+    ----------
+    x : (npoints, ndims) 2-D ndarray of floats
+        Data point coordinates.
+    y : (npoints, ...) N-D ndarray of float or complex
+        Data values. The length of `y` along the first axis must be equal to
+        the length of `x`.
+    rescale : boolean, optional
+        Rescale points to unit cube before performing interpolation.
+        This is useful if some of the input dimensions have
+        incommensurable units and differ by many orders of magnitude.
+
+        .. versionadded:: 0.14.0
+    tree_options : dict, optional
+        Options passed to the underlying ``cKDTree``.
+
+        .. versionadded:: 0.17.0
+
+    See Also
+    --------
+    griddata :
+        Interpolate unstructured D-D data.
+    LinearNDInterpolator :
+        Piecewise linear interpolator in N dimensions.
+    CloughTocher2DInterpolator :
+        Piecewise cubic, C1 smooth, curvature-minimizing interpolator in 2D.
+    interpn : Interpolation on a regular grid or rectilinear grid.
+    RegularGridInterpolator : Interpolator on a regular or rectilinear grid
+                              in arbitrary dimensions (`interpn` wraps this
+                              class).
+
+    Notes
+    -----
+    Uses ``scipy.spatial.cKDTree``
+
+    .. note:: For data on a regular grid use `interpn` instead.
+
+    Examples
+    --------
+    We can interpolate values on a 2D plane:
+
+    >>> from scipy.interpolate import NearestNDInterpolator
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> rng = np.random.default_rng()
+    >>> x = rng.random(10) - 0.5
+    >>> y = rng.random(10) - 0.5
+    >>> z = np.hypot(x, y)
+    >>> X = np.linspace(min(x), max(x))
+    >>> Y = np.linspace(min(y), max(y))
+    >>> X, Y = np.meshgrid(X, Y)  # 2D grid for interpolation
+    >>> interp = NearestNDInterpolator(list(zip(x, y)), z)
+    >>> Z = interp(X, Y)
+    >>> plt.pcolormesh(X, Y, Z, shading='auto')
+    >>> plt.plot(x, y, "ok", label="input point")
+    >>> plt.legend()
+    >>> plt.colorbar()
+    >>> plt.axis("equal")
+    >>> plt.show()
+
+    """
+
+    def __init__(self, x, y, rescale=False, tree_options=None):
+        NDInterpolatorBase.__init__(self, x, y, rescale=rescale,
+                                    need_contiguous=False,
+                                    need_values=False)
+        if tree_options is None:
+            tree_options = dict()
+        self.tree = cKDTree(self.points, **tree_options)
+        self.values = np.asarray(y)
+
+    def __call__(self, *args, **query_options):
+        """
+        Evaluate interpolator at given points.
+
+        Parameters
+        ----------
+        x1, x2, ... xn : array-like of float
+            Points where to interpolate data at.
+            x1, x2, ... xn can be array-like of float with broadcastable shape.
+            or x1 can be array-like of float with shape ``(..., ndim)``
+        **query_options
+            This allows ``eps``, ``p``, ``distance_upper_bound``, and ``workers``
+            being passed to the cKDTree's query function to be explicitly set.
+            See `scipy.spatial.cKDTree.query` for an overview of the different options.
+
+            .. versionadded:: 1.12.0
+
+        """
+        # For the sake of enabling subclassing, NDInterpolatorBase._set_xi performs
+        # some operations which are not required by NearestNDInterpolator.__call__, 
+        # hence here we operate on xi directly, without calling a parent class function.
+        xi = _ndim_coords_from_arrays(args, ndim=self.points.shape[1])
+        xi = self._check_call_shape(xi)
+        xi = self._scale_x(xi)
+
+        # We need to handle two important cases:
+        # (1) the case where xi has trailing dimensions (..., ndim), and
+        # (2) the case where y has trailing dimensions
+        # We will first flatten xi to deal with case (1),
+        # do the computation in flattened array while retaining y's dimensionality,
+        # and then reshape the interpolated values back to match xi's shape.
+
+        # Flatten xi for the query
+        xi_flat = xi.reshape(-1, xi.shape[-1])
+        original_shape = xi.shape
+        flattened_shape = xi_flat.shape
+
+        # if distance_upper_bound is set to not be infinite,
+        # then we need to consider the case where cKDtree
+        # does not find any points within distance_upper_bound to return.
+        # It marks those points as having infinte distance, which is what will be used
+        # below to mask the array and return only the points that were deemed
+        # to have a close enough neighbor to return something useful.
+        dist, i = self.tree.query(xi_flat, **query_options)
+        valid_mask = np.isfinite(dist)
+
+        # create a holder interp_values array and fill with nans.
+        if self.values.ndim > 1:
+            interp_shape = flattened_shape[:-1] + self.values.shape[1:]
+        else:
+            interp_shape = flattened_shape[:-1]
+
+        if np.issubdtype(self.values.dtype, np.complexfloating):
+            interp_values = np.full(interp_shape, np.nan, dtype=self.values.dtype)
+        else:
+            interp_values = np.full(interp_shape, np.nan)
+
+        interp_values[valid_mask] = self.values[i[valid_mask], ...]
+
+        if self.values.ndim > 1:
+            new_shape = original_shape[:-1] + self.values.shape[1:]
+        else:
+            new_shape = original_shape[:-1]
+        interp_values = interp_values.reshape(new_shape)
+
+        return interp_values
+
+
+#------------------------------------------------------------------------------
+# Convenience interface function
+#------------------------------------------------------------------------------
+
+
+def griddata(points, values, xi, method='linear', fill_value=np.nan,
+             rescale=False):
+    """
+    Convenience function for interpolating unstructured data in multiple dimensions.
+
+    Parameters
+    ----------
+    points : 2-D ndarray of floats with shape (n, D), or length D tuple of 1-D ndarrays with shape (n,).
+        Data point coordinates.
+    values : ndarray of float or complex, shape (n,)
+        Data values.
+    xi : 2-D ndarray of floats with shape (m, D), or length D tuple of ndarrays broadcastable to the same shape.
+        Points at which to interpolate data.
+    method : {'linear', 'nearest', 'cubic'}, optional
+        Method of interpolation. One of
+
+        ``nearest``
+          return the value at the data point closest to
+          the point of interpolation. See `NearestNDInterpolator` for
+          more details.
+
+        ``linear``
+          tessellate the input point set to N-D
+          simplices, and interpolate linearly on each simplex. See
+          `LinearNDInterpolator` for more details.
+
+        ``cubic`` (1-D)
+          return the value determined from a cubic
+          spline.
+
+        ``cubic`` (2-D)
+          return the value determined from a
+          piecewise cubic, continuously differentiable (C1), and
+          approximately curvature-minimizing polynomial surface. See
+          `CloughTocher2DInterpolator` for more details.
+    fill_value : float, optional
+        Value used to fill in for requested points outside of the
+        convex hull of the input points. If not provided, then the
+        default is ``nan``. This option has no effect for the
+        'nearest' method.
+    rescale : bool, optional
+        Rescale points to unit cube before performing interpolation.
+        This is useful if some of the input dimensions have
+        incommensurable units and differ by many orders of magnitude.
+
+        .. versionadded:: 0.14.0
+
+    Returns
+    -------
+    ndarray
+        Array of interpolated values.
+
+    See Also
+    --------
+    LinearNDInterpolator :
+        Piecewise linear interpolator in N dimensions.
+    NearestNDInterpolator :
+        Nearest-neighbor interpolator in N dimensions.
+    CloughTocher2DInterpolator :
+        Piecewise cubic, C1 smooth, curvature-minimizing interpolator in 2D.
+    interpn : Interpolation on a regular grid or rectilinear grid.
+    RegularGridInterpolator : Interpolator on a regular or rectilinear grid
+                              in arbitrary dimensions (`interpn` wraps this
+                              class).
+
+    Notes
+    -----
+
+    .. versionadded:: 0.9
+
+    .. note:: For data on a regular grid use `interpn` instead.
+
+    Examples
+    --------
+
+    Suppose we want to interpolate the 2-D function
+
+    >>> import numpy as np
+    >>> def func(x, y):
+    ...     return x*(1-x)*np.cos(4*np.pi*x) * np.sin(4*np.pi*y**2)**2
+
+    on a grid in [0, 1]x[0, 1]
+
+    >>> grid_x, grid_y = np.mgrid[0:1:100j, 0:1:200j]
+
+    but we only know its values at 1000 data points:
+
+    >>> rng = np.random.default_rng()
+    >>> points = rng.random((1000, 2))
+    >>> values = func(points[:,0], points[:,1])
+
+    This can be done with `griddata` -- below we try out all of the
+    interpolation methods:
+
+    >>> from scipy.interpolate import griddata
+    >>> grid_z0 = griddata(points, values, (grid_x, grid_y), method='nearest')
+    >>> grid_z1 = griddata(points, values, (grid_x, grid_y), method='linear')
+    >>> grid_z2 = griddata(points, values, (grid_x, grid_y), method='cubic')
+
+    One can see that the exact result is reproduced by all of the
+    methods to some degree, but for this smooth function the piecewise
+    cubic interpolant gives the best results:
+
+    >>> import matplotlib.pyplot as plt
+    >>> plt.subplot(221)
+    >>> plt.imshow(func(grid_x, grid_y).T, extent=(0,1,0,1), origin='lower')
+    >>> plt.plot(points[:,0], points[:,1], 'k.', ms=1)
+    >>> plt.title('Original')
+    >>> plt.subplot(222)
+    >>> plt.imshow(grid_z0.T, extent=(0,1,0,1), origin='lower')
+    >>> plt.title('Nearest')
+    >>> plt.subplot(223)
+    >>> plt.imshow(grid_z1.T, extent=(0,1,0,1), origin='lower')
+    >>> plt.title('Linear')
+    >>> plt.subplot(224)
+    >>> plt.imshow(grid_z2.T, extent=(0,1,0,1), origin='lower')
+    >>> plt.title('Cubic')
+    >>> plt.gcf().set_size_inches(6, 6)
+    >>> plt.show()
+
+    """ # numpy/numpydoc#87  # noqa: E501
+
+    points = _ndim_coords_from_arrays(points)
+
+    if points.ndim < 2:
+        ndim = points.ndim
+    else:
+        ndim = points.shape[-1]
+
+    if ndim == 1 and method in ('nearest', 'linear', 'cubic'):
+        from ._interpolate import interp1d
+        points = points.ravel()
+        if isinstance(xi, tuple):
+            if len(xi) != 1:
+                raise ValueError("invalid number of dimensions in xi")
+            xi, = xi
+        # Sort points/values together, necessary as input for interp1d
+        idx = np.argsort(points)
+        points = points[idx]
+        values = values[idx]
+        if method == 'nearest':
+            fill_value = 'extrapolate'
+        ip = interp1d(points, values, kind=method, axis=0, bounds_error=False,
+                      fill_value=fill_value)
+        return ip(xi)
+    elif method == 'nearest':
+        ip = NearestNDInterpolator(points, values, rescale=rescale)
+        return ip(xi)
+    elif method == 'linear':
+        ip = LinearNDInterpolator(points, values, fill_value=fill_value,
+                                  rescale=rescale)
+        return ip(xi)
+    elif method == 'cubic' and ndim == 2:
+        ip = CloughTocher2DInterpolator(points, values, fill_value=fill_value,
+                                        rescale=rescale)
+        return ip(xi)
+    else:
+        raise ValueError(
+            f"Unknown interpolation method {method!r} for {ndim} dimensional data"
+        )

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_pade.py

@@ -0,0 +1,67 @@
+from numpy import zeros, asarray, eye, poly1d, hstack, r_
+from scipy import linalg
+
+__all__ = ["pade"]
+
+def pade(an, m, n=None):
+    """
+    Return Pade approximation to a polynomial as the ratio of two polynomials.
+
+    Parameters
+    ----------
+    an : (N,) array_like
+        Taylor series coefficients.
+    m : int
+        The order of the returned approximating polynomial `q`.
+    n : int, optional
+        The order of the returned approximating polynomial `p`. By default,
+        the order is ``len(an)-1-m``.
+
+    Returns
+    -------
+    p, q : Polynomial class
+        The Pade approximation of the polynomial defined by `an` is
+        ``p(x)/q(x)``.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.interpolate import pade
+    >>> e_exp = [1.0, 1.0, 1.0/2.0, 1.0/6.0, 1.0/24.0, 1.0/120.0]
+    >>> p, q = pade(e_exp, 2)
+
+    >>> e_exp.reverse()
+    >>> e_poly = np.poly1d(e_exp)
+
+    Compare ``e_poly(x)`` and the Pade approximation ``p(x)/q(x)``
+
+    >>> e_poly(1)
+    2.7166666666666668
+
+    >>> p(1)/q(1)
+    2.7179487179487181
+
+    """
+    an = asarray(an)
+    if n is None:
+        n = len(an) - 1 - m
+        if n < 0:
+            raise ValueError("Order of q <m> must be smaller than len(an)-1.")
+    if n < 0:
+        raise ValueError("Order of p <n> must be greater than 0.")
+    N = m + n
+    if N > len(an)-1:
+        raise ValueError("Order of q+p <m+n> must be smaller than len(an).")
+    an = an[:N+1]
+    Akj = eye(N+1, n+1, dtype=an.dtype)
+    Bkj = zeros((N+1, m), dtype=an.dtype)
+    for row in range(1, m+1):
+        Bkj[row,:row] = -(an[:row])[::-1]
+    for row in range(m+1, N+1):
+        Bkj[row,:] = -(an[row-m:row])[::-1]
+    C = hstack((Akj, Bkj))
+    pq = linalg.solve(C, an)
+    p = pq[:n+1]
+    q = r_[1.0, pq[n+1:]]
+    return poly1d(p[::-1]), poly1d(q[::-1])
+

