"""Check of items 1 and 2 of 07-ilang-weight/08-field-speed (v2) against the exact evolution of one field object (N_f = 1, n = 1/|X|) from its lowest state without the source, under the fixed contract with the source g_s Phi_{x_s} (sudden switching; the gradual switching is withdrawn by the question's note of 2026-10-21). Also checks the finite-coupling bounds (8.5), (8.18) and the axis front form (8.6) for D = 3. The source sits at x_s = 0. The one-object contract -t_f A + g(lam)|0><0| and the start (uniform state) are invariant under the point group of the torus that fixes 0, so the state stays in the invariant sector (orbit basis); the evolution there is exact. With psi = exp(-i E0 lam)(c0 + g chi), chi solves i chi' = (H - E0) chi + f P c0 exactly. The made field is reported in units of 2 n g_s / t_f: phi = delta rho / (2 n g_s / t_f); static mark phi_st = -Lambda^+. """ import itertools import json import math import time from pathlib import Path import numpy as np import scipy.sparse as sp from scipy.special import comb, erfc, jv OUT = Path(__file__).parent / "output" OUT.mkdir(exist_ok=True) TF = 1.0 LOG = [] RES = {} def log(*a): s = " ".join(str(x) for x in a) print(s, flush=True) LOG.append(s) # ---------------------------------------------------------------- lattice and sector def sector(L, D): h = L // 2 base = h + 1 reps = np.array(list(itertools.combinations_with_replacement(range(base), D)), dtype=np.int64) def key(a): a = np.sort(np.minimum(a % L, (-a) % L), axis=-1) k = np.zeros(a.shape[:-1], dtype=np.int64) for mu in range(D): k = k * base + a[..., mu] return k rk = key(reps) assert np.all(np.diff(rk) > 0) # orbit size: sign choices times distinct permutations signs = np.prod(np.where((reps == 0) | (reps == h), 1, 2), axis=1) # distinct permutations: D! / prod over values of (multiplicity)!; for sorted reps of length <= 3 perm_div = np.ones(len(reps)) if D == 2: perm_div = np.where(reps[:, 0] == reps[:, 1], 2.0, 1.0) elif D == 3: e01, e12 = reps[:, 0] == reps[:, 1], reps[:, 1] == reps[:, 2] perm_div = np.where(e01 & e12, 6.0, np.where(e01 | e12, 2.0, 1.0)) size = (signs * math.factorial(D) / perm_div).astype(float) assert abs(size.sum() - L ** D) < 0.5 rows, cols = [], [] for mu in range(D): for s in (1, -1): y = reps.copy() y[:, mu] += s rows.append(np.arange(len(reps))) cols.append(np.searchsorted(rk, key(y))) rows, cols = np.concatenate(rows), np.concatenate(cols) n = sp.coo_matrix((np.ones(len(rows)), (rows, cols)), shape=(len(reps),) * 2).tocsr().tocoo() H0 = sp.csr_matrix((-TF * np.sqrt(size[n.row] / size[n.col]) * n.data, (n.row, n.col)), shape=n.shape) X = float(L ** D) def axis(d): a = np.zeros((1, D), dtype=np.int64) a[0, 0] = d return int(np.searchsorted(rk, key(a))[0]) return dict(L=L, D=D, M=len(reps), size=size, H0=H0, X=X, c0=np.sqrt(size / X), E0=-2.0 * D * TF, axis=axis) def lam_plus_axis(L, D, rmax): """Lambda^+(r e_1) on the torus from its Fourier sum, (4.4) of 06-ilang-source/04-profile; also S_2.""" k = 2 * np.pi * np.arange(L) / L w1 = 4 * np.sin(k / 2) ** 2 others = np.zeros(1) for _ in range(D - 1): others = (others[:, None] + w1[None, :]).ravel() S = np.zeros(L) S2 = 0.0 for i in range(L): tot = w1[i] + others if i == 0: tot = tot[1:] S[i] = (1 / tot).sum() S2 += (1 / tot ** 2).sum() r = np.arange(rmax + 1) return (np.cos(np.outer(r, k)) @ S) / L ** D, S2 / L ** D def phi_from_chi(sec, sel, chi, g): c0, size = sec["c0"][sel][:, None], sec["size"][sel][:, None] return TF * sec["X"] * (c0 * chi.real + 0.5 * g * np.abs(chi) ** 2) / size # ---------------------------------------------------------------- evolutions def sudden_dense(sec, g, lams, sel, chunk=2000, eig=None): if eig is None: H = sec["H0"].toarray() H[0, 0] += g eig = np.linalg.eigh(H) E, V = eig mu = E - sec["E0"] mu = np.where(np.abs(mu) < 1e-14, 1e-14, mu) Vs = V[sel, :] * (V[0, :] / np.sqrt(sec["X"]))[None, :] out = np.empty((len(sel), len(lams))) for i in range(0, len(lams), chunk): lc = lams[i:i + chunk] chi = Vs @ (np.expm1(-1j * np.outer(mu, lc)) / mu[:, None]) out[:, i:i + chunk] = phi_from_chi(sec, sel, chi, g) return out def first_order_dense(sec, lams, sel, chunk=2000): E, V = np.linalg.eigh(sec["H0"].toarray()) eps = E - sec["E0"] pos = eps > 1e-9 w = V[sel][:, pos] * V[0, pos][None, :] / np.sqrt(sec["size"][sel])[:, None] st = -TF * (w @ (1 / eps[pos])) out = np.empty((len(sel), len(lams))) for i in range(0, len(lams), chunk): lc = lams[i:i + chunk] out[:, i:i + chunk] = TF * (w @ ((np.cos(np.outer(eps[pos], lc)) - 1) / eps[pos][:, None])) return out, st class Cheb: """Chebyshev expansions of exp(-i x dl) and (exp(-i x dl) - 1)/x on [a, b] (spectrum of A = H - E0).""" def __init__(self, a, b, dl): self.c, self.h = (a + b) / 2, (b - a) / 2 K = int(self.h * dl + 12 * (self.h * dl) ** (1 / 3) + 20) k = np.arange(K) pref = np.where(k == 0, 1.0, 2.0) * (-1j) ** k def cU(s): return np.exp(-1j * self.c * s) * pref * jv(k, self.h * s) # exp(-i x dl) = sum_k cU_k(dl) T_k(y); (exp(-i x dl) - 1)/x = -i int_0^dl exp(-i x s) ds xg, wg = np.polynomial.legendre.leggauss(int((abs(self.c) + self.h) * dl) + 64) s = 0.5 * dl * (xg + 1) cUd = cU(dl) cPd = -1j * 0.5 * dl * sum(wq * cU(sq) for wq, sq in zip(wg, s)) assert abs(jv(K - 1, self.h * dl)) < 1e-17 keep = np.where((np.abs(cUd) > 1e-17) | (np.abs(cPd) > 1e-17 * dl))[0] Kt = max(int(keep.max()) + 1, 2) self.coef = np.stack([cUd[:Kt], cPd[:Kt]], axis=1) # columns: U, Phi def apply(self, matvec, V, coef): """sum_k T_k(A~) V * coef[k]; V has shape (M, ncol), coef (K, ncol).""" t0, t1 = V, (matvec(V) - self.c * V) / self.h s = coef[0] * t0 + coef[1] * t1 for ck in coef[2:]: t0, t1 = t1, 2 * (matvