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import logging
from typing import Optional
import numpy as np
import numpy.typing as npt
from scipy.optimize import curve_fit
logger = logging.getLogger(__name__)
class EnvelopeMixin:
"""Mixin for Gaussian envelope generation, fitting, and peak symmetry analysis."""
def smooth_gaussian_pattern(self, barip: list[list], fwhm: float, num_points_per_fwhm: int = 100) -> list[list]:
"""
Generate smooth Gaussian isotope pattern with guaranteed high resolution sampling.
Args:
barip: Bar isotope pattern [[mz_values], [intensities]]
fwhm: Full width at half maximum
num_points_per_fwhm: Number of sampling points per FWHM (default: 100 for very smooth curves)
Returns:
[[mz_values], [intensities]] - smoothed Gaussian pattern
"""
if not barip or len(barip[0]) == 0:
return [[], []]
mz_bar = np.array(barip[0])
int_bar = np.array(barip[1])
# Define m/z range: extend ±3*FWHM from min/max peaks (covers 99.7% of Gaussian)
mz_min = np.min(mz_bar) - 3 * fwhm
mz_max = np.max(mz_bar) + 3 * fwhm
# Calculate step size for smooth curve: FWHM / num_points_per_fwhm
step = fwhm / num_points_per_fwhm
# Generate high-resolution m/z grid
mz_grid = np.arange(mz_min, mz_max + step, step)
intensity_grid = np.zeros_like(mz_grid)
# Sigma (standard deviation) from FWHM: FWHM = 2.355 * sigma
sigma = fwhm / 2.355
# Sum Gaussian peaks for each isotope
for center_mz, height in zip(mz_bar, int_bar):
# Generate normalized Gaussian: exp(-(x-center)^2 / (2*sigma^2))
gaussian_contrib = np.exp(-0.5 * ((mz_grid - center_mz) / sigma) ** 2)
# Scale by height
intensity_grid += gaussian_contrib * height
# Normalize to 100
if np.max(intensity_grid) > 0:
intensity_grid = (intensity_grid / np.max(intensity_grid)) * 100.0
return [mz_grid.tolist(), intensity_grid.tolist()]
def calculate_peak_symmetry(
self,
mz_values: npt.NDArray[np.float64],
intensity_values: npt.NDArray[np.float64],
center_mz: float,
window: float = 2.0,
) -> dict:
"""
Calculate symmetry of a peak around its center.
Returns symmetry score (0-1, where 1 is perfectly symmetric)
and skewness indicator.
A symmetric peak suggests a clean, single species (like a nanocluster).
An asymmetric peak may indicate fragmentation, impurities, or overlapping peaks.
"""
# Extract region around peak
mask = (mz_values >= center_mz - window) & (mz_values <= center_mz + window)
region_mz = mz_values[mask]
region_int = intensity_values[mask]
if len(region_mz) < 5:
return {'symmetry_score': 0.0, 'skewness': 0.0, 'is_symmetric': False, 'note': 'Insufficient data points'}
# Find peak apex
max_idx = np.argmax(region_int)
apex_mz = region_mz[max_idx]
max_intensity = region_int[max_idx]
# Divide into left and right sides from apex
left_mz = region_mz[: max_idx + 1]
left_int = region_int[: max_idx + 1]
right_mz = region_mz[max_idx:]
right_int = region_int[max_idx:]
if len(left_mz) < 2 or len(right_mz) < 2:
return {'symmetry_score': 0.0, 'skewness': 0.0, 'is_symmetric': False, 'note': 'Peak too narrow'}
# Calculate statistical skewness
mean_mz = np.average(region_mz, weights=region_int)
variance = np.average((region_mz - mean_mz) ** 2, weights=region_int)
std_dev = np.sqrt(variance)
if std_dev > 0:
skewness = np.average(((region_mz - mean_mz) / std_dev) ** 3, weights=region_int)
else:
skewness = 0.0
# Compare left and right sides by mirroring around apex
max_distance = min(apex_mz - region_mz[0], region_mz[-1] - apex_mz)
symmetry_scores = []
symmetry_weights = []