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_polyint.py

@@ -0,0 +1,1029 @@
+import warnings
+from types import GenericAlias
+
+import numpy as np
+from scipy.special import factorial
+from scipy._lib._util import (_asarray_validated, float_factorial, check_random_state,
+                              _transition_to_rng)
+
+
+__all__ = ["KroghInterpolator", "krogh_interpolate",
+           "BarycentricInterpolator", "barycentric_interpolate",
+           "approximate_taylor_polynomial"]
+
+
+def _isscalar(x):
+    """Check whether x is if a scalar type, or 0-dim"""
+    return np.isscalar(x) or hasattr(x, 'shape') and x.shape == ()
+
+
+class _Interpolator1D:
+    """
+    Common features in univariate interpolation
+
+    Deal with input data type and interpolation axis rolling. The
+    actual interpolator can assume the y-data is of shape (n, r) where
+    `n` is the number of x-points, and `r` the number of variables,
+    and use self.dtype as the y-data type.
+
+    Attributes
+    ----------
+    _y_axis
+        Axis along which the interpolation goes in the original array
+    _y_extra_shape
+        Additional trailing shape of the input arrays, excluding
+        the interpolation axis.
+    dtype
+        Dtype of the y-data arrays. Can be set via _set_dtype, which
+        forces it to be float or complex.
+
+    Methods
+    -------
+    __call__
+    _prepare_x
+    _finish_y
+    _reshape_yi
+    _set_yi
+    _set_dtype
+    _evaluate
+
+    """
+
+    __slots__ = ('_y_axis', '_y_extra_shape', 'dtype')
+
+    # generic type compatibility with scipy-stubs
+    __class_getitem__ = classmethod(GenericAlias)
+
+    def __init__(self, xi=None, yi=None, axis=None):
+        self._y_axis = axis
+        self._y_extra_shape = None
+        self.dtype = None
+        if yi is not None:
+            self._set_yi(yi, xi=xi, axis=axis)
+
+    def __call__(self, x):
+        """
+        Evaluate the interpolant
+
+        Parameters
+        ----------
+        x : array_like
+            Point or points at which to evaluate the interpolant.
+
+        Returns
+        -------
+        y : array_like
+            Interpolated values. Shape is determined by replacing
+            the interpolation axis in the original array with the shape of `x`.
+
+        Notes
+        -----
+        Input values `x` must be convertible to `float` values like `int`
+        or `float`.
+
+        """
+        x, x_shape = self._prepare_x(x)
+        y = self._evaluate(x)
+        return self._finish_y(y, x_shape)
+
+    def _evaluate(self, x):
+        """
+        Actually evaluate the value of the interpolator.
+        """
+        raise NotImplementedError()
+
+    def _prepare_x(self, x):
+        """Reshape input x array to 1-D"""
+        x = _asarray_validated(x, check_finite=False, as_inexact=True)
+        x_shape = x.shape
+        return x.ravel(), x_shape
+
+    def _finish_y(self, y, x_shape):
+        """Reshape interpolated y back to an N-D array similar to initial y"""
+        y = y.reshape(x_shape + self._y_extra_shape)
+        if self._y_axis != 0 and x_shape != ():
+            nx = len(x_shape)
+            ny = len(self._y_extra_shape)
+            s = (list(range(nx, nx + self._y_axis))
+                 + list(range(nx)) + list(range(nx+self._y_axis, nx+ny)))
+            y = y.transpose(s)
+        return y
+
+    def _reshape_yi(self, yi, check=False):
+        yi = np.moveaxis(np.asarray(yi), self._y_axis, 0)
+        if check and yi.shape[1:] != self._y_extra_shape:
+            ok_shape = (f"{self._y_extra_shape[-self._y_axis:]!r} + (N,) + "
+                        f"{self._y_extra_shape[:-self._y_axis]!r}")
+            raise ValueError(f"Data must be of shape {ok_shape}")
+        return yi.reshape((yi.shape[0], -1))
+
+    def _set_yi(self, yi, xi=None, axis=None):
+        if axis is None:
+            axis = self._y_axis
+        if axis is None:
+            raise ValueError("no interpolation axis specified")
+
+        yi = np.asarray(yi)
+
+        shape = yi.shape
+        if shape == ():
+            shape = (1,)
+        if xi is not None and shape[axis] != len(xi):
+            raise ValueError("x and y arrays must be equal in length along "
+                             "interpolation axis.")
+
+        self._y_axis = (axis % yi.ndim)
+        self._y_extra_shape = yi.shape[:self._y_axis] + yi.shape[self._y_axis+1:]
+        self.dtype = None
+        self._set_dtype(yi.dtype)
+
+    def _set_dtype(self, dtype, union=False):
+        if np.issubdtype(dtype, np.complexfloating) \
+               or np.issubdtype(self.dtype, np.complexfloating):
+            self.dtype = np.complex128
+        else:
+            if not union or self.dtype != np.complex128:
+                self.dtype = np.float64
+
+
+class _Interpolator1DWithDerivatives(_Interpolator1D):
+    def derivatives(self, x, der=None):
+        """
+        Evaluate several derivatives of the polynomial at the point `x`
+
+        Produce an array of derivatives evaluated at the point `x`.
+
+        Parameters
+        ----------
+        x : array_like
+            Point or points at which to evaluate the derivatives
+        der : int or list or None, optional
+            How many derivatives to evaluate, or None for all potentially
+            nonzero derivatives (that is, a number equal to the number
+            of points), or a list of derivatives to evaluate. This number
+            includes the function value as the '0th' derivative.
+
+        Returns
+        -------
+        d : ndarray
+            Array with derivatives; ``d[j]`` contains the jth derivative.
+            Shape of ``d[j]`` is determined by replacing the interpolation
+            axis in the original array with the shape of `x`.
+
+        Examples
+        --------
+        >>> from scipy.interpolate import KroghInterpolator
+        >>> KroghInterpolator([0,0,0],[1,2,3]).derivatives(0)
+        array([1.0,2.0,3.0])
+        >>> KroghInterpolator([0,0,0],[1,2,3]).derivatives([0,0])
+        array([[1.0,1.0],
+               [2.0,2.0],
+               [3.0,3.0]])
+
+        """
+        x, x_shape = self._prepare_x(x)
+        y = self._evaluate_derivatives(x, der)
+
+        y = y.reshape((y.shape[0],) + x_shape + self._y_extra_shape)
+        if self._y_axis != 0 and x_shape != ():
+            nx = len(x_shape)
+            ny = len(self._y_extra_shape)
+            s = ([0] + list(range(nx+1, nx + self._y_axis+1))
+                 + list(range(1, nx+1)) +
+                 list(range(nx+1+self._y_axis, nx+ny+1)))
+            y = y.transpose(s)
+        return y
+
+    def derivative(self, x, der=1):
+        """
+        Evaluate a single derivative of the polynomial at the point `x`.
+
+        Parameters
+        ----------
+        x : array_like
+            Point or points at which to evaluate the derivatives
+
+        der : integer, optional
+            Which derivative to evaluate (default: first derivative).
+            This number includes the function value as 0th derivative.
+
+        Returns
+        -------
+        d : ndarray
+            Derivative interpolated at the x-points. Shape of `d` is
+            determined by replacing the interpolation axis in the
+            original array with the shape of `x`.
+
+        Notes
+        -----
+        This may be computed by evaluating all derivatives up to the desired
+        one (using self.derivatives()) and then discarding the rest.
+
+        """
+        x, x_shape = self._prepare_x(x)
+        y = self._evaluate_derivatives(x, der+1)
+        return self._finish_y(y[der], x_shape)
+
+    def _evaluate_derivatives(self, x, der=None):
+        """
+        Actually evaluate the derivatives.
+
+        Parameters
+        ----------
+        x : array_like
+            1D array of points at which to evaluate the derivatives
+        der : integer, optional
+            The number of derivatives to evaluate, from 'order 0' (der=1)
+            to order der-1.  If omitted, return all possibly-non-zero
+            derivatives, ie 0 to order n-1.
+
+        Returns
+        -------
+        d : ndarray
+            Array of shape ``(der, x.size, self.yi.shape[1])`` containing
+            the derivatives from 0 to der-1
+        """
+        raise NotImplementedError()
+
+
+class KroghInterpolator(_Interpolator1DWithDerivatives):
+    """Krogh interpolator (C∞ smooth).
+
+    The polynomial passes through all the pairs ``(xi, yi)``. One may
+    additionally specify a number of derivatives at each point `xi`;
+    this is done by repeating the value `xi` and specifying the
+    derivatives as successive `yi` values.
+
+    Allows evaluation of the polynomial and all its derivatives.
+    For reasons of numerical stability, this function does not compute
+    the coefficients of the polynomial, although they can be obtained
+    by evaluating all the derivatives.
+
+    Parameters
+    ----------
+    xi : array_like, shape (npoints, )
+        Known x-coordinates. Must be sorted in increasing order.
+    yi : array_like, shape (..., npoints, ...)
+        Known y-coordinates. When an xi occurs two or more times in
+        a row, the corresponding yi's represent derivative values. The length of `yi`
+        along the interpolation axis must be equal to the length of `xi`. Use the
+        `axis` parameter to select the correct axis.
+    axis : int, optional
+        Axis in the `yi` array corresponding to the x-coordinate values. Defaults to
+        ``axis=0``.
+
+    Notes
+    -----
+    Be aware that the algorithms implemented here are not necessarily
+    the most numerically stable known. Moreover, even in a world of
+    exact computation, unless the x coordinates are chosen very
+    carefully - Chebyshev zeros (e.g., cos(i*pi/n)) are a good choice -
+    polynomial interpolation itself is a very ill-conditioned process
+    due to the Runge phenomenon. In general, even with well-chosen
+    x values, degrees higher than about thirty cause problems with
+    numerical instability in this code.
+
+    Based on [1]_.
+
+    References
+    ----------
+    .. [1] Krogh, "Efficient Algorithms for Polynomial Interpolation
+        and Numerical Differentiation", 1970.
+
+    Examples
+    --------
+    To produce a polynomial that is zero at 0 and 1 and has
+    derivative 2 at 0, call
+
+    >>> from scipy.interpolate import KroghInterpolator
+    >>> KroghInterpolator([0,0,1],[0,2,0])
+
+    This constructs the quadratic :math:`2x^2-2x`. The derivative condition
+    is indicated by the repeated zero in the `xi` array; the corresponding
+    yi values are 0, the function value, and 2, the derivative value.
+
+    For another example, given `xi`, `yi`, and a derivative `ypi` for each
+    point, appropriate arrays can be constructed as:
+
+    >>> import numpy as np
+    >>> rng = np.random.default_rng()
+    >>> xi = np.linspace(0, 1, 5)
+    >>> yi, ypi = rng.random((2, 5))
+    >>> xi_k, yi_k = np.repeat(xi, 2), np.ravel(np.dstack((yi,ypi)))
+    >>> KroghInterpolator(xi_k, yi_k)
+
+    To produce a vector-valued polynomial, supply a higher-dimensional
+    array for `yi`:
+
+    >>> KroghInterpolator([0,1],[[2,3],[4,5]])
+
+    This constructs a linear polynomial giving (2,3) at 0 and (4,5) at 1.
+
+    """
+
+    def __init__(self, xi, yi, axis=0):
+        super().__init__(xi, yi, axis)
+
+        self.xi = np.asarray(xi)
+        self.yi = self._reshape_yi(yi)
+        self.n, self.r = self.yi.shape
+
+        if (deg := self.xi.size) > 30:
+            warnings.warn(f"{deg} degrees provided, degrees higher than about"
+                          " thirty cause problems with numerical instability "
+                          "with 'KroghInterpolator'", stacklevel=2)
+
+        c = np.zeros((self.n+1, self.r), dtype=self.dtype)
+        c[0] = self.yi[0]
+        Vk = np.zeros((self.n, self.r), dtype=self.dtype)
+        for k in range(1, self.n):
+            s = 0
+            while s <= k and xi[k-s] == xi[k]:
+                s += 1
+            s -= 1
+            Vk[0] = self.yi[k]/float_factorial(s)
+            for i in range(k-s):
+                if xi[i] == xi[k]:
+                    raise ValueError("Elements of `xi` can't be equal.")
+                if s == 0:
+                    Vk[i+1] = (c[i]-Vk[i])/(xi[i]-xi[k])
+                else:
+                    Vk[i+1] = (Vk[i+1]-Vk[i])/(xi[i]-xi[k])
+            c[k] = Vk[k-s]
+        self.c = c
+
+    def _evaluate(self, x):
+        pi = 1
+        p = np.zeros((len(x), self.r), dtype=self.dtype)
+        p += self.c[0,np.newaxis,:]
+        for k in range(1, self.n):
+            w = x - self.xi[k-1]
+            pi = w*pi
+            p += pi[:,np.newaxis] * self.c[k]
+        return p
+
+    def _evaluate_derivatives(self, x, der=None):
+        n = self.n
+        r = self.r
+
+        if der is None:
+            der = self.n
+
+        pi = np.zeros((n, len(x)))
+        w = np.zeros((n, len(x)))
+        pi[0] = 1
+        p = np.zeros((len(x), self.r), dtype=self.dtype)
+        p += self.c[0, np.newaxis, :]
+
+        for k in range(1, n):
+            w[k-1] = x - self.xi[k-1]
+            pi[k] = w[k-1] * pi[k-1]
+            p += pi[k, :, np.newaxis] * self.c[k]
+
+        cn = np.zeros((max(der, n+1), len(x), r), dtype=self.dtype)
+        cn[:n+1, :, :] += self.c[:n+1, np.newaxis, :]
+        cn[0] = p
+        for k in range(1, n):
+            for i in range(1, n-k+1):
+                pi[i] = w[k+i-1]*pi[i-1] + pi[i]
+                cn[k] = cn[k] + pi[i, :, np.newaxis]*cn[k+i]
+            cn[k] *= float_factorial(k)
+
+        cn[n, :, :] = 0
+        return cn[:der]
+
+
+def krogh_interpolate(xi, yi, x, der=0, axis=0):
+    """Convenience function for Krogh interpolation.
+
+    See `KroghInterpolator` for more details.
+
+    Parameters
+    ----------
+    xi : array_like
+        Interpolation points (known x-coordinates).
+    yi : array_like
+        Known y-coordinates, of shape ``(xi.size, R)``. Interpreted as
+        vectors of length R, or scalars if R=1.
+    x : array_like
+        Point or points at which to evaluate the derivatives.
+    der : int or list or None, optional
+        How many derivatives to evaluate, or None for all potentially
+        nonzero derivatives (that is, a number equal to the number
+        of points), or a list of derivatives to evaluate. This number
+        includes the function value as the '0th' derivative.
+    axis : int, optional
+        Axis in the `yi` array corresponding to the x-coordinate values.
+
+    Returns
+    -------
+    d : ndarray
+        If the interpolator's values are R-D then the
+        returned array will be the number of derivatives by N by R.
+        If `x` is a scalar, the middle dimension will be dropped; if
+        the `yi` are scalars then the last dimension will be dropped.
+
+    See Also
+    --------
+    KroghInterpolator : Krogh interpolator
+
+    Notes
+    -----
+    Construction of the interpolating polynomial is a relatively expensive
+    process. If you want to evaluate it repeatedly consider using the class
+    KroghInterpolator (which is what this function uses).
+
+    Examples
+    --------
+    We can interpolate 2D observed data using Krogh interpolation:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> from scipy.interpolate import krogh_interpolate
+    >>> x_observed = np.linspace(0.0, 10.0, 11)
+    >>> y_observed = np.sin(x_observed)
+    >>> x = np.linspace(min(x_observed), max(x_observed), num=100)
+    >>> y = krogh_interpolate(x_observed, y_observed, x)
+    >>> plt.plot(x_observed, y_observed, "o", label="observation")
+    >>> plt.plot(x, y, label="krogh interpolation")
+    >>> plt.legend()
+    >>> plt.show()
+    """
+
+    P = KroghInterpolator(xi, yi, axis=axis)
+    if der == 0:
+        return P(x)
+    elif _isscalar(der):
+        return P.derivative(x, der=der)
+    else:
+        return P.derivatives(x, der=np.amax(der)+1)[der]
+
+
+def approximate_taylor_polynomial(f,x,degree,scale,order=None):
+    """
+    Estimate the Taylor polynomial of f at x by polynomial fitting.
+
+    Parameters
+    ----------
+    f : callable
+        The function whose Taylor polynomial is sought. Should accept
+        a vector of `x` values.
+    x : scalar
+        The point at which the polynomial is to be evaluated.
+    degree : int
+        The degree of the Taylor polynomial
+    scale : scalar
+        The width of the interval to use to evaluate the Taylor polynomial.
+        Function values spread over a range this wide are used to fit the
+        polynomial. Must be chosen carefully.
+    order : int or None, optional
+        The order of the polynomial to be used in the fitting; `f` will be
+        evaluated ``order+1`` times. If None, use `degree`.
+
+    Returns
+    -------
+    p : poly1d instance
+        The Taylor polynomial (translated to the origin, so that
+        for example p(0)=f(x)).
+
+    Notes
+    -----
+    The appropriate choice of "scale" is a trade-off; too large and the
+    function differs from its Taylor polynomial too much to get a good
+    answer, too small and round-off errors overwhelm the higher-order terms.
+    The algorithm used becomes numerically unstable around order 30 even
+    under ideal circumstances.
+
+    Choosing order somewhat larger than degree may improve the higher-order
+    terms.
+
+    Examples
+    --------
+    We can calculate Taylor approximation polynomials of sin function with
+    various degrees:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> from scipy.interpolate import approximate_taylor_polynomial
+    >>> x = np.linspace(-10.0, 10.0, num=100)
+    >>> plt.plot(x, np.sin(x), label="sin curve")
+    >>> for degree in np.arange(1, 15, step=2):
+    ...     sin_taylor = approximate_taylor_polynomial(np.sin, 0, degree, 1,
+    ...                                                order=degree + 2)
+    ...     plt.plot(x, sin_taylor(x), label=f"degree={degree}")
+    >>> plt.legend(bbox_to_anchor=(1.05, 1), loc='upper left',
+    ...            borderaxespad=0.0, shadow=True)
+    >>> plt.tight_layout()
+    >>> plt.axis([-10, 10, -10, 10])
+    >>> plt.show()
+
+    """
+    if order is None:
+        order = degree
+
+    n = order+1
+    # Choose n points that cluster near the endpoints of the interval in
+    # a way that avoids the Runge phenomenon. Ensure, by including the
+    # endpoint or not as appropriate, that one point always falls at x
+    # exactly.
+    xs = scale*np.cos(np.linspace(0,np.pi,n,endpoint=n % 1)) + x
+
+    P = KroghInterpolator(xs, f(xs))
+    d = P.derivatives(x,der=degree+1)
+
+    return np.poly1d((d/factorial(np.arange(degree+1)))[::-1])
+
+
+class BarycentricInterpolator(_Interpolator1DWithDerivatives):
+    r"""Barycentric (Lagrange with improved stability) interpolator (C∞ smooth).
+
+    Constructs a polynomial that passes through a given set of points.
+    Allows evaluation of the polynomial and all its derivatives,
+    efficient changing of the y-values to be interpolated,
+    and updating by adding more x- and y-values. For numerical stability, a barycentric
+    representation is used rather than computing the coefficients of the polynomial
+    directly.
+
+
+    Parameters
+    ----------
+    xi : array_like, shape (npoints, )
+        1-D array of x-coordinates of the points the polynomial
+        should pass through
+    yi : array_like, shape (..., npoints, ...), optional
+        N-D array of y-coordinates of the points the polynomial should pass through.
+        If None, the y values will be supplied later via the `set_y` method.
+        The length of `yi` along the interpolation axis must be equal to the length
+        of `xi`. Use the ``axis`` parameter to select correct axis.
+    axis : int, optional
+        Axis in the yi array corresponding to the x-coordinate values. Defaults
+        to ``axis=0``.
+    wi : array_like, optional
+        The barycentric weights for the chosen interpolation points `xi`.
+        If absent or None, the weights will be computed from `xi` (default).
+        This allows for the reuse of the weights `wi` if several interpolants
+        are being calculated using the same nodes `xi`, without re-computation. This
+        also allows for computing the weights explicitly for some choices of
+        `xi` (see notes).
+    rng : {None, int, `numpy.random.Generator`}, optional
+        If `rng` is passed by keyword, types other than `numpy.random.Generator` are
+        passed to `numpy.random.default_rng` to instantiate a ``Generator``.
+        If `rng` is already a ``Generator`` instance, then the provided instance is
+        used. Specify `rng` for repeatable interpolation.
+
+        If this argument `random_state` is passed by keyword,
+        legacy behavior for the argument `random_state` applies:
+
+        - If `random_state` is None (or `numpy.random`), the `numpy.random.RandomState`
+          singleton is used.
+        - If `random_state` is an int, a new ``RandomState`` instance is used,
+          seeded with `random_state`.
+        - If `random_state` is already a ``Generator`` or ``RandomState`` instance then
+          that instance is used.
+
+        .. versionchanged:: 1.15.0
+            As part of the `SPEC-007 <https://scientific-python.org/specs/spec-0007/>`_
+            transition from use of `numpy.random.RandomState` to
+            `numpy.random.Generator` this keyword was changed from `random_state` to `rng`.
+            For an interim period, both keywords will continue to work (only specify
+            one of them). After the interim period using the `random_state` keyword will emit
+            warnings. The behavior of the `random_state` and `rng` keywords is outlined above.
+
+    Notes
+    -----
+    This method is a variant of Lagrange polynomial interpolation [1]_ based on [2]_.
+    Instead of using Lagrange's or Newton's formula, the polynomial is represented by
+    the barycentric formula
+
+    .. math::
+
+        p(x) =
+        \frac{\sum_{i=1}^m\ w_i y_i / (x - x_i)}{\sum_{i=1}^m w_i / (x - x_i)},
+
+    where :math:`w_i` are the barycentric weights computed with the general formula
+
+    .. math::
+
+        w_i = \left( \prod_{k \neq i} x_i - x_k \right)^{-1}.
+
+    This is the same barycentric form used by `AAA` and `FloaterHormannInterpolator`.
+    However, in contrast, the weights :math:`w_i` are defined such that
+    :math:`p(x)` is a polynomial rather than a rational function.
+
+    The barycentric representation avoids many of the problems associated with
+    polynomial interpolation caused by floating-point arithmetic. However, it does not
+    avoid issues that are intrinsic to polynomial interpolation. Namely, if the
+    x-coordinates are equally spaced, then the weights can be computed explicitly using
+    the formula from [2]_
+
+    .. math::
+
+        w_i = (-1)^i {n \choose i},
+
+    where :math:`n` is the number of x-coordinates. As noted in [2]_, this means that
+    for large :math:`n` the weights vary by exponentially large factors, leading to the
+    Runge phenomenon.
+
+    To avoid this ill-conditioning, the x-coordinates should be clustered at the
+    endpoints of the interval. An excellent choice of points on the interval
+    :math:`[a,b]` are Chebyshev points of the second kind
+
+    .. math::
+
+        x_i = \frac{a + b}{2} + \frac{a - b}{2}\cos(i\pi/n).
+
+    in which case the weights can be computed explicitly as
+
+    .. math::
+
+        w_i = \begin{cases}
+                  (-1)^i/2 & i = 0,n \\
+                  (-1)^i   & \text{otherwise}
+              \end{cases}.
+
+    See [2]_ for more infomation. Note that for large :math:`n`, computing the weights
+    explicitly (see examples) will be faster than the generic formula.
+
+    References
+    ----------
+    .. [1] https://en.wikipedia.org/wiki/Lagrange_polynomial
+    .. [2] Jean-Paul Berrut and Lloyd N. Trefethen, "Barycentric Lagrange
+           Interpolation", SIAM Review 2004 46:3, 501-517
+           :doi:`10.1137/S0036144502417715`
+
+    Examples
+    --------
+    To produce a quintic barycentric interpolant approximating the function
+    :math:`\sin x`, and its first four derivatives, using six randomly-spaced
+    nodes in :math:`(0, \pi/2)`:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> from scipy.interpolate import BarycentricInterpolator
+    >>> rng = np.random.default_rng()
+    >>> xi = rng.random(6) * np.pi/2
+    >>> f, f_d1, f_d2, f_d3, f_d4 = np.sin, np.cos, lambda x: -np.sin(x), lambda x: -np.cos(x), np.sin
+    >>> P = BarycentricInterpolator(xi, f(xi), random_state=rng)
+    >>> fig, axs = plt.subplots(5, 1, sharex=True, layout='constrained', figsize=(7,10))
+    >>> x = np.linspace(0, np.pi, 100)
+    >>> axs[0].plot(x, P(x), 'r:', x, f(x), 'k--', xi, f(xi), 'xk')
+    >>> axs[1].plot(x, P.derivative(x), 'r:', x, f_d1(x), 'k--', xi, f_d1(xi), 'xk')
+    >>> axs[2].plot(x, P.derivative(x, 2), 'r:', x, f_d2(x), 'k--', xi, f_d2(xi), 'xk')
+    >>> axs[3].plot(x, P.derivative(x, 3), 'r:', x, f_d3(x), 'k--', xi, f_d3(xi), 'xk')
+    >>> axs[4].plot(x, P.derivative(x, 4), 'r:', x, f_d4(x), 'k--', xi, f_d4(xi), 'xk')
+    >>> axs[0].set_xlim(0, np.pi)
+    >>> axs[4].set_xlabel(r"$x$")
+    >>> axs[4].set_xticks([i * np.pi / 4 for i in range(5)],
+    ...                   ["0", r"$\frac{\pi}{4}$", r"$\frac{\pi}{2}$", r"$\frac{3\pi}{4}$", r"$\pi$"])
+    >>> for ax, label in zip(axs, ("$f(x)$", "$f'(x)$", "$f''(x)$", "$f^{(3)}(x)$", "$f^{(4)}(x)$")):
+    ...     ax.set_ylabel(label)
+    >>> labels = ['Interpolation nodes', 'True function $f$', 'Barycentric interpolation']
+    >>> axs[0].legend(axs[0].get_lines()[::-1], labels, bbox_to_anchor=(0., 1.02, 1., .102),
+    ...               loc='lower left', ncols=3, mode="expand", borderaxespad=0., frameon=False)
+    >>> plt.show()
+
+    Next, we show how using Chebyshev points of the second kind avoids the
+    Runge phenomenon. In this example, we also compute the weights explicitly.
+
+    >>> n = 20
+    >>> def f(x): return np.abs(x) + 0.5*x - x**2
+    >>> i = np.arange(n)
+    >>> x_cheb = np.cos(i*np.pi/(n - 1))  # Chebyshev points on [-1, 1]
+    >>> w_i_cheb = (-1.)**i  # Explicit formula for weights of Chebyshev points
+    >>> w_i_cheb[[0, -1]] /= 2
+    >>> p_cheb = BarycentricInterpolator(x_cheb, f(x_cheb), wi=w_i_cheb)
+    >>> x_equi = np.linspace(-1, 1, n)
+    >>> p_equi = BarycentricInterpolator(x_equi, f(x_equi))
+    >>> xx = np.linspace(-1, 1, 1000)
+    >>> fig, ax = plt.subplots()
+    >>> ax.plot(xx, f(xx), label="Original Function")
+    >>> ax.plot(xx, p_cheb(xx), "--", label="Chebshev Points")
+    >>> ax.plot(xx, p_equi(xx), "--", label="Equally Spaced Points")
+    >>> ax.set(xlabel="$x$", ylabel="$f(x)$", xlim=[-1, 1])
+    >>> ax.legend()
+    >>> plt.show()
+
+    """ # numpy/numpydoc#87  # noqa: E501
+
+    @_transition_to_rng("random_state", replace_doc=False)
+    def __init__(self, xi, yi=None, axis=0, *, wi=None, rng=None):
+        super().__init__(xi, yi, axis)
+
+        rng = check_random_state(rng)
+
+        self.xi = np.asarray(xi, dtype=np.float64)
+        self.set_yi(yi)
+        self.n = len(self.xi)
+
+        # cache derivative object to avoid re-computing the weights with every call.
+        self._diff_cij = None
+
+        if wi is not None:
+            self.wi = wi
+        else:
+            # See page 510 of Berrut and Trefethen 2004 for an explanation of the
+            # capacity scaling and the suggestion of using a random permutation of
+            # the input factors.
+            # At the moment, the permutation is not performed for xi that are
+            # appended later through the add_xi interface. It's not clear to me how
+            # to implement that and it seems that most situations that require
+            # these numerical stability improvements will be able to provide all
+            # the points to the constructor.
+            self._inv_capacity = 4.0 / (np.max(self.xi) - np.min(self.xi))
+            permute = rng.permutation(self.n, )
+            inv_permute = np.zeros(self.n, dtype=np.int32)
+            inv_permute[permute] = np.arange(self.n)
+            self.wi = np.zeros(self.n)
+
+            for i in range(self.n):
+                dist = self._inv_capacity * (self.xi[i] - self.xi[permute])
+                dist[inv_permute[i]] = 1.0
+                prod = np.prod(dist)
+                if prod == 0.0:
+                    raise ValueError("Interpolation points xi must be"
+                                     " distinct.")
+                self.wi[i] = 1.0 / prod
+
+    def set_yi(self, yi, axis=None):
+        """
+        Update the y values to be interpolated
+
+        The barycentric interpolation algorithm requires the calculation
+        of weights, but these depend only on the `xi`. The `yi` can be changed
+        at any time.
+
+        Parameters
+        ----------
+        yi : array_like
+            The y-coordinates of the points the polynomial will pass through.
+            If None, the y values must be supplied later.
+        axis : int, optional
+            Axis in the `yi` array corresponding to the x-coordinate values.
+
+        """
+        if yi is None:
+            self.yi = None
+            return
+        self._set_yi(yi, xi=self.xi, axis=axis)
+        self.yi = self._reshape_yi(yi)
+        self.n, self.r = self.yi.shape
+        self._diff_baryint = None
+
+    def add_xi(self, xi, yi=None):
+        """
+        Add more x values to the set to be interpolated
+
+        The barycentric interpolation algorithm allows easy updating by
+        adding more points for the polynomial to pass through.
+
+        Parameters
+        ----------
+        xi : array_like
+            The x coordinates of the points that the polynomial should pass
+            through.
+        yi : array_like, optional
+            The y coordinates of the points the polynomial should pass through.
+            Should have shape ``(xi.size, R)``; if R > 1 then the polynomial is
+            vector-valued.
+            If `yi` is not given, the y values will be supplied later. `yi`
+            should be given if and only if the interpolator has y values
+            specified.
+
+        Notes
+        -----
+        The new points added by `add_xi` are not randomly permuted
+        so there is potential for numerical instability,
+        especially for a large number of points. If this
+        happens, please reconstruct interpolation from scratch instead.
+        """
+        if yi is not None:
+            if self.yi is None:
+                raise ValueError("No previous yi value to update!")
+            yi = self._reshape_yi(yi, check=True)
+            self.yi = np.vstack((self.yi,yi))
+        else:
+            if self.yi is not None:
+                raise ValueError("No update to yi provided!")
+        old_n = self.n
+        self.xi = np.concatenate((self.xi,xi))
+        self.n = len(self.xi)
+        self.wi **= -1
+        old_wi = self.wi
+        self.wi = np.zeros(self.n)
+        self.wi[:old_n] = old_wi
+        for j in range(old_n, self.n):
+            self.wi[:j] *= self._inv_capacity * (self.xi[j]-self.xi[:j])
+            self.wi[j] = np.multiply.reduce(
+                self._inv_capacity * (self.xi[:j]-self.xi[j])
+            )
+        self.wi **= -1
+        self._diff_cij = None
+        self._diff_baryint = None
+
+    def __call__(self, x):
+        """Evaluate the interpolating polynomial at the points x
+
+        Parameters
+        ----------
+        x : array_like
+            Point or points at which to evaluate the interpolant.
+
+        Returns
+        -------
+        y : array_like
+            Interpolated values. Shape is determined by replacing
+            the interpolation axis in the original array with the shape of `x`.
+
+        Notes
+        -----
+        Currently the code computes an outer product between `x` and the
+        weights, that is, it constructs an intermediate array of size
+        ``(N, len(x))``, where N is the degree of the polynomial.
+        """
+        return _Interpolator1D.__call__(self, x)
+
+    def _evaluate(self, x):
+        if x.size == 0:
+            p = np.zeros((0, self.r), dtype=self.dtype)
+        else:
+            c = x[..., np.newaxis] - self.xi
+            z = c == 0
+            c[z] = 1
+            c = self.wi / c
+            with np.errstate(divide='ignore'):
+                p = np.dot(c, self.yi) / np.sum(c, axis=-1)[..., np.newaxis]
+            # Now fix where x==some xi
+            r = np.nonzero(z)
+            if len(r) == 1:  # evaluation at a scalar
+                if len(r[0]) > 0:  # equals one of the points
+                    p = self.yi[r[0][0]]
+            else:
+                p[r[:-1]] = self.yi[r[-1]]
+        return p
+
+    def derivative(self, x, der=1):
+        """
+        Evaluate a single derivative of the polynomial at the point x.
+
+        Parameters
+        ----------
+        x : array_like
+            Point or points at which to evaluate the derivatives
+        der : integer, optional
+            Which derivative to evaluate (default: first derivative).
+            This number includes the function value as 0th derivative.
+
+        Returns
+        -------
+        d : ndarray
+            Derivative interpolated at the x-points. Shape of `d` is
+            determined by replacing the interpolation axis in the
+            original array with the shape of `x`.
+        """
+        x, x_shape = self._prepare_x(x)
+        y = self._evaluate_derivatives(x, der+1, all_lower=False)
+        return self._finish_y(y, x_shape)
+
+    def _evaluate_derivatives(self, x, der=None, all_lower=True):
+        # NB: der here is not the order of the highest derivative;
+        # instead, it is the size of the derivatives matrix that
+        # would be returned with all_lower=True, including the
+        # '0th' derivative (the undifferentiated function).
+        # E.g. to evaluate the 5th derivative alone, call
+        # _evaluate_derivatives(x, der=6, all_lower=False).
+
+        if (not all_lower) and (x.size == 0 or self.r == 0):
+            return np.zeros((0, self.r), dtype=self.dtype)
+
+        if (not all_lower) and der == 1:
+            return self._evaluate(x)
+
+        if (not all_lower) and (der > self.n):
+            return np.zeros((len(x), self.r), dtype=self.dtype)
+
+        if der is None:
+            der = self.n
+
+        if all_lower and (x.size == 0 or self.r == 0):
+            return np.zeros((der, len(x), self.r), dtype=self.dtype)
+
+        if self._diff_cij is None:
+            # c[i,j] = xi[i] - xi[j]
+            c = self.xi[:, np.newaxis] - self.xi
+
+            # avoid division by 0 (diagonal entries are so far zero by construction)
+            np.fill_diagonal(c, 1)
+
+            # c[i,j] = (w[j] / w[i]) / (xi[i] - xi[j]) (equation 9.4)
+            c = self.wi/ (c * self.wi[..., np.newaxis])
+
+            # fill in correct diagonal entries: each column sums to 0
+            np.fill_diagonal(c, 0)
+
+            # calculate diagonal
+            # c[j,j] = -sum_{i != j} c[i,j] (equation 9.5)
+            d = -c.sum(axis=1)
+            # c[i,j] = l_j(x_i)
+            np.fill_diagonal(c, d)
+
+            self._diff_cij = c
+
+        if self._diff_baryint is None:
+            # initialise and cache derivative interpolator and cijs;
+            # reuse weights wi (which depend only on interpolation points xi),
+            # to avoid unnecessary re-computation
+            self._diff_baryint = BarycentricInterpolator(xi=self.xi,
+                                                         yi=self._diff_cij @ self.yi,
+                                                         wi=self.wi)
+            self._diff_baryint._diff_cij = self._diff_cij
+
+        if all_lower:
+            # assemble matrix of derivatives from order 0 to order der-1,
+            # in the format required by _Interpolator1DWithDerivatives.
+            cn = np.zeros((der, len(x), self.r), dtype=self.dtype)
+            for d in range(der):
+                cn[d, :, :] = self._evaluate_derivatives(x, d+1, all_lower=False)
+            return cn
+
+        # recursively evaluate only the derivative requested
+        return self._diff_baryint._evaluate_derivatives(x, der-1, all_lower=False)
+
+
+def barycentric_interpolate(xi, yi, x, axis=0, *, der=0, rng=None):
+    """Convenience function for barycentric interpolation.
+
+    Constructs a polynomial that passes through a given set of points,
+    then evaluates the polynomial. For reasons of numerical stability,
+    this function does not compute the coefficients of the polynomial.
+
+    This function uses a "barycentric interpolation" method that treats
+    the problem as a special case of rational function interpolation.
+    This algorithm is quite stable, numerically, but even in a world of
+    exact computation, unless the `x` coordinates are chosen very
+    carefully - Chebyshev zeros (e.g., cos(i*pi/n)) are a good choice -
+    polynomial interpolation itself is a very ill-conditioned process
+    due to the Runge phenomenon.
+
+    Parameters
+    ----------
+    xi : array_like
+        1-D array of x coordinates of the points the polynomial should
+        pass through
+    yi : array_like
+        The y coordinates of the points the polynomial should pass through.
+    x : scalar or array_like
+        Point or points at which to evaluate the interpolant.
+    axis : int, optional
+        Axis in the `yi` array corresponding to the x-coordinate values.
+    der : int or list or None, optional
+        How many derivatives to evaluate, or None for all potentially
+        nonzero derivatives (that is, a number equal to the number
+        of points), or a list of derivatives to evaluate. This number
+        includes the function value as the '0th' derivative.
+    rng : `numpy.random.Generator`, optional
+        Pseudorandom number generator state. When `rng` is None, a new
+        `numpy.random.Generator` is created using entropy from the
+        operating system. Types other than `numpy.random.Generator` are
+        passed to `numpy.random.default_rng` to instantiate a ``Generator``.
+
+    Returns
+    -------
+    y : scalar or array_like
+        Interpolated values. Shape is determined by replacing
+        the interpolation axis in the original array with the shape of `x`.
+
+    See Also
+    --------
+    BarycentricInterpolator : Barycentric interpolator
+
+    Notes
+    -----
+    Construction of the interpolation weights is a relatively slow process.
+    If you want to call this many times with the same xi (but possibly
+    varying yi or x) you should use the class `BarycentricInterpolator`.
+    This is what this function uses internally.
+
+    Examples
+    --------
+    We can interpolate 2D observed data using barycentric interpolation:
+
+    >>> import numpy as np
+    >>> import matplotlib.pyplot as plt
+    >>> from scipy.interpolate import barycentric_interpolate
+    >>> x_observed = np.linspace(0.0, 10.0, 11)
+    >>> y_observed = np.sin(x_observed)
+    >>> x = np.linspace(min(x_observed), max(x_observed), num=100)
+    >>> y = barycentric_interpolate(x_observed, y_observed, x)
+    >>> plt.plot(x_observed, y_observed, "o", label="observation")
+    >>> plt.plot(x, y, label="barycentric interpolation")
+    >>> plt.legend()
+    >>> plt.show()
+
+    """
+    P = BarycentricInterpolator(xi, yi, axis=axis, rng=rng)
+    if der == 0:
+        return P(x)
+    elif _isscalar(der):
+        return P.derivative(x, der=der)
+    else:
+        return P.derivatives(x, der=np.amax(der)+1)[der]

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_rbf.py

@@ -0,0 +1,292 @@
+"""rbf - Radial basis functions for interpolation/smoothing scattered N-D data.
+
+Written by John Travers <jtravs@gmail.com>, February 2007
+Based closely on Matlab code by Alex Chirokov
+Additional, large, improvements by Robert Hetland
+Some additional alterations by Travis Oliphant
+Interpolation with multi-dimensional target domain by Josua Sassen
+
+Permission to use, modify, and distribute this software is given under the
+terms of the SciPy (BSD style) license. See LICENSE.txt that came with
+this distribution for specifics.
+
+NO WARRANTY IS EXPRESSED OR IMPLIED. USE AT YOUR OWN RISK.
+
+Copyright (c) 2006-2007, Robert Hetland <hetland@tamu.edu>
+Copyright (c) 2007, John Travers <jtravs@gmail.com>
+
+Redistribution and use in source and binary forms, with or without
+modification, are permitted provided that the following conditions are
+met:
+
+    * Redistributions of source code must retain the above copyright
+       notice, this list of conditions and the following disclaimer.
+
+    * Redistributions in binary form must reproduce the above
+       copyright notice, this list of conditions and the following
+       disclaimer in the documentation and/or other materials provided
+       with the distribution.
+
+    * Neither the name of Robert Hetland nor the names of any
+       contributors may be used to endorse or promote products derived
+       from this software without specific prior written permission.
+
+THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
+"AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
+LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR
+A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT
+OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL,
+SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT
+LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE,
+DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY
+THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT
+(INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE
+OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
+"""
+import numpy as np
+
+from scipy import linalg
+from scipy.special import xlogy
+from scipy.spatial.distance import cdist, pdist, squareform
+from scipy._lib._array_api import xp_capabilities
+
+__all__ = ['Rbf']
+
+
+@xp_capabilities(out_of_scope=True)
+class Rbf:
+    """
+    Rbf(*args, **kwargs)
+
+    Class for radial basis function interpolation of functions from
+    N-D scattered data to an M-D domain (legacy).
+
+    .. legacy:: class
+
+        `Rbf` is legacy code, for new usage please use `RBFInterpolator`
+        instead.
+
+    Parameters
+    ----------
+    *args : arrays
+        x, y, z, ..., d, where x, y, z, ... are the coordinates of the nodes
+        and d is the array of values at the nodes
+    function : str or callable, optional
+        The radial basis function, based on the radius, r, given by the norm
+        (default is Euclidean distance); the default is 'multiquadric'::
+
+            'multiquadric': sqrt((r/self.epsilon)**2 + 1)
+            'inverse': 1.0/sqrt((r/self.epsilon)**2 + 1)
+            'gaussian': exp(-(r/self.epsilon)**2)
+            'linear': r
+            'cubic': r**3
+            'quintic': r**5
+            'thin_plate': r**2 * log(r)
+
+        If callable, then it must take 2 arguments (self, r). The epsilon
+        parameter will be available as self.epsilon. Other keyword
+        arguments passed in will be available as well.
+
+    epsilon : float, optional
+        Adjustable constant for gaussian or multiquadrics functions
+        - defaults to approximate average distance between nodes (which is
+        a good start).
+    smooth : float, optional
+        Values greater than zero increase the smoothness of the
+        approximation. 0 is for interpolation (default), the function will
+        always go through the nodal points in this case.
+    norm : str, callable, optional
+        A function that returns the 'distance' between two points, with
+        inputs as arrays of positions (x, y, z, ...), and an output as an
+        array of distance. E.g., the default: 'euclidean', such that the result
+        is a matrix of the distances from each point in ``x1`` to each point in
+        ``x2``. For more options, see documentation of
+        `scipy.spatial.distances.cdist`.
+    mode : str, optional
+        Mode of the interpolation, can be '1-D' (default) or 'N-D'. When it is
+        '1-D' the data `d` will be considered as 1-D and flattened
+        internally. When it is 'N-D' the data `d` is assumed to be an array of
+        shape (n_samples, m), where m is the dimension of the target domain.
+
+
+    Attributes
+    ----------
+    N : int
+        The number of data points (as determined by the input arrays).
+    di : ndarray
+        The 1-D array of data values at each of the data coordinates `xi`.
+    xi : ndarray
+        The 2-D array of data coordinates.
+    function : str or callable
+        The radial basis function. See description under Parameters.
+    epsilon : float
+        Parameter used by gaussian or multiquadrics functions. See Parameters.
+    smooth : float
+        Smoothing parameter. See description under Parameters.
+    norm : str or callable
+        The distance function. See description under Parameters.
+    mode : str
+        Mode of the interpolation. See description under Parameters.
+    nodes : ndarray
+        A 1-D array of node values for the interpolation.
+    A : internal property, do not use
+
+    See Also
+    --------
+    RBFInterpolator
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.interpolate import Rbf
+    >>> rng = np.random.default_rng()
+    >>> x, y, z, d = rng.random((4, 50))
+    >>> rbfi = Rbf(x, y, z, d)  # radial basis function interpolator instance
+    >>> xi = yi = zi = np.linspace(0, 1, 20)
+    >>> di = rbfi(xi, yi, zi)   # interpolated values
+    >>> di.shape
+    (20,)
+
+    """
+    # Available radial basis functions that can be selected as strings;
+    # they all start with _h_ (self._init_function relies on that)
+    def _h_multiquadric(self, r):
+        return np.sqrt((1.0/self.epsilon*r)**2 + 1)
+
+    def _h_inverse_multiquadric(self, r):
+        return 1.0/np.sqrt((1.0/self.epsilon*r)**2 + 1)
+
+    def _h_gaussian(self, r):
+        return np.exp(-(1.0/self.epsilon*r)**2)
+
+    def _h_linear(self, r):
+        return r
+
+    def _h_cubic(self, r):
+        return r**3
+
+    def _h_quintic(self, r):
+        return r**5
+
+    def _h_thin_plate(self, r):
+        return xlogy(r**2, r)
+
+    # Setup self._function and do smoke test on initial r
+    def _init_function(self, r):
+        if isinstance(self.function, str):
+            self.function = self.function.lower()
+            _mapped = {'inverse': 'inverse_multiquadric',
+                       'inverse multiquadric': 'inverse_multiquadric',
+                       'thin-plate': 'thin_plate'}
+            if self.function in _mapped:
+                self.function = _mapped[self.function]
+
+            func_name = "_h_" + self.function
+            if hasattr(self, func_name):
+                self._function = getattr(self, func_name)
+            else:
+                functionlist = [x[3:] for x in dir(self)
+                                if x.startswith('_h_')]
+                raise ValueError("function must be a callable or one of " +
+                                 ", ".join(functionlist))
+            self._function = getattr(self, "_h_"+self.function)
+        elif callable(self.function):
+            allow_one = False
+            if hasattr(self.function, 'func_code') or \
+               hasattr(self.function, '__code__'):
+                val = self.function
+                allow_one = True
+            elif hasattr(self.function, "__call__"):
+                val = self.function.__call__.__func__
+            else:
+                raise ValueError("Cannot determine number of arguments to "
+                                 "function")
+
+            argcount = val.__code__.co_argcount
+            if allow_one and argcount == 1:
+                self._function = self.function
+            elif argcount == 2:
+                self._function = self.function.__get__(self, Rbf)
+            else:
+                raise ValueError("Function argument must take 1 or 2 "
+                                 "arguments.")
+
+        a0 = self._function(r)
+        if a0.shape != r.shape:
+            raise ValueError("Callable must take array and return array of "
+                             "the same shape")
+        return a0
+
+    def __init__(self, *args, **kwargs):
+        # `args` can be a variable number of arrays; we flatten them and store
+        # them as a single 2-D array `xi` of shape (n_args-1, array_size),
+        # plus a 1-D array `di` for the values.
+        # All arrays must have the same number of elements
+        self.xi = np.asarray([np.asarray(a, dtype=np.float64).flatten()
+                              for a in args[:-1]])
+        self.N = self.xi.shape[-1]
+
+        self.mode = kwargs.pop('mode', '1-D')
+
+        if self.mode == '1-D':
+            self.di = np.asarray(args[-1]).flatten()
+            self._target_dim = 1
+        elif self.mode == 'N-D':
+            self.di = np.asarray(args[-1])
+            self._target_dim = self.di.shape[-1]
+        else:
+            raise ValueError("Mode has to be 1-D or N-D.")
+
+        if not all([x.size == self.di.shape[0] for x in self.xi]):
+            raise ValueError("All arrays must be equal length.")
+
+        self.norm = kwargs.pop('norm', 'euclidean')
+        self.epsilon = kwargs.pop('epsilon', None)
+        if self.epsilon is None:
+            # default epsilon is the "the average distance between nodes" based
+            # on a bounding hypercube
+            ximax = np.amax(self.xi, axis=1)
+            ximin = np.amin(self.xi, axis=1)
+            edges = ximax - ximin
+            edges = edges[np.nonzero(edges)]
+            self.epsilon = np.power(np.prod(edges)/self.N, 1.0/edges.size)
+
+        self.smooth = kwargs.pop('smooth', 0.0)
+        self.function = kwargs.pop('function', 'multiquadric')
+
+        # attach anything left in kwargs to self for use by any user-callable
+        # function or to save on the object returned.
+        for item, value in kwargs.items():
+            setattr(self, item, value)
+
+        # Compute weights
+        if self._target_dim > 1:  # If we have more than one target dimension,
+            # we first factorize the matrix
+            self.nodes = np.zeros((self.N, self._target_dim), dtype=self.di.dtype)
+            lu, piv = linalg.lu_factor(self.A)
+            for i in range(self._target_dim):
+                self.nodes[:, i] = linalg.lu_solve((lu, piv), self.di[:, i])
+        else:
+            self.nodes = linalg.solve(self.A, self.di)
+
+    @property
+    def A(self):
+        # this only exists for backwards compatibility: self.A was available
+        # and, at least technically, public.
+        r = squareform(pdist(self.xi.T, self.norm))  # Pairwise norm
+        return self._init_function(r) - np.eye(self.N)*self.smooth
+
+    def _call_norm(self, x1, x2):
+        return cdist(x1.T, x2.T, self.norm)
+
+    def __call__(self, *args):
+        args = [np.asarray(x) for x in args]
+        if not all([x.shape == y.shape for x in args for y in args]):
+            raise ValueError("Array lengths must be equal")
+        if self._target_dim > 1:
+            shp = args[0].shape + (self._target_dim,)
+        else:
+            shp = args[0].shape
+        xa = np.asarray([a.flatten() for a in args], dtype=np.float64)
+        r = self._call_norm(xa, self.xi)
+        return np.dot(self._function(r), self.nodes).reshape(shp)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_rbfinterp_common.py

@@ -0,0 +1,32 @@
+# Impl routines common for all backends
+from itertools import combinations_with_replacement
+from math import comb
+
+def _monomial_powers_impl(ndim, degree):
+    """Return the powers for each monomial in a polynomial.
+
+    Parameters
+    ----------
+    ndim : int
+        Number of variables in the polynomial.
+    degree : int
+        Degree of the polynomial.
+
+    Returns
+    -------
+    (nmonos, ndim) int ndarray
+        Array where each row contains the powers for each variable in a
+        monomial.
+
+    """
+    nmonos = comb(degree + ndim, ndim)
+    out = [[0]*ndim for _ in range(nmonos)]
+    count = 0
+    for deg in range(degree + 1):
+        for mono in combinations_with_replacement(range(ndim), deg):
+            # `mono` is a tuple of variables in the current monomial with
+            # multiplicity indicating power (e.g., (0, 1, 1) represents x*y**2)
+            for var in mono:
+                out[count][var] += 1
+            count += 1
+    return out

