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| """Exact and numerical checks for tolerance-threshold completion. | |
| At an exact polynomial minimax tolerance, a vanishing higher-degree admixture | |
| creates a strict margin that dominates the finite-gap Hermite remainder, | |
| without changing the lower-degree energy exponent. The two examples below | |
| use entirely rational polynomials and exact band-error certificates. | |
| """ | |
| from pathlib import Path | |
| import json | |
| import mpmath as mp | |
| import sympy as sp | |
| from spectral_control import MomentProblem, polynomial_jets, polyval, real | |
| ROOT = Path(__file__).resolve().parents[1] | |
| DPS = 160 | |
| def number(value): | |
| return mp.nstr(value, 75) | |
| def rational(value): | |
| value = sp.Rational(value) | |
| return mp.mpf(str(value.p))/mp.mpf(str(value.q)) | |
| def coefficients(poly, x, degree): | |
| return [rational(sp.expand(poly).coeff(x, k)) for k in range(degree+1)] | |
| def confluent_limit(degree, scaled_coefficients): | |
| """Use one-node derivative kernels, not a colliding-node extrapolation.""" | |
| p = MomentProblem([2], degree, [[1]], [[0]*(degree+1)], impulse=0) | |
| data = mp.matrix(len(p.rows), 1) | |
| for k, c in enumerate(scaled_coefficients): | |
| # Derivative kernels are k! times the Taylor-coefficient kernels. | |
| data[1+2*k] = mp.factorial(k)*rational(c) | |
| return (data.T*mp.lu_solve(p.G, data))[0] | |
| def realize_mix(low_coefficients, high_coefficients, n, N, gap, dps=DPS): | |
| mp.mp.dps = dps | |
| gap = real(gap) | |
| alpha = gap**(N-n) | |
| coeffs = [(1-alpha)*(low_coefficients[k] if k < len(low_coefficients) else 0) | |
| + alpha*high_coefficients[k] for k in range(N+1)] | |
| m = (N-1)//2 | |
| jets = polynomial_jets(coeffs, [-mp.mpf("0.5"), mp.mpf("0.5")], gap, m) | |
| p = MomentProblem([2-gap/2, 2+gap/2], m, [[1], [1]], jets, impulse=0) | |
| return p, coeffs | |
| def run(): | |
| mp.mp.dps = DPS | |
| x, delta = sp.symbols("x delta", real=True) | |
| a, r = sp.Rational(1, 2), sp.Rational(1, 4) | |
| P1 = -2*x | |
| P3 = (32*x**3-26*x)/9 | |
| # The standard integrated polynomial with A=a+r has error 113/301, | |
| # exceeding 1/3. This rational monotone degree-five substitute does better. | |
| P5 = (-810*x+1920*x**3-2048*x**5)/229 | |
| original_P5 = (-810*x+960*x**3-512*x**5)/301 | |
| checks = [] | |
| def check(name, condition, **details): | |
| record = {"name": name, "passed": bool(condition), **details} | |
| checks.append(record) | |
| if not condition: | |
| raise AssertionError(json.dumps(record, indent=2)) | |
| for name, poly in [("P1", P1), ("P3", P3), ("P5", P5)]: | |
| check(f"{name} exact oddness and nominal values", | |
| sp.expand(poly.subs(x, -x)+poly) == 0 and | |
| sp.simplify(poly.subs(x, -a)-1) == 0 and | |
| sp.simplify(poly.subs(x, a)+1) == 0) | |
| check("linear exact band error is 1/2", | |
| abs(P1.subs(x, a-r)+1) == sp.Rational(1, 2) and | |
| abs(P1.subs(x, a+r)+1) == sp.Rational(1, 2)) | |
| check("cubic endpoints have error 1/3", | |
| P3.subs(x, a-r)+1 == sp.Rational(1, 3) and | |
| P3.subs(x, a+r)+1 == sp.Rational(1, 3)) | |
| # On the positive interval, Q3=-P3 is concave. Its only stationary point | |
| # is sqrt(39)/12 and its value is 13 sqrt(39)/81; the squared inequality | |
| # below proves the interior overshoot is no larger than 1/3. | |
| stationary = sp.sqrt(39)/12 | |
| check("cubic interior critical value respects global 1/3 error", | |
| sp.simplify(sp.diff(P3, x).subs(x, stationary)) == 0 and | |
| sp.simplify((-P3).subs(x, stationary)-13*sp.sqrt(39)/81) == 0 and | |
| sp.Integer(13)**2*39 <= sp.Integer(108)**2) | |
| check("quintic is globally monotone by an exact square factorization", | |