num_points = min(20, int(max_distance / 0.05)) # Finer sampling for better accuracy
for i in range(1, num_points + 1):
offset = (i / num_points) * max_distance
# Find intensity at left and right positions
left_pos = apex_mz - offset
right_pos = apex_mz + offset
# Interpolate intensities
left_intensity = np.interp(left_pos, left_mz, left_int, left=0, right=0)
right_intensity = np.interp(right_pos, right_mz, right_int, left=0, right=0)
# Calculate local symmetry, weighted by average intensity
# so high-signal regions near apex matter more than low-signal tails
avg_intensity = (left_intensity + right_intensity) / 2.0
if avg_intensity > 0:
local_asym = abs(left_intensity - right_intensity) / (left_intensity + right_intensity)
symmetry_scores.append(1.0 - local_asym)
symmetry_weights.append(avg_intensity)
# Overall symmetry score (intensity-weighted average)
if symmetry_scores and symmetry_weights:
symmetry_score = float(np.average(symmetry_scores, weights=symmetry_weights))
else:
symmetry_score = 0.0
# Determine if peak is symmetric
is_symmetric = symmetry_score > 0.7 and abs(skewness) < 0.5
# Generate interpretation
if symmetry_score > 0.85 and abs(skewness) < 0.3:
note = 'Highly symmetric - likely clean nanocluster'
elif symmetry_score > 0.7 and abs(skewness) < 0.5:
note = 'Moderately symmetric - good quality'
elif symmetry_score > 0.5:
note = 'Slightly asymmetric - may have impurities'
else:
note = 'Asymmetric - possible fragmentation or overlapping peaks'
return {
'symmetry_score': float(symmetry_score),
'skewness': float(skewness),
'is_symmetric': bool(is_symmetric), # Convert numpy bool to Python bool
'note': note,
'apex_mz': float(apex_mz),
}
def generate_experimental_gaussian_envelope(
self, exp_mz: npt.NDArray[np.float64], exp_int: npt.NDArray[np.float64], resolution: int
) -> tuple[Optional[npt.NDArray], Optional[npt.NDArray]]:
"""
Generate smooth Gaussian envelope for experimental data.
Uses Gaussian smoothing with kernel based on instrument resolution.
This will show the natural asymmetry of the experimental data.
"""
try:
logger.debug('GENERATE_EXPERIMENTAL_GAUSSIAN_ENVELOPE CALLED')
logger.debug(f'Input: {len(exp_mz)} m/z points, resolution={resolution}')
if len(exp_mz) == 0 or len(exp_int) == 0:
logger.warning('FAILED: Empty input data')
return None, None
# Convert to numpy arrays
exp_mz = np.array(exp_mz)
exp_int = np.array(exp_int)
# Calculate FWHM and sigma from resolution
peak_center = np.average(exp_mz, weights=exp_int)
fwhm = peak_center / resolution
sigma = fwhm / 2.355 # Convert FWHM to sigma
logger.debug(f'Peak center: {peak_center:.4f}, FWHM: {fwhm:.6f}, sigma: {sigma:.6f}')
# SMART APPROACH: Find apex (local maximum) of each isotope peak
# Then use the SAME smooth_gaussian_pattern function as theoretical data
# This ensures consistent smooth curves!
from scipy.signal import find_peaks
# Find local maxima (apex of each isotope peak)
# Use a small distance to separate isotope peaks (~0.2 Da for typical spacing)
min_distance = int(0.2 / np.median(np.diff(exp_mz))) if len(exp_mz) > 1 else 2
peaks_idx, properties = find_peaks(
exp_int, distance=max(2, min_distance), prominence=np.max(exp_int) * 0.05
)
if len(peaks_idx) < 3:
# Not enough peaks found - use all data points
logger.debug(f'Found only {len(peaks_idx)} apex points, using all data')
apex_mz = exp_mz
apex_int = exp_int
else:
# Extract apex points
all_apex_mz = exp_mz[peaks_idx]
all_apex_int = exp_int[peaks_idx]
logger.debug(f'Found {len(all_apex_mz)} apex points (local maxima)')