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_rbfinterp_xp.py

@@ -0,0 +1,266 @@
+"""
+'Generic' Array API backend for RBF interpolation.
+
+The general logic is this: `_rbfinterp.py` implements the user API and calls
+into either `_rbfinterp_np` (the "numpy backend"), or `_rbfinterp_xp` (the
+"generic backend".
+
+The numpy backend offloads performance-critical computations to the
+pythran-compiled `_rbfinterp_pythran` extension. This way, the call chain is
+
+    _rbfinterp.py <-- _rbfinterp_np.py <-- _rbfinterp_pythran.py
+
+The "generic" backend here is a drop-in replacement of the API of
+`_rbfinterp_np.py` for use in `_rbfinterp.py` with non-numpy arrays.
+
+The implementation closely follows `_rbfinterp_np + _rbfinterp_pythran`, with
+the following differences:
+
+  -  We used vectorized code not explicit loops in `_build_system` and
+     `_build_evaluation_coefficients`; this is more torch/jax friendly;
+  - RBF kernels are also "vectorized" and not scalar: they receive an
+    array of norms not a single norm;
+  - RBF kernels accept an extra xp= argument;
+
+In general, we would prefer less code duplication. The main blocker ATM is
+that pythran cannot compile functions with an xp= argument where xp is numpy.
+"""
+from numpy.linalg import LinAlgError
+from ._rbfinterp_common import _monomial_powers_impl
+
+
+def _monomial_powers(ndim, degree, xp):
+    out = _monomial_powers_impl(ndim, degree)
+    out = xp.asarray(out)
+    if out.shape[0] == 0:
+        out = xp.reshape(out, (0, ndim))
+    return out
+
+
+def _build_and_solve_system(y, d, smoothing, kernel, epsilon, powers, xp):
+    """Build and solve the RBF interpolation system of equations.
+
+    Parameters
+    ----------
+    y : (P, N) float ndarray
+        Data point coordinates.
+    d : (P, S) float ndarray
+        Data values at `y`.
+    smoothing : (P,) float ndarray
+        Smoothing parameter for each data point.
+    kernel : str
+        Name of the RBF.
+    epsilon : float
+        Shape parameter.
+    powers : (R, N) int ndarray
+        The exponents for each monomial in the polynomial.
+
+    Returns
+    -------
+    coeffs : (P + R, S) float ndarray
+        Coefficients for each RBF and monomial.
+    shift : (N,) float ndarray
+        Domain shift used to create the polynomial matrix.
+    scale : (N,) float ndarray
+        Domain scaling used to create the polynomial matrix.
+
+    """
+    lhs, rhs, shift, scale = _build_system(
+        y, d, smoothing, kernel, epsilon, powers, xp
+        )
+    try:
+        coeffs = xp.linalg.solve(lhs, rhs)
+    except Exception:
+        # Best-effort attempt to emit a helpful message.
+        # `_rbfinterp_np` backend gives better diagnostics; it is hard to
+        # match it in a backend-agnostic way: e.g. jax emits no error at all,
+        # and instead returns an array of nans for a singular `lhs`.
+        msg = "Singular matrix"
+        nmonos = powers.shape[0]
+        if nmonos > 0:
+            pmat = polynomial_matrix((y - shift)/scale, powers, xp=xp)
+            rank = xp.linalg.matrix_rank(pmat)
+            if rank < nmonos:
+                msg = (
+                    "Singular matrix. The matrix of monomials evaluated at "
+                    "the data point coordinates does not have full column "
+                    f"rank ({rank}/{nmonos})."
+                    )
+        raise LinAlgError(msg)
+
+    return shift, scale, coeffs
+
+
+def linear(r, xp):
+    return -r
+
+
+def thin_plate_spline(r, xp):
+    # NB: changed w.r.t. pythran, vectorized
+    return xp.where(r == 0, 0, r**2 * xp.log(r))
+
+
+def cubic(r, xp):
+    return r**3
+
+
+def quintic(r, xp):
+    return -r**5
+
+
+def multiquadric(r, xp):
+    return -xp.sqrt(r**2 + 1)
+
+
+def inverse_multiquadric(r, xp):
+    return 1.0 / xp.sqrt(r**2 + 1.0)
+
+
+def inverse_quadratic(r, xp):
+    return 1.0 / (r**2 + 1.0)
+
+
+def gaussian(r, xp):
+    return xp.exp(-r**2)
+
+
+NAME_TO_FUNC = {
+   "linear": linear,
+   "thin_plate_spline": thin_plate_spline,
+   "cubic": cubic,
+   "quintic": quintic,
+   "multiquadric": multiquadric,
+   "inverse_multiquadric": inverse_multiquadric,
+   "inverse_quadratic": inverse_quadratic,
+   "gaussian": gaussian
+   }
+
+
+def kernel_matrix(x, kernel_func, xp):
+    """Evaluate RBFs, with centers at `x`, at `x`."""
+    return kernel_func(
+        xp.linalg.vector_norm(x[None, :, :] - x[:, None, :], axis=-1), xp
+    )
+
+
+def polynomial_matrix(x, powers, xp):
+    """Evaluate monomials, with exponents from `powers`, at `x`."""
+    return xp.prod(x[:, None, :] ** powers, axis=-1)
+
+
+def _build_system(y, d, smoothing, kernel, epsilon, powers, xp):
+    """Build the system used to solve for the RBF interpolant coefficients.
+
+    Parameters
+    ----------
+    y : (P, N) float ndarray
+        Data point coordinates.
+    d : (P, S) float ndarray
+        Data values at `y`.
+    smoothing : (P,) float ndarray
+        Smoothing parameter for each data point.
+    kernel : str
+        Name of the RBF.
+    epsilon : float
+        Shape parameter.
+    powers : (R, N) int ndarray
+        The exponents for each monomial in the polynomial.
+
+    Returns
+    -------
+    lhs : (P + R, P + R) float ndarray
+        Left-hand side matrix.
+    rhs : (P + R, S) float ndarray
+        Right-hand side matrix.
+    shift : (N,) float ndarray
+        Domain shift used to create the polynomial matrix.
+    scale : (N,) float ndarray
+        Domain scaling used to create the polynomial matrix.
+
+    """
+    s = d.shape[1]
+    r = powers.shape[0]
+    kernel_func = NAME_TO_FUNC[kernel]
+
+    # Shift and scale the polynomial domain to be between -1 and 1
+    mins = xp.min(y, axis=0)
+    maxs = xp.max(y, axis=0)
+    shift = (maxs + mins)/2
+    scale = (maxs - mins)/2
+    # The scale may be zero if there is a single point or all the points have
+    # the same value for some dimension. Avoid division by zero by replacing
+    # zeros with ones.
+    scale = xp.where(scale == 0.0, 1.0, scale)
+
+    yeps = y*epsilon
+    yhat = (y - shift)/scale
+
+    out_kernels  = kernel_matrix(yeps, kernel_func, xp)
+    out_poly = polynomial_matrix(yhat, powers, xp)
+
+    lhs = xp.concat(
+        [
+         xp.concat((out_kernels, out_poly), axis=1),
+         xp.concat((out_poly.T, xp.zeros((r, r))), axis=1)
+        ]
+    , axis=0) + xp.diag(xp.concat([smoothing, xp.zeros(r)]))
+
+    rhs = xp.concat([d, xp.zeros((r, s))], axis=0)
+
+    return lhs, rhs, shift, scale
+
+
+def _build_evaluation_coefficients(
+    x, y, kernel, epsilon, powers, shift, scale, xp
+):
+    """Construct the coefficients needed to evaluate
+    the RBF.
+
+    Parameters
+    ----------
+    x : (Q, N) float ndarray
+        Evaluation point coordinates.
+    y : (P, N) float ndarray
+        Data point coordinates.
+    kernel : str
+        Name of the RBF.
+    epsilon : float
+        Shape parameter.
+    powers : (R, N) int ndarray
+        The exponents for each monomial in the polynomial.
+    shift : (N,) float ndarray
+        Shifts the polynomial domain for numerical stability.
+    scale : (N,) float ndarray
+        Scales the polynomial domain for numerical stability.
+
+    Returns
+    -------
+    (Q, P + R) float ndarray
+
+    """
+    kernel_func = NAME_TO_FUNC[kernel]
+
+    yeps = y*epsilon
+    xeps = x*epsilon
+    xhat = (x - shift)/scale
+
+    # NB: changed w.r.t. pythran
+    vec = xp.concat(
+        [
+            kernel_func(
+                xp.linalg.vector_norm(
+                    xeps[:, None, :] - yeps[None, :, :], axis=-1
+                ), xp
+            ),
+            xp.prod(xhat[:, None, :] ** powers, axis=-1)
+        ], axis=-1
+    )
+
+    return vec
+
+
+def compute_interpolation(x, y, kernel, epsilon, powers, shift, scale, coeffs, xp):
+    vec = _build_evaluation_coefficients(
+        x, y, kernel, epsilon, powers, shift, scale, xp
+    )
+    return vec @ coeffs

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/_rgi.py

@@ -0,0 +1,812 @@
+__all__ = ['RegularGridInterpolator', 'interpn']
+
+import itertools
+from types import GenericAlias
+
+import numpy as np
+
+import scipy.sparse.linalg as ssl
+from scipy._lib._array_api import array_namespace, xp_capabilities
+from scipy._lib.array_api_compat import is_array_api_obj
+
+from ._interpnd import _ndim_coords_from_arrays
+from ._cubic import PchipInterpolator
+from ._rgi_cython import evaluate_linear_2d, find_indices
+from ._bsplines import make_interp_spline
+from ._fitpack2 import RectBivariateSpline
+from ._ndbspline import make_ndbspl
+
+
+def _check_points(points):
+    descending_dimensions = []
+    grid = []
+    for i, p in enumerate(points):
+        # early make points float
+        # see https://github.com/scipy/scipy/pull/17230
+        p = np.asarray(p, dtype=float)
+        if not np.all(p[1:] > p[:-1]):
+            if np.all(p[1:] < p[:-1]):
+                # input is descending, so make it ascending
+                descending_dimensions.append(i)
+                p = np.flip(p)
+            else:
+                raise ValueError(
+                    f"The points in dimension {i} must be strictly ascending or "
+                    f"descending"
+                )
+        # see https://github.com/scipy/scipy/issues/17716
+        p = np.ascontiguousarray(p)
+        grid.append(p)
+    return tuple(grid), tuple(descending_dimensions)
+
+
+def _check_dimensionality(points, values):
+    if len(points) > values.ndim:
+        raise ValueError(
+            f"There are {len(points)} point arrays, but values has "
+            f"{values.ndim} dimensions"
+        )
+    for i, p in enumerate(points):
+        if not np.asarray(p).ndim == 1:
+            raise ValueError(f"The points in dimension {i} must be 1-dimensional")
+        if not values.shape[i] == len(p):
+            raise ValueError(
+                f"There are {len(p)} points and {values.shape[i]} values in "
+                f"dimension {i}"
+            )
+
+
+@xp_capabilities(
+    cpu_only=True, jax_jit=False,
+    skip_backends=[
+        ("dask.array",
+         "https://github.com/data-apis/array-api-extra/issues/488")
+    ]
+)
+class RegularGridInterpolator:
+    """Interpolator of specified order on a rectilinear grid in N ≥ 1 dimensions.
+
+    The data must be defined on a rectilinear grid; that is, a rectangular
+    grid with even or uneven spacing. Linear, nearest-neighbor, spline
+    interpolations are supported. After setting up the interpolator object,
+    the interpolation method may be chosen at each evaluation.
+
+    Parameters
+    ----------
+    points : tuple of ndarray of float, with shapes (m1, ), ..., (mn, )
+        The points defining the regular grid in n dimensions. The points in
+        each dimension (i.e. every elements of the points tuple) must be
+        strictly ascending or descending.
+
+    values : array_like, shape (m1, ..., mn, ...)
+        The data on the regular grid in n dimensions. Complex data is
+        accepted.
+
+    method : str, optional
+        The method of interpolation to perform. Supported are "linear",
+        "nearest", "slinear", "cubic", "quintic" and "pchip". This
+        parameter will become the default for the object's ``__call__``
+        method. Default is "linear".
+
+    bounds_error : bool, optional
+        If True, when interpolated values are requested outside of the
+        domain of the input data, a ValueError is raised.
+        If False, then `fill_value` is used.
+        Default is True.
+
+    fill_value : float or None, optional
+        The value to use for points outside of the interpolation domain.
+        If None, values outside the domain are extrapolated.
+        Default is ``np.nan``.
+
+    solver : callable, optional
+        Only used for methods "slinear", "cubic" and "quintic".
+        Sparse linear algebra solver for construction of the NdBSpline instance.
+        Default is the iterative solver `scipy.sparse.linalg.gcrotmk`.
+
+        .. versionadded:: 1.13
+
+    solver_args: dict, optional
+        Additional arguments to pass to `solver`, if any.
+
+        .. versionadded:: 1.13
+
+    Methods
+    -------
+    __call__
+
+    Attributes
+    ----------
+    grid : tuple of ndarrays
+        The points defining the regular grid in n dimensions.
+        This tuple defines the full grid via
+        ``np.meshgrid(*grid, indexing='ij')``
+    values : ndarray
+        Data values at the grid.
+    method : str
+        Interpolation method.
+    fill_value : float or ``None``
+        Use this value for out-of-bounds arguments to `__call__`.
+    bounds_error : bool
+        If ``True``, out-of-bounds argument raise a ``ValueError``.
+
+    Notes
+    -----
+    Contrary to `LinearNDInterpolator` and `NearestNDInterpolator`, this class
+    avoids expensive triangulation of the input data by taking advantage of the
+    regular grid structure.
+
+    In other words, this class assumes that the data is defined on a
+    *rectilinear* grid.
+
+    .. versionadded:: 0.14
+
+    The 'slinear'(k=1), 'cubic'(k=3), and 'quintic'(k=5) methods are
+    tensor-product spline interpolators, where `k` is the spline degree,
+    If any dimension has fewer points than `k` + 1, an error will be raised.
+
+    .. versionadded:: 1.9
+
+    If the input data is such that dimensions have incommensurate
+    units and differ by many orders of magnitude, the interpolant may have
+    numerical artifacts. Consider rescaling the data before interpolating.
+
+    **Choosing a solver for spline methods**
+
+    Spline methods, "slinear", "cubic" and "quintic" involve solving a
+    large sparse linear system at instantiation time. Depending on data,
+    the default solver may or may not be adequate. When it is not, you may
+    need to experiment with an optional `solver` argument, where you may
+    choose between the direct solver (`scipy.sparse.linalg.spsolve`) or
+    iterative solvers from `scipy.sparse.linalg`. You may need to supply
+    additional parameters via the optional `solver_args` parameter (for instance,
+    you may supply the starting value or target tolerance). See the
+    `scipy.sparse.linalg` documentation for the full list of available options.
+
+    Alternatively, you may instead use the legacy methods, "slinear_legacy",
+    "cubic_legacy" and "quintic_legacy". These methods allow faster construction
+    but evaluations will be much slower.
+
+    **Rounding rule at half points with `nearest` method**
+
+    The rounding rule with the `nearest` method at half points is rounding *down*.
+
+
+    Examples
+    --------
+    **Evaluate a function on the points of a 3-D grid**
+
+    As a first example, we evaluate a simple example function on the points of
+    a 3-D grid:
+
+    >>> from scipy.interpolate import RegularGridInterpolator
+    >>> import numpy as np
+    >>> def f(x, y, z):
+    ...     return 2 * x**3 + 3 * y**2 - z
+    >>> x = np.linspace(1, 4, 11)
+    >>> y = np.linspace(4, 7, 22)
+    >>> z = np.linspace(7, 9, 33)
+    >>> xg, yg ,zg = np.meshgrid(x, y, z, indexing='ij', sparse=True)
+    >>> data = f(xg, yg, zg)
+
+    ``data`` is now a 3-D array with ``data[i, j, k] = f(x[i], y[j], z[k])``.
+    Next, define an interpolating function from this data:
+
+    >>> interp = RegularGridInterpolator((x, y, z), data)
+
+    Evaluate the interpolating function at the two points
+    ``(x,y,z) = (2.1, 6.2, 8.3)`` and ``(3.3, 5.2, 7.1)``:
+
+    >>> pts = np.array([[2.1, 6.2, 8.3],
+    ...                 [3.3, 5.2, 7.1]])
+    >>> interp(pts)
+    array([ 125.80469388,  146.30069388])
+
+    which is indeed a close approximation to
+
+    >>> f(2.1, 6.2, 8.3), f(3.3, 5.2, 7.1)
+    (125.54200000000002, 145.894)
+
+    **Interpolate and extrapolate a 2D dataset**
+
+    As a second example, we interpolate and extrapolate a 2D data set:
+
+    >>> x, y = np.array([-2, 0, 4]), np.array([-2, 0, 2, 5])
+    >>> def ff(x, y):
+    ...     return x**2 + y**2
+
+    >>> xg, yg = np.meshgrid(x, y, indexing='ij')
+    >>> data = ff(xg, yg)
+    >>> interp = RegularGridInterpolator((x, y), data,
+    ...                                  bounds_error=False, fill_value=None)
+
+    >>> import matplotlib.pyplot as plt
+    >>> fig = plt.figure()
+    >>> ax = fig.add_subplot(projection='3d')
+    >>> ax.scatter(xg.ravel(), yg.ravel(), data.ravel(),
+    ...            s=60, c='k', label='data')
+
+    Evaluate and plot the interpolator on a finer grid
+
+    >>> xx = np.linspace(-4, 9, 31)
+    >>> yy = np.linspace(-4, 9, 31)
+    >>> X, Y = np.meshgrid(xx, yy, indexing='ij')
+
+    >>> # interpolator
+    >>> ax.plot_wireframe(X, Y, interp((X, Y)), rstride=3, cstride=3,
+    ...                   alpha=0.4, color='m', label='linear interp')
+
+    >>> # ground truth
+    >>> ax.plot_wireframe(X, Y, ff(X, Y), rstride=3, cstride=3,
+    ...                   alpha=0.4, label='ground truth')
+    >>> plt.legend()
+    >>> plt.show()
+
+    Other examples are given
+    :ref:`in the tutorial <tutorial-interpolate_regular_grid_interpolator>`.
+
+    See Also
+    --------
+    NearestNDInterpolator : Nearest neighbor interpolator on *unstructured*
+                            data in N dimensions
+
+    LinearNDInterpolator : Piecewise linear interpolator on *unstructured* data
+                           in N dimensions
+
+    interpn : a convenience function which wraps `RegularGridInterpolator`
+
+    scipy.ndimage.map_coordinates : interpolation on grids with equal spacing
+                                    (suitable for e.g., N-D image resampling)
+
+    References
+    ----------
+    .. [1] Python package *regulargrid* by Johannes Buchner, see
+           https://pypi.python.org/pypi/regulargrid/
+    .. [2] Wikipedia, "Trilinear interpolation",
+           https://en.wikipedia.org/wiki/Trilinear_interpolation
+    .. [3] Weiser, Alan, and Sergio E. Zarantonello. "A note on piecewise linear
+           and multilinear table interpolation in many dimensions." MATH.
+           COMPUT. 50.181 (1988): 189-196.
+           https://www.ams.org/journals/mcom/1988-50-181/S0025-5718-1988-0917826-0/S0025-5718-1988-0917826-0.pdf
+           :doi:`10.1090/S0025-5718-1988-0917826-0`
+
+    """
+    # this class is based on code originally programmed by Johannes Buchner,
+    # see https://github.com/JohannesBuchner/regulargrid
+
+    _SPLINE_DEGREE_MAP = {"slinear": 1, "cubic": 3, "quintic": 5, 'pchip': 3,
+                          "slinear_legacy": 1, "cubic_legacy": 3, "quintic_legacy": 5,}
+    _SPLINE_METHODS_recursive = {"slinear_legacy", "cubic_legacy",
+                                "quintic_legacy", "pchip"}
+    _SPLINE_METHODS_ndbspl = {"slinear", "cubic", "quintic"}
+    _SPLINE_METHODS = list(_SPLINE_DEGREE_MAP.keys())
+    _ALL_METHODS = ["linear", "nearest"] + _SPLINE_METHODS
+
+    # generic type compatibility with scipy-stubs
+    __class_getitem__ = classmethod(GenericAlias)
+
+    def __init__(self, points, values, method="linear", bounds_error=True,
+                 fill_value=np.nan, *, solver=None, solver_args=None):
+        if method not in self._ALL_METHODS:
+            raise ValueError(f"Method '{method}' is not defined")
+        elif method in self._SPLINE_METHODS:
+            self._validate_grid_dimensions(points, method)   # NB: uses np.atleast_1d
+
+        try:
+            xp = array_namespace(*points, values)
+        except Exception as e:
+            # either "duck-type" values or a user error?
+            xp = array_namespace(*points) # still forbid mixed namespaces in `points`
+            try:
+                xp_v = array_namespace(values)
+            except Exception:
+                # "duck-type" values indeed, continue with `xp` as the namespace
+                pass
+            else:
+                # both `points` and `values` are array API objects, check consistency
+                if xp_v != xp:
+                    raise e
+
+        self._asarray = xp.asarray
+        self.method = method
+        self._spline = None
+        self.bounds_error = bounds_error
+        self._grid, self._descending_dimensions = _check_points(points)
+        self._values = self._check_values(values)
+        self._check_dimensionality(self._grid, self._values)
+        self.fill_value = self._check_fill_value(self._values, fill_value)
+        if self._descending_dimensions:
+            self._values = np.flip(values, axis=self._descending_dimensions)
+        if self.method == "pchip" and np.iscomplexobj(self._values):
+            msg = ("`PchipInterpolator` only works with real values. If you are trying "
+                   "to use the real components of the passed array, use `np.real` on "
+                   "the array before passing to `RegularGridInterpolator`.")
+            raise ValueError(msg)
+        if method in self._SPLINE_METHODS_ndbspl:
+            if solver_args is None:
+                solver_args = {}
+            self._spline = self._construct_spline(method, solver, **solver_args)
+        else:
+            if solver is not None or solver_args:
+                raise ValueError(
+                    f"{method =} does not accept the 'solver' argument. Got "
+                    f" {solver = } and with arguments {solver_args}."
+                )
+
+    def _construct_spline(self, method, solver=None, **solver_args):
+        if solver is None:
+            solver = ssl.gcrotmk
+        spl = make_ndbspl(
+                self._grid, self._values, self._SPLINE_DEGREE_MAP[method],
+                solver=solver, **solver_args
+              )
+        return spl
+
+    def _check_dimensionality(self, grid, values):
+        _check_dimensionality(grid, values)
+
+    def _check_points(self, points):
+        return _check_points(points)
+
+    def _check_values(self, values):
+        if is_array_api_obj(values):
+            values = np.asarray(values)
+
+        if not hasattr(values, 'ndim'):
+            # allow reasonable duck-typed values
+            values = np.asarray(values)
+
+        if hasattr(values, 'dtype') and hasattr(values, 'astype'):
+            if not np.issubdtype(values.dtype, np.inexact):
+                values = values.astype(float)
+
+        return values
+
+    def _check_fill_value(self, values, fill_value):
+        if fill_value is not None:
+            fill_value_dtype = np.asarray(fill_value).dtype
+            if (hasattr(values, 'dtype') and not
+                    np.can_cast(fill_value_dtype, values.dtype,
+                                casting='same_kind')):
+                raise ValueError("fill_value must be either 'None' or "
+                                 "of a type compatible with values")
+        return fill_value
+
+    def __call__(self, xi, method=None, *, nu=None):
+        """
+        Interpolation at coordinates.
+
+        Parameters
+        ----------
+        xi : ndarray of shape (..., ndim)
+            The coordinates to evaluate the interpolator at.
+
+        method : str, optional
+            The method of interpolation to perform. Supported are "linear",
+            "nearest", "slinear", "cubic", "quintic" and "pchip". Default is
+            the method chosen when the interpolator was created.
+
+        nu : sequence of ints, length ndim, optional
+            If not None, the orders of the derivatives to evaluate.
+            Each entry must be non-negative.
+            Only allowed for methods "slinear", "cubic" and "quintic".
+
+            .. versionadded:: 1.13
+
+        Returns
+        -------
+        values_x : ndarray, shape xi.shape[:-1] + values.shape[ndim:]
+            Interpolated values at `xi`. See notes for behaviour when
+            ``xi.ndim == 1``.
+
+        Notes
+        -----
+        In the case that ``xi.ndim == 1`` a new axis is inserted into
+        the 0 position of the returned array, values_x, so its shape is
+        instead ``(1,) + values.shape[ndim:]``.
+
+        Examples
+        --------
+        Here we define a nearest-neighbor interpolator of a simple function
+
+        >>> import numpy as np
+        >>> x, y = np.array([0, 1, 2]), np.array([1, 3, 7])
+        >>> def f(x, y):
+        ...     return x**2 + y**2
+        >>> data = f(*np.meshgrid(x, y, indexing='ij', sparse=True))
+        >>> from scipy.interpolate import RegularGridInterpolator
+        >>> interp = RegularGridInterpolator((x, y), data, method='nearest')
+
+        By construction, the interpolator uses the nearest-neighbor
+        interpolation
+
+        >>> interp([[1.5, 1.3], [0.3, 4.5]])
+        array([2., 9.])
+
+        We can however evaluate the linear interpolant by overriding the
+        `method` parameter
+
+        >>> interp([[1.5, 1.3], [0.3, 4.5]], method='linear')
+        array([ 4.7, 24.3])
+        """
+        _spline = self._spline
+        method = self.method if method is None else method
+        is_method_changed = self.method != method
+        if method not in self._ALL_METHODS:
+            raise ValueError(f"Method '{method}' is not defined")
+        if is_method_changed and method in self._SPLINE_METHODS_ndbspl:
+            _spline = self._construct_spline(method)
+
+        if nu is not None and method not in self._SPLINE_METHODS_ndbspl:
+            raise ValueError(
+                f"Can only compute derivatives for methods "
+                f"{self._SPLINE_METHODS_ndbspl}, got {method =}."
+            )
+
+        xi, xi_shape, ndim, nans, out_of_bounds = self._prepare_xi(xi)
+
+        if method == "linear":
+            indices, norm_distances = self._find_indices(xi.T)
+            if (ndim == 2 and hasattr(self._values, 'dtype') and
+                    self._values.ndim == 2 and self._values.flags.writeable and
+                    self._values.dtype in (np.float64, np.complex128) and
+                    self._values.dtype.byteorder == '='):
+                # until cython supports const fused types, the fast path
+                # cannot support non-writeable values
+                # a fast path
+                out = np.empty(indices.shape[1], dtype=self._values.dtype)
+                result = evaluate_linear_2d(self._values,
+                                            indices,
+                                            norm_distances,
+                                            self._grid,
+                                            out)
+            else:
+                result = self._evaluate_linear(indices, norm_distances)
+        elif method == "nearest":
+            indices, norm_distances = self._find_indices(xi.T)
+            result = self._evaluate_nearest(indices, norm_distances)
+        elif method in self._SPLINE_METHODS:
+            if is_method_changed:
+                self._validate_grid_dimensions(self._grid, method)
+            if method in self._SPLINE_METHODS_recursive:
+                result = self._evaluate_spline(xi, method)
+            else:
+                result = _spline(xi, nu=nu)
+
+        if not self.bounds_error and self.fill_value is not None:
+            result[out_of_bounds] = self.fill_value
+
+        # f(nan) = nan, if any
+        if np.any(nans):
+            result[nans] = np.nan
+        return self._asarray(result.reshape(xi_shape[:-1] + self._values.shape[ndim:]))
+
+    @property
+    def grid(self):
+        return tuple(self._asarray(p) for p in self._grid)
+
+    @property
+    def values(self):
+        return self._asarray(self._values)
+
+    def _prepare_xi(self, xi):
+        ndim = len(self._grid)
+        xi = _ndim_coords_from_arrays(xi, ndim=ndim)
+        if xi.shape[-1] != ndim:
+            raise ValueError("The requested sample points xi have dimension "
+                             f"{xi.shape[-1]} but this "
+                             f"RegularGridInterpolator has dimension {ndim}")
+
+        xi_shape = xi.shape
+        xi = xi.reshape(-1, xi_shape[-1])
+        xi = np.asarray(xi, dtype=float)
+
+        # find nans in input
+        nans = np.any(np.isnan(xi), axis=-1)
+
+        if self.bounds_error:
+            for i, p in enumerate(xi.T):
+                if not np.logical_and(np.all(self._grid[i][0] <= p),
+                                      np.all(p <= self._grid[i][-1])):
+                    raise ValueError(
+                        f"One of the requested xi is out of bounds in dimension {i}"
+                    )
+            out_of_bounds = None
+        else:
+            out_of_bounds = self._find_out_of_bounds(xi.T)
+
+        return xi, xi_shape, ndim, nans, out_of_bounds
+
+    def _evaluate_linear(self, indices, norm_distances):
+        # slice for broadcasting over trailing dimensions in self._values
+        vslice = (slice(None),) + (None,)*(self._values.ndim - len(indices))
+
+        # Compute shifting up front before zipping everything together
+        shift_norm_distances = [1 - yi for yi in norm_distances]
+        shift_indices = [i + 1 for i in indices]
+
+        # The formula for linear interpolation in 2d takes the form:
+        # values = self._values[(i0, i1)] * (1 - y0) * (1 - y1) + \
+        #          self._values[(i0, i1 + 1)] * (1 - y0) * y1 + \
+        #          self._values[(i0 + 1, i1)] * y0 * (1 - y1) + \
+        #          self._values[(i0 + 1, i1 + 1)] * y0 * y1
+        # We pair i with 1 - yi (zipped1) and i + 1 with yi (zipped2)
+        zipped1 = zip(indices, shift_norm_distances)
+        zipped2 = zip(shift_indices, norm_distances)
+
+        # Take all products of zipped1 and zipped2 and iterate over them
+        # to get the terms in the above formula. This corresponds to iterating
+        # over the vertices of a hypercube.
+        hypercube = itertools.product(*zip(zipped1, zipped2))
+        value = np.array([0.])
+        for h in hypercube:
+            edge_indices, weights = zip(*h)
+            weight = np.array([1.])
+            for w in weights:
+                weight = weight * w
+            term = np.asarray(self._values[edge_indices]) * weight[vslice]
+            value = value + term   # cannot use += because broadcasting
+        return value
+
+    def _evaluate_nearest(self, indices, norm_distances):
+        idx_res = [np.where(yi <= .5, i, i + 1)
+                   for i, yi in zip(indices, norm_distances)]
+        return self._values[tuple(idx_res)]
+
+    def _validate_grid_dimensions(self, points, method):
+        k = self._SPLINE_DEGREE_MAP[method]
+        for i, point in enumerate(points):
+            ndim = len(np.atleast_1d(point))
+            if ndim <= k:
+                raise ValueError(f"There are {ndim} points in dimension {i},"
+                                 f" but method {method} requires at least "
+                                 f" {k+1} points per dimension.")
+
+    def _evaluate_spline(self, xi, method):
+        # ensure xi is 2D list of points to evaluate (`m` is the number of
+        # points and `n` is the number of interpolation dimensions,
+        # ``n == len(self._grid)``.)
+        if xi.ndim == 1:
+            xi = xi.reshape((1, xi.size))
+        m, n = xi.shape
+
+        # Reorder the axes: n-dimensional process iterates over the
+        # interpolation axes from the last axis downwards: E.g. for a 4D grid
+        # the order of axes is 3, 2, 1, 0. Each 1D interpolation works along
+        # the 0th axis of its argument array (for 1D routine it's its ``y``
+        # array). Thus permute the interpolation axes of `values` *and keep
+        # trailing dimensions trailing*.
+        axes = tuple(range(self._values.ndim))
+        axx = axes[:n][::-1] + axes[n:]
+        values = self._values.transpose(axx)
+
+        if method == 'pchip':
+            _eval_func = self._do_pchip
+        else:
+            _eval_func = self._do_spline_fit
+        k = self._SPLINE_DEGREE_MAP[method]
+
+        # Non-stationary procedure: difficult to vectorize this part entirely
+        # into numpy-level operations. Unfortunately this requires explicit
+        # looping over each point in xi.
+
+        # can at least vectorize the first pass across all points in the
+        # last variable of xi.
+        last_dim = n - 1
+        first_values = _eval_func(self._grid[last_dim],
+                                  values,
+                                  xi[:, last_dim],
+                                  k)
+
+        # the rest of the dimensions have to be on a per point-in-xi basis
+        shape = (m, *self._values.shape[n:])
+        result = np.empty(shape, dtype=self._values.dtype)
+        for j in range(m):
+            # Main process: Apply 1D interpolate in each dimension
+            # sequentially, starting with the last dimension.
+            # These are then "folded" into the next dimension in-place.
+            folded_values = first_values[j, ...]
+            for i in range(last_dim-1, -1, -1):
+                # Interpolate for each 1D from the last dimensions.
+                # This collapses each 1D sequence into a scalar.
+                folded_values = _eval_func(self._grid[i],
+                                           folded_values,
+                                           xi[j, i],
+                                           k)
+            result[j, ...] = folded_values
+
+        return result
+
+    @staticmethod
+    def _do_spline_fit(x, y, pt, k):
+        local_interp = make_interp_spline(x, y, k=k, axis=0)
+        values = local_interp(pt)
+        return values
+
+    @staticmethod
+    def _do_pchip(x, y, pt, k):
+        local_interp = PchipInterpolator(x, y, axis=0)
+        values = local_interp(pt)
+        return values
+
+    def _find_indices(self, xi):
+        return find_indices(self._grid, xi)
+
+    def _find_out_of_bounds(self, xi):
+        # check for out of bounds xi
+        out_of_bounds = np.zeros((xi.shape[1]), dtype=bool)
+        # iterate through dimensions
+        for x, grid in zip(xi, self._grid):
+            out_of_bounds += x < grid[0]
+            out_of_bounds += x > grid[-1]
+        return out_of_bounds
+
+
+def interpn(points, values, xi, method="linear", bounds_error=True,
+            fill_value=np.nan):
+    """
+    Multidimensional interpolation on regular or rectilinear grids.
+
+    Strictly speaking, not all regular grids are supported - this function
+    works on *rectilinear* grids, that is, a rectangular grid with even or
+    uneven spacing.
+
+    Parameters
+    ----------
+    points : tuple of ndarray of float, with shapes (m1, ), ..., (mn, )
+        The points defining the regular grid in n dimensions. The points in
+        each dimension (i.e. every elements of the points tuple) must be
+        strictly ascending or descending.
+
+    values : array_like, shape (m1, ..., mn, ...)
+        The data on the regular grid in n dimensions. Complex data is
+        accepted.
+    xi : ndarray of shape (..., ndim)
+        The coordinates to sample the gridded data at
+
+    method : str, optional
+        The method of interpolation to perform. Supported are "linear",
+        "nearest", "slinear", "cubic", "quintic", "pchip", and "splinef2d".
+        "splinef2d" is only supported for 2-dimensional data.
+
+    bounds_error : bool, optional
+        If True, when interpolated values are requested outside of the
+        domain of the input data, a ValueError is raised.
+        If False, then `fill_value` is used.
+
+    fill_value : number, optional
+        If provided, the value to use for points outside of the
+        interpolation domain. If None, values outside
+        the domain are extrapolated.  Extrapolation is not supported by method
+        "splinef2d".
+
+    Returns
+    -------
+    values_x : ndarray, shape xi.shape[:-1] + values.shape[ndim:]
+        Interpolated values at `xi`. See notes for behaviour when
+        ``xi.ndim == 1``.
+
+    See Also
+    --------
+    NearestNDInterpolator : Nearest neighbor interpolation on unstructured
+                            data in N dimensions
+    LinearNDInterpolator : Piecewise linear interpolant on unstructured data
+                           in N dimensions
+    RegularGridInterpolator : interpolation on a regular or rectilinear grid
+                              in arbitrary dimensions (`interpn` wraps this
+                              class).
+    RectBivariateSpline : Bivariate spline approximation over a rectangular mesh
+    scipy.ndimage.map_coordinates : interpolation on grids with equal spacing
+                                    (suitable for e.g., N-D image resampling)
+
+    Notes
+    -----
+
+    .. versionadded:: 0.14
+
+    In the case that ``xi.ndim == 1`` a new axis is inserted into
+    the 0 position of the returned array, values_x, so its shape is
+    instead ``(1,) + values.shape[ndim:]``.
+
+    If the input data is such that input dimensions have incommensurate
+    units and differ by many orders of magnitude, the interpolant may have
+    numerical artifacts. Consider rescaling the data before interpolation.
+
+    Examples
+    --------
+    Evaluate a simple example function on the points of a regular 3-D grid:
+
+    >>> import numpy as np
+    >>> from scipy.interpolate import interpn
+    >>> def value_func_3d(x, y, z):
+    ...     return 2 * x + 3 * y - z
+    >>> x = np.linspace(0, 4, 5)
+    >>> y = np.linspace(0, 5, 6)
+    >>> z = np.linspace(0, 6, 7)
+    >>> points = (x, y, z)
+    >>> values = value_func_3d(*np.meshgrid(*points, indexing='ij'))
+
+    Evaluate the interpolating function at a point
+
+    >>> point = np.array([2.21, 3.12, 1.15])
+    >>> print(interpn(points, values, point))
+    [12.63]
+
+    Compare with value at point by function
+
+    >>> value_func_3d(*point)
+    12.63 # up to rounding
+
+    Since the function is linear, the interpolation is exact using linear method.
+
+    """
+    # sanity check 'method' kwarg
+    if method not in ["linear", "nearest", "cubic", "quintic", "pchip",
+                      "splinef2d", "slinear",
+                      "slinear_legacy", "cubic_legacy", "quintic_legacy"]:
+        raise ValueError("interpn only understands the methods 'linear', "
+                         "'nearest', 'slinear', 'cubic', 'quintic', 'pchip', "
+                         f"and 'splinef2d'. You provided {method}.")
+
+    if not hasattr(values, 'ndim'):
+        values = np.asarray(values)
+
+    ndim = values.ndim
+    if ndim > 2 and method == "splinef2d":
+        raise ValueError("The method splinef2d can only be used for "
+                         "2-dimensional input data")
+    if not bounds_error and fill_value is None and method == "splinef2d":
+        raise ValueError("The method splinef2d does not support extrapolation.")
+
+    # sanity check consistency of input dimensions
+    if len(points) > ndim:
+        raise ValueError(
+            f"There are {len(points)} point arrays, but values has {ndim} dimensions"
+        )
+    if len(points) != ndim and method == 'splinef2d':
+        raise ValueError("The method splinef2d can only be used for "
+                         "scalar data with one point per coordinate")
+
+    grid, descending_dimensions = _check_points(points)
+    _check_dimensionality(grid, values)
+
+    # sanity check requested xi
+    xi = _ndim_coords_from_arrays(xi, ndim=len(grid))
+    if xi.shape[-1] != len(grid):
+        raise ValueError(
+            f"The requested sample points xi have dimension {xi.shape[-1]}, "
+            f"but this RegularGridInterpolator has dimension {len(grid)}"
+        )
+
+    if bounds_error:
+        for i, p in enumerate(xi.T):
+            if not np.logical_and(np.all(grid[i][0] <= p),
+                                  np.all(p <= grid[i][-1])):
+                raise ValueError(
+                    f"One of the requested xi is out of bounds in dimension {i}"
+                )
+
+    # perform interpolation
+    if method in RegularGridInterpolator._ALL_METHODS:
+        interp = RegularGridInterpolator(points, values, method=method,
+                                         bounds_error=bounds_error,
+                                         fill_value=fill_value)
+        return interp(xi)
+    elif method == "splinef2d":
+        xi_shape = xi.shape
+        xi = xi.reshape(-1, xi.shape[-1])
+
+        # RectBivariateSpline doesn't support fill_value; we need to wrap here
+        idx_valid = np.all((grid[0][0] <= xi[:, 0], xi[:, 0] <= grid[0][-1],
+                            grid[1][0] <= xi[:, 1], xi[:, 1] <= grid[1][-1]),
+                           axis=0)
+        result = np.empty_like(xi[:, 0])
+
+        # make a copy of values for RectBivariateSpline
+        interp = RectBivariateSpline(points[0], points[1], values[:])
+        result[idx_valid] = interp.ev(xi[idx_valid, 0], xi[idx_valid, 1])
+        result[np.logical_not(idx_valid)] = fill_value
+
+        return result.reshape(xi_shape[:-1])
+    else:
+        raise ValueError(f"unknown {method = }")