| sp.factor(sp.diff(P5, x)+10*(9-32*x**2)**2/229) == 0) | |
| e5 = sp.Rational(109, 458) | |
| check("quintic exact uniform band error is 109/458 below 1/3", | |
| P5.subs(x, a-r) == -sp.Rational(349, 458) and | |
| P5.subs(x, a+r) == -sp.Rational(567, 458) and e5 < sp.Rational(1, 3)) | |
| check("original A=3/4 quintic is correctly rejected at this threshold", | |
| 1+original_P5.subs(x, a-r) == sp.Rational(113, 301) and | |
| sp.Rational(113, 301) > sp.Rational(1, 3)) | |
| specs = [ | |
| {"name": "linear_threshold", "n": 1, "N": 3, | |
| "low": P1, "high": P3, "tau": sp.Rational(1, 2), | |
| "higher_error": sp.Rational(1, 3), | |
| "gaps": ["0.01", "0.003", "0.001", "0.0003", "0.0001"], | |
| "expected_vector": [0, -2, 0, sp.Rational(32, 9)]}, | |
| {"name": "cubic_threshold", "n": 3, "N": 5, | |
| "low": P3, "high": P5, "tau": sp.Rational(1, 3), | |
| "higher_error": e5, | |
| "gaps": ["0.001", "0.0001", "0.00001", "0.000003", "0.000001"], | |
| "expected_vector": [0, 0, 0, sp.Rational(32, 9), 0, -sp.Rational(2048, 229)]}, | |
| ] | |
| cases, all_residuals = [], [] | |
| for spec in specs: | |
| n, N = spec["n"], spec["N"] | |
| mix = sp.expand((1-delta**(N-n))*spec["low"]+delta**(N-n)*spec["high"]) | |
| scaled_coefficients = [sp.cancel(delta**(n-k)*mix.coeff(x, k)) for k in range(N+1)] | |
| limits = [sp.limit(c, delta, 0, dir="+") for c in scaled_coefficients] | |
| check(f"{spec['name']} exact finite scaled coefficient vector", | |
| limits == spec["expected_vector"] and | |
| all(sp.denom(c).subs(delta, 0) != 0 for c in scaled_coefficients), | |
| exact_limit_vector=[str(c) for c in limits]) | |
| check(f"{spec['name']} mixture preserves nominal identities exactly", | |
| sp.simplify(mix.subs(x, -a)-1) == 0 and | |
| sp.simplify(mix.subs(x, a)+1) == 0) | |
| lo = coefficients(spec["low"], x, n) | |
| hi = coefficients(spec["high"], x, N) | |
| expected = confluent_limit(N, limits) | |
| tau = rational(spec["tau"]) | |
| strict_difference = rational(spec["tau"]-spec["higher_error"]) | |
| m, R = (N-1)//2, N+1 | |
| max_product = (mp.mpf(5)/16)**(m+1) | |
| points, energy_errors, band_checks, remainder_checks = [], [], [], [] | |
| # The two outer and two inner band endpoints and nominal centers. | |
| sample_x = [-mp.mpf(3)/4, -mp.mpf(1)/2, -mp.mpf(1)/4, | |
| mp.mpf(1)/4, mp.mpf(1)/2, mp.mpf(3)/4] | |
| for gap_string in spec["gaps"]: | |
| gap = real(gap_string) | |
| p, coeffs = realize_mix(lo, hi, n, N, gap) | |
| all_residuals.append(p.solve_residual) | |
| scaled_energy = gap**(2*n)*p.energy | |
| energy_error = abs(scaled_energy/expected-1) | |
| energy_errors.append(energy_error) | |
| margin = gap**(N-n)*strict_difference | |
| remainder = gap**R*max_product*p.moment_norm(R)*mp.sqrt(p.energy)/mp.factorial(R) | |
| polynomial_bound = tau-margin | |
| analytic_bound = polynomial_bound+remainder | |
| max_sample_error, max_profile_difference = mp.mpf(0), mp.mpf(0) | |
| for xx in sample_x: | |
| target = mp.mpf(1) if xx < 0 else -mp.mpf(1) | |
| response = p.response(2+gap*xx) | |
| max_sample_error = max(max_sample_error, abs(response-target)) | |
| max_profile_difference = max(max_profile_difference, | |
| abs(response-polyval(coeffs, xx))) | |
| band_checks.append(max_sample_error <= analytic_bound+mp.mpf("1e-70")) | |
| remainder_checks.append(max_profile_difference <= remainder+mp.mpf("1e-70")) | |
| points.append({"gap": gap_string, "energy": number(p.energy), | |
| "scaled_energy": number(scaled_energy), | |
| "relative_error_to_confluent_limit": number(energy_error), | |
| "strict_polynomial_margin": number(margin), | |
| "uniform_Hermite_remainder_bound": number(remainder), | |
| "remainder_to_margin_ratio": number(remainder/margin), | |