# FILTER: keep apex points that form a contiguous series with the
# most-intense apex. Walk left/right until a gap larger than
# 2.5 × median isotope spacing is encountered (the next envelope).
# This adapts to envelope width — narrow at low mass, wider at high
# mass where many Ag atoms broaden the isotope distribution.
max_apex_idx = int(np.argmax(all_apex_int))
spacings = np.diff(all_apex_mz)
median_spacing = float(np.median(spacings)) if len(spacings) >= 1 else 0.334
gap_threshold = max(median_spacing * 3.0, 0.5)
start = max_apex_idx
end = max_apex_idx
while end + 1 < len(all_apex_mz) and (all_apex_mz[end + 1] - all_apex_mz[end]) <= gap_threshold:
end += 1
while start - 1 >= 0 and (all_apex_mz[start] - all_apex_mz[start - 1]) <= gap_threshold:
start -= 1
apex_mz = all_apex_mz[start : end + 1]
apex_int = all_apex_int[start : end + 1]
logger.debug(
f'Kept {len(apex_mz)} contiguous apex points '
f'[{apex_mz[0]:.4f}, {apex_mz[-1]:.4f}] around max at '
f'{all_apex_mz[max_apex_idx]:.4f} (gap_threshold={gap_threshold:.3f})'
)
if len(apex_mz) < 3:
logger.debug(f'Too few contiguous points, using all {len(all_apex_mz)} apex points')
apex_mz = all_apex_mz
apex_int = all_apex_int
# CHECK FOR ALTERNATING INTENSITY PATTERN (same logic as charge detection)
# At low charge states (z=2), isotope peaks are ~0.5 Da apart with deep
# valleys; find_peaks picks up both real isotope apexes AND minor peaks
# in the valleys, creating a high-low-high-low pattern that shifts the
# smooth envelope centroid. Replace minor peaks' intensities with
# interpolated values from major peaks to correct the envelope shape
# while preserving the full m/z range for display.
if len(apex_int) >= 4:
intensity_diffs = np.diff(apex_int)
signs = np.sign(intensity_diffs)
sign_changes = np.diff(signs)
alternation_ratio = np.sum(sign_changes != 0) / len(sign_changes) if len(sign_changes) > 0 else 0
if alternation_ratio > 0.8:
even_sum = np.sum(apex_int[0::2])
odd_sum = np.sum(apex_int[1::2])
if even_sum >= odd_sum:
major_idx = np.arange(0, len(apex_int), 2)
minor_idx = np.arange(1, len(apex_int), 2)
else:
major_idx = np.arange(1, len(apex_int), 2)
minor_idx = np.arange(0, len(apex_int), 2)
# Interpolate minor peak intensities from major peaks
interp_int = np.interp(apex_mz[minor_idx], apex_mz[major_idx], apex_int[major_idx])
apex_int = apex_int.copy()
apex_int[minor_idx] = interp_int
logger.info(
f'Alternating pattern detected (ratio={alternation_ratio:.2f}): '
f'interpolated {len(minor_idx)} minor peaks from {len(major_idx)} major peaks'
)
# Create SMOOTH envelope by interpolating apex points + Gaussian smoothing
# STEP 1: Interpolate apex points to create smooth curve
# STEP 2: Apply Gaussian smoothing based on instrument resolution
from scipy.interpolate import UnivariateSpline
from scipy.ndimage import gaussian_filter1d
# Create fine m/z grid
mz_min = np.min(apex_mz)
mz_max = np.max(apex_mz)
num_points = int((mz_max - mz_min) / (fwhm / 100)) + 1
mz_grid = np.linspace(mz_min, mz_max, num_points)
# STEP 1: Interpolate apex points with cubic spline
if len(apex_mz) >= 4:
spline = UnivariateSpline(apex_mz, apex_int, s=0, k=3) # cubic, no smoothing
intensity_interp = spline(mz_grid)
logger.debug(f'STEP 1: Cubic spline through {len(apex_mz)} apex -> {len(mz_grid)} points')