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/dfitpack.py

@@ -0,0 +1,24 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'spalde',
+    'splder',
+    'splev',
+    'splint',
+    'sproot',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="dfitpack",
+                                   private_modules=["_dfitpack"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/fitpack.py

@@ -0,0 +1,31 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'BSpline',
+    'bisplev',
+    'bisplrep',
+    'insert',
+    'spalde',
+    'splantider',
+    'splder',
+    'splev',
+    'splint',
+    'splprep',
+    'splrep',
+    'sproot',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="fitpack",
+                                   private_modules=["_fitpack_py"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/fitpack2.py

@@ -0,0 +1,29 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'BivariateSpline',
+    'InterpolatedUnivariateSpline',
+    'LSQBivariateSpline',
+    'LSQSphereBivariateSpline',
+    'LSQUnivariateSpline',
+    'RectBivariateSpline',
+    'RectSphereBivariateSpline',
+    'SmoothBivariateSpline',
+    'SmoothSphereBivariateSpline',
+    'UnivariateSpline',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="fitpack2",
+                                   private_modules=["_fitpack2"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/interpnd.py

@@ -0,0 +1,21 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'CloughTocher2DInterpolator',
+    'LinearNDInterpolator',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="interpnd",
+                                   private_modules=["_interpnd"], all=__all__,
+                                   attribute=name, dep_version="1.17.0")

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/ndgriddata.py

@@ -0,0 +1,23 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'CloughTocher2DInterpolator',
+    'LinearNDInterpolator',
+    'NearestNDInterpolator',
+    'griddata',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="ndgriddata",
+                                   private_modules=["_ndgriddata"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/interpolate/polyint.py

@@ -0,0 +1,24 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.interpolate` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'BarycentricInterpolator',
+    'KroghInterpolator',
+    'approximate_taylor_polynomial',
+    'barycentric_interpolate',
+    'krogh_interpolate',
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="interpolate", module="polyint",
+                                   private_modules=["_polyint"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/__init__.py

@@ -0,0 +1,121 @@
+"""
+==================================
+Input and output (:mod:`scipy.io`)
+==================================
+
+.. currentmodule:: scipy.io
+
+.. toctree::
+   :hidden:
+
+   io.matlab
+
+SciPy has many modules, classes, and functions available to read data
+from and write data to a variety of file formats.
+
+.. seealso:: `NumPy IO routines <https://www.numpy.org/devdocs/reference/routines.io.html>`__
+
+MATLAB® files
+=============
+
+.. autosummary::
+   :toctree: generated/
+
+   loadmat - Read a MATLAB style mat file (version 4 through 7.1)
+   savemat - Write a MATLAB style mat file (version 4 through 7.1)
+   whosmat - List contents of a MATLAB style mat file (version 4 through 7.1)
+
+For low-level MATLAB reading and writing utilities, see `scipy.io.matlab`.
+
+IDL® files
+==========
+
+.. autosummary::
+   :toctree: generated/
+
+   readsav - Read an IDL 'save' file
+
+Matrix Market files
+===================
+
+.. autosummary::
+   :toctree: generated/
+
+   mminfo - Query matrix info from Matrix Market formatted file
+   mmread - Read matrix from Matrix Market formatted file
+   mmwrite - Write matrix to Matrix Market formatted file
+
+Unformatted Fortran files
+===============================
+
+.. autosummary::
+   :toctree: generated/
+
+   FortranFile - A file object for unformatted sequential Fortran files
+   FortranEOFError - Exception indicating the end of a well-formed file
+   FortranFormattingError - Exception indicating an inappropriate end
+
+Netcdf
+======
+
+.. autosummary::
+   :toctree: generated/
+
+   netcdf_file - A file object for NetCDF data
+   netcdf_variable - A data object for the netcdf module
+
+Harwell-Boeing files
+====================
+
+.. autosummary::
+   :toctree: generated/
+
+   hb_read   -- read H-B file
+   hb_write  -- write H-B file
+
+Wav sound files (:mod:`scipy.io.wavfile`)
+=========================================
+
+.. module:: scipy.io.wavfile
+
+.. autosummary::
+   :toctree: generated/
+
+   read
+   write
+   WavFileWarning
+
+Arff files (:mod:`scipy.io.arff`)
+=================================
+
+.. module:: scipy.io.arff
+
+.. autosummary::
+   :toctree: generated/
+
+   loadarff
+   MetaData
+   ArffError
+   ParseArffError
+"""
+# matfile read and write
+from .matlab import loadmat, savemat, whosmat
+
+# netCDF file support
+from ._netcdf import netcdf_file, netcdf_variable
+
+# Fortran file support
+from ._fortran import FortranFile, FortranEOFError, FortranFormattingError
+
+from ._fast_matrix_market import mminfo, mmread, mmwrite
+from ._idl import readsav
+from ._harwell_boeing import hb_read, hb_write
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import arff, harwell_boeing, idl, mmio, netcdf, wavfile
+
+__all__ = [s for s in dir() if not s.startswith('_')]
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/_fortran.py

@@ -0,0 +1,354 @@
+"""
+Module to read / write Fortran unformatted sequential files.
+
+This is in the spirit of code written by Neil Martinsen-Burrell and Joe Zuntz.
+
+"""
+import warnings
+import numpy as np
+
+__all__ = ['FortranFile', 'FortranEOFError', 'FortranFormattingError']
+
+
+class FortranEOFError(TypeError, OSError):
+    """Indicates that the file ended properly.
+
+    This error descends from TypeError because the code used to raise
+    TypeError (and this was the only way to know that the file had
+    ended) so users might have ``except TypeError:``.
+
+    """
+    pass
+
+
+class FortranFormattingError(TypeError, OSError):
+    """Indicates that the file ended mid-record.
+
+    Descends from TypeError for backward compatibility.
+
+    """
+    pass
+
+
+class FortranFile:
+    """
+    A file object for unformatted sequential files from Fortran code.
+
+    Parameters
+    ----------
+    filename : file or str
+        Open file object or filename.
+    mode : {'r', 'w'}, optional
+        Read-write mode, default is 'r'.
+    header_dtype : dtype, optional
+        Data type of the header. Size and endianness must match the input/output file.
+
+    Notes
+    -----
+    These files are broken up into records of unspecified types. The size of
+    each record is given at the start (although the size of this header is not
+    standard) and the data is written onto disk without any formatting. Fortran
+    compilers supporting the BACKSPACE statement will write a second copy of
+    the size to facilitate backwards seeking.
+
+    This class only supports files written with both sizes for the record.
+    It also does not support the subrecords used in Intel and gfortran compilers
+    for records which are greater than 2GB with a 4-byte header.
+
+    An example of an unformatted sequential file in Fortran would be written as::
+
+        OPEN(1, FILE=myfilename, FORM='unformatted')
+
+        WRITE(1) myvariable
+
+    Since this is a non-standard file format, whose contents depend on the
+    compiler and the endianness of the machine, caution is advised. Files from
+    gfortran 4.8.0 and gfortran 4.1.2 on x86_64 are known to work.
+
+    Consider using Fortran direct-access files or files from the newer Stream
+    I/O, which can be easily read by `numpy.fromfile`.
+
+    Examples
+    --------
+    To create an unformatted sequential Fortran file:
+
+    >>> from scipy.io import FortranFile
+    >>> import numpy as np
+    >>> f = FortranFile('test.unf', 'w')
+    >>> f.write_record(np.array([1,2,3,4,5], dtype=np.int32))
+    >>> f.write_record(np.linspace(0,1,20).reshape((5,4)).T)
+    >>> f.close()
+
+    To read this file:
+
+    >>> f = FortranFile('test.unf', 'r')
+    >>> print(f.read_ints(np.int32))
+    [1 2 3 4 5]
+    >>> print(f.read_reals(float).reshape((5,4), order="F"))
+    [[0.         0.05263158 0.10526316 0.15789474]
+     [0.21052632 0.26315789 0.31578947 0.36842105]
+     [0.42105263 0.47368421 0.52631579 0.57894737]
+     [0.63157895 0.68421053 0.73684211 0.78947368]
+     [0.84210526 0.89473684 0.94736842 1.        ]]
+    >>> f.close()
+
+    Or, in Fortran::
+
+        integer :: a(5), i
+        double precision :: b(5,4)
+        open(1, file='test.unf', form='unformatted')
+        read(1) a
+        read(1) b
+        close(1)
+        write(*,*) a
+        do i = 1, 5
+            write(*,*) b(i,:)
+        end do
+
+    """
+    def __init__(self, filename, mode='r', header_dtype=np.uint32):
+        if header_dtype is None:
+            raise ValueError('Must specify dtype')
+
+        header_dtype = np.dtype(header_dtype)
+        if header_dtype.kind != 'u':
+            warnings.warn("Given a dtype which is not unsigned.", stacklevel=2)
+
+        if mode not in 'rw' or len(mode) != 1:
+            raise ValueError('mode must be either r or w')
+
+        if hasattr(filename, 'seek'):
+            self._fp = filename
+        else:
+            self._fp = open(filename, f'{mode}b')
+
+        self._header_dtype = header_dtype
+
+    def _read_size(self, eof_ok=False):
+        n = self._header_dtype.itemsize
+        b = self._fp.read(n)
+        if (not b) and eof_ok:
+            raise FortranEOFError("End of file occurred at end of record")
+        elif len(b) < n:
+            raise FortranFormattingError(
+                "End of file in the middle of the record size")
+        return int(np.frombuffer(b, dtype=self._header_dtype, count=1)[0])
+
+    def write_record(self, *items):
+        """
+        Write a record (including sizes) to the file.
+
+        Parameters
+        ----------
+        *items : array_like
+            The data arrays to write.
+
+        Notes
+        -----
+        Writes data items to a file::
+
+            write_record(a.T, b.T, c.T, ...)
+
+            write(1) a, b, c, ...
+
+        Note that data in multidimensional arrays is written in
+        row-major order --- to make them read correctly by Fortran
+        programs, you need to transpose the arrays yourself when
+        writing them.
+
+        """
+        items = tuple(np.asarray(item) for item in items)
+        total_size = sum(item.nbytes for item in items)
+
+        nb = np.array([total_size], dtype=self._header_dtype)
+
+        nb.tofile(self._fp)
+        for item in items:
+            item.tofile(self._fp)
+        nb.tofile(self._fp)
+
+    def read_record(self, *dtypes, **kwargs):
+        """
+        Reads a record of a given type from the file.
+
+        Parameters
+        ----------
+        *dtypes : dtypes, optional
+            Data type(s) specifying the size and endianness of the data.
+
+        Returns
+        -------
+        data : ndarray
+            A 1-D array object.
+
+        Raises
+        ------
+        FortranEOFError
+            To signal that no further records are available
+        FortranFormattingError
+            To signal that the end of the file was encountered
+            part-way through a record
+
+        Notes
+        -----
+        If the record contains a multidimensional array, you can specify
+        the size in the dtype. For example::
+
+            INTEGER var(5,4)
+
+        can be read with::
+
+            read_record('(4,5)i4').T
+
+        Note that this function does **not** assume the file data is in Fortran
+        column major order, so you need to (i) swap the order of dimensions
+        when reading and (ii) transpose the resulting array.
+
+        Alternatively, you can read the data as a 1-D array and handle the
+        ordering yourself. For example::
+
+            read_record('i4').reshape(5, 4, order='F')
+
+        For records that contain several variables or mixed types (as opposed
+        to single scalar or array types), give them as separate arguments::
+
+            double precision :: a
+            integer :: b
+            write(1) a, b
+
+            record = f.read_record('<f4', '<i4')
+            a = record[0]  # first number
+            b = record[1]  # second number
+
+        and if any of the variables are arrays, the shape can be specified as
+        the third item in the relevant dtype::
+
+            double precision :: a
+            integer :: b(3,4)
+            write(1) a, b
+
+            record = f.read_record('<f4', np.dtype(('<i4', (4, 3))))
+            a = record[0]
+            b = record[1].T
+
+        NumPy also supports a short syntax for this kind of type::
+
+            record = f.read_record('<f4', '(3,3)<i4')
+
+        See Also
+        --------
+        read_reals
+        read_ints
+
+        """
+        dtype = kwargs.pop('dtype', None)
+        if kwargs:
+            raise ValueError(f"Unknown keyword arguments {tuple(kwargs.keys())}")
+
+        if dtype is not None:
+            dtypes = dtypes + (dtype,)
+        elif not dtypes:
+            raise ValueError('Must specify at least one dtype')
+
+        first_size = self._read_size(eof_ok=True)
+
+        dtypes = tuple(np.dtype(dtype) for dtype in dtypes)
+        block_size = sum(dtype.itemsize for dtype in dtypes)
+
+        num_blocks, remainder = divmod(first_size, block_size)
+        if remainder != 0:
+            raise ValueError(f'Size obtained ({first_size}) is not a multiple of the '
+                             f'dtypes given ({block_size}).')
+
+        if len(dtypes) != 1 and first_size != block_size:
+            # Fortran does not write mixed type array items in interleaved order,
+            # and it's not possible to guess the sizes of the arrays that were written.
+            # The user must specify the exact sizes of each of the arrays.
+            raise ValueError(f'Size obtained ({first_size}) does not match with the '
+                             f'expected size ({block_size}) of multi-item record')
+
+        data = []
+        for dtype in dtypes:
+            r = np.fromfile(self._fp, dtype=dtype, count=num_blocks)
+            if len(r) != num_blocks:
+                raise FortranFormattingError(
+                    "End of file in the middle of a record")
+            if dtype.shape != ():
+                # Squeeze outmost block dimension for array items
+                if num_blocks == 1:
+                    assert r.shape == (1,) + dtype.shape
+                    r = r[0]
+
+            data.append(r)
+
+        second_size = self._read_size()
+        if first_size != second_size:
+            raise ValueError('Sizes do not agree in the header and footer for '
+                             'this record - check header dtype')
+
+        # Unpack result
+        if len(dtypes) == 1:
+            return data[0]
+        else:
+            return tuple(data)
+
+    def read_ints(self, dtype='i4'):
+        """
+        Reads a record of a given type from the file, defaulting to an integer
+        type (``INTEGER*4`` in Fortran).
+
+        Parameters
+        ----------
+        dtype : dtype, optional
+            Data type specifying the size and endianness of the data.
+
+        Returns
+        -------
+        data : ndarray
+            A 1-D array object.
+
+        See Also
+        --------
+        read_reals
+        read_record
+
+        """
+        return self.read_record(dtype)
+
+    def read_reals(self, dtype='f8'):
+        """
+        Reads a record of a given type from the file, defaulting to a floating
+        point number (``real*8`` in Fortran).
+
+        Parameters
+        ----------
+        dtype : dtype, optional
+            Data type specifying the size and endianness of the data.
+
+        Returns
+        -------
+        data : ndarray
+            A 1-D array object.
+
+        See Also
+        --------
+        read_ints
+        read_record
+
+        """
+        return self.read_record(dtype)
+
+    def close(self):
+        """
+        Closes the file. It is unsupported to call any other methods off this
+        object after closing it. Note that this class supports the 'with'
+        statement in modern versions of Python, to call this automatically
+
+        """
+        self._fp.close()
+
+    def __enter__(self):
+        return self
+
+    def __exit__(self, type, value, tb):
+        self.close()