| "analytic_uniform_band_error_bound": number(analytic_bound), | |
| "analytically_certified_below_tolerance": bool(analytic_bound < tau), | |
| "sampled_maximum_actual_error": number(max_sample_error), | |
| "sampled_maximum_polynomial_difference": number(max_profile_difference), | |
| "solve_residual": number(p.solve_residual)}) | |
| check(f"{spec['name']} energy retains exponent 2n at exact tolerance", | |
| energy_errors[-1] < mp.mpf("1e-6") and | |
| energy_errors[-1] < energy_errors[0]/10 and | |
| energy_errors[-1] < energy_errors[-2], | |
| predicted_exponent=2*n, final_relative_error=number(energy_errors[-1])) | |
| check(f"{spec['name']} strict margin dominates the whole-band remainder", | |
| all(p["analytically_certified_below_tolerance"] for p in points[-2:]), | |
| final_remainder_to_margin=points[-1]["remainder_to_margin_ratio"]) | |
| check(f"{spec['name']} direct frequency responses respect the analytic bounds", | |
| all(band_checks) and all(remainder_checks)) | |
| cases.append({"name": spec["name"], "radius": "1/4", "tau": str(spec["tau"]), | |
| "n": n, "N": N, "energy_exponent": 2*n, | |
| "lower_polynomial": str(spec["low"]), | |
| "higher_polynomial": str(spec["high"]), | |
| "higher_polynomial_exact_band_error": str(spec["higher_error"]), | |
| "mixture": str(mix), | |
| "strict_margin_coefficient": str(spec["tau"]-spec["higher_error"]), | |
| "exact_scaled_coefficient_limit": [str(c) for c in limits], | |
| "predicted_exact_energy_limit": number(expected), | |
| "points": points}) | |
| # Precision sensitivity of the smallest-gap, cubic-threshold example. | |
| spec = specs[-1] | |
| mp.mp.dps = 160 | |
| lo = coefficients(spec["low"], x, spec["n"]) | |
| hi = coefficients(spec["high"], x, spec["N"]) | |
| lower, _ = realize_mix(lo, hi, spec["n"], spec["N"], spec["gaps"][-1], dps=160) | |
| lower_energy = lower.energy | |
| mp.mp.dps = 180 | |
| lo = coefficients(spec["low"], x, spec["n"]) | |
| hi = coefficients(spec["high"], x, spec["N"]) | |
| higher, _ = realize_mix(lo, hi, spec["n"], spec["N"], spec["gaps"][-1], dps=180) | |
| discrepancy = abs(lower_energy/higher.energy-1) | |
| check("160-to-180-digit threshold energy agreement at gap 1e-6", | |
| discrepancy < mp.mpf("1e-60"), relative_discrepancy=number(discrepancy)) | |
| max_residual = max(all_residuals) | |
| check("all boundary systems meet a strict nominal moment residual", | |
| max_residual < mp.mpf("1e-70"), maximum_residual=number(max_residual)) | |
| report = { | |
| "scope": "Exact nominal targets and uniform interval-frequency tolerance, fixed T=6, Omega=2, polynomial weight q=4", | |
| "claim": "Threshold tolerances retain exponent 2 n_tau by a vanishing higher-degree polynomial admixture", | |
| "important_distinction": "The analytic whole-band bound is global; sampled actual errors are only corroboration", | |
| "working_decimal_precision": DPS, | |
| "cases": cases, | |
| "precision_comparison_relative_discrepancy": number(discrepancy), | |
| "maximum_nominal_moment_residual": number(max_residual), | |
| "checks": checks, "check_count": len(checks), | |
| "passed": all(c["passed"] for c in checks), | |
| } | |
| path = ROOT / "results" / "boundary_completion.json" | |
| path.parent.mkdir(parents=True, exist_ok=True) | |
| path.write_text(json.dumps(report, indent=2)+"\n") | |
| print(json.dumps({"passed": report["passed"], "check_count": len(checks), | |
| "report": str(path), "precision_discrepancy": number(discrepancy), | |
| "maximum_residual": number(max_residual), | |
| "final_certificates": [{"case": c["name"], "tau": c["tau"], | |
| "gap": c["points"][-1]["gap"], | |
| "bound": c["points"][-1]["analytic_uniform_band_error_bound"]} | |
| for c in cases]})) | |
| if __name__ == "__main__": | |
| run() | |