else:
intensity_interp = np.interp(mz_grid, apex_mz, apex_int)
logger.debug(f'STEP 1: Linear interpolation through {len(apex_mz)} apex -> {len(mz_grid)} points')
# STEP 2: Apply STRONGER Gaussian smoothing for better curve fitting
mz_step = (mz_max - mz_min) / num_points if num_points > 1 else fwhm / 100
sigma_pixels = (sigma / mz_step) * 15.0 # 15x stronger smoothing for better Gaussian fit
intensity_grid = gaussian_filter1d(intensity_interp, sigma=sigma_pixels, mode='nearest')
logger.debug(f'STEP 2: STRONG Gaussian smoothing (sigma={sigma:.6f} m/z x 15 = {sigma_pixels:.2f} pixels)')
# Clip negative values (artifacts from edge smoothing)
intensity_grid = np.maximum(intensity_grid, 0.0)
# Normalize to 100
if np.max(intensity_grid) > 0:
intensity_grid = (intensity_grid / np.max(intensity_grid)) * 100.0
logger.info(f'SUCCESS: Smooth envelope from {len(apex_mz)} apex points')
logger.debug(f'Envelope: {len(mz_grid)} points, m/z [{np.min(mz_grid):.4f}, {np.max(mz_grid):.4f}]')
return mz_grid, intensity_grid
except Exception as e:
logger.exception(f'[generate_experimental_gaussian_envelope] Exception: {str(e)}')
return None, None
def fit_gaussian_to_smooth_envelope(
self,
mz_array: Optional[npt.NDArray[np.float64]],
int_array: Optional[npt.NDArray[np.float64]],
resolution: int,
context: str = '',
) -> tuple[Optional[float], Optional[float], bool]:
"""
Fit Gaussian to pre-smoothed isotope envelope to extract X₀ (centroid) and σ.
This is used by routes to fit experimental envelopes after they've been
smoothed by generate_experimental_gaussian_envelope().
Approach:
1. Find apex points in the data
2. Find valley boundaries (left/right) by scanning from center
3. Fit Gaussian to ALL data points between valleys
Args:
mz_array: Pre-smoothed m/z values
int_array: Pre-smoothed intensity values
resolution: Instrument resolution (for initial sigma estimate)
context: Optional context string for debug messages
Returns:
(x0, sigma, fit_succeeded): Fitted centroid and width, with success flag
Falls back to apex values if fit fails (fit_succeeded=False)
"""
from scipy.signal import find_peaks
# Igor Pro-style 4-parameter Gaussian: f(x) = y0 + A × exp(-((x - x₀) / w)²)
def gaussian(x, y0, A, x0, width):
return y0 + A * np.exp(-(((x - x0) / width) ** 2))
if mz_array is None or int_array is None or len(mz_array) <= 3:
return None, None, False
mz_array = np.array(mz_array)
int_array = np.array(int_array)
try:
# Step 1: Find apex points to determine valley boundaries
peaks_idx, _ = find_peaks(int_array, distance=2, prominence=np.max(int_array) * 0.05)
if len(peaks_idx) >= 5:
mz_apex = mz_array[peaks_idx]
int_apex = int_array[peaks_idx]
# Find center (highest apex)
center_idx = np.argmax(int_apex)
# Scan left to find valley
left_bound_idx = 0
for i in range(center_idx - 1, 0, -1):
if i > 0 and int_apex[i] < int_apex[i - 1]:
if int_apex[i] < int_apex[i + 1] * 0.9:
left_bound_idx = i
break
# Scan right to find valley
right_bound_idx = len(int_apex) - 1
for i in range(center_idx + 1, len(int_apex)):
if i < len(int_apex) - 1 and int_apex[i] < int_apex[i + 1]:
if int_apex[i] < int_apex[i - 1] * 0.9:
right_bound_idx = i
break
# Get m/z boundaries from valleys
left_mz = mz_apex[left_bound_idx]