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/_idl.py

@@ -0,0 +1,917 @@
+# IDLSave - a python module to read IDL 'save' files
+# Copyright (c) 2010 Thomas P. Robitaille
+
+# Many thanks to Craig Markwardt for publishing the Unofficial Format
+# Specification for IDL .sav files, without which this Python module would not
+# exist (http://cow.physics.wisc.edu/~craigm/idl/savefmt).
+
+# This code was developed by with permission from ITT Visual Information
+# Systems. IDL(r) is a registered trademark of ITT Visual Information Systems,
+# Inc. for their Interactive Data Language software.
+
+# Permission is hereby granted, free of charge, to any person obtaining a
+# copy of this software and associated documentation files (the "Software"),
+# to deal in the Software without restriction, including without limitation
+# the rights to use, copy, modify, merge, publish, distribute, sublicense,
+# and/or sell copies of the Software, and to permit persons to whom the
+# Software is furnished to do so, subject to the following conditions:
+
+# The above copyright notice and this permission notice shall be included in
+# all copies or substantial portions of the Software.
+
+# THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR
+# IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY,
+# FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE
+# AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
+# LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING
+# FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER
+# DEALINGS IN THE SOFTWARE.
+
+__all__ = ['readsav']
+
+import struct
+import numpy as np
+import tempfile
+import zlib
+import warnings
+
+# Define the different data types that can be found in an IDL save file
+DTYPE_DICT = {1: '>u1',
+              2: '>i2',
+              3: '>i4',
+              4: '>f4',
+              5: '>f8',
+              6: '>c8',
+              7: '|O',
+              8: '|O',
+              9: '>c16',
+              10: '|O',
+              11: '|O',
+              12: '>u2',
+              13: '>u4',
+              14: '>i8',
+              15: '>u8'}
+
+# Define the different record types that can be found in an IDL save file
+RECTYPE_DICT = {0: "START_MARKER",
+                1: "COMMON_VARIABLE",
+                2: "VARIABLE",
+                3: "SYSTEM_VARIABLE",
+                6: "END_MARKER",
+                10: "TIMESTAMP",
+                12: "COMPILED",
+                13: "IDENTIFICATION",
+                14: "VERSION",
+                15: "HEAP_HEADER",
+                16: "HEAP_DATA",
+                17: "PROMOTE64",
+                19: "NOTICE",
+                20: "DESCRIPTION"}
+
+# Define a dictionary to contain structure definitions
+STRUCT_DICT = {}
+
+
+def _align_32(f):
+    '''Align to the next 32-bit position in a file'''
+
+    pos = f.tell()
+    if pos % 4 != 0:
+        f.seek(pos + 4 - pos % 4)
+    return
+
+
+def _skip_bytes(f, n):
+    '''Skip `n` bytes'''
+    f.read(n)
+    return
+
+
+def _read_bytes(f, n):
+    '''Read the next `n` bytes'''
+    return f.read(n)
+
+
+def _read_byte(f):
+    '''Read a single byte'''
+    return np.uint8(struct.unpack('>B', f.read(4)[:1])[0])
+
+
+def _read_long(f):
+    '''Read a signed 32-bit integer'''
+    return np.int32(struct.unpack('>l', f.read(4))[0])
+
+
+def _read_int16(f):
+    '''Read a signed 16-bit integer'''
+    return np.int16(struct.unpack('>h', f.read(4)[2:4])[0])
+
+
+def _read_int32(f):
+    '''Read a signed 32-bit integer'''
+    return np.int32(struct.unpack('>i', f.read(4))[0])
+
+
+def _read_int64(f):
+    '''Read a signed 64-bit integer'''
+    return np.int64(struct.unpack('>q', f.read(8))[0])
+
+
+def _read_uint16(f):
+    '''Read an unsigned 16-bit integer'''
+    return np.uint16(struct.unpack('>H', f.read(4)[2:4])[0])
+
+
+def _read_uint32(f):
+    '''Read an unsigned 32-bit integer'''
+    return np.uint32(struct.unpack('>I', f.read(4))[0])
+
+
+def _read_uint64(f):
+    '''Read an unsigned 64-bit integer'''
+    return np.uint64(struct.unpack('>Q', f.read(8))[0])
+
+
+def _read_float32(f):
+    '''Read a 32-bit float'''
+    return np.float32(struct.unpack('>f', f.read(4))[0])
+
+
+def _read_float64(f):
+    '''Read a 64-bit float'''
+    return np.float64(struct.unpack('>d', f.read(8))[0])
+
+
+class Pointer:
+    '''Class used to define pointers'''
+
+    def __init__(self, index):
+        self.index = index
+        return
+
+
+class ObjectPointer(Pointer):
+    '''Class used to define object pointers'''
+    pass
+
+
+def _read_string(f):
+    '''Read a string'''
+    length = _read_long(f)
+    if length > 0:
+        chars = _read_bytes(f, length).decode('latin1')
+        _align_32(f)
+    else:
+        chars = ''
+    return chars
+
+
+def _read_string_data(f):
+    '''Read a data string (length is specified twice)'''
+    length = _read_long(f)
+    if length > 0:
+        length = _read_long(f)
+        string_data = _read_bytes(f, length)
+        _align_32(f)
+    else:
+        string_data = ''
+    return string_data
+
+
+def _read_data(f, dtype):
+    '''Read a variable with a specified data type'''
+    if dtype == 1:
+        if _read_int32(f) != 1:
+            raise Exception("Error occurred while reading byte variable")
+        return _read_byte(f)
+    elif dtype == 2:
+        return _read_int16(f)
+    elif dtype == 3:
+        return _read_int32(f)
+    elif dtype == 4:
+        return _read_float32(f)
+    elif dtype == 5:
+        return _read_float64(f)
+    elif dtype == 6:
+        real = _read_float32(f)
+        imag = _read_float32(f)
+        return np.complex64(real + imag * 1j)
+    elif dtype == 7:
+        return _read_string_data(f)
+    elif dtype == 8:
+        raise Exception("Should not be here - please report this")
+    elif dtype == 9:
+        real = _read_float64(f)
+        imag = _read_float64(f)
+        return np.complex128(real + imag * 1j)
+    elif dtype == 10:
+        return Pointer(_read_int32(f))
+    elif dtype == 11:
+        return ObjectPointer(_read_int32(f))
+    elif dtype == 12:
+        return _read_uint16(f)
+    elif dtype == 13:
+        return _read_uint32(f)
+    elif dtype == 14:
+        return _read_int64(f)
+    elif dtype == 15:
+        return _read_uint64(f)
+    else:
+        raise Exception(f"Unknown IDL type: {dtype} - please report this")
+
+
+def _read_structure(f, array_desc, struct_desc):
+    '''
+    Read a structure, with the array and structure descriptors given as
+    `array_desc` and `structure_desc` respectively.
+    '''
+
+    nrows = array_desc['nelements']
+    columns = struct_desc['tagtable']
+
+    dtype = []
+    for col in columns:
+        if col['structure'] or col['array']:
+            dtype.append(((col['name'].lower(), col['name']), np.object_))
+        else:
+            if col['typecode'] in DTYPE_DICT:
+                dtype.append(((col['name'].lower(), col['name']),
+                                    DTYPE_DICT[col['typecode']]))
+            else:
+                raise Exception(f"Variable type {col['typecode']} not implemented")
+
+    structure = np.rec.recarray((nrows, ), dtype=dtype)
+
+    for i in range(nrows):
+        for col in columns:
+            dtype = col['typecode']
+            if col['structure']:
+                structure[col['name']][i] = _read_structure(f,
+                                      struct_desc['arrtable'][col['name']],
+                                      struct_desc['structtable'][col['name']])
+            elif col['array']:
+                structure[col['name']][i] = _read_array(f, dtype,
+                                      struct_desc['arrtable'][col['name']])
+            else:
+                structure[col['name']][i] = _read_data(f, dtype)
+
+    # Reshape structure if needed
+    if array_desc['ndims'] > 1:
+        dims = array_desc['dims'][:int(array_desc['ndims'])]
+        dims.reverse()
+        structure = structure.reshape(dims)
+
+    return structure
+
+
+def _read_array(f, typecode, array_desc):
+    '''
+    Read an array of type `typecode`, with the array descriptor given as
+    `array_desc`.
+    '''
+
+    if typecode in [1, 3, 4, 5, 6, 9, 13, 14, 15]:
+
+        if typecode == 1:
+            nbytes = _read_int32(f)
+            if nbytes != array_desc['nbytes']:
+                warnings.warn("Not able to verify number of bytes from header",
+                              stacklevel=3)
+
+        # Read bytes as numpy array
+        array = np.frombuffer(f.read(array_desc['nbytes']),
+                              dtype=DTYPE_DICT[typecode])
+
+    elif typecode in [2, 12]:
+
+        # These are 2 byte types, need to skip every two as they are not packed
+
+        array = np.frombuffer(f.read(array_desc['nbytes']*2),
+                              dtype=DTYPE_DICT[typecode])[1::2]
+
+    else:
+
+        # Read bytes into list
+        array = []
+        for i in range(array_desc['nelements']):
+            dtype = typecode
+            data = _read_data(f, dtype)
+            array.append(data)
+
+        array = np.array(array, dtype=np.object_)
+
+    # Reshape array if needed
+    if array_desc['ndims'] > 1:
+        dims = array_desc['dims'][:int(array_desc['ndims'])]
+        dims.reverse()
+        array = array.reshape(dims)
+
+    # Go to next alignment position
+    _align_32(f)
+
+    return array
+
+
+def _read_record(f):
+    '''Function to read in a full record'''
+
+    record = {'rectype': _read_long(f)}
+
+    nextrec = _read_uint32(f)
+    nextrec += _read_uint32(f).astype(np.int64) * 2**32
+
+    _skip_bytes(f, 4)
+
+    if record['rectype'] not in RECTYPE_DICT:
+        raise Exception(f"Unknown RECTYPE: {record['rectype']}")
+
+    record['rectype'] = RECTYPE_DICT[record['rectype']]
+
+    if record['rectype'] in ["VARIABLE", "HEAP_DATA"]:
+
+        if record['rectype'] == "VARIABLE":
+            record['varname'] = _read_string(f)
+        else:
+            record['heap_index'] = _read_long(f)
+            _skip_bytes(f, 4)
+
+        rectypedesc = _read_typedesc(f)
+
+        if rectypedesc['typecode'] == 0:
+
+            if nextrec == f.tell():
+                record['data'] = None  # Indicates NULL value
+            else:
+                raise ValueError("Unexpected type code: 0")
+
+        else:
+
+            varstart = _read_long(f)
+            if varstart != 7:
+                raise Exception("VARSTART is not 7")
+
+            if rectypedesc['structure']:
+                record['data'] = _read_structure(f, rectypedesc['array_desc'],
+                                                    rectypedesc['struct_desc'])
+            elif rectypedesc['array']:
+                record['data'] = _read_array(f, rectypedesc['typecode'],
+                                                rectypedesc['array_desc'])
+            else:
+                dtype = rectypedesc['typecode']
+                record['data'] = _read_data(f, dtype)
+
+    elif record['rectype'] == "TIMESTAMP":
+
+        _skip_bytes(f, 4*256)
+        record['date'] = _read_string(f)
+        record['user'] = _read_string(f)
+        record['host'] = _read_string(f)
+
+    elif record['rectype'] == "VERSION":
+
+        record['format'] = _read_long(f)
+        record['arch'] = _read_string(f)
+        record['os'] = _read_string(f)
+        record['release'] = _read_string(f)
+
+    elif record['rectype'] == "IDENTIFICATON":
+
+        record['author'] = _read_string(f)
+        record['title'] = _read_string(f)
+        record['idcode'] = _read_string(f)
+
+    elif record['rectype'] == "NOTICE":
+
+        record['notice'] = _read_string(f)
+
+    elif record['rectype'] == "DESCRIPTION":
+
+        record['description'] = _read_string_data(f)
+
+    elif record['rectype'] == "HEAP_HEADER":
+
+        record['nvalues'] = _read_long(f)
+        record['indices'] = [_read_long(f) for _ in range(record['nvalues'])]
+
+    elif record['rectype'] == "COMMONBLOCK":
+
+        record['nvars'] = _read_long(f)
+        record['name'] = _read_string(f)
+        record['varnames'] = [_read_string(f) for _ in range(record['nvars'])]
+
+    elif record['rectype'] == "END_MARKER":
+
+        record['end'] = True
+
+    elif record['rectype'] == "UNKNOWN":
+
+        warnings.warn("Skipping UNKNOWN record", stacklevel=3)
+
+    elif record['rectype'] == "SYSTEM_VARIABLE":
+
+        warnings.warn("Skipping SYSTEM_VARIABLE record", stacklevel=3)
+
+    else:
+
+        raise Exception(f"record['rectype']={record['rectype']} not implemented")
+
+    f.seek(nextrec)
+
+    return record
+
+
+def _read_typedesc(f):
+    '''Function to read in a type descriptor'''
+
+    typedesc = {'typecode': _read_long(f), 'varflags': _read_long(f)}
+
+    if typedesc['varflags'] & 2 == 2:
+        raise Exception("System variables not implemented")
+
+    typedesc['array'] = typedesc['varflags'] & 4 == 4
+    typedesc['structure'] = typedesc['varflags'] & 32 == 32
+
+    if typedesc['structure']:
+        typedesc['array_desc'] = _read_arraydesc(f)
+        typedesc['struct_desc'] = _read_structdesc(f)
+    elif typedesc['array']:
+        typedesc['array_desc'] = _read_arraydesc(f)
+
+    return typedesc
+
+
+def _read_arraydesc(f):
+    '''Function to read in an array descriptor'''
+
+    arraydesc = {'arrstart': _read_long(f)}
+
+    if arraydesc['arrstart'] == 8:
+
+        _skip_bytes(f, 4)
+
+        arraydesc['nbytes'] = _read_long(f)
+        arraydesc['nelements'] = _read_long(f)
+        arraydesc['ndims'] = _read_long(f)
+
+        _skip_bytes(f, 8)
+
+        arraydesc['nmax'] = _read_long(f)
+
+        arraydesc['dims'] = [_read_long(f) for _ in range(arraydesc['nmax'])]
+
+    elif arraydesc['arrstart'] == 18:
+
+        warnings.warn("Using experimental 64-bit array read", stacklevel=3)
+
+        _skip_bytes(f, 8)
+
+        arraydesc['nbytes'] = _read_uint64(f)
+        arraydesc['nelements'] = _read_uint64(f)
+        arraydesc['ndims'] = _read_long(f)
+
+        _skip_bytes(f, 8)
+
+        arraydesc['nmax'] = 8
+
+        arraydesc['dims'] = []
+        for d in range(arraydesc['nmax']):
+            v = _read_long(f)
+            if v != 0:
+                raise Exception("Expected a zero in ARRAY_DESC")
+            arraydesc['dims'].append(_read_long(f))
+
+    else:
+        raise Exception(f"Unknown ARRSTART: {arraydesc['arrstart']}")
+
+    return arraydesc
+
+
+def _read_structdesc(f):
+    '''Function to read in a structure descriptor'''
+
+    structdesc = {}
+
+    structstart = _read_long(f)
+    if structstart != 9:
+        raise Exception("STRUCTSTART should be 9")
+
+    structdesc['name'] = _read_string(f)
+    predef = _read_long(f)
+    structdesc['ntags'] = _read_long(f)
+    structdesc['nbytes'] = _read_long(f)
+
+    structdesc['predef'] = predef & 1
+    structdesc['inherits'] = predef & 2
+    structdesc['is_super'] = predef & 4
+
+    if not structdesc['predef']:
+
+        structdesc['tagtable'] = [_read_tagdesc(f)
+                                  for _ in range(structdesc['ntags'])]
+
+        for tag in structdesc['tagtable']:
+            tag['name'] = _read_string(f)
+
+        structdesc['arrtable'] = {tag['name']: _read_arraydesc(f)
+                                  for tag in structdesc['tagtable']
+                                  if tag['array']}
+
+        structdesc['structtable'] = {tag['name']: _read_structdesc(f)
+                                     for tag in structdesc['tagtable']
+                                     if tag['structure']}
+
+        if structdesc['inherits'] or structdesc['is_super']:
+            structdesc['classname'] = _read_string(f)
+            structdesc['nsupclasses'] = _read_long(f)
+            structdesc['supclassnames'] = [
+                _read_string(f) for _ in range(structdesc['nsupclasses'])]
+            structdesc['supclasstable'] = [
+                _read_structdesc(f) for _ in range(structdesc['nsupclasses'])]
+
+        STRUCT_DICT[structdesc['name']] = structdesc
+
+    else:
+
+        if structdesc['name'] not in STRUCT_DICT:
+            raise Exception("PREDEF=1 but can't find definition")
+
+        structdesc = STRUCT_DICT[structdesc['name']]
+
+    return structdesc
+
+
+def _read_tagdesc(f):
+    '''Function to read in a tag descriptor'''
+
+    tagdesc = {'offset': _read_long(f)}
+
+    if tagdesc['offset'] == -1:
+        tagdesc['offset'] = _read_uint64(f)
+
+    tagdesc['typecode'] = _read_long(f)
+    tagflags = _read_long(f)
+
+    tagdesc['array'] = tagflags & 4 == 4
+    tagdesc['structure'] = tagflags & 32 == 32
+    tagdesc['scalar'] = tagdesc['typecode'] in DTYPE_DICT
+    # Assume '10'x is scalar
+
+    return tagdesc
+
+
+def _replace_heap(variable, heap):
+
+    if isinstance(variable, Pointer):
+
+        while isinstance(variable, Pointer):
+
+            if variable.index == 0:
+                variable = None
+            else:
+                if variable.index in heap:
+                    variable = heap[variable.index]
+                else:
+                    warnings.warn("Variable referenced by pointer not found "
+                                  "in heap: variable will be set to None",
+                                  stacklevel=3)
+                    variable = None
+
+        replace, new = _replace_heap(variable, heap)
+
+        if replace:
+            variable = new
+
+        return True, variable
+
+    elif isinstance(variable, np.rec.recarray):
+
+        # Loop over records
+        for ir, record in enumerate(variable):
+
+            replace, new = _replace_heap(record, heap)
+
+            if replace:
+                variable[ir] = new
+
+        return False, variable
+
+    elif isinstance(variable, np.record):
+
+        # Loop over values
+        for iv, value in enumerate(variable):
+
+            replace, new = _replace_heap(value, heap)
+
+            if replace:
+                variable[iv] = new
+
+        return False, variable
+
+    elif isinstance(variable, np.ndarray):
+
+        # Loop over values if type is np.object_
+        if variable.dtype.type is np.object_:
+
+            for iv in range(variable.size):
+
+                replace, new = _replace_heap(variable.item(iv), heap)
+
+                if replace:
+                    variable.reshape(-1)[iv] = new
+
+        return False, variable
+
+    else:
+
+        return False, variable
+
+
+class AttrDict(dict):
+    '''
+    A case-insensitive dictionary with access via item, attribute, and call
+    notations:
+
+        >>> from scipy.io._idl import AttrDict
+        >>> d = AttrDict()
+        >>> d['Variable'] = 123
+        >>> d['Variable']
+        123
+        >>> d.Variable
+        123
+        >>> d.variable
+        123
+        >>> d('VARIABLE')
+        123
+        >>> d['missing']
+        Traceback (most recent error last):
+        ...
+        KeyError: 'missing'
+        >>> d.missing
+        Traceback (most recent error last):
+        ...
+        AttributeError: 'AttrDict' object has no attribute 'missing'
+    '''
+
+    def __init__(self, init=None):
+        if init is None:
+            init = {}
+        dict.__init__(self, init)
+
+    def __getitem__(self, name):
+        return super().__getitem__(name.lower())
+
+    def __setitem__(self, key, value):
+        return super().__setitem__(key.lower(), value)
+
+    def __getattr__(self, name):
+        try:
+            return self.__getitem__(name)
+        except KeyError:
+            raise AttributeError(
+                f"'{type(self)}' object has no attribute '{name}'") from None
+
+    __setattr__ = __setitem__
+    __call__ = __getitem__
+
+
+def readsav(file_name, idict=None, python_dict=False,
+            uncompressed_file_name=None, verbose=False):
+    """
+    Read an IDL .sav file.
+
+    Parameters
+    ----------
+    file_name : str
+        Name of the IDL save file.
+    idict : dict, optional
+        Dictionary in which to insert .sav file variables.
+    python_dict : bool, optional
+        By default, the object return is not a Python dictionary, but a
+        case-insensitive dictionary with item, attribute, and call access
+        to variables. To get a standard Python dictionary, set this option
+        to True.
+    uncompressed_file_name : str, optional
+        This option only has an effect for .sav files written with the
+        /compress option. If a file name is specified, compressed .sav
+        files are uncompressed to this file. Otherwise, readsav will use
+        the `tempfile` module to determine a temporary filename
+        automatically, and will remove the temporary file upon successfully
+        reading it in.
+    verbose : bool, optional
+        Whether to print out information about the save file, including
+        the records read, and available variables.
+
+    Returns
+    -------
+    idl_dict : AttrDict or dict
+        If `python_dict` is set to False (default), this function returns a
+        case-insensitive dictionary with item, attribute, and call access
+        to variables. If `python_dict` is set to True, this function
+        returns a Python dictionary with all variable names in lowercase.
+        If `idict` was specified, then variables are written to the
+        dictionary specified, and the updated dictionary is returned.
+
+    Examples
+    --------
+    >>> from os.path import dirname, join as pjoin
+    >>> import scipy.io as sio
+    >>> from scipy.io import readsav
+
+    Get the filename for an example .sav file from the tests/data directory.
+
+    >>> data_dir = pjoin(dirname(sio.__file__), 'tests', 'data')
+    >>> sav_fname = pjoin(data_dir, 'array_float32_1d.sav')
+
+    Load the .sav file contents.
+
+    >>> sav_data = readsav(sav_fname)
+
+    Get keys of the .sav file contents.
+
+    >>> print(sav_data.keys())
+    dict_keys(['array1d'])
+
+    Access a content with a key.
+
+    >>> print(sav_data['array1d'])
+    [0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0.
+     0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0.
+     0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0.
+     0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0.
+     0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0. 0.
+     0. 0. 0.]
+
+    """
+
+    # Initialize record and variable holders
+    records = []
+    if python_dict or idict:
+        variables = {}
+    else:
+        variables = AttrDict()
+
+    # Open the IDL file
+    f = open(file_name, 'rb')
+
+    # Read the signature, which should be 'SR'
+    signature = _read_bytes(f, 2)
+    if signature != b'SR':
+        raise Exception(f"Invalid SIGNATURE: {signature}")
+
+    # Next, the record format, which is '\x00\x04' for normal .sav
+    # files, and '\x00\x06' for compressed .sav files.
+    recfmt = _read_bytes(f, 2)
+
+    if recfmt == b'\x00\x04':
+        pass
+
+    elif recfmt == b'\x00\x06':
+
+        if verbose:
+            print("IDL Save file is compressed")
+
+        if uncompressed_file_name:
+            fout = open(uncompressed_file_name, 'w+b')
+        else:
+            fout = tempfile.NamedTemporaryFile(suffix='.sav')
+
+        if verbose:
+            print(f" -> expanding to {fout.name}")
+
+        # Write header
+        fout.write(b'SR\x00\x04')
+
+        # Cycle through records
+        while True:
+
+            # Read record type
+            rectype = _read_long(f)
+            fout.write(struct.pack('>l', int(rectype)))
+
+            # Read position of next record and return as int
+            nextrec = _read_uint32(f)
+            nextrec += _read_uint32(f).astype(np.int64) * 2**32
+
+            # Read the unknown 4 bytes
+            unknown = f.read(4)
+
+            # Check if the end of the file has been reached
+            if RECTYPE_DICT[rectype] == 'END_MARKER':
+                modval = np.int64(2**32)
+                fout.write(struct.pack('>I', int(nextrec) % modval))
+                fout.write(
+                    struct.pack('>I', int((nextrec - (nextrec % modval)) / modval))
+                )
+                fout.write(unknown)
+                break
+
+            # Find current position
+            pos = f.tell()
+
+            # Decompress record
+            rec_string = zlib.decompress(f.read(nextrec-pos))
+
+            # Find new position of next record
+            nextrec = fout.tell() + len(rec_string) + 12
+
+            # Write out record
+            fout.write(struct.pack('>I', int(nextrec % 2**32)))
+            fout.write(struct.pack('>I', int((nextrec - (nextrec % 2**32)) / 2**32)))
+            fout.write(unknown)
+            fout.write(rec_string)
+
+        # Close the original compressed file
+        f.close()
+
+        # Set f to be the decompressed file, and skip the first four bytes
+        f = fout
+        f.seek(4)
+
+    else:
+        raise Exception(f"Invalid RECFMT: {recfmt}")
+
+    # Loop through records, and add them to the list
+    while True:
+        r = _read_record(f)
+        records.append(r)
+        if 'end' in r:
+            if r['end']:
+                break
+
+    # Close the file
+    f.close()
+
+    # Find heap data variables
+    heap = {}
+    for r in records:
+        if r['rectype'] == "HEAP_DATA":
+            heap[r['heap_index']] = r['data']
+
+    # Find all variables
+    for r in records:
+        if r['rectype'] == "VARIABLE":
+            replace, new = _replace_heap(r['data'], heap)
+            if replace:
+                r['data'] = new
+            variables[r['varname'].lower()] = r['data']
+
+    if verbose:
+
+        # Print out timestamp info about the file
+        for record in records:
+            if record['rectype'] == "TIMESTAMP":
+                print("-"*50)
+                print(f"Date: {record['date']}")
+                print(f"User: {record['user']}")
+                print(f"Host: {record['host']}")
+                break
+
+        # Print out version info about the file
+        for record in records:
+            if record['rectype'] == "VERSION":
+                print("-"*50)
+                print(f"Format: {record['format']}")
+                print(f"Architecture: {record['arch']}")
+                print(f"Operating System: {record['os']}")
+                print(f"IDL Version: {record['release']}")
+                break
+
+        # Print out identification info about the file
+        for record in records:
+            if record['rectype'] == "IDENTIFICATON":
+                print("-"*50)
+                print(f"Author: {record['author']}")
+                print(f"Title: {record['title']}")
+                print(f"ID Code: {record['idcode']}")
+                break
+
+        # Print out descriptions saved with the file
+        for record in records:
+            if record['rectype'] == "DESCRIPTION":
+                print("-"*50)
+                print(f"Description: {record['description']}")
+                break
+
+        print("-"*50)
+        print(f"Successfully read {len(records)} records of which:")
+
+        # Create convenience list of record types
+        rectypes = [r['rectype'] for r in records]
+
+        for rt in set(rectypes):
+            if rt != 'END_MARKER':
+                print(f" - {rectypes.count(rt)} are of type {rt}")
+        print("-"*50)
+
+        if 'VARIABLE' in rectypes:
+            print("Available variables:")
+            for var in variables:
+                print(f" - {var} [{type(variables[var])}]")
+            print("-"*50)
+
+    if idict:
+        for var in variables:
+            idict[var] = variables[var]
+        return idict
+    else:
+        return variables

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/_mmio.py

@@ -0,0 +1,968 @@
+"""
+  Matrix Market I/O in Python.
+  See http://math.nist.gov/MatrixMarket/formats.html
+  for information about the Matrix Market format.
+"""
+#
+# Author: Pearu Peterson <pearu@cens.ioc.ee>
+# Created: October, 2004
+#
+# References:
+#  http://math.nist.gov/MatrixMarket/
+#
+import os
+
+import numpy as np
+from numpy import (asarray, real, imag, conj, zeros, ndarray, concatenate,
+                   ones, can_cast)
+
+from scipy.sparse import coo_array, issparse, coo_matrix
+
+__all__ = ['mminfo', 'mmread', 'mmwrite', 'MMFile']
+
+
+# -----------------------------------------------------------------------------
+def asstr(s):
+    if isinstance(s, bytes):
+        return s.decode('latin1')
+    return str(s)
+
+
+def mminfo(source):
+    """
+    Return size and storage parameters from Matrix Market file-like 'source'.
+
+    Parameters
+    ----------
+    source : str or file-like
+        Matrix Market filename (extension .mtx) or open file-like object
+
+    Returns
+    -------
+    rows : int
+        Number of matrix rows.
+    cols : int
+        Number of matrix columns.
+    entries : int
+        Number of non-zero entries of a sparse matrix
+        or rows*cols for a dense matrix.
+    format : str
+        Either 'coordinate' or 'array'.
+    field : str
+        Either 'real', 'complex', 'pattern', or 'integer'.
+    symmetry : str
+        Either 'general', 'symmetric', 'skew-symmetric', or 'hermitian'.
+
+    Examples
+    --------
+    >>> from io import StringIO
+    >>> from scipy.io import mminfo
+
+    >>> text = '''%%MatrixMarket matrix coordinate real general
+    ...  5 5 7
+    ...  2 3 1.0
+    ...  3 4 2.0
+    ...  3 5 3.0
+    ...  4 1 4.0
+    ...  4 2 5.0
+    ...  4 3 6.0
+    ...  4 4 7.0
+    ... '''
+
+
+    ``mminfo(source)`` returns the number of rows, number of columns,
+    format, field type and symmetry attribute of the source file.
+
+    >>> mminfo(StringIO(text))
+    (5, 5, 7, 'coordinate', 'real', 'general')
+    """
+    return MMFile.info(source)
+
+# -----------------------------------------------------------------------------
+
+
+def mmread(source, *, spmatrix=True):
+    """
+    Reads the contents of a Matrix Market file-like 'source' into a matrix.
+
+    Parameters
+    ----------
+    source : str or file-like
+        Matrix Market filename (extensions .mtx, .mtz.gz)
+        or open file-like object.
+    spmatrix : bool, optional (default: True)
+        If ``True``, return sparse matrix. Otherwise return sparse array.
+
+    Returns
+    -------
+    a : ndarray or coo_array or coo_matrix
