"""Exact one-arc cosine-transform mass-budget relaxation. Coordinates are on R/(pi Z). The shifted orientation measure mu obeys H'' + H = mu; equivalently H(t) = .5 integral |sin(t-u)| dmu(u). The support function H is at least 1, and its integral is total mass L. The numerical routines illustrate a proved continuum theorem. They do not test geometric opacity or construct an opaque barrier. """ from dataclasses import dataclass import math import numpy as np from scipy.optimize import brentq @dataclass(frozen=True) class SoftGapSolution: beta: float eta: float regime: str value: float critical_budget: float plateau_halfwidth: float cap_width: float dual_multiplier: float def solve_soft_gap(beta, eta): """Return the exact formula, with one scalar root in the middle regime.""" beta, eta = float(beta), float(eta) if not 0.0 < beta < math.pi / 2: raise ValueError("beta must lie strictly between 0 and pi/2") if eta < 0 or not math.isfinite(eta): raise ValueError("eta must be finite and nonnegative") critical = 2 * math.tan(beta / 2) if eta <= critical: b = 2*math.sin(beta/2)**2 / math.cos(beta) value = math.pi + 2 * (math.tan(beta) - beta) - b * eta return SoftGapSolution(beta, eta, "central atom", value, critical, 0.0, beta, b) if eta < 2 * beta: s = brentq(lambda x: 2*x + 2*math.tan((beta-x)/2) - eta, 0.0, beta, xtol=5e-15) d = beta - s value = math.pi + 4 * math.tan(d / 2) - 2 * d return SoftGapSolution(beta, eta, "contact plateau", value, critical, s, d, 2*math.sin(d/2)**2 / math.cos(d)) return SoftGapSolution(beta, eta, "uniform", math.pi, critical, beta, 0.0, 0.0) def circle_coordinate(t): return (np.asarray(t, dtype=float) + math.pi/2) % math.pi - math.pi/2 def extremizer_h(t, solution): """The primal continuum extremizer H, including all regimes.""" a = np.abs(circle_coordinate(t)) z = np.full_like(a, 1.0) p = solution if p.regime == "central atom": mask = a < p.beta A = (2 - p.eta*math.sin(p.beta)) / math.cos(p.beta) z = np.where(mask, .5*(A*np.cos(a) + p.eta*np.sin(a)), z) elif p.regime == "contact plateau": mask = (a > p.plateau_halfwidth) & (a < p.beta) cap = np.cos(a-(p.plateau_halfwidth+p.beta)/2) / math.cos(p.cap_width/2) z = np.where(mask, cap, z) return z def dual_w(t, solution): """The supported dual test function 0 <= w <= b*1_I.""" a = np.abs(circle_coordinate(t)) p = solution if p.regime == "uniform": return np.zeros_like(a) d, s = p.cap_width, p.plateau_halfwidth numerator = np.cos(np.maximum(a-s, 0.0)) - math.cos(d) denominator = math.cos(d) return np.where(a >= p.beta, 0.0, np.where(a <= s, p.dual_multiplier, numerator/denominator)) def measure_decomposition(solution): """Return uniform-density intervals and (position, mass) atoms of mu. Arc endpoints +/-beta are excluded from the budget. Zero-width intervals and coincident zero atoms have no effect. """ p = solution if p.regime == "uniform": return [(-math.pi/2, math.pi/2)], [] intervals = [(-math.pi/2, -p.beta), (p.beta, math.pi/2)] if p.regime == "central atom": edge = math.tan(p.beta) - p.eta/(2*math.cos(p.beta)) atoms = [(-p.beta, edge), (0.0, p.eta), (p.beta, edge)] else: s = p.plateau_halfwidth if s > 0: intervals.append((-s, s)) mass = math.tan(p.cap_width/2) atoms = [(-p.beta, mass), (-s, mass), (s, mass), (p.beta, mass)] return intervals, atoms def mass_in_open_arc(solution): intervals, atoms = measure_decomposition(solution) beta = solution.beta diffuse = sum(max(0.0, min(b,beta)-max(a,-beta)) for a,b in intervals) atomic = sum(m for x,m in atoms if -beta < x < beta) return diffuse + atomic def total_mass(solution): intervals, atoms = measure_decomposition(solution) return sum(b-a for a,b in intervals) + sum(m for x,m in atoms) def value_curve(beta, budgets): return np.array([solve_soft_gap(beta, eta).value for eta in budgets])