right_mz = mz_apex[right_bound_idx]
# Extract ALL data points between valleys
mask = (mz_array >= left_mz) & (mz_array <= right_mz)
mz_fit = mz_array[mask]
int_fit = int_array[mask]
if context:
logger.debug(
f'[{context}] Valley boundaries: [{left_mz:.4f}, {right_mz:.4f}], fitting {len(mz_fit)} points'
)
else:
# Fallback: use all data
mz_fit = mz_array
int_fit = int_array
if context:
logger.debug(f'[{context}] Too few apexes ({len(peaks_idx)}), using all {len(mz_fit)} points')
if len(mz_fit) < 3:
mz_fit = mz_array
int_fit = int_array
# Step 2: Fit Igor-style 4-parameter Gaussian to data between valleys
max_idx = np.argmax(int_fit)
A_init = int_fit[max_idx]
x0_init = mz_fit[max_idx]
fwhm_estimate = x0_init / resolution
sigma_init = fwhm_estimate / 2.355
width_init = sigma_init * np.sqrt(2)
y0_init = np.min(int_fit)
popt, pcov = curve_fit(
gaussian,
mz_fit,
int_fit,
p0=[y0_init, A_init, x0_init, width_init],
bounds=(
[-A_init * 0.1, 0, mz_fit[0], 0.001],
[A_init * 0.5, A_init * 2, mz_fit[-1], fwhm_estimate * 2 * np.sqrt(2)],
),
maxfev=5000,
)
x0 = float(popt[2])
sigma = float(abs(popt[3]) / np.sqrt(2))
if context:
logger.debug(f'[{context}] Gaussian fit: X0={x0:.4f} m/z, sigma={sigma:.6f} m/z')
return x0, sigma, True
except Exception as e:
if context:
logger.warning(f'[{context}] Gaussian fit failed ({str(e)}), using apex fallback')
# Fallback: use apex of smooth envelope
max_idx = np.argmax(int_array)
x0 = float(mz_array[max_idx])
fwhm = x0 / resolution
sigma = float(fwhm / 2.355)
return x0, sigma, False
def detect_peak_asymmetry_visual(
self, mz_array: npt.NDArray[np.float64], int_array: npt.NDArray[np.float64], threshold_ratio: float = 0.3
) -> tuple[bool, int, str]:
"""
Detect peak asymmetry using visual characteristics:
- Count local maxima (multiple bumps = asymmetric)
- Check for shoulders (secondary peaks)
- Measure envelope smoothness
Returns: (is_asymmetric, num_maxima, details)
"""
try:
if len(mz_array) < 5:
return False, 1, 'Too few points'
mz_array = np.array(mz_array)
int_array = np.array(int_array)
# Normalize intensity
max_int = np.max(int_array)
if max_int == 0:
return False, 1, 'Zero intensity'
int_norm = int_array / max_int
# Find local maxima (peaks)
from scipy.signal import find_peaks
# Detect peaks with minimum height (to avoid noise)
# Prominence helps identify significant peaks vs noise
peaks, properties = find_peaks(
int_norm,
height=threshold_ratio, # At least 30% of max height
prominence=0.1, # Must be prominent enough
distance=3, # Separated by at least 3 points
)
num_maxima = len(peaks)
# Determine if asymmetric based on number of significant maxima
is_asymmetric = num_maxima > 1
details = f'{num_maxima} local maxima detected'
if num_maxima > 1:
peak_positions = [f'{mz_array[p]:.2f}' for p in peaks]
details += f' at m/z: {", ".join(peak_positions)}'
logger.debug(f'[Visual asymmetry detection] {details} -> {"ASYMMETRIC" if is_asymmetric else "SYMMETRIC"}')
return is_asymmetric, num_maxima, details
except Exception as e:
logger.error(f'[detect_peak_asymmetry_visual] Error: {str(e)}')
return False, 1, f'Error: {str(e)}'
def calculate_peak_skewness(
self, mz_array: npt.NDArray[np.float64], int_array: npt.NDArray[np.float64]
) -> Optional[float]:
"""
Calculate peak skewness (asymmetry measure).