+        Dense or sparse array depending on the matrix format in the
+        Matrix Market file.
+
+    Examples
+    --------
+    >>> from io import StringIO
+    >>> from scipy.io import mmread
+
+    >>> text = '''%%MatrixMarket matrix coordinate real general
+    ...  5 5 7
+    ...  2 3 1.0
+    ...  3 4 2.0
+    ...  3 5 3.0
+    ...  4 1 4.0
+    ...  4 2 5.0
+    ...  4 3 6.0
+    ...  4 4 7.0
+    ... '''
+
+    ``mmread(source)`` returns the data as sparse matrix in COO format.
+
+    >>> m = mmread(StringIO(text), spmatrix=False)
+    >>> m
+    <COOrdinate sparse array of dtype 'float64'
+         with 7 stored elements and shape (5, 5)>
+    >>> m.toarray()
+    array([[0., 0., 0., 0., 0.],
+           [0., 0., 1., 0., 0.],
+           [0., 0., 0., 2., 3.],
+           [4., 5., 6., 7., 0.],
+           [0., 0., 0., 0., 0.]])
+    """
+    return MMFile().read(source, spmatrix=spmatrix)
+
+# -----------------------------------------------------------------------------
+
+
+def mmwrite(target, a, comment='', field=None, precision=None, symmetry=None):
+    r"""
+    Writes the sparse or dense array `a` to Matrix Market file-like `target`.
+
+    Parameters
+    ----------
+    target : str or file-like
+        Matrix Market filename (extension .mtx) or open file-like object.
+    a : array like
+        Sparse or dense 2-D array.
+    comment : str, optional
+        Comments to be prepended to the Matrix Market file.
+    field : None or str, optional
+        Either 'real', 'complex', 'pattern', or 'integer'.
+    precision : None or int, optional
+        Number of digits to display for real or complex values.
+    symmetry : None or str, optional
+        Either 'general', 'symmetric', 'skew-symmetric', or 'hermitian'.
+        If symmetry is None the symmetry type of 'a' is determined by its
+        values.
+
+    Returns
+    -------
+    None
+
+    Examples
+    --------
+    >>> from io import BytesIO
+    >>> import numpy as np
+    >>> from scipy.sparse import coo_array
+    >>> from scipy.io import mmwrite
+
+    Write a small NumPy array to a matrix market file.  The file will be
+    written in the ``'array'`` format.
+
+    >>> a = np.array([[1.0, 0, 0, 0], [0, 2.5, 0, 6.25]])
+    >>> target = BytesIO()
+    >>> mmwrite(target, a)
+    >>> print(target.getvalue().decode('latin1'))
+    %%MatrixMarket matrix array real general
+    %
+    2 4
+    1
+    0
+    0
+    2.5
+    0
+    0
+    0
+    6.25
+
+    Add a comment to the output file, and set the precision to 3.
+
+    >>> target = BytesIO()
+    >>> mmwrite(target, a, comment='\n Some test data.\n', precision=3)
+    >>> print(target.getvalue().decode('latin1'))
+    %%MatrixMarket matrix array real general
+    %
+    % Some test data.
+    %
+    2 4
+    1.00e+00
+    0.00e+00
+    0.00e+00
+    2.50e+00
+    0.00e+00
+    0.00e+00
+    0.00e+00
+    6.25e+00
+
+    Convert to a sparse matrix before calling ``mmwrite``.  This will
+    result in the output format being ``'coordinate'`` rather than
+    ``'array'``.
+
+    >>> target = BytesIO()
+    >>> mmwrite(target, coo_array(a), precision=3)
+    >>> print(target.getvalue().decode('latin1'))
+    %%MatrixMarket matrix coordinate real general
+    %
+    2 4 3
+    1 1 1.00e+00
+    2 2 2.50e+00
+    2 4 6.25e+00
+
+    Write a complex Hermitian array to a matrix market file.  Note that
+    only six values are actually written to the file; the other values
+    are implied by the symmetry.
+
+    >>> z = np.array([[3, 1+2j, 4-3j], [1-2j, 1, -5j], [4+3j, 5j, 2.5]])
+    >>> z
+    array([[ 3. +0.j,  1. +2.j,  4. -3.j],
+           [ 1. -2.j,  1. +0.j, -0. -5.j],
+           [ 4. +3.j,  0. +5.j,  2.5+0.j]])
+
+    >>> target = BytesIO()
+    >>> mmwrite(target, z, precision=2)
+    >>> print(target.getvalue().decode('latin1'))
+    %%MatrixMarket matrix array complex hermitian
+    %
+    3 3
+    3.0e+00 0.0e+00
+    1.0e+00 -2.0e+00
+    4.0e+00 3.0e+00
+    1.0e+00 0.0e+00
+    0.0e+00 5.0e+00
+    2.5e+00 0.0e+00
+
+    """
+    MMFile().write(target, a, comment, field, precision, symmetry)
+
+
+###############################################################################
+class MMFile:
+    __slots__ = ('_rows',
+                 '_cols',
+                 '_entries',
+                 '_format',
+                 '_field',
+                 '_symmetry')
+
+    @property
+    def rows(self):
+        return self._rows
+
+    @property
+    def cols(self):
+        return self._cols
+
+    @property
+    def entries(self):
+        return self._entries
+
+    @property
+    def format(self):
+        return self._format
+
+    @property
+    def field(self):
+        return self._field
+
+    @property
+    def symmetry(self):
+        return self._symmetry
+
+    @property
+    def has_symmetry(self):
+        return self._symmetry in (self.SYMMETRY_SYMMETRIC,
+                                  self.SYMMETRY_SKEW_SYMMETRIC,
+                                  self.SYMMETRY_HERMITIAN)
+
+    # format values
+    FORMAT_COORDINATE = 'coordinate'
+    FORMAT_ARRAY = 'array'
+    FORMAT_VALUES = (FORMAT_COORDINATE, FORMAT_ARRAY)
+
+    @classmethod
+    def _validate_format(self, format):
+        if format not in self.FORMAT_VALUES:
+            msg = f'unknown format type {format}, must be one of {self.FORMAT_VALUES}'
+            raise ValueError(msg)
+
+    # field values
+    FIELD_INTEGER = 'integer'
+    FIELD_UNSIGNED = 'unsigned-integer'
+    FIELD_REAL = 'real'
+    FIELD_COMPLEX = 'complex'
+    FIELD_PATTERN = 'pattern'
+    FIELD_VALUES = (FIELD_INTEGER, FIELD_UNSIGNED, FIELD_REAL, FIELD_COMPLEX,
+                    FIELD_PATTERN)
+
+    @classmethod
+    def _validate_field(self, field):
+        if field not in self.FIELD_VALUES:
+            msg = f'unknown field type {field}, must be one of {self.FIELD_VALUES}'
+            raise ValueError(msg)
+
+    # symmetry values
+    SYMMETRY_GENERAL = 'general'
+    SYMMETRY_SYMMETRIC = 'symmetric'
+    SYMMETRY_SKEW_SYMMETRIC = 'skew-symmetric'
+    SYMMETRY_HERMITIAN = 'hermitian'
+    SYMMETRY_VALUES = (SYMMETRY_GENERAL, SYMMETRY_SYMMETRIC,
+                       SYMMETRY_SKEW_SYMMETRIC, SYMMETRY_HERMITIAN)
+
+    @classmethod
+    def _validate_symmetry(self, symmetry):
+        if symmetry not in self.SYMMETRY_VALUES:
+            raise ValueError(f'unknown symmetry type {symmetry}, '
+                             f'must be one of {self.SYMMETRY_VALUES}')
+
+    DTYPES_BY_FIELD = {FIELD_INTEGER: 'intp',
+                       FIELD_UNSIGNED: 'uint64',
+                       FIELD_REAL: 'd',
+                       FIELD_COMPLEX: 'D',
+                       FIELD_PATTERN: 'd'}
+
+    # -------------------------------------------------------------------------
+    @staticmethod
+    def reader():
+        pass
+
+    # -------------------------------------------------------------------------
+    @staticmethod
+    def writer():
+        pass
+
+    # -------------------------------------------------------------------------
+    @classmethod
+    def info(self, source):
+        """
+        Return size, storage parameters from Matrix Market file-like 'source'.
+
+        Parameters
+        ----------
+        source : str or file-like
+            Matrix Market filename (extension .mtx) or open file-like object
+
+        Returns
+        -------
+        rows : int
+            Number of matrix rows.
+        cols : int
+            Number of matrix columns.
+        entries : int
+            Number of non-zero entries of a sparse matrix
+            or rows*cols for a dense matrix.
+        format : str
+            Either 'coordinate' or 'array'.
+        field : str
+            Either 'real', 'complex', 'pattern', or 'integer'.
+        symmetry : str
+            Either 'general', 'symmetric', 'skew-symmetric', or 'hermitian'.
+        """
+
+        stream, close_it = self._open(source)
+
+        try:
+
+            # read and validate header line
+            line = stream.readline()
+            mmid, matrix, format, field, symmetry = \
+                (asstr(part.strip()) for part in line.split())
+            if not mmid.startswith('%%MatrixMarket'):
+                raise ValueError('source is not in Matrix Market format')
+            if not matrix.lower() == 'matrix':
+                raise ValueError("Problem reading file header: " + line)
+
+            # http://math.nist.gov/MatrixMarket/formats.html
+            if format.lower() == 'array':
+                format = self.FORMAT_ARRAY
+            elif format.lower() == 'coordinate':
+                format = self.FORMAT_COORDINATE
+
+            # skip comments
+            # line.startswith('%')
+            while line:
+                if line.lstrip() and line.lstrip()[0] in ['%', 37]:
+                    line = stream.readline()
+                else:
+                    break
+
+            # skip empty lines
+            while not line.strip():
+                line = stream.readline()
+
+            split_line = line.split()
+            if format == self.FORMAT_ARRAY:
+                if not len(split_line) == 2:
+                    raise ValueError("Header line not of length 2: " +
+                                     line.decode('ascii'))
+                rows, cols = map(int, split_line)
+                entries = rows * cols
+            else:
+                if not len(split_line) == 3:
+                    raise ValueError("Header line not of length 3: " +
+                                     line.decode('ascii'))
+                rows, cols, entries = map(int, split_line)
+
+            return (rows, cols, entries, format, field.lower(),
+                    symmetry.lower())
+
+        finally:
+            if close_it:
+                stream.close()
+
+    # -------------------------------------------------------------------------
+    @staticmethod
+    def _open(filespec, mode='rb'):
+        """ Return an open file stream for reading based on source.
+
+        If source is a file name, open it (after trying to find it with mtx and
+        gzipped mtx extensions). Otherwise, just return source.
+
+        Parameters
+        ----------
+        filespec : str or file-like
+            String giving file name or file-like object
+        mode : str, optional
+            Mode with which to open file, if `filespec` is a file name.
+
+        Returns
+        -------
+        fobj : file-like
+            Open file-like object.
+        close_it : bool
+            True if the calling function should close this file when done,
+            false otherwise.
+        """
+        # If 'filespec' is path-like (str, pathlib.Path, os.DirEntry, other class
+        # implementing a '__fspath__' method), try to convert it to str. If this
+        # fails by throwing a 'TypeError', assume it's an open file handle and
+        # return it as-is.
+        try:
+            filespec = os.fspath(filespec)
+        except TypeError:
+            return filespec, False
+
+        # 'filespec' is definitely a str now
+
+        # open for reading
+        if mode[0] == 'r':
+
+            # determine filename plus extension
+            if not os.path.isfile(filespec):
+                if os.path.isfile(filespec+'.mtx'):
+                    filespec = filespec + '.mtx'
+                elif os.path.isfile(filespec+'.mtx.gz'):
+                    filespec = filespec + '.mtx.gz'
+                elif os.path.isfile(filespec+'.mtx.bz2'):
+                    filespec = filespec + '.mtx.bz2'
+            # open filename
+            if filespec.endswith('.gz'):
+                import gzip
+                stream = gzip.open(filespec, mode)
+            elif filespec.endswith('.bz2'):
+                import bz2
+                stream = bz2.BZ2File(filespec, 'rb')
+            else:
+                stream = open(filespec, mode)
+
+        # open for writing
+        else:
+            if filespec[-4:] != '.mtx':
+                filespec = filespec + '.mtx'
+            stream = open(filespec, mode)
+
+        return stream, True
+
+    # -------------------------------------------------------------------------
+    @staticmethod
+    def _get_symmetry(a):
+        m, n = a.shape
+        if m != n:
+            return MMFile.SYMMETRY_GENERAL
+        issymm = True
+        isskew = True
+        isherm = a.dtype.char in 'FD'
+
+        # sparse input
+        if issparse(a):
+            # check if number of nonzero entries of lower and upper triangle
+            # matrix are equal
+            a = a.tocoo()
+            (row, col) = a.nonzero()
+            if (row < col).sum() != (row > col).sum():
+                return MMFile.SYMMETRY_GENERAL
+
+            # define iterator over symmetric pair entries
+            a = a.todok()
+
+            def symm_iterator():
+                for ((i, j), aij) in a.items():
+                    if i > j:
+                        aji = a[j, i]
+                        yield (aij, aji, False)
+                    elif i == j:
+                        yield (aij, aij, True)
+
+        # non-sparse input
+        else:
+            # define iterator over symmetric pair entries
+            def symm_iterator():
+                for j in range(n):
+                    for i in range(j, n):
+                        aij, aji = a[i][j], a[j][i]
+                        yield (aij, aji, i == j)
+
+        # check for symmetry
+        # yields aij, aji, is_diagonal
+        for (aij, aji, is_diagonal) in symm_iterator():
+            if isskew and is_diagonal and aij != 0:
+                isskew = False
+            else:
+                if issymm and aij != aji:
+                    issymm = False
+                with np.errstate(over="ignore"):
+                    # This can give a warning for uint dtypes, so silence that
+                    if isskew and aij != -aji:
+                        isskew = False
+                if isherm and aij != conj(aji):
+                    isherm = False
+            if not (issymm or isskew or isherm):
+                break
+
+        # return symmetry value
+        if issymm:
+            return MMFile.SYMMETRY_SYMMETRIC
+        if isskew:
+            return MMFile.SYMMETRY_SKEW_SYMMETRIC
+        if isherm:
+            return MMFile.SYMMETRY_HERMITIAN
+        return MMFile.SYMMETRY_GENERAL
+
+    # -------------------------------------------------------------------------
+    @staticmethod
+    def _field_template(field, precision):
+        return {MMFile.FIELD_REAL: '%%.%ie\n' % precision,
+                MMFile.FIELD_INTEGER: '%i\n',
+                MMFile.FIELD_UNSIGNED: '%u\n',
+                MMFile.FIELD_COMPLEX: '%%.%ie %%.%ie\n' %
+                    (precision, precision)
+                }.get(field, None)
+
+    # -------------------------------------------------------------------------
+    def __init__(self, **kwargs):
+        self._init_attrs(**kwargs)
+
+    # -------------------------------------------------------------------------
+    def read(self, source, *, spmatrix=True):
+        """
+        Reads the contents of a Matrix Market file-like 'source' into a matrix.
+
+        Parameters
+        ----------
+        source : str or file-like
+            Matrix Market filename (extensions .mtx, .mtz.gz)
+            or open file object.
+        spmatrix : bool, optional (default: True)
+            If ``True``, return sparse matrix. Otherwise return sparse array.
+
+        Returns
+        -------
+        a : ndarray or coo_array or coo_matrix
+            Dense or sparse array depending on the matrix format in the
+            Matrix Market file.
+        """
+        stream, close_it = self._open(source)
+
+        try:
+            self._parse_header(stream)
+            data = self._parse_body(stream)
+
+        finally:
+            if close_it:
+                stream.close()
+        if spmatrix and isinstance(data, coo_array):
+            data = coo_matrix(data)
+        return data
+
+
+    # -------------------------------------------------------------------------
+    def write(self, target, a, comment='', field=None, precision=None,
+              symmetry=None):
+        """
+        Writes sparse or dense array `a` to Matrix Market file-like `target`.
+
+        Parameters
+        ----------
+        target : str or file-like
+            Matrix Market filename (extension .mtx) or open file-like object.
+        a : array like
+            Sparse or dense 2-D array.
+        comment : str, optional
+            Comments to be prepended to the Matrix Market file.
+        field : None or str, optional
+            Either 'real', 'complex', 'pattern', or 'integer'.
+        precision : None or int, optional
+            Number of digits to display for real or complex values.
+        symmetry : None or str, optional
+            Either 'general', 'symmetric', 'skew-symmetric', or 'hermitian'.
+            If symmetry is None the symmetry type of 'a' is determined by its
+            values.
+        """
+
+        stream, close_it = self._open(target, 'wb')
+
+        try:
+            self._write(stream, a, comment, field, precision, symmetry)
+
+        finally:
+            if close_it:
+                stream.close()
+            else:
+                stream.flush()
+
+    # -------------------------------------------------------------------------
+    def _init_attrs(self, **kwargs):
+        """
+        Initialize each attributes with the corresponding keyword arg value
+        or a default of None
+        """
+
+        attrs = self.__class__.__slots__
+        public_attrs = [attr[1:] for attr in attrs]
+        invalid_keys = set(kwargs.keys()) - set(public_attrs)
+
+        if invalid_keys:
+            raise ValueError(f"found {tuple(invalid_keys)} invalid keyword "
+                             f"arguments, please only use {public_attrs}")
+
+        for attr in attrs:
+            setattr(self, attr, kwargs.get(attr[1:], None))
+
+    # -------------------------------------------------------------------------
+    def _parse_header(self, stream):
+        rows, cols, entries, format, field, symmetry = \
+            self.__class__.info(stream)
+        self._init_attrs(rows=rows, cols=cols, entries=entries, format=format,
+                         field=field, symmetry=symmetry)
+
+    # -------------------------------------------------------------------------
+    def _parse_body(self, stream):
+        rows, cols, entries, format, field, symm = (self.rows, self.cols,
+                                                    self.entries, self.format,
+                                                    self.field, self.symmetry)
+
+        dtype = self.DTYPES_BY_FIELD.get(field, None)
+
+        has_symmetry = self.has_symmetry
+        is_integer = field == self.FIELD_INTEGER
+        is_unsigned_integer = field == self.FIELD_UNSIGNED
+        is_complex = field == self.FIELD_COMPLEX
+        is_skew = symm == self.SYMMETRY_SKEW_SYMMETRIC
+        is_herm = symm == self.SYMMETRY_HERMITIAN
+        is_pattern = field == self.FIELD_PATTERN
+
+        if format == self.FORMAT_ARRAY:
+            a = zeros((rows, cols), dtype=dtype)
+            line = 1
+            i, j = 0, 0
+            if is_skew:
+                a[i, j] = 0
+                if i < rows - 1:
+                    i += 1
+            while line:
+                line = stream.readline()
+                # line.startswith('%')
+                if not line or line[0] in ['%', 37] or not line.strip():
+                    continue
+                if is_integer:
+                    aij = int(line)
+                elif is_unsigned_integer:
+                    aij = int(line)
+                elif is_complex:
+                    aij = complex(*map(float, line.split()))
+                else:
+                    aij = float(line)
+                a[i, j] = aij
+                if has_symmetry and i != j:
+                    if is_skew:
+                        a[j, i] = -aij
+                    elif is_herm:
+                        a[j, i] = conj(aij)
+                    else:
+                        a[j, i] = aij
+                if i < rows-1:
+                    i = i + 1
+                else:
+                    j = j + 1
+                    if not has_symmetry:
+                        i = 0
+                    else:
+                        i = j
+                        if is_skew:
+                            a[i, j] = 0
+                            if i < rows-1:
+                                i += 1
+
+            if is_skew:
+                if not (i in [0, j] and j == cols - 1):
+                    raise ValueError("Parse error, did not read all lines.")
+            else:
+                if not (i in [0, j] and j == cols):
+                    raise ValueError("Parse error, did not read all lines.")
+
+        elif format == self.FORMAT_COORDINATE:
+            # Read sparse COOrdinate format
+
+            if entries == 0:
+                # empty matrix
+                return coo_array((rows, cols), dtype=dtype)
+
+            I = zeros(entries, dtype='intc')
+            J = zeros(entries, dtype='intc')
+            if is_pattern:
+                V = ones(entries, dtype='int8')
+            elif is_integer:
+                V = zeros(entries, dtype='intp')
+            elif is_unsigned_integer:
+                V = zeros(entries, dtype='uint64')
+            elif is_complex:
+                V = zeros(entries, dtype='complex')
+            else:
+                V = zeros(entries, dtype='float')
+
+            entry_number = 0
+            for line in stream:
+                # line.startswith('%')
+                if not line or line[0] in ['%', 37] or not line.strip():
+                    continue
+
+                if entry_number+1 > entries:
+                    raise ValueError("'entries' in header is smaller than "
+                                     "number of entries")
+                l = line.split()
+                I[entry_number], J[entry_number] = map(int, l[:2])
+
+                if not is_pattern:
+                    if is_integer:
+                        V[entry_number] = int(l[2])
+                    elif is_unsigned_integer:
+                        V[entry_number] = int(l[2])
+                    elif is_complex:
+                        V[entry_number] = complex(*map(float, l[2:]))
+                    else:
+                        V[entry_number] = float(l[2])
+                entry_number += 1
+            if entry_number < entries:
+                raise ValueError("'entries' in header is larger than "
+                                 "number of entries")
+
+            I -= 1  # adjust indices (base 1 -> base 0)
+            J -= 1
+
+            if has_symmetry:
+                mask = (I != J)       # off diagonal mask
+                od_I = I[mask]
+                od_J = J[mask]
+                od_V = V[mask]
+
+                I = concatenate((I, od_J))
+                J = concatenate((J, od_I))
+
+                if is_skew:
+                    od_V *= -1
+                elif is_herm:
+                    od_V = od_V.conjugate()
+
+                V = concatenate((V, od_V))
+
+            a = coo_array((V, (I, J)), shape=(rows, cols), dtype=dtype)
+        else:
+            raise NotImplementedError(format)
+
+        return a
+
+    #  ------------------------------------------------------------------------
+    def _write(self, stream, a, comment='', field=None, precision=None,
+               symmetry=None):
+        if isinstance(a, list) or isinstance(a, ndarray) or \
+           isinstance(a, tuple) or hasattr(a, '__array__'):
+            rep = self.FORMAT_ARRAY
+            a = asarray(a)
+            if len(a.shape) != 2:
+                raise ValueError('Expected 2 dimensional array')
+            rows, cols = a.shape
+
+            if field is not None:
+
+                if field == self.FIELD_INTEGER:
+                    if not can_cast(a.dtype, 'intp'):
+                        raise OverflowError("mmwrite does not support integer "
+                                            "dtypes larger than native 'intp'.")
+                    a = a.astype('intp')
+                elif field == self.FIELD_REAL:
+                    if a.dtype.char not in 'fd':
+                        a = a.astype('d')
+                elif field == self.FIELD_COMPLEX:
+                    if a.dtype.char not in 'FD':
+                        a = a.astype('D')
+
+        else:
+            if not issparse(a):
+                raise ValueError(f'unknown matrix type: {type(a)}')
+
+            rep = 'coordinate'
+            rows, cols = a.shape
+
+        typecode = a.dtype.char
+
+        if precision is None:
+            if typecode in 'fF':
+                precision = 8
+            else:
+                precision = 16
+        if field is None:
+            kind = a.dtype.kind
+            if kind == 'i':
+                if not can_cast(a.dtype, 'intp'):
+                    raise OverflowError("mmwrite does not support integer "
+                                        "dtypes larger than native 'intp'.")
+                field = 'integer'
+            elif kind == 'f':
+                field = 'real'
+            elif kind == 'c':
+                field = 'complex'
+            elif kind == 'u':
+                field = 'unsigned-integer'
+            else:
+                raise TypeError('unexpected dtype kind ' + kind)
+
+        if symmetry is None:
+            symmetry = self._get_symmetry(a)
+
+        # validate rep, field, and symmetry
+        self.__class__._validate_format(rep)
+        self.__class__._validate_field(field)
+        self.__class__._validate_symmetry(symmetry)
+
+        # write initial header line
+        data = f'%%MatrixMarket matrix {rep} {field} {symmetry}\n'
+        stream.write(data.encode('latin1'))
+
+        # write comments
+        for line in comment.split('\n'):
+            data = f'%{line}\n'
+            stream.write(data.encode('latin1'))
+
+        template = self._field_template(field, precision)
+        # write dense format
+        if rep == self.FORMAT_ARRAY:
+            # write shape spec
+            data = '%i %i\n' % (rows, cols)
+            stream.write(data.encode('latin1'))
+
+            if field in (self.FIELD_INTEGER, self.FIELD_REAL,
+                         self.FIELD_UNSIGNED):
+                if symmetry == self.SYMMETRY_GENERAL:
+                    for j in range(cols):
+                        for i in range(rows):
+                            data = template % a[i, j]
+                            stream.write(data.encode('latin1'))
+
+                elif symmetry == self.SYMMETRY_SKEW_SYMMETRIC:
+                    for j in range(cols):
+                        for i in range(j + 1, rows):
+                            data = template % a[i, j]
+                            stream.write(data.encode('latin1'))
+
+                else:
+                    for j in range(cols):
+                        for i in range(j, rows):
+                            data = template % a[i, j]
+                            stream.write(data.encode('latin1'))
+
+            elif field == self.FIELD_COMPLEX:
+
+                if symmetry == self.SYMMETRY_GENERAL:
+                    for j in range(cols):
+                        for i in range(rows):
+                            aij = a[i, j]
+                            data = template % (real(aij), imag(aij))
+                            stream.write(data.encode('latin1'))
+                else:
+                    for j in range(cols):
+                        for i in range(j, rows):
+                            aij = a[i, j]
+                            data = template % (real(aij), imag(aij))
+                            stream.write(data.encode('latin1'))
+
+            elif field == self.FIELD_PATTERN:
+                raise ValueError('pattern type inconsisted with dense format')
+
+            else:
+                raise TypeError(f'Unknown field type {field}')
+
+        # write sparse format
+        else:
+            coo = a.tocoo()  # convert to COOrdinate format
+
+            # if symmetry format used, remove values above main diagonal
+            if symmetry != self.SYMMETRY_GENERAL:
+                lower_triangle_mask = coo.row >= coo.col
+                coo = coo_array((coo.data[lower_triangle_mask],
+                                (coo.row[lower_triangle_mask],
+                                 coo.col[lower_triangle_mask])),
+                                shape=coo.shape)
+
+            # write shape spec
+            data = '%i %i %i\n' % (rows, cols, coo.nnz)
+            stream.write(data.encode('latin1'))
+
+            template = self._field_template(field, precision-1)
+
+            if field == self.FIELD_PATTERN:
+                for r, c in zip(coo.row+1, coo.col+1):
+                    data = "%i %i\n" % (r, c)
+                    stream.write(data.encode('latin1'))
+            elif field in (self.FIELD_INTEGER, self.FIELD_REAL,
+                           self.FIELD_UNSIGNED):
+                for r, c, d in zip(coo.row+1, coo.col+1, coo.data):
+                    data = ("%i %i " % (r, c)) + (template % d)
+                    stream.write(data.encode('latin1'))
+            elif field == self.FIELD_COMPLEX:
+                for r, c, d in zip(coo.row+1, coo.col+1, coo.data):
+                    data = ("%i %i " % (r, c)) + (template % (d.real, d.imag))
+                    stream.write(data.encode('latin1'))
+            else:
+                raise TypeError(f'Unknown field type {field}')
+
+
+def _is_fromfile_compatible(stream):
+    """
+    Check whether `stream` is compatible with numpy.fromfile.
+
+    Passing a gzipped file object to ``fromfile/fromstring`` doesn't work with
+    Python 3.
+    """
+
+    bad_cls = []
+    try:
+        import gzip
+        bad_cls.append(gzip.GzipFile)
+    except ImportError:
+        pass
+    try:
+        import bz2
+        bad_cls.append(bz2.BZ2File)
+    except ImportError:
+        pass
+
+    bad_cls = tuple(bad_cls)
+    return not isinstance(stream, bad_cls)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/_netcdf.py