Skewness = 0: perfectly symmetric
Skewness > 0: right-tailed (tailing to higher m/z)
Skewness < 0: left-tailed (tailing to lower m/z)
Returns: skewness value
"""
try:
mz_array = np.array(mz_array, dtype=float)
int_array = np.array(int_array, dtype=float)
if len(mz_array) < 3 or np.sum(int_array) == 0:
return None
# Calculate mean (weighted by intensity)
mean = np.sum(mz_array * int_array) / np.sum(int_array)
# Calculate standard deviation
variance = np.sum(int_array * (mz_array - mean) ** 2) / np.sum(int_array)
std_dev = np.sqrt(variance)
if std_dev == 0:
return 0.0
# Calculate skewness: (mean - mode) / std_dev
# Approximate mode as the m/z with maximum intensity
mode_idx = np.argmax(int_array)
mode = mz_array[mode_idx]
skewness = (mean - mode) / std_dev
return float(skewness)
except Exception as e:
logger.error(f'[calculate_peak_skewness] Exception: {str(e)}')
return None
def weighted_average_centroid(
self, mz_array: npt.NDArray[np.float64], int_array: npt.NDArray[np.float64]
) -> tuple[Optional[float], Optional[float]]:
"""
Calculate centroid using weighted average method.
This is used for general centroid calculations.
Returns x₀ = Σ(m/z × intensity) / Σ(intensity) and σ (weighted std dev)
"""
try:
if len(mz_array) == 0 or len(int_array) == 0:
logger.warning('[weighted_average_centroid] Empty arrays')
return None, None
# Convert to numpy arrays
mz_array = np.array(mz_array, dtype=float)
int_array = np.array(int_array, dtype=float)
total_intensity = np.sum(int_array)
if total_intensity == 0 or np.isnan(total_intensity) or np.isinf(total_intensity):
logger.warning(f'[weighted_average_centroid] Invalid total intensity: {total_intensity}')
return None, None
# Weighted average: x₀ = Σ(m/z × intensity) / Σ(intensity)
x0 = np.sum(mz_array * int_array) / total_intensity
# Weighted standard deviation: σ = sqrt(Σ(intensity × (m/z - x₀)²) / Σ(intensity))
sigma = np.sqrt(np.sum(int_array * (mz_array - x0) ** 2) / total_intensity)
if np.isnan(x0) or np.isinf(x0):
return None, None
logger.debug(f'[weighted_average_centroid] x0={x0:.4f}, sigma={sigma:.4f}')
return float(x0), float(sigma)
except Exception as e:
logger.error(f'[weighted_average_centroid] Exception: {str(e)}')
return None, None
def gaussian_fit_centroid(
self, mz_array: npt.NDArray[np.float64], int_array: npt.NDArray[np.float64], return_quality: bool = False
) -> tuple:
"""
Fit Gaussian curve to isotope envelope: f(x) = A × exp(-(x - x₀)² / (2σ²))
This is the STANDARD method used for composition determination (X₀ error calculation).
Parameters:
- return_quality: If True, also return R² goodness-of-fit metric
Returns:
- (x0, sigma, x0_error) if return_quality=False
- (x0, sigma, x0_error, r_squared) if return_quality=True
- x0_error is the standard error of the fitted x₀ parameter from covariance matrix
"""
try:
if len(mz_array) == 0 or len(int_array) == 0:
logger.warning(
f'[gaussian_fit_centroid] Empty arrays: mz length={len(mz_array)}, int length={len(int_array)}'
)
if return_quality:
return None, None, None, None
else:
return None, None, None
# Convert to numpy arrays
mz_array = np.array(mz_array, dtype=float)
int_array = np.array(int_array, dtype=float)
if len(mz_array) < 3:
logger.warning('[gaussian_fit_centroid] Need at least 3 points for fitting')
if return_quality:
return None, None, None, None
else:
return None, None, None
total_intensity = np.sum(int_array)
if total_intensity == 0 or np.isnan(total_intensity) or np.isinf(total_intensity):
logger.warning(f'[gaussian_fit_centroid] Invalid total intensity: {total_intensity}')
if return_quality:
return None, None, None, None
else:
return None, None, None
# NEW APPROACH: Find apex envelope, then find valleys in envelope, then fit
# Step 1: Find apex points of individual isotope peaks
from scipy.signal import find_peaks
# Find local maxima (apex of each isotope peak)
peaks_idx, _ = find_peaks(int_array, distance=2, prominence=np.max(int_array) * 0.05)
if len(peaks_idx) >= 5:
# Extract apex points (envelope)
mz_apex = mz_array[peaks_idx]
int_apex = int_array[peaks_idx]
logger.debug(f'[gaussian_fit_centroid] Found {len(peaks_idx)} isotope peak apexes')
# Step 2: Find the highest apex (center of envelope)
center_idx = np.argmax(int_apex)
# Step 3: Find valleys in the envelope (left and right of center)
# A valley must be both a local dip (relative criterion) AND
# below 40% of center intensity (absolute criterion) to avoid
# triggering on noise fluctuations in broad complex envelopes.
center_intensity = int_apex[center_idx]
valley_threshold = center_intensity * 0.4
# Scan left from center to find minimum
left_bound_idx = 0
for i in range(center_idx - 1, 0, -1):
if i > 0 and int_apex[i] < int_apex[i - 1]:
if int_apex[i] < int_apex[i + 1] * 0.9 and int_apex[i] < valley_threshold:
left_bound_idx = i
break
# Scan right from center to find minimum
right_bound_idx = len(int_apex) - 1
for i in range(center_idx + 1, len(int_apex)):
if i < len(int_apex) - 1 and int_apex[i] < int_apex[i + 1]:
if int_apex[i] < int_apex[i - 1] * 0.9 and int_apex[i] < valley_threshold:
right_bound_idx = i
break
# Step 4: Extract apex points BETWEEN envelope valleys
mz_fit = mz_apex[left_bound_idx : right_bound_idx + 1]
int_fit = int_apex[left_bound_idx : right_bound_idx + 1]
logger.debug(
f'[gaussian_fit_centroid] Envelope valleys: left={left_bound_idx}, center={center_idx}, right={right_bound_idx}'
)
logger.debug(f'[gaussian_fit_centroid] Fitting to {len(mz_fit)} apex points between envelope valleys')
else:
# Fallback: if too few peaks, use all apex points or top 70%
if len(peaks_idx) >= 3:
mz_fit = mz_array[peaks_idx]
int_fit = int_array[peaks_idx]
logger.warning(f'[gaussian_fit_centroid] Only {len(peaks_idx)} apexes, using all')
else:
logger.warning('[gaussian_fit_centroid] Too few apexes, using top 70%')
max_intensity = np.max(int_array)
threshold = max_intensity * 0.70
high_intensity_mask = int_array >= threshold
mz_fit = mz_array[high_intensity_mask]
int_fit = int_array[high_intensity_mask]
if len(mz_fit) < 3:
logger.error('[gaussian_fit_centroid] Too few points, using all data')
mz_fit = mz_array
int_fit = int_array
# Initial guesses for Gaussian parameters
# Amplitude: maximum intensity
A_guess = np.max(int_fit)
# Center: m/z of the maximum intensity point (apex)
max_idx = np.argmax(int_fit)
x0_guess = mz_fit[max_idx]
# Width: estimate from data range
mz_min_fit = np.min(mz_fit)
mz_max_fit = np.max(mz_fit)
mz_range_fit = mz_max_fit - mz_min_fit
sigma_guess = mz_range_fit / 4.0 # Narrower estimate since we're fitting top only
# Ensure reasonable initial guesses
if sigma_guess < 0.01:
sigma_guess = 0.5
# Overall data range for bounds
mz_min_all = np.min(mz_array)
mz_max_all = np.max(mz_array)
# Baseline guess: minimum intensity in fitting region
max_int_fit = np.max(int_fit)
y0_guess = min(np.min(int_fit), max_int_fit * 0.4)
logger.debug(
f'[gaussian_fit_centroid] Initial guesses: x0={x0_guess:.4f} (apex), sigma={sigma_guess:.4f}, A={A_guess:.2e}, y0={y0_guess:.2e}'
)
# Igor Pro-style 4-parameter Gaussian: f(x) = y0 + A × exp(-((x - x₀) / w)²)
# where w = sqrt(2) × σ, so exponent = -(x - x₀)² / (2σ²)
def gaussian(x, y0, A, x0, width):