@@ -0,0 +1,1104 @@
+"""
+NetCDF reader/writer module.
+
+This module is used to read and create NetCDF files. NetCDF files are
+accessed through the `netcdf_file` object. Data written to and from NetCDF
+files are contained in `netcdf_variable` objects. Attributes are given
+as member variables of the `netcdf_file` and `netcdf_variable` objects.
+
+This module implements the Scientific.IO.NetCDF API to read and create
+NetCDF files. The same API is also used in the PyNIO and pynetcdf
+modules, allowing these modules to be used interchangeably when working
+with NetCDF files.
+
+Only NetCDF3 is supported here; for NetCDF4 see
+`netCDF4-python <http://unidata.github.io/netcdf4-python/>`__,
+which has a similar API.
+
+"""
+
+# TODO:
+# * properly implement ``_FillValue``.
+# * fix character variables.
+# * implement PAGESIZE for Python 2.6?
+
+# The Scientific.IO.NetCDF API allows attributes to be added directly to
+# instances of ``netcdf_file`` and ``netcdf_variable``. To differentiate
+# between user-set attributes and instance attributes, user-set attributes
+# are automatically stored in the ``_attributes`` attribute by overloading
+#``__setattr__``. This is the reason why the code sometimes uses
+#``obj.__dict__['key'] = value``, instead of simply ``obj.key = value``;
+# otherwise the key would be inserted into userspace attributes.
+
+
+__all__ = ['netcdf_file', 'netcdf_variable']
+
+
+import warnings
+import weakref
+from operator import mul
+from platform import python_implementation
+
+import mmap as mm
+
+import numpy as np
+from numpy import frombuffer, dtype, empty, array, asarray
+from numpy import little_endian as LITTLE_ENDIAN
+from functools import reduce
+
+
+IS_PYPY = python_implementation() == 'PyPy'
+
+ABSENT = b'\x00\x00\x00\x00\x00\x00\x00\x00'
+ZERO = b'\x00\x00\x00\x00'
+NC_BYTE = b'\x00\x00\x00\x01'
+NC_CHAR = b'\x00\x00\x00\x02'
+NC_SHORT = b'\x00\x00\x00\x03'
+NC_INT = b'\x00\x00\x00\x04'
+NC_FLOAT = b'\x00\x00\x00\x05'
+NC_DOUBLE = b'\x00\x00\x00\x06'
+NC_DIMENSION = b'\x00\x00\x00\n'
+NC_VARIABLE = b'\x00\x00\x00\x0b'
+NC_ATTRIBUTE = b'\x00\x00\x00\x0c'
+FILL_BYTE = b'\x81'
+FILL_CHAR = b'\x00'
+FILL_SHORT = b'\x80\x01'
+FILL_INT = b'\x80\x00\x00\x01'
+FILL_FLOAT = b'\x7C\xF0\x00\x00'
+FILL_DOUBLE = b'\x47\x9E\x00\x00\x00\x00\x00\x00'
+
+TYPEMAP = {NC_BYTE: ('b', 1),
+           NC_CHAR: ('c', 1),
+           NC_SHORT: ('h', 2),
+           NC_INT: ('i', 4),
+           NC_FLOAT: ('f', 4),
+           NC_DOUBLE: ('d', 8)}
+
+FILLMAP = {NC_BYTE: FILL_BYTE,
+           NC_CHAR: FILL_CHAR,
+           NC_SHORT: FILL_SHORT,
+           NC_INT: FILL_INT,
+           NC_FLOAT: FILL_FLOAT,
+           NC_DOUBLE: FILL_DOUBLE}
+
+REVERSE = {('b', 1): NC_BYTE,
+           ('B', 1): NC_CHAR,
+           ('c', 1): NC_CHAR,
+           ('h', 2): NC_SHORT,
+           ('i', 4): NC_INT,
+           ('f', 4): NC_FLOAT,
+           ('d', 8): NC_DOUBLE,
+
+           # these come from asarray(1).dtype.char and asarray('foo').dtype.char,
+           # used when getting the types from generic attributes.
+           ('l', 4): NC_INT,
+           ('S', 1): NC_CHAR}
+
+
+class netcdf_file:
+    """
+    A file object for NetCDF data.
+
+    A `netcdf_file` object has two standard attributes: `dimensions` and
+    `variables`. The values of both are dictionaries, mapping dimension
+    names to their associated lengths and variable names to variables,
+    respectively. Application programs should never modify these
+    dictionaries.
+
+    All other attributes correspond to global attributes defined in the
+    NetCDF file. Global file attributes are created by assigning to an
+    attribute of the `netcdf_file` object.
+
+    Parameters
+    ----------
+    filename : string or file-like
+        string -> filename
+    mode : {'r', 'w', 'a'}, optional
+        read-write-append mode, default is 'r'
+    mmap : None or bool, optional
+        Whether to mmap `filename` when reading.  Default is True
+        when `filename` is a file name, False when `filename` is a
+        file-like object. Note that when mmap is in use, data arrays
+        returned refer directly to the mmapped data on disk, and the
+        file cannot be closed as long as references to it exist.
+    version : {1, 2}, optional
+        version of netcdf to read / write, where 1 means *Classic
+        format* and 2 means *64-bit offset format*.  Default is 1.  See
+        `here <https://docs.unidata.ucar.edu/nug/current/netcdf_introduction.html#select_format>`__
+        for more info.
+    maskandscale : bool, optional
+        Whether to automatically scale and/or mask data based on attributes.
+        Default is False.
+
+    Notes
+    -----
+    This module is derived from
+    `pupynere <https://bitbucket.org/robertodealmeida/pupynere/>`_.
+    The major advantage of this module over other modules is that it doesn't
+    require the code to be linked to the NetCDF libraries. However, for a more
+    recent version of the NetCDF standard and additional features, please consider
+    the permissively-licensed
+    `netcdf4-python <https://unidata.github.io/netcdf4-python/>`_.
+
+    NetCDF files are a self-describing binary data format. The file contains
+    metadata that describes the dimensions and variables in the file. More
+    details about NetCDF files can be found `here
+    <https://www.unidata.ucar.edu/software/netcdf/guide_toc.html>`__. There
+    are three main sections to a NetCDF data structure:
+
+    1. Dimensions
+    2. Variables
+    3. Attributes
+
+    The dimensions section records the name and length of each dimension used
+    by the variables. The variables would then indicate which dimensions it
+    uses and any attributes such as data units, along with containing the data
+    values for the variable. It is good practice to include a
+    variable that is the same name as a dimension to provide the values for
+    that axes. Lastly, the attributes section would contain additional
+    information such as the name of the file creator or the instrument used to
+    collect the data.
+
+    When writing data to a NetCDF file, there is often the need to indicate the
+    'record dimension'. A record dimension is the unbounded dimension for a
+    variable. For example, a temperature variable may have dimensions of
+    latitude, longitude and time. If one wants to add more temperature data to
+    the NetCDF file as time progresses, then the temperature variable should
+    have the time dimension flagged as the record dimension.
+
+    In addition, the NetCDF file header contains the position of the data in
+    the file, so access can be done in an efficient manner without loading
+    unnecessary data into memory. It uses the ``mmap`` module to create
+    Numpy arrays mapped to the data on disk, for the same purpose.
+
+    Note that when `netcdf_file` is used to open a file with mmap=True
+    (default for read-only), arrays returned by it refer to data
+    directly on the disk. The file should not be closed, and cannot be cleanly
+    closed when asked, if such arrays are alive. You may want to copy data arrays
+    obtained from mmapped Netcdf file if they are to be processed after the file
+    is closed, see the example below.
+
+    Examples
+    --------
+    To create a NetCDF file:
+
+    >>> from scipy.io import netcdf_file
+    >>> import numpy as np
+    >>> f = netcdf_file('simple.nc', 'w')
+    >>> f.history = 'Created for a test'
+    >>> f.createDimension('time', 10)
+    >>> time = f.createVariable('time', 'i', ('time',))
+    >>> time[:] = np.arange(10)
+    >>> time.units = 'days since 2008-01-01'
+    >>> f.close()
+
+    Note the assignment of ``arange(10)`` to ``time[:]``.  Exposing the slice
+    of the time variable allows for the data to be set in the object, rather
+    than letting ``arange(10)`` overwrite the ``time`` variable.
+
+    To read the NetCDF file we just created:
+
+    >>> from scipy.io import netcdf_file
+    >>> f = netcdf_file('simple.nc', 'r')
+    >>> print(f.history)
+    b'Created for a test'
+    >>> time = f.variables['time']
+    >>> print(time.units)
+    b'days since 2008-01-01'
+    >>> print(time.shape)
+    (10,)
+    >>> print(time[-1])
+    9
+
+    NetCDF files, when opened read-only, return arrays that refer
+    directly to memory-mapped data on disk:
+
+    >>> data = time[:]
+
+    If the data is to be processed after the file is closed, it needs
+    to be copied to main memory:
+
+    >>> data = time[:].copy()
+    >>> del time
+    >>> f.close()
+    >>> data.mean()
+    4.5
+
+    A NetCDF file can also be used as context manager:
+
+    >>> from scipy.io import netcdf_file
+    >>> with netcdf_file('simple.nc', 'r') as f:
+    ...     print(f.history)
+    b'Created for a test'
+
+    """
+    def __init__(self, filename, mode='r', mmap=None, version=1,
+                 maskandscale=False):
+        """Initialize netcdf_file from fileobj (str or file-like)."""
+        if mode not in 'rwa':
+            raise ValueError("Mode must be either 'r', 'w' or 'a'.")
+
+        if hasattr(filename, 'seek'):  # file-like
+            self.fp = filename
+            self.filename = 'None'
+            if mmap is None:
+                mmap = False
+            elif mmap and not hasattr(filename, 'fileno'):
+                raise ValueError('Cannot use file object for mmap')
+        else:  # maybe it's a string
+            self.filename = filename
+            omode = 'r+' if mode == 'a' else mode
+            self.fp = open(self.filename, f'{omode}b')
+            if mmap is None:
+                # Mmapped files on PyPy cannot be usually closed
+                # before the GC runs, so it's better to use mmap=False
+                # as the default.
+                mmap = (not IS_PYPY)
+
+        if mode != 'r':
+            # Cannot read write-only files
+            mmap = False
+
+        self.use_mmap = mmap
+        self.mode = mode
+        self.version_byte = version
+        self.maskandscale = maskandscale
+
+        self.dimensions = {}
+        self.variables = {}
+
+        self._dims = []
+        self._recs = 0
+        self._recsize = 0
+
+        self._mm = None
+        self._mm_buf = None
+        if self.use_mmap:
+            self._mm = mm.mmap(self.fp.fileno(), 0, access=mm.ACCESS_READ)
+            self._mm_buf = np.frombuffer(self._mm, dtype=np.int8)
+
+        self._attributes = {}
+
+        if mode in 'ra':
+            self._read()
+
+    def __setattr__(self, attr, value):
+        # Store user defined attributes in a separate dict,
+        # so we can save them to file later.
+        try:
+            self._attributes[attr] = value
+        except AttributeError:
+            pass
+        self.__dict__[attr] = value
+
+    def close(self):
+        """Closes the NetCDF file."""
+        if hasattr(self, 'fp') and not self.fp.closed:
+            try:
+                self.flush()
+            finally:
+                self.variables = {}
+                if self._mm_buf is not None:
+                    ref = weakref.ref(self._mm_buf)
+                    self._mm_buf = None
+                    if ref() is None:
+                        # self._mm_buf is gc'd, and we can close the mmap
+                        self._mm.close()
+                    else:
+                        # we cannot close self._mm, since self._mm_buf is
+                        # alive and there may still be arrays referring to it
+                        warnings.warn(
+                            "Cannot close a netcdf_file opened with mmap=True, when "
+                            "netcdf_variables or arrays referring to its data still "
+                            "exist. All data arrays obtained from such files refer "
+                            "directly to data on disk, and must be copied before the "
+                            "file can be cleanly closed. "
+                            "(See netcdf_file docstring for more information on mmap.)",
+                            category=RuntimeWarning, stacklevel=2,
+                        )
+                self._mm = None
+                self.fp.close()
+    __del__ = close
+
+    def __enter__(self):
+        return self
+
+    def __exit__(self, type, value, traceback):
+        self.close()
+
+    def createDimension(self, name, length):
+        """
+        Adds a dimension to the Dimension section of the NetCDF data structure.
+
+        Note that this function merely adds a new dimension that the variables can
+        reference. The values for the dimension, if desired, should be added as
+        a variable using `createVariable`, referring to this dimension.
+
+        Parameters
+        ----------
+        name : str
+            Name of the dimension (Eg, 'lat' or 'time').
+        length : int
+            Length of the dimension.
+
+        See Also
+        --------
+        createVariable
+
+        """
+        if length is None and self._dims:
+            raise ValueError("Only first dimension may be unlimited!")
+
+        self.dimensions[name] = length
+        self._dims.append(name)
+
+    def createVariable(self, name, type, dimensions):
+        """
+        Create an empty variable for the `netcdf_file` object, specifying its data
+        type and the dimensions it uses.
+
+        Parameters
+        ----------
+        name : str
+            Name of the new variable.
+        type : dtype or str
+            Data type of the variable.
+        dimensions : sequence of str
+            List of the dimension names used by the variable, in the desired order.
+
+        Returns
+        -------
+        variable : netcdf_variable
+            The newly created ``netcdf_variable`` object.
+            This object has also been added to the `netcdf_file` object as well.
+
+        See Also
+        --------
+        createDimension
+
+        Notes
+        -----
+        Any dimensions to be used by the variable should already exist in the
+        NetCDF data structure or should be created by `createDimension` prior to
+        creating the NetCDF variable.
+
+        """
+        shape = tuple([self.dimensions[dim] for dim in dimensions])
+        shape_ = tuple([dim or 0 for dim in shape])  # replace None with 0 for NumPy
+
+        type = dtype(type)
+        typecode, size = type.char, type.itemsize
+        if (typecode, size) not in REVERSE:
+            raise ValueError(f"NetCDF 3 does not support type {type}")
+
+        # convert to big endian always for NetCDF 3
+        data = empty(shape_, dtype=type.newbyteorder("B"))
+        self.variables[name] = netcdf_variable(
+                data, typecode, size, shape, dimensions,
+                maskandscale=self.maskandscale)
+        return self.variables[name]
+
+    def flush(self):
+        """
+        Perform a sync-to-disk flush if the `netcdf_file` object is in write mode.
+
+        See Also
+        --------
+        sync : Identical function
+
+        """
+        if hasattr(self, 'mode') and self.mode in 'wa':
+            self._write()
+    sync = flush
+
+    def _write(self):
+        self.fp.seek(0)
+        self.fp.write(b'CDF')
+        self.fp.write(array(self.version_byte, '>b').tobytes())
+
+        # Write headers and data.
+        self._write_numrecs()
+        self._write_dim_array()
+        self._write_gatt_array()
+        self._write_var_array()
+
+    def _write_numrecs(self):
+        # Get highest record count from all record variables.
+        for var in self.variables.values():
+            if var.isrec and len(var.data) > self._recs:
+                self.__dict__['_recs'] = len(var.data)
+        self._pack_int(self._recs)
+
+    def _write_dim_array(self):
+        if self.dimensions:
+            self.fp.write(NC_DIMENSION)
+            self._pack_int(len(self.dimensions))
+            for name in self._dims:
+                self._pack_string(name)
+                length = self.dimensions[name]
+                self._pack_int(length or 0)  # replace None with 0 for record dimension
+        else:
+            self.fp.write(ABSENT)
+
+    def _write_gatt_array(self):
+        self._write_att_array(self._attributes)
+
+    def _write_att_array(self, attributes):
+        if attributes:
+            self.fp.write(NC_ATTRIBUTE)
+            self._pack_int(len(attributes))
+            for name, values in attributes.items():
+                self._pack_string(name)
+                self._write_att_values(values)
+        else:
+            self.fp.write(ABSENT)
+
+    def _write_var_array(self):
+        if self.variables:
+            self.fp.write(NC_VARIABLE)
+            self._pack_int(len(self.variables))
+
+            # Sort variable names non-recs first, then recs.
+            def sortkey(n):
+                v = self.variables[n]
+                if v.isrec:
+                    return (-1,)
+                return v._shape
+            variables = sorted(self.variables, key=sortkey, reverse=True)
+
+            # Set the metadata for all variables.
+            for name in variables:
+                self._write_var_metadata(name)
+            # Now that we have the metadata, we know the vsize of
+            # each record variable, so we can calculate recsize.
+            self.__dict__['_recsize'] = sum([
+                    var._vsize for var in self.variables.values()
+                    if var.isrec])
+            # Set the data for all variables.
+            for name in variables:
+                self._write_var_data(name)
+        else:
+            self.fp.write(ABSENT)
+
+    def _write_var_metadata(self, name):
+        var = self.variables[name]
+
+        self._pack_string(name)
+        self._pack_int(len(var.dimensions))
+        for dimname in var.dimensions:
+            dimid = self._dims.index(dimname)
+            self._pack_int(dimid)
+
+        self._write_att_array(var._attributes)
+
+        nc_type = REVERSE[var.typecode(), var.itemsize()]
+        self.fp.write(nc_type)
+
+        if not var.isrec:
+            vsize = var.data.size * var.data.itemsize
+            vsize += -vsize % 4
+        else:  # record variable
+            try:
+                vsize = var.data[0].size * var.data.itemsize
+            except IndexError:
+                vsize = 0
+            rec_vars = len([v for v in self.variables.values()
+                            if v.isrec])
+            if rec_vars > 1:
+                vsize += -vsize % 4
+        self.variables[name].__dict__['_vsize'] = vsize
+        self._pack_int(vsize)
+
+        # Pack a bogus begin, and set the real value later.
+        self.variables[name].__dict__['_begin'] = self.fp.tell()
+        self._pack_begin(0)
+
+    def _write_var_data(self, name):
+        var = self.variables[name]
+
+        # Set begin in file header.
+        the_beguine = self.fp.tell()
+        self.fp.seek(var._begin)
+        self._pack_begin(the_beguine)
+        self.fp.seek(the_beguine)
+
+        # Write data.
+        if not var.isrec:
+            self.fp.write(var.data.tobytes())
+            count = var.data.size * var.data.itemsize
+            self._write_var_padding(var, var._vsize - count)
+        else:  # record variable
+            # Handle rec vars with shape[0] < nrecs.
+            if self._recs > len(var.data):
+                shape = (self._recs,) + var.data.shape[1:]
+                # Resize in-place does not always work since
+                # the array might not be single-segment
+                try:
+                    var.data.resize(shape)
+                except ValueError:
+                    dtype = var.data.dtype
+                    var.__dict__['data'] = np.resize(var.data, shape).astype(dtype)
+
+            pos0 = pos = self.fp.tell()
+            for rec in var.data:
+                # Apparently scalars cannot be converted to big endian. If we
+                # try to convert a ``=i4`` scalar to, say, '>i4' the dtype
+                # will remain as ``=i4``.
+                if not rec.shape and (rec.dtype.byteorder == '<' or
+                        (rec.dtype.byteorder == '=' and LITTLE_ENDIAN)):
+                    rec = rec.byteswap()
+                self.fp.write(rec.tobytes())
+                # Padding
+                count = rec.size * rec.itemsize
+                self._write_var_padding(var, var._vsize - count)
+                pos += self._recsize
+                self.fp.seek(pos)
+            self.fp.seek(pos0 + var._vsize)
+
+    def _write_var_padding(self, var, size):
+        encoded_fill_value = var._get_encoded_fill_value()
+        num_fills = size // len(encoded_fill_value)
+        self.fp.write(encoded_fill_value * num_fills)
+
+    def _write_att_values(self, values):
+        if hasattr(values, 'dtype'):
+            nc_type = REVERSE[values.dtype.char, values.dtype.itemsize]
+        else:
+            types = [(int, NC_INT), (float, NC_FLOAT), (str, NC_CHAR)]
+
+            # bytes index into scalars in py3k. Check for "string" types
+            if isinstance(values, str | bytes):
+                sample = values
+            else:
+                try:
+                    sample = values[0]  # subscriptable?
+                except TypeError:
+                    sample = values     # scalar
+
+            for class_, nc_type in types:
+                if isinstance(sample, class_):
+                    break
+
+        typecode, size = TYPEMAP[nc_type]
+        dtype_ = f'>{typecode}'
+        # asarray() dies with bytes and '>c' in py3k. Change to 'S'
+        dtype_ = 'S' if dtype_ == '>c' else dtype_
+
+        values = asarray(values, dtype=dtype_)
+
+        self.fp.write(nc_type)
+
+        if values.dtype.char == 'S':
+            nelems = values.itemsize
+        else:
+            nelems = values.size
+        self._pack_int(nelems)
+
+        if not values.shape and (values.dtype.byteorder == '<' or
+                (values.dtype.byteorder == '=' and LITTLE_ENDIAN)):
+            values = values.byteswap()
+        self.fp.write(values.tobytes())
+        count = values.size * values.itemsize
+        self.fp.write(b'\x00' * (-count % 4))  # pad
+
+    def _read(self):
+        # Check magic bytes and version
+        magic = self.fp.read(3)
+        if not magic == b'CDF':
+            raise TypeError(f"Error: {self.filename} is not a valid NetCDF 3 file")
+        self.__dict__['version_byte'] = frombuffer(self.fp.read(1), '>b')[0]
+
+        # Read file headers and set data.
+        self._read_numrecs()
+        self._read_dim_array()
+        self._read_gatt_array()
+        self._read_var_array()
+
+    def _read_numrecs(self):
+        self.__dict__['_recs'] = self._unpack_int()
+
+    def _read_dim_array(self):
+        header = self.fp.read(4)
+        if header not in [ZERO, NC_DIMENSION]:
+            raise ValueError("Unexpected header.")
+        count = self._unpack_int()
+
+        for dim in range(count):
+            name = self._unpack_string().decode('latin1')
+            length = self._unpack_int() or None  # None for record dimension
+            self.dimensions[name] = length
+            self._dims.append(name)  # preserve order
+
+    def _read_gatt_array(self):
+        for k, v in self._read_att_array().items():
+            self.__setattr__(k, v)
+
+    def _read_att_array(self):
+        header = self.fp.read(4)
+        if header not in [ZERO, NC_ATTRIBUTE]:
+            raise ValueError("Unexpected header.")
+        count = self._unpack_int()
+
+        attributes = {}
+        for attr in range(count):
+            name = self._unpack_string().decode('latin1')
+            attributes[name] = self._read_att_values()
+        return attributes
+
+    def _read_var_array(self):
+        header = self.fp.read(4)
+        if header not in [ZERO, NC_VARIABLE]:
+            raise ValueError("Unexpected header.")
+
+        begin = 0
+        dtypes = {'names': [], 'formats': []}
+        rec_vars = []
+        count = self._unpack_int()
+        for var in range(count):
+            (name, dimensions, shape, attributes,
+             typecode, size, dtype_, begin_, vsize) = self._read_var()
+            # https://www.unidata.ucar.edu/software/netcdf/guide_toc.html
+            # Note that vsize is the product of the dimension lengths
+            # (omitting the record dimension) and the number of bytes
+            # per value (determined from the type), increased to the
+            # next multiple of 4, for each variable. If a record
+            # variable, this is the amount of space per record. The
+            # netCDF "record size" is calculated as the sum of the
+            # vsize's of all the record variables.
+            #
+            # The vsize field is actually redundant, because its value
+            # may be computed from other information in the header. The
+            # 32-bit vsize field is not large enough to contain the size
+            # of variables that require more than 2^32 - 4 bytes, so
+            # 2^32 - 1 is used in the vsize field for such variables.
+            if shape and shape[0] is None:  # record variable
+                rec_vars.append(name)
+                # The netCDF "record size" is calculated as the sum of
+                # the vsize's of all the record variables.
+                self.__dict__['_recsize'] += vsize
+                if begin == 0:
+                    begin = begin_
+                dtypes['names'].append(name)
+                dtypes['formats'].append(str(shape[1:]) + dtype_)
+
+                # Handle padding with a virtual variable.
+                if typecode in 'bch':
+                    actual_size = reduce(mul, (1,) + shape[1:]) * size
+                    padding = -actual_size % 4
+                    if padding:
+                        dtypes['names'].append(f'_padding_{var}')
+                        dtypes['formats'].append(f'({padding},)>b')
+
+                # Data will be set later.
+                data = None
+            else:  # not a record variable
+                # Calculate size to avoid problems with vsize (above)
+                a_size = reduce(mul, shape, 1) * size
+                if self.use_mmap:
+                    data = self._mm_buf[begin_:begin_+a_size].view(dtype=dtype_)
+                    data = data.reshape(shape)
+                else:
+                    pos = self.fp.tell()
+                    self.fp.seek(begin_)
+                    data = frombuffer(self.fp.read(a_size), dtype=dtype_
+                                      ).copy()
+                    data = data.reshape(shape)
+                    self.fp.seek(pos)
+
+            # Add variable.
+            self.variables[name] = netcdf_variable(
+                    data, typecode, size, shape, dimensions, attributes,
+                    maskandscale=self.maskandscale)
+
+        if rec_vars:
+            # Remove padding when only one record variable.
+            if len(rec_vars) == 1:
+                dtypes['names'] = dtypes['names'][:1]
+                dtypes['formats'] = dtypes['formats'][:1]
+
+            # Build rec array.
+            if self.use_mmap:
+                buf = self._mm_buf[begin:begin+self._recs*self._recsize]
+                rec_array = buf.view(dtype=dtypes)
+                rec_array = rec_array.reshape((self._recs,))
+            else:
+                pos = self.fp.tell()
+                self.fp.seek(begin)
+                rec_array = frombuffer(self.fp.read(self._recs*self._recsize),
+                                       dtype=dtypes).copy()
+                rec_array = rec_array.reshape((self._recs,))
+                self.fp.seek(pos)
+
+            for var in rec_vars:
+                self.variables[var].__dict__['data'] = rec_array[var]
+
+    def _read_var(self):
+        name = self._unpack_string().decode('latin1')
+        dimensions = []
+        shape = []
+        dims = self._unpack_int()
+
+        for i in range(dims):
+            dimid = self._unpack_int()
+            dimname = self._dims[dimid]
+            dimensions.append(dimname)
+            dim = self.dimensions[dimname]
+            shape.append(dim)
+        dimensions = tuple(dimensions)
+        shape = tuple(shape)
+
+        attributes = self._read_att_array()
+        nc_type = self.fp.read(4)
+        vsize = self._unpack_int()
+        begin = [self._unpack_int, self._unpack_int64][self.version_byte-1]()
+
+        typecode, size = TYPEMAP[nc_type]
+        dtype_ = f'>{typecode}'
+
+        return name, dimensions, shape, attributes, typecode, size, dtype_, begin, vsize
+
+    def _read_att_values(self):
+        nc_type = self.fp.read(4)
+        n = self._unpack_int()
+
+        typecode, size = TYPEMAP[nc_type]
+
+        count = n*size
+        values = self.fp.read(int(count))
+        self.fp.read(-count % 4)  # read padding
+
+        if typecode != 'c':
+            values = frombuffer(values, dtype=f'>{typecode}').copy()
+            if values.shape == (1,):
+                values = values[0]
+        else:
+            values = values.rstrip(b'\x00')
+        return values
+
+    def _pack_begin(self, begin):
+        if self.version_byte == 1:
+            self._pack_int(begin)
+        elif self.version_byte == 2:
+            self._pack_int64(begin)
+
+    def _pack_int(self, value):
+        self.fp.write(array(value, '>i').tobytes())
+    _pack_int32 = _pack_int
+
+    def _unpack_int(self):
+        return int(frombuffer(self.fp.read(4), '>i')[0])
+    _unpack_int32 = _unpack_int
+
+    def _pack_int64(self, value):
+        self.fp.write(array(value, '>q').tobytes())
+
+    def _unpack_int64(self):
+        return frombuffer(self.fp.read(8), '>q')[0]
+
+    def _pack_string(self, s):
+        count = len(s)
+        self._pack_int(count)
+        self.fp.write(s.encode('latin1'))
+        self.fp.write(b'\x00' * (-count % 4))  # pad
+
+    def _unpack_string(self):
+        count = self._unpack_int()
+        s = self.fp.read(count).rstrip(b'\x00')
+        self.fp.read(-count % 4)  # read padding
+        return s
+
+
+class netcdf_variable:
+    """
+    A data object for netcdf files.
+
+    `netcdf_variable` objects are constructed by calling the method
+    `netcdf_file.createVariable` on the `netcdf_file` object. `netcdf_variable`
+    objects behave much like array objects defined in numpy, except that their
+    data resides in a file. Data is read by indexing and written by assigning
+    to an indexed subset; the entire array can be accessed by the index ``[:]``
+    or (for scalars) by using the methods `getValue` and `assignValue`.
+    `netcdf_variable` objects also have attribute `shape` with the same meaning
+    as for arrays, but the shape cannot be modified. There is another read-only
+    attribute `dimensions`, whose value is the tuple of dimension names.
+
+    All other attributes correspond to variable attributes defined in
+    the NetCDF file. Variable attributes are created by assigning to an
+    attribute of the `netcdf_variable` object.
+
+    Parameters
+    ----------
+    data : array_like
+        The data array that holds the values for the variable.
+        Typically, this is initialized as empty, but with the proper shape.
+    typecode : dtype character code
+        Desired data-type for the data array.
+    size : int
+        Desired element size for the data array.
+    shape : sequence of ints
+        The shape of the array. This should match the lengths of the
+        variable's dimensions.
+    dimensions : sequence of strings
+        The names of the dimensions used by the variable. Must be in the
+        same order of the dimension lengths given by `shape`.
+    attributes : dict, optional
+        Attribute values (any type) keyed by string names. These attributes
+        become attributes for the netcdf_variable object.
+    maskandscale : bool, optional
+        Whether to automatically scale and/or mask data based on attributes.
+        Default is False.
+
+
+    Attributes
+    ----------
+    dimensions : list of str
+        List of names of dimensions used by the variable object.
+    isrec, shape
+        Properties
+
+    See also
+    --------
+    isrec, shape
+
+    Notes
+    -----
+    For a more recent version of the NetCDF standard and additional features, please
+    consider the permissively-licensed
+    `netcdf4-python <https://unidata.github.io/netcdf4-python/>`_.
+
+    """
+    def __init__(self, data, typecode, size, shape, dimensions,
+                 attributes=None,
+                 maskandscale=False):
+        self.data = data
+        self._typecode = typecode
+        self._size = size
+        self._shape = shape
+        self.dimensions = dimensions
+        self.maskandscale = maskandscale
+
+        self._attributes = attributes or {}
+        for k, v in self._attributes.items():
+            self.__dict__[k] = v
+
+    def __setattr__(self, attr, value):
+        # Store user defined attributes in a separate dict,
+        # so we can save them to file later.
+        try:
+            self._attributes[attr] = value
+        except AttributeError:
+            pass
+        self.__dict__[attr] = value
+
+    def isrec(self):
+        """Returns whether the variable has a record dimension or not.
+
+        A record dimension is a dimension along which additional data could be
+        easily appended in the netcdf data structure without much rewriting of
+        the data file. This attribute is a read-only property of the
+        `netcdf_variable`.
+
+        """
+        return bool(self.data.shape) and not self._shape[0]
+    isrec = property(isrec)
+
+    def shape(self):
+        """Returns the shape tuple of the data variable.
+
+        This is a read-only attribute and can not be modified in the
+        same manner of other numpy arrays.
+        """
+        return self.data.shape
+    shape = property(shape)
+
+    def getValue(self):
+        """
+        Retrieve a scalar value from a `netcdf_variable` of length one.
+
+        Raises
+        ------
+        ValueError
+            If the netcdf variable is an array of length greater than one,
+            this exception will be raised.
+
+        """
+        return self.data.item()
+
+    def assignValue(self, value):
+        """
+        Assign a scalar value to a `netcdf_variable` of length one.
+
+        Parameters
+        ----------
+        value : scalar
+            Scalar value (of compatible type) to assign to a length-one netcdf
+            variable. This value will be written to file.
+
+        Raises
+        ------
+        ValueError
+            If the input is not a scalar, or if the destination is not a length-one
+            netcdf variable.
+
+        """
+        if not self.data.flags.writeable:
+            # Work-around for a bug in NumPy.  Calling itemset() on a read-only
+            # memory-mapped array causes a seg. fault.
+            # See NumPy ticket #1622, and SciPy ticket #1202.
+            # This check for `writeable` can be removed when the oldest version
+            # of NumPy still supported by scipy contains the fix for #1622.
+            raise RuntimeError("variable is not writeable")
+
+        self.data[:] = value
+
+    def typecode(self):
+        """
+        Return the typecode of the variable.
+
+        Returns
+        -------
+        typecode : char
+            The character typecode of the variable (e.g., 'i' for int).
+
+        """
+        return self._typecode
+
+    def itemsize(self):
+        """
+        Return the itemsize of the variable.
+
+        Returns
+        -------
+        itemsize : int
+            The element size of the variable (e.g., 8 for float64).
+
+        """
+        return self._size
+
+    def __getitem__(self, index):
+        if not self.maskandscale:
+            return self.data[index]
+
+        data = self.data[index].copy()
+        missing_value = self._get_missing_value()
+        data = self._apply_missing_value(data, missing_value)
+        scale_factor = self._attributes.get('scale_factor')
+        add_offset = self._attributes.get('add_offset')
+        if add_offset is not None or scale_factor is not None:
+            data = data.astype(np.float64)
+        if scale_factor is not None:
+            data = data * scale_factor
+        if add_offset is not None:
+            data += add_offset
+
+        return data
+
+    def __setitem__(self, index, data):
+        if self.maskandscale:
+            missing_value = (
+                    self._get_missing_value() or
+                    getattr(data, 'fill_value', 999999))
+            self._attributes.setdefault('missing_value', missing_value)
+            self._attributes.setdefault('_FillValue', missing_value)
+            data = ((data - self._attributes.get('add_offset', 0.0)) /
+                    self._attributes.get('scale_factor', 1.0))
+            data = np.ma.asarray(data).filled(missing_value)
+            if self._typecode not in 'fd' and data.dtype.kind == 'f':
+                data = np.round(data)
+
+        # Expand data for record vars?
+        if self.isrec:
+            if isinstance(index, tuple):
+                rec_index = index[0]
+            else:
+                rec_index = index
+            if isinstance(rec_index, slice):
+                recs = (rec_index.start or 0) + len(data)
+            else:
+                recs = rec_index + 1
+            if recs > len(self.data):
+                shape = (recs,) + self._shape[1:]
+                # Resize in-place does not always work since
+                # the array might not be single-segment
+                try:
+                    self.data.resize(shape)
+                except ValueError:
+                    dtype = self.data.dtype
+                    self.__dict__['data'] = np.resize(self.data, shape).astype(dtype)
+        self.data[index] = data
+
+    def _default_encoded_fill_value(self):
+        """
+        The default encoded fill-value for this Variable's data type.
+        """
+        nc_type = REVERSE[self.typecode(), self.itemsize()]
+        return FILLMAP[nc_type]
+
+    def _get_encoded_fill_value(self):
+        """
+        Returns the encoded fill value for this variable as bytes.
+
+        This is taken from either the _FillValue attribute, or the default fill
+        value for this variable's data type.
+        """
+        if '_FillValue' in self._attributes:
+            fill_value = np.array(self._attributes['_FillValue'],
+                                  dtype=self.data.dtype).tobytes()
+            if len(fill_value) == self.itemsize():
+                return fill_value
+            else:
+                return self._default_encoded_fill_value()
+        else:
+            return self._default_encoded_fill_value()
+
+    def _get_missing_value(self):
+        """
+        Returns the value denoting "no data" for this variable.
+
+        If this variable does not have a missing/fill value, returns None.
+
+        If both _FillValue and missing_value are given, give precedence to
+        _FillValue. The netCDF standard gives special meaning to _FillValue;
+        missing_value is  just used for compatibility with old datasets.
+        """
+
+        if '_FillValue' in self._attributes:
+            missing_value = self._attributes['_FillValue']
+        elif 'missing_value' in self._attributes:
+            missing_value = self._attributes['missing_value']
+        else:
+            missing_value = None
+
+        return missing_value
+
+    @staticmethod
+    def _apply_missing_value(data, missing_value):
+        """
+        Applies the given missing value to the data array.
+
+        Returns a numpy.ma array, with any value equal to missing_value masked
+        out (unless missing_value is None, in which case the original array is
+        returned).
+        """
+
+        if missing_value is None:
+            newdata = data
+        else:
+            try:
+                missing_value_isnan = np.isnan(missing_value)
+            except (TypeError, NotImplementedError):
+                # some data types (e.g., characters) cannot be tested for NaN
+                missing_value_isnan = False
+
+            if missing_value_isnan:
+                mymask = np.isnan(data)
+            else:
+                mymask = (data == missing_value)
+
+            newdata = np.ma.masked_where(mymask, data)
+
+        return newdata
+
+
+NetCDFFile = netcdf_file
+NetCDFVariable = netcdf_variable