return y0 + A * np.exp(-(((x - x0) / width) ** 2))
# Fit Gaussian curve to HIGH-INTENSITY data only
try:
from scipy.optimize import curve_fit
width_guess = sigma_guess * np.sqrt(2)
# Allow x0 to vary within the full valley boundaries
bounds = (
[-max_int_fit * 0.1, 0, mz_min_all, 0.01], # Lower bounds: [y0_min, A_min, x0_min, width_min]
[max_int_fit * 0.5, np.inf, mz_max_all, (mz_max_all - mz_min_all) * 2], # Upper bounds
)
logger.debug(f'[gaussian_fit_centroid] x0 bounds: [{mz_min_all:.4f}, {mz_max_all:.4f}]')
popt, pcov = curve_fit(
gaussian,
mz_fit, # Fit to high-intensity points only
int_fit,
p0=[y0_guess, A_guess, x0_guess, width_guess],
bounds=bounds,
maxfev=10000,
ftol=1e-10, # Function tolerance for convergence (more precise)
xtol=1e-10, # Parameter tolerance for convergence (more precise)
)
y0_fit, A_fit, x0_fit, width_fit = popt
sigma_fit = width_fit / np.sqrt(2)
# Calculate standard errors from covariance matrix
# pcov diagonal gives variance of parameters, sqrt gives standard error
perr = np.sqrt(np.diag(pcov))
y0_err, A_err, x0_err, width_err = perr
# Validate fitted parameters
if np.isnan(x0_fit) or np.isinf(x0_fit) or np.isnan(sigma_fit) or np.isinf(sigma_fit):
raise ValueError('Fit returned invalid parameters')
# Calculate R² (coefficient of determination) if requested
if return_quality:
# Predicted values from fitted Gaussian
y_pred = gaussian(mz_array, y0_fit, A_fit, x0_fit, width_fit)
# Calculate R²
ss_res = np.sum((int_array - y_pred) ** 2) # Residual sum of squares
ss_tot = np.sum((int_array - np.mean(int_array)) ** 2) # Total sum of squares
r_squared = 1 - (ss_res / ss_tot) if ss_tot > 0 else 0.0
logger.debug(
f'[gaussian_fit_centroid] Gaussian fit: x₀={x0_fit:.4f}±{x0_err:.4f}, σ={sigma_fit:.4f}, y0={y0_fit:.2e}, R²={r_squared:.4f}'
)
return float(x0_fit), float(sigma_fit), float(x0_err), float(r_squared)
else:
logger.debug(
f'[gaussian_fit_centroid] Gaussian fit: x₀={x0_fit:.4f}±{x0_err:.4f}, σ={sigma_fit:.4f}, y0={y0_fit:.2e}'
)
return float(x0_fit), float(sigma_fit), float(x0_err)
except Exception as fit_error:
# If Gaussian fit fails, fall back to weighted average
logger.warning(
f'[gaussian_fit_centroid] Gaussian fit failed ({fit_error}), using weighted average fallback'
)
x0_fallback = x0_guess
sigma_fallback = sigma_guess
if np.isnan(x0_fallback) or np.isinf(x0_fallback):
if return_quality:
return None, None, None, None
else:
return None, None, None
if return_quality:
return (
float(x0_fallback),
float(sigma_fallback),
None,
0.0,
) # No fitting error, R² = 0 indicates fit failed
else:
return float(x0_fallback), float(sigma_fallback), None # No fitting error available
except Exception as e:
logger.exception(f'[gaussian_fit_centroid] Exception: {str(e)}')
if return_quality:
return None, None, None, None
else:
return None, None, None
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