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/harwell_boeing.py

@@ -0,0 +1,17 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.io` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = ["hb_read", "hb_write"]  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="io", module="harwell_boeing",
+                                   private_modules=["_harwell_boeing"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/idl.py

@@ -0,0 +1,17 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.io` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = ["readsav"]  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="io", module="idl",
+                                   private_modules=["_idl"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/mmio.py

@@ -0,0 +1,17 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.io` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = ["mminfo", "mmread", "mmwrite"]  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="io", module="mmio",
+                                   private_modules=["_mmio"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/netcdf.py

@@ -0,0 +1,17 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.io` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = ["netcdf_file", "netcdf_variable"]  # noqa: F822
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="io", module="netcdf",
+                                   private_modules=["_netcdf"], all=__all__,
+                                   attribute=name)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/io/wavfile.py

@@ -0,0 +1,944 @@
+"""
+Module to read / write wav files using NumPy arrays
+
+Functions
+---------
+`read`: Return the sample rate (in samples/sec) and data from a WAV file.
+
+`write`: Write a NumPy array as a WAV file.
+
+"""
+import io
+import os
+import sys
+import numpy as np
+import struct
+import warnings
+from enum import IntEnum
+
+
+__all__ = [
+    'WavFileWarning',
+    'read',
+    'write'
+]
+
+
+class WavFileWarning(UserWarning):
+    """
+    Warning for WAV files with format issues that can still be read.
+    
+    Raised when a WAV file has problems like missing metadata or 
+    non-standard formatting, but can still be processed successfully.
+    """
+    pass
+
+
+class SeekEmulatingReader:
+    """
+    Tracks stream position, provides tell(), and emulates only those
+    seeks that can be supported by reading forward. Other seeks raise
+    io.UnsupportedOperation. Note that this class implements only the
+    minimum necessary to keep wavfile.read() happy.
+    """
+    def __init__(self, reader):
+        self.reader = reader
+        self.pos = 0
+
+    def read(self, size=-1, /):
+        data = self.reader.read(size)
+        self.pos += len(data)
+        return data
+    
+    def seek(self, offset, whence=os.SEEK_SET, /):
+        match whence:
+            case os.SEEK_SET if offset >= self.pos:
+                self.read(offset - self.pos) # convert to relative
+            case os.SEEK_CUR if offset >= 0:
+                self.read(offset) # advance by offset
+            case os.SEEK_END if offset == 0:
+                self.read() # advance to end of stream
+            case _:
+                raise io.UnsupportedOperation("SeekEmulatingReader was asked to emulate"
+                                              " a seek operation it does not support.")
+        return self.pos
+    
+    def tell(self):
+        return self.pos
+    
+    def close(self):
+        self.reader.close()
+    
+    # np.fromfile expects to be able to call flush(), and _read_data_chunk
+    # expects to catch io.UnsupportedOperation if np.fromfile fails.
+    def flush(self):
+        raise io.UnsupportedOperation("SeekEmulatingReader can't flush.")
+
+
+class WAVE_FORMAT(IntEnum):
+    """
+    WAVE form wFormatTag IDs
+
+    Complete list is in mmreg.h in Windows 10 SDK.  ALAC and OPUS are the
+    newest additions, in v10.0.14393 2016-07
+    """
+    UNKNOWN = 0x0000
+    PCM = 0x0001
+    ADPCM = 0x0002
+    IEEE_FLOAT = 0x0003
+    VSELP = 0x0004
+    IBM_CVSD = 0x0005
+    ALAW = 0x0006
+    MULAW = 0x0007
+    DTS = 0x0008
+    DRM = 0x0009
+    WMAVOICE9 = 0x000A
+    WMAVOICE10 = 0x000B
+    OKI_ADPCM = 0x0010
+    DVI_ADPCM = 0x0011
+    IMA_ADPCM = 0x0011  # Duplicate
+    MEDIASPACE_ADPCM = 0x0012
+    SIERRA_ADPCM = 0x0013
+    G723_ADPCM = 0x0014
+    DIGISTD = 0x0015
+    DIGIFIX = 0x0016
+    DIALOGIC_OKI_ADPCM = 0x0017
+    MEDIAVISION_ADPCM = 0x0018
+    CU_CODEC = 0x0019
+    HP_DYN_VOICE = 0x001A
+    YAMAHA_ADPCM = 0x0020
+    SONARC = 0x0021
+    DSPGROUP_TRUESPEECH = 0x0022
+    ECHOSC1 = 0x0023
+    AUDIOFILE_AF36 = 0x0024
+    APTX = 0x0025
+    AUDIOFILE_AF10 = 0x0026
+    PROSODY_1612 = 0x0027
+    LRC = 0x0028
+    DOLBY_AC2 = 0x0030
+    GSM610 = 0x0031
+    MSNAUDIO = 0x0032
+    ANTEX_ADPCME = 0x0033
+    CONTROL_RES_VQLPC = 0x0034
+    DIGIREAL = 0x0035
+    DIGIADPCM = 0x0036
+    CONTROL_RES_CR10 = 0x0037
+    NMS_VBXADPCM = 0x0038
+    CS_IMAADPCM = 0x0039
+    ECHOSC3 = 0x003A
+    ROCKWELL_ADPCM = 0x003B
+    ROCKWELL_DIGITALK = 0x003C
+    XEBEC = 0x003D
+    G721_ADPCM = 0x0040
+    G728_CELP = 0x0041
+    MSG723 = 0x0042
+    INTEL_G723_1 = 0x0043
+    INTEL_G729 = 0x0044
+    SHARP_G726 = 0x0045
+    MPEG = 0x0050
+    RT24 = 0x0052
+    PAC = 0x0053
+    MPEGLAYER3 = 0x0055
+    LUCENT_G723 = 0x0059
+    CIRRUS = 0x0060
+    ESPCM = 0x0061
+    VOXWARE = 0x0062
+    CANOPUS_ATRAC = 0x0063
+    G726_ADPCM = 0x0064
+    G722_ADPCM = 0x0065
+    DSAT = 0x0066
+    DSAT_DISPLAY = 0x0067
+    VOXWARE_BYTE_ALIGNED = 0x0069
+    VOXWARE_AC8 = 0x0070
+    VOXWARE_AC10 = 0x0071
+    VOXWARE_AC16 = 0x0072
+    VOXWARE_AC20 = 0x0073
+    VOXWARE_RT24 = 0x0074
+    VOXWARE_RT29 = 0x0075
+    VOXWARE_RT29HW = 0x0076
+    VOXWARE_VR12 = 0x0077
+    VOXWARE_VR18 = 0x0078
+    VOXWARE_TQ40 = 0x0079
+    VOXWARE_SC3 = 0x007A
+    VOXWARE_SC3_1 = 0x007B
+    SOFTSOUND = 0x0080
+    VOXWARE_TQ60 = 0x0081
+    MSRT24 = 0x0082
+    G729A = 0x0083
+    MVI_MVI2 = 0x0084
+    DF_G726 = 0x0085
+    DF_GSM610 = 0x0086
+    ISIAUDIO = 0x0088
+    ONLIVE = 0x0089
+    MULTITUDE_FT_SX20 = 0x008A
+    INFOCOM_ITS_G721_ADPCM = 0x008B
+    CONVEDIA_G729 = 0x008C
+    CONGRUENCY = 0x008D
+    SBC24 = 0x0091
+    DOLBY_AC3_SPDIF = 0x0092
+    MEDIASONIC_G723 = 0x0093
+    PROSODY_8KBPS = 0x0094
+    ZYXEL_ADPCM = 0x0097
+    PHILIPS_LPCBB = 0x0098
+    PACKED = 0x0099
+    MALDEN_PHONYTALK = 0x00A0
+    RACAL_RECORDER_GSM = 0x00A1
+    RACAL_RECORDER_G720_A = 0x00A2
+    RACAL_RECORDER_G723_1 = 0x00A3
+    RACAL_RECORDER_TETRA_ACELP = 0x00A4
+    NEC_AAC = 0x00B0
+    RAW_AAC1 = 0x00FF
+    RHETOREX_ADPCM = 0x0100
+    IRAT = 0x0101
+    VIVO_G723 = 0x0111
+    VIVO_SIREN = 0x0112
+    PHILIPS_CELP = 0x0120
+    PHILIPS_GRUNDIG = 0x0121
+    DIGITAL_G723 = 0x0123
+    SANYO_LD_ADPCM = 0x0125
+    SIPROLAB_ACEPLNET = 0x0130
+    SIPROLAB_ACELP4800 = 0x0131
+    SIPROLAB_ACELP8V3 = 0x0132
+    SIPROLAB_G729 = 0x0133
+    SIPROLAB_G729A = 0x0134
+    SIPROLAB_KELVIN = 0x0135
+    VOICEAGE_AMR = 0x0136
+    G726ADPCM = 0x0140
+    DICTAPHONE_CELP68 = 0x0141
+    DICTAPHONE_CELP54 = 0x0142
+    QUALCOMM_PUREVOICE = 0x0150
+    QUALCOMM_HALFRATE = 0x0151
+    TUBGSM = 0x0155
+    MSAUDIO1 = 0x0160
+    WMAUDIO2 = 0x0161
+    WMAUDIO3 = 0x0162
+    WMAUDIO_LOSSLESS = 0x0163
+    WMASPDIF = 0x0164
+    UNISYS_NAP_ADPCM = 0x0170
+    UNISYS_NAP_ULAW = 0x0171
+    UNISYS_NAP_ALAW = 0x0172
+    UNISYS_NAP_16K = 0x0173
+    SYCOM_ACM_SYC008 = 0x0174
+    SYCOM_ACM_SYC701_G726L = 0x0175
+    SYCOM_ACM_SYC701_CELP54 = 0x0176
+    SYCOM_ACM_SYC701_CELP68 = 0x0177
+    KNOWLEDGE_ADVENTURE_ADPCM = 0x0178
+    FRAUNHOFER_IIS_MPEG2_AAC = 0x0180
+    DTS_DS = 0x0190
+    CREATIVE_ADPCM = 0x0200
+    CREATIVE_FASTSPEECH8 = 0x0202
+    CREATIVE_FASTSPEECH10 = 0x0203
+    UHER_ADPCM = 0x0210
+    ULEAD_DV_AUDIO = 0x0215
+    ULEAD_DV_AUDIO_1 = 0x0216
+    QUARTERDECK = 0x0220
+    ILINK_VC = 0x0230
+    RAW_SPORT = 0x0240
+    ESST_AC3 = 0x0241
+    GENERIC_PASSTHRU = 0x0249
+    IPI_HSX = 0x0250
+    IPI_RPELP = 0x0251
+    CS2 = 0x0260
+    SONY_SCX = 0x0270
+    SONY_SCY = 0x0271
+    SONY_ATRAC3 = 0x0272
+    SONY_SPC = 0x0273
+    TELUM_AUDIO = 0x0280
+    TELUM_IA_AUDIO = 0x0281
+    NORCOM_VOICE_SYSTEMS_ADPCM = 0x0285
+    FM_TOWNS_SND = 0x0300
+    MICRONAS = 0x0350
+    MICRONAS_CELP833 = 0x0351
+    BTV_DIGITAL = 0x0400
+    INTEL_MUSIC_CODER = 0x0401
+    INDEO_AUDIO = 0x0402
+    QDESIGN_MUSIC = 0x0450
+    ON2_VP7_AUDIO = 0x0500
+    ON2_VP6_AUDIO = 0x0501
+    VME_VMPCM = 0x0680
+    TPC = 0x0681
+    LIGHTWAVE_LOSSLESS = 0x08AE
+    OLIGSM = 0x1000
+    OLIADPCM = 0x1001
+    OLICELP = 0x1002
+    OLISBC = 0x1003
+    OLIOPR = 0x1004
+    LH_CODEC = 0x1100
+    LH_CODEC_CELP = 0x1101
+    LH_CODEC_SBC8 = 0x1102
+    LH_CODEC_SBC12 = 0x1103
+    LH_CODEC_SBC16 = 0x1104
+    NORRIS = 0x1400
+    ISIAUDIO_2 = 0x1401
+    SOUNDSPACE_MUSICOMPRESS = 0x1500
+    MPEG_ADTS_AAC = 0x1600
+    MPEG_RAW_AAC = 0x1601
+    MPEG_LOAS = 0x1602
+    NOKIA_MPEG_ADTS_AAC = 0x1608
+    NOKIA_MPEG_RAW_AAC = 0x1609
+    VODAFONE_MPEG_ADTS_AAC = 0x160A
+    VODAFONE_MPEG_RAW_AAC = 0x160B
+    MPEG_HEAAC = 0x1610
+    VOXWARE_RT24_SPEECH = 0x181C
+    SONICFOUNDRY_LOSSLESS = 0x1971
+    INNINGS_TELECOM_ADPCM = 0x1979
+    LUCENT_SX8300P = 0x1C07
+    LUCENT_SX5363S = 0x1C0C
+    CUSEEME = 0x1F03
+    NTCSOFT_ALF2CM_ACM = 0x1FC4
+    DVM = 0x2000
+    DTS2 = 0x2001
+    MAKEAVIS = 0x3313
+    DIVIO_MPEG4_AAC = 0x4143
+    NOKIA_ADAPTIVE_MULTIRATE = 0x4201
+    DIVIO_G726 = 0x4243
+    LEAD_SPEECH = 0x434C
+    LEAD_VORBIS = 0x564C
+    WAVPACK_AUDIO = 0x5756
+    OGG_VORBIS_MODE_1 = 0x674F
+    OGG_VORBIS_MODE_2 = 0x6750
+    OGG_VORBIS_MODE_3 = 0x6751
+    OGG_VORBIS_MODE_1_PLUS = 0x676F
+    OGG_VORBIS_MODE_2_PLUS = 0x6770
+    OGG_VORBIS_MODE_3_PLUS = 0x6771
+    ALAC = 0x6C61
+    _3COM_NBX = 0x7000  # Can't have leading digit
+    OPUS = 0x704F
+    FAAD_AAC = 0x706D
+    AMR_NB = 0x7361
+    AMR_WB = 0x7362
+    AMR_WP = 0x7363
+    GSM_AMR_CBR = 0x7A21
+    GSM_AMR_VBR_SID = 0x7A22
+    COMVERSE_INFOSYS_G723_1 = 0xA100
+    COMVERSE_INFOSYS_AVQSBC = 0xA101
+    COMVERSE_INFOSYS_SBC = 0xA102
+    SYMBOL_G729_A = 0xA103
+    VOICEAGE_AMR_WB = 0xA104
+    INGENIENT_G726 = 0xA105
+    MPEG4_AAC = 0xA106
+    ENCORE_G726 = 0xA107
+    ZOLL_ASAO = 0xA108
+    SPEEX_VOICE = 0xA109
+    VIANIX_MASC = 0xA10A
+    WM9_SPECTRUM_ANALYZER = 0xA10B
+    WMF_SPECTRUM_ANAYZER = 0xA10C
+    GSM_610 = 0xA10D
+    GSM_620 = 0xA10E
+    GSM_660 = 0xA10F
+    GSM_690 = 0xA110
+    GSM_ADAPTIVE_MULTIRATE_WB = 0xA111
+    POLYCOM_G722 = 0xA112
+    POLYCOM_G728 = 0xA113
+    POLYCOM_G729_A = 0xA114
+    POLYCOM_SIREN = 0xA115
+    GLOBAL_IP_ILBC = 0xA116
+    RADIOTIME_TIME_SHIFT_RADIO = 0xA117
+    NICE_ACA = 0xA118
+    NICE_ADPCM = 0xA119
+    VOCORD_G721 = 0xA11A
+    VOCORD_G726 = 0xA11B
+    VOCORD_G722_1 = 0xA11C
+    VOCORD_G728 = 0xA11D
+    VOCORD_G729 = 0xA11E
+    VOCORD_G729_A = 0xA11F
+    VOCORD_G723_1 = 0xA120
+    VOCORD_LBC = 0xA121
+    NICE_G728 = 0xA122
+    FRACE_TELECOM_G729 = 0xA123
+    CODIAN = 0xA124
+    FLAC = 0xF1AC
+    EXTENSIBLE = 0xFFFE
+    DEVELOPMENT = 0xFFFF
+
+
+KNOWN_WAVE_FORMATS = {WAVE_FORMAT.PCM, WAVE_FORMAT.IEEE_FLOAT}
+
+
+def _raise_bad_format(format_tag):
+    try:
+        format_name = WAVE_FORMAT(format_tag).name
+    except ValueError:
+        format_name = f'{format_tag:#06x}'
+    raise ValueError(f"Unknown wave file format: {format_name}. Supported "
+                     "formats: " +
+                     ', '.join(x.name for x in KNOWN_WAVE_FORMATS))
+
+
+def _read_fmt_chunk(fid, is_big_endian):
+    """
+    Returns
+    -------
+    size : int
+        size of format subchunk in bytes (minus 8 for "fmt " and itself)
+    format_tag : int
+        PCM, float, or compressed format
+    channels : int
+        number of channels
+    fs : int
+        sampling frequency in samples per second
+    bytes_per_second : int
+        overall byte rate for the file
+    block_align : int
+        bytes per sample, including all channels
+    bit_depth : int
+        bits per sample
+
+    Notes
+    -----
+    Assumes file pointer is immediately after the 'fmt ' id
+    """
+    if is_big_endian:
+        fmt = '>'
+    else:
+        fmt = '<'
+
+    size = struct.unpack(fmt+'I', fid.read(4))[0]
+
+    if size < 16:
+        raise ValueError("Binary structure of wave file is not compliant")
+
+    res = struct.unpack(fmt+'HHIIHH', fid.read(16))
+    bytes_read = 16
+
+    format_tag, channels, fs, bytes_per_second, block_align, bit_depth = res
+
+    if format_tag == WAVE_FORMAT.EXTENSIBLE and size >= (16+2):
+        ext_chunk_size = struct.unpack(fmt+'H', fid.read(2))[0]
+        bytes_read += 2
+        if ext_chunk_size >= 22:
+            extensible_chunk_data = fid.read(22)
+            bytes_read += 22
+            raw_guid = extensible_chunk_data[2+4:2+4+16]
+            # GUID template {XXXXXXXX-0000-0010-8000-00AA00389B71} (RFC-2361)
+            # MS GUID byte order: first three groups are native byte order,
+            # rest is Big Endian
+            if is_big_endian:
+                tail = b'\x00\x00\x00\x10\x80\x00\x00\xAA\x00\x38\x9B\x71'
+            else:
+                tail = b'\x00\x00\x10\x00\x80\x00\x00\xAA\x00\x38\x9B\x71'
+            if raw_guid.endswith(tail):
+                format_tag = struct.unpack(fmt+'I', raw_guid[:4])[0]
+        else:
+            raise ValueError("Binary structure of wave file is not compliant")
+
+    if format_tag not in KNOWN_WAVE_FORMATS:
+        _raise_bad_format(format_tag)
+
+    # move file pointer to next chunk
+    if size > bytes_read:
+        fid.read(size - bytes_read)
+
+    # fmt should always be 16, 18 or 40, but handle it just in case
+    _handle_pad_byte(fid, size)
+
+    if format_tag == WAVE_FORMAT.PCM:
+        if bytes_per_second != fs * block_align:
+            raise ValueError("WAV header is invalid: nAvgBytesPerSec must"
+                             " equal product of nSamplesPerSec and"
+                             " nBlockAlign, but file has nSamplesPerSec ="
+                             f" {fs}, nBlockAlign = {block_align}, and"
+                             f" nAvgBytesPerSec = {bytes_per_second}")
+
+    return (size, format_tag, channels, fs, bytes_per_second, block_align,
+            bit_depth)
+
+
+def _read_data_chunk(fid, format_tag, channels, bit_depth, is_big_endian, is_rf64,
+                     block_align, mmap=False, rf64_chunk_size=None):
+    """
+    Notes
+    -----
+    Assumes file pointer is immediately after the 'data' id
+
+    It's possible to not use all available bits in a container, or to store
+    samples in a container bigger than necessary, so bytes_per_sample uses
+    the actual reported container size (nBlockAlign / nChannels).  Real-world
+    examples:
+
+    Adobe Audition's "24-bit packed int (type 1, 20-bit)"
+
+        nChannels = 2, nBlockAlign = 6, wBitsPerSample = 20
+
+    http://www-mmsp.ece.mcgill.ca/Documents/AudioFormats/WAVE/Samples/AFsp/M1F1-int12-AFsp.wav
+    is:
+
+        nChannels = 2, nBlockAlign = 4, wBitsPerSample = 12
+
+    http://www-mmsp.ece.mcgill.ca/Documents/AudioFormats/WAVE/Docs/multichaudP.pdf
+    gives an example of:
+
+        nChannels = 2, nBlockAlign = 8, wBitsPerSample = 20
+    """
+    if is_big_endian:
+        fmt = '>'
+    else:
+        fmt = '<'
+
+    # Size of the data subchunk in bytes
+    if not is_rf64:
+        size = struct.unpack(fmt+'I', fid.read(4))[0]
+    else:
+        # chunk size is stored in global file header for RF64
+        size = rf64_chunk_size
+        # skip data chunk size as it is 0xFFFFFFF
+        fid.read(4)
+
+    # Number of bytes per sample (sample container size)
+    bytes_per_sample = block_align // channels
+    n_samples = size // bytes_per_sample
+
+    if format_tag == WAVE_FORMAT.PCM:
+        if 1 <= bit_depth <= 8:
+            dtype = 'u1'  # WAV of 8-bit integer or less are unsigned
+        elif bytes_per_sample in {3, 5, 6, 7}:
+            # No compatible dtype.  Load as raw bytes for reshaping later.
+            dtype = 'V1'
+        elif bit_depth <= 64:
+            # Remaining bit depths can map directly to signed numpy dtypes
+            dtype = f'{fmt}i{bytes_per_sample}'
+        else:
+            raise ValueError("Unsupported bit depth: the WAV file "
+                             f"has {bit_depth}-bit integer data.")
+    elif format_tag == WAVE_FORMAT.IEEE_FLOAT:
+        if bit_depth in {32, 64}:
+            dtype = f'{fmt}f{bytes_per_sample}'
+        else:
+            raise ValueError("Unsupported bit depth: the WAV file "
+                             f"has {bit_depth}-bit floating-point data.")
+    else:
+        _raise_bad_format(format_tag)
+
+    start = fid.tell()
+    if not mmap:
+        try:
+            count = size if dtype == 'V1' else n_samples
+            data = np.fromfile(fid, dtype=dtype, count=count)
+        except io.UnsupportedOperation:  # not a C-like file
+            fid.seek(start, 0)  # just in case it seeked, though it shouldn't
+            data = np.frombuffer(fid.read(size), dtype=dtype)
+
+        if dtype == 'V1':
+            # Rearrange raw bytes into smallest compatible numpy dtype
+            dt = f'{fmt}i4' if bytes_per_sample == 3 else f'{fmt}i8'
+            a = np.zeros((len(data) // bytes_per_sample, np.dtype(dt).itemsize),
+                            dtype='V1')
+            if is_big_endian:
+                a[:, :bytes_per_sample] = data.reshape((-1, bytes_per_sample))
+            else:
+                a[:, -bytes_per_sample:] = data.reshape((-1, bytes_per_sample))
+            data = a.view(dt).reshape(a.shape[:-1])
+    else:
+        if bytes_per_sample in {1, 2, 4, 8}:
+            start = fid.tell()
+            data = np.memmap(fid, dtype=dtype, mode='c', offset=start,
+                                shape=(n_samples,))
+            fid.seek(start + size)
+        else:
+            raise ValueError("mmap=True not compatible with "
+                             f"{bytes_per_sample}-byte container size.")
+
+    _handle_pad_byte(fid, size)
+
+    if channels > 1:
+        data = data.reshape(-1, channels)
+    return data
+
+
+def _skip_unknown_chunk(fid, is_big_endian):
+    if is_big_endian:
+        fmt = '>I'
+    else:
+        fmt = '<I'
+
+    data = fid.read(4)
+    # call unpack() and seek() only if we have really read data from file
+    # otherwise empty read at the end of the file would trigger
+    # unnecessary exception at unpack() call
+    # in case data equals somehow to 0, there is no need for seek() anyway
+    if data:
+        size = struct.unpack(fmt, data)[0]
+        fid.seek(size, 1)
+        _handle_pad_byte(fid, size)
+
+
+def _read_riff_chunk(fid):
+    str1 = fid.read(4)  # File signature
+    if str1 == b'RIFF':
+        is_rf64 = False
+        is_big_endian = False
+        fmt = '<I'
+    elif str1 == b'RIFX':
+        is_rf64 = False
+        is_big_endian = True
+        fmt = '>I'
+    elif str1 == b'RF64':
+        is_rf64 = True
+        is_big_endian = False
+        fmt = '<Q'
+    else:
+        # There are also .wav files with "FFIR" or "XFIR" signatures?
+        raise ValueError(f"File format {repr(str1)} not understood. Only "
+                         "'RIFF', 'RIFX', and 'RF64' supported.")
+    # Size of entire file
+    if not is_rf64:
+        file_size = struct.unpack(fmt, fid.read(4))[0] + 8
+        rf64_chunk_size = None
+        str2 = fid.read(4)
+    else:
+        # Skip 0xFFFFFFFF (-1) bytes
+        fid.read(4)
+        str2 = fid.read(4)
+        str3 = fid.read(4)
+        if str3 != b'ds64':
+            raise ValueError("Invalid RF64 file: ds64 chunk not found.")
+        ds64_size = struct.unpack("<I", fid.read(4))[0]
+        file_size = struct.unpack(fmt, fid.read(8))[0] + 8
+        rf64_chunk_size = struct.unpack('<Q', fid.read(8))[0]
+        # Ignore additional attributes of ds64 chunk like sample count, tables, etc.
+        # and just skip to the next chunk
+        fid.seek(ds64_size - 16, 1)
+
+    if str2 != b'WAVE':
+        raise ValueError(f"Not a WAV file. RIFF form type is {repr(str2)}.")
+
+    return file_size, is_big_endian, is_rf64, rf64_chunk_size
+
+
+def _handle_pad_byte(fid, size):
+    # "If the chunk size is an odd number of bytes, a pad byte with value zero
+    # is written after ckData." So we need to seek past this after each chunk.
+    if size % 2:
+        fid.seek(1, 1)
+
+
+def read(filename, mmap=False):
+    """
+    Open a WAV file.
+
+    Return the sample rate (in samples/sec) and data from an LPCM WAV file.
+
+    Parameters
+    ----------
+    filename : string or open file handle
+        Input WAV file.
+    mmap : bool, optional
+        Whether to read data as memory-mapped (default: False).  Not compatible
+        with some bit depths; see Notes.  Only to be used on real files.
+
+        .. versionadded:: 0.12.0
+
+    Returns
+    -------
+    rate : int
+        Sample rate of WAV file.
+    data : numpy array
+        Data read from WAV file. Data-type is determined from the file;
+        see Notes.  Data is 1-D for 1-channel WAV, or 2-D of shape
+        (Nsamples, Nchannels) otherwise. If a file-like input without a
+        C-like file descriptor (e.g., :class:`python:io.BytesIO`) is
+        passed, this will not be writeable.
+
+    Notes
+    -----
+    Common data types: [1]_
+
+    =====================  ===========  ===========  =============
+         WAV format            Min          Max       NumPy dtype
+    =====================  ===========  ===========  =============
+    32-bit floating-point  -1.0         +1.0         float32
+    32-bit integer PCM     -2147483648  +2147483647  int32
+    24-bit integer PCM     -2147483648  +2147483392  int32
+    16-bit integer PCM     -32768       +32767       int16
+    8-bit integer PCM      0            255          uint8
+    =====================  ===========  ===========  =============
+
+    WAV files can specify arbitrary bit depth, and this function supports
+    reading any integer PCM depth from 1 to 64 bits.  Data is returned in the
+    smallest compatible numpy int type, in left-justified format.  8-bit and
+    lower is unsigned, while 9-bit and higher is signed.
+
+    For example, 24-bit data will be stored as int32, with the MSB of the
+    24-bit data stored at the MSB of the int32, and typically the least
+    significant byte is 0x00.  (However, if a file actually contains data past
+    its specified bit depth, those bits will be read and output, too. [2]_)
+
+    This bit justification and sign matches WAV's native internal format, which
+    allows memory mapping of WAV files that use 1, 2, 4, or 8 bytes per sample
+    (so 24-bit files cannot be memory-mapped, but 32-bit can).
+
+    IEEE float PCM in 32- or 64-bit format is supported, with or without mmap.
+    Values exceeding [-1, +1] are not clipped.
+
+    Non-linear PCM (mu-law, A-law) is not supported.
+
+    References
+    ----------
+    .. [1] IBM Corporation and Microsoft Corporation, "Multimedia Programming
+       Interface and Data Specifications 1.0", section "Data Format of the
+       Samples", August 1991
+       http://www.tactilemedia.com/info/MCI_Control_Info.html
+    .. [2] Adobe Systems Incorporated, "Adobe Audition 3 User Guide", section
+       "Audio file formats: 24-bit Packed Int (type 1, 20-bit)", 2007
+
+    Examples
+    --------
+    >>> from os.path import dirname, join as pjoin
+    >>> from scipy.io import wavfile
+    >>> import scipy.io
+
+    Get the filename for an example .wav file from the tests/data directory.
+
+    >>> data_dir = pjoin(dirname(scipy.io.__file__), 'tests', 'data')
+    >>> wav_fname = pjoin(data_dir, 'test-44100Hz-2ch-32bit-float-be.wav')
+
+    Load the .wav file contents.
+
+    >>> samplerate, data = wavfile.read(wav_fname)
+    >>> print(f"number of channels = {data.shape[1]}")
+    number of channels = 2
+    >>> length = data.shape[0] / samplerate
+    >>> print(f"length = {length}s")
+    length = 0.01s
+
+    Plot the waveform.
+
+    >>> import matplotlib.pyplot as plt
+    >>> import numpy as np
+    >>> time = np.linspace(0., length, data.shape[0])
+    >>> plt.plot(time, data[:, 0], label="Left channel")
+    >>> plt.plot(time, data[:, 1], label="Right channel")
+    >>> plt.legend()
+    >>> plt.xlabel("Time [s]")
+    >>> plt.ylabel("Amplitude")
+    >>> plt.show()
+
+    """
+    if hasattr(filename, 'read'):
+        fid = filename
+        mmap = False
+    else:
+        fid = open(filename, 'rb')
+    
+    if not (was_seekable := fid.seekable()):
+        fid = SeekEmulatingReader(fid)
+
+    try:
+        file_size, is_big_endian, is_rf64, rf64_chunk_size = _read_riff_chunk(fid)
+        fmt_chunk_received = False
+        data_chunk_received = False
+        while fid.tell() < file_size:
+            # read the next chunk
+            chunk_id = fid.read(4)
+
+            if not chunk_id:
+                if data_chunk_received:
+                    # End of file but data successfully read
+                    warnings.warn(
+                        f"Reached EOF prematurely; finished at {fid.tell():d} bytes, "
+                        f"expected {file_size:d} bytes from header.",
+                        WavFileWarning, stacklevel=2)
+                    break
+                else:
+                    raise ValueError("Unexpected end of file.")
+            elif len(chunk_id) < 4:
+                msg = f"Incomplete chunk ID: {repr(chunk_id)}"
+                # If we have the data, ignore the broken chunk
+                if fmt_chunk_received and data_chunk_received:
+                    warnings.warn(msg + ", ignoring it.", WavFileWarning,
+                                  stacklevel=2)
+                else:
+                    raise ValueError(msg)
+
+            if chunk_id == b'fmt ':
+                fmt_chunk_received = True
+                fmt_chunk = _read_fmt_chunk(fid, is_big_endian)
+                format_tag, channels, fs = fmt_chunk[1:4]
+                bit_depth = fmt_chunk[6]
+                block_align = fmt_chunk[5]
+            elif chunk_id == b'fact':
+                _skip_unknown_chunk(fid, is_big_endian)
+            elif chunk_id == b'data':
+                data_chunk_received = True
+                if not fmt_chunk_received:
+                    raise ValueError("No fmt chunk before data")
+                data = _read_data_chunk(fid, format_tag, channels, bit_depth,
+                                        is_big_endian, is_rf64, block_align,
+                                        mmap, rf64_chunk_size)
+            elif chunk_id == b'LIST':
+                # Someday this could be handled properly but for now skip it
+                _skip_unknown_chunk(fid, is_big_endian)
+            elif chunk_id in {b'JUNK', b'Fake'}:
+                # Skip alignment chunks without warning
+                _skip_unknown_chunk(fid, is_big_endian)
+            else:
+                warnings.warn("Chunk (non-data) not understood, skipping it.",
+                              WavFileWarning, stacklevel=2)
+                _skip_unknown_chunk(fid, is_big_endian)
+    finally:
+        if not hasattr(filename, 'read'):
+            fid.close()
+        elif was_seekable:
+            # Rewind, if we are able, so that caller can do something
+            # else with the raw WAV stream.
+            fid.seek(0)
+
+    return fs, data
+
+
+def write(filename, rate, data):
+    """
+    Write a NumPy array as a WAV file.
+
+    Parameters
+    ----------
+    filename : string or open file handle
+        Output wav file.
+    rate : int
+        The sample rate (in samples/sec).
+    data : ndarray
+        A 1-D or 2-D NumPy array of either integer or float data-type.
+
+    Notes
+    -----
+    * Writes a simple uncompressed WAV file.
+    * To write multiple-channels, use a 2-D array of shape
+      (Nsamples, Nchannels).
+    * The bits-per-sample and PCM/float will be determined by the data-type.
+
+    Common data types: [1]_
+
+    =====================  ===========  ===========  =============
+         WAV format            Min          Max       NumPy dtype
+    =====================  ===========  ===========  =============
+    32-bit floating-point  -1.0         +1.0         float32
+    32-bit PCM             -2147483648  +2147483647  int32
+    16-bit PCM             -32768       +32767       int16
+    8-bit PCM              0            255          uint8
+    =====================  ===========  ===========  =============
+
+    Note that 8-bit PCM is unsigned.
+
+    References
+    ----------
+    .. [1] IBM Corporation and Microsoft Corporation, "Multimedia Programming
+       Interface and Data Specifications 1.0", section "Data Format of the
+       Samples", August 1991
+       http://www.tactilemedia.com/info/MCI_Control_Info.html
+
+    Examples
+    --------
+    Create a 100Hz sine wave, sampled at 44100Hz.
+    Write to 16-bit PCM, Mono.
+
+    >>> from scipy.io.wavfile import write
+    >>> import numpy as np
+    >>> samplerate = 44100; fs = 100
+    >>> t = np.linspace(0., 1., samplerate)
+    >>> amplitude = np.iinfo(np.int16).max
+    >>> data = amplitude * np.sin(2. * np.pi * fs * t)
+    >>> write("example.wav", samplerate, data.astype(np.int16))
+
+    """
+    if hasattr(filename, 'write'):
+        fid = filename
+    else:
+        fid = open(filename, 'wb')
+
+    fs = rate
+
+    try:
+        dkind = data.dtype.kind
+        allowed_dtypes = ['float32', 'float64',
+                          'uint8', 'int16', 'int32', 'int64']
+        if data.dtype.name not in allowed_dtypes:
+            raise ValueError(f"Unsupported data type '{data.dtype}'")
+
+        header_data = b''
+
+        header_data += b'RIFF'
+        header_data += b'\x00\x00\x00\x00'
+        header_data += b'WAVE'
+
+        # fmt chunk
+        header_data += b'fmt '
+        if dkind == 'f':
+            format_tag = WAVE_FORMAT.IEEE_FLOAT
+        else:
+            format_tag = WAVE_FORMAT.PCM
+        if data.ndim == 1:
+            channels = 1
+        else:
+            channels = data.shape[1]
+        bit_depth = data.dtype.itemsize * 8
+        bytes_per_second = fs*(bit_depth // 8)*channels
+        block_align = channels * (bit_depth // 8)
+
+        fmt_chunk_data = struct.pack('<HHIIHH', format_tag, channels, fs,
+                                     bytes_per_second, block_align, bit_depth)
+        if not (dkind == 'i' or dkind == 'u'):
+            # add cbSize field for non-PCM files
+            fmt_chunk_data += b'\x00\x00'
+
+        header_data += struct.pack('<I', len(fmt_chunk_data))
+        header_data += fmt_chunk_data
+
+        # check data size (needs to be immediately before the data chunk)
+        # if too large for standard RIFF, use RF64 instead
+        resulting_file_size = len(header_data) + 4 + 4 + data.nbytes
+        is_rf64 = (resulting_file_size - 8) > 0xFFFFFFFF
+        if is_rf64:
+            header_data = b''
+            header_data += b'RF64'
+            header_data += b'\xFF\xFF\xFF\xFF'
+            header_data += b'WAVE'
+            header_data += b'ds64'
+            # size of ds64 chunk
+            header_data += struct.pack('<I', 28)
+            # will be filled later with real file size
+            header_data += struct.pack('<Q', 0)
+            header_data += struct.pack('<Q', data.nbytes)
+            header_data += struct.pack('<Q', data.shape[0])
+            # ignore 'table' field for now
+            header_data += struct.pack('<I', 0)
+            header_data += b'fmt '
+            header_data += struct.pack('<I', len(fmt_chunk_data))
+            header_data += fmt_chunk_data
+
+        # fact chunk (non-PCM files)
+        if not (dkind == 'i' or dkind == 'u'):
+            header_data += b'fact'
+            header_data += struct.pack('<II', 4, data.shape[0])
+
+        fid.write(header_data)
+
+        # data chunk
+        fid.write(b'data')
+        # write data chunk size, unless its too big in which case 0xFFFFFFFF is written
+        fid.write(struct.pack('<I', min(data.nbytes, 4294967295)))
+
+        if data.dtype.byteorder == '>' or (data.dtype.byteorder == '=' and
+                                           sys.byteorder == 'big'):
+            data = data.byteswap()
+        _array_tofile(fid, data)
+
+        # Determine file size and place it in correct
+        # position at start of the file or the data chunk.
+        size = fid.tell()
+        if not is_rf64:
+            fid.seek(4)
+            fid.write(struct.pack('<I', size-8))
+        else:
+            fid.seek(20)
+            fid.write(struct.pack('<Q', size-8))
+
+    finally:
+        if not hasattr(filename, 'write'):
+            fid.close()
+        else:
+            fid.seek(0)
+
+
+def _array_tofile(fid, data):
+    # ravel gives a c-contiguous buffer
+    fid.write(data.ravel().view('b').data)

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/linalg/__init__.pxd

@@ -0,0 +1 @@
+from scipy.linalg cimport cython_blas, cython_lapack

data/conda_envs/evalclaw/lib/python3.11/site-packages/scipy/linalg/__init__.py

@@ -0,0 +1,234 @@
+"""
+====================================
+Linear algebra (:mod:`scipy.linalg`)
+====================================
+
+.. currentmodule:: scipy.linalg
+
+.. toctree::
+   :hidden:
+
+   linalg.blas
+   linalg.cython_blas
+   linalg.cython_lapack
+   linalg.interpolative
+   linalg.lapack
+
+Linear algebra functions.
+
+.. eventually, we should replace the numpy.linalg HTML link with just `numpy.linalg`
+
+.. seealso::
+
+   `numpy.linalg <https://www.numpy.org/devdocs/reference/routines.linalg.html>`__
+   for more linear algebra functions. Note that identically named
+   functions from `scipy.linalg` may offer more or slightly differing
+   functionality.
+
+
+Basics
+======
+
+.. autosummary::
+   :toctree: generated/
+
+   inv - Find the inverse of a square matrix
+   solve - Solve a linear system of equations
+   solve_banded - Solve a banded linear system
+   solveh_banded - Solve a Hermitian or symmetric banded system
+   solve_circulant - Solve a circulant system
+   solve_triangular - Solve a triangular matrix
+   solve_toeplitz - Solve a toeplitz matrix
+   matmul_toeplitz - Multiply a Toeplitz matrix with an array.
+   det - Find the determinant of a square matrix
+   norm - Matrix and vector norm
+   lstsq - Solve a linear least-squares problem
+   pinv - Pseudo-inverse (Moore-Penrose) using lstsq
+   pinvh - Pseudo-inverse of hermitian matrix
+   khatri_rao - Khatri-Rao product of two arrays
+   orthogonal_procrustes - Solve an orthogonal Procrustes problem
+   matrix_balance - Balance matrix entries with a similarity transformation
+   subspace_angles - Compute the subspace angles between two matrices
+   bandwidth - Return the lower and upper bandwidth of an array
+   issymmetric - Check if a square 2D array is symmetric
+   ishermitian - Check if a square 2D array is Hermitian
+   LinAlgError
+   LinAlgWarning
+
+Eigenvalue Problems
+===================
+
+.. autosummary::
+   :toctree: generated/
+
+   eig - Find the eigenvalues and eigenvectors of a square matrix
+   eigvals - Find just the eigenvalues of a square matrix
+   eigh - Find the e-vals and e-vectors of a Hermitian or symmetric matrix
+   eigvalsh - Find just the eigenvalues of a Hermitian or symmetric matrix
+   eig_banded - Find the eigenvalues and eigenvectors of a banded matrix
+   eigvals_banded - Find just the eigenvalues of a banded matrix
+   eigh_tridiagonal - Find the eigenvalues and eigenvectors of a tridiagonal matrix
+   eigvalsh_tridiagonal - Find just the eigenvalues of a tridiagonal matrix
+
+Decompositions
+==============
+
+.. autosummary::
+   :toctree: generated/
+
+   lu - LU decomposition of a matrix
+   lu_factor - LU decomposition returning unordered matrix and pivots
+   lu_solve - Solve Ax=b using back substitution with output of lu_factor
+   svd - Singular value decomposition of a matrix
+   svdvals - Singular values of a matrix
+   diagsvd - Construct matrix of singular values from output of svd
+   orth - Construct orthonormal basis for the range of A using svd
+   null_space - Construct orthonormal basis for the null space of A using svd
+   ldl - LDL.T decomposition of a Hermitian or a symmetric matrix.
+   cholesky - Cholesky decomposition of a matrix
+   cholesky_banded - Cholesky decomp. of a sym. or Hermitian banded matrix
+   cho_factor - Cholesky decomposition for use in solving a linear system
+   cho_solve - Solve previously factored linear system
+   cho_solve_banded - Solve previously factored banded linear system
+   polar - Compute the polar decomposition.
+   qr - QR decomposition of a matrix
+   qr_multiply - QR decomposition and multiplication by Q
+   qr_update - Rank k QR update
+   qr_delete - QR downdate on row or column deletion
+   qr_insert - QR update on row or column insertion
+   rq - RQ decomposition of a matrix
+   qz - QZ decomposition of a pair of matrices
+   ordqz - QZ decomposition of a pair of matrices with reordering
+   schur - Schur decomposition of a matrix
+   rsf2csf - Real to complex Schur form
+   hessenberg - Hessenberg form of a matrix
+   cdf2rdf - Complex diagonal form to real diagonal block form
+   cossin - Cosine sine decomposition of a unitary or orthogonal matrix
+
+.. seealso::
+
+   `scipy.linalg.interpolative` -- Interpolative matrix decompositions
+
+
+Matrix Functions
+================
+
+.. autosummary::
+   :toctree: generated/
+
+   expm - Matrix exponential
+   logm - Matrix logarithm
+   cosm - Matrix cosine
+   sinm - Matrix sine
+   tanm - Matrix tangent
+   coshm - Matrix hyperbolic cosine
+   sinhm - Matrix hyperbolic sine
+   tanhm - Matrix hyperbolic tangent
+   signm - Matrix sign
+   sqrtm - Matrix square root
+   funm - Evaluating an arbitrary matrix function
+   expm_frechet - Frechet derivative of the matrix exponential
+   expm_cond - Relative condition number of expm in the Frobenius norm
+   fractional_matrix_power - Fractional matrix power
+
+
+Matrix Equation Solvers
+=======================
+
+.. autosummary::
+   :toctree: generated/
+
+   solve_sylvester - Solve the Sylvester matrix equation
+   solve_continuous_are - Solve the continuous-time algebraic Riccati equation
+   solve_discrete_are - Solve the discrete-time algebraic Riccati equation
+   solve_continuous_lyapunov - Solve the continuous-time Lyapunov equation
+   solve_discrete_lyapunov - Solve the discrete-time Lyapunov equation
+
+
+Sketches and Random Projections
+===============================
+
+.. autosummary::
+   :toctree: generated/
+
+   clarkson_woodruff_transform - Applies the Clarkson Woodruff Sketch (a.k.a CountMin Sketch)
+
+Special Matrices
+================
+
+.. autosummary::
+   :toctree: generated/
+
+   block_diag - Construct a block diagonal matrix from submatrices
+   circulant - Circulant matrix
+   companion - Companion matrix
+   convolution_matrix - Convolution matrix
+   dft - Discrete Fourier transform matrix
+   fiedler - Fiedler matrix
+   fiedler_companion - Fiedler companion matrix
+   hadamard - Hadamard matrix of order 2**n
+   hankel - Hankel matrix
+   helmert - Helmert matrix
+   hilbert - Hilbert matrix
+   invhilbert - Inverse Hilbert matrix
+   leslie - Leslie matrix
+   pascal - Pascal matrix
+   invpascal - Inverse Pascal matrix
+   toeplitz - Toeplitz matrix
+
+Low-level routines
+==================
+
+.. autosummary::
+   :toctree: generated/
+
+   get_blas_funcs
+   get_lapack_funcs
+   find_best_blas_type
+
+.. seealso::
+
+   `scipy.linalg.blas` -- Low-level BLAS functions
+
+   `scipy.linalg.lapack` -- Low-level LAPACK functions
+
+   `scipy.linalg.cython_blas` -- Low-level BLAS functions for Cython
+
+   `scipy.linalg.cython_lapack` -- Low-level LAPACK functions for Cython
+
+"""  # noqa: E501
+
+from ._misc import *
+from ._cythonized_array_utils import *
+from ._basic import *
+from ._decomp import *
+from ._decomp_lu import *
+from ._decomp_ldl import *
+from ._decomp_cholesky import *
+from ._decomp_qr import *
+from ._decomp_qz import *
+from ._decomp_svd import *
+from ._decomp_schur import *
+from ._decomp_polar import *
+from ._matfuncs import *
+from .blas import *
+from .lapack import *
+from ._special_matrices import *
+from ._solvers import *
+from ._procrustes import *
+from ._decomp_update import *
+from ._sketches import *
+from ._decomp_cossin import *
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import (
+    decomp, decomp_cholesky, decomp_lu, decomp_qr, decomp_svd, decomp_schur,
+    basic, misc, special_matrices, matfuncs,
+)
+
+__all__ = [s for s in dir() if not s.startswith('_')]
+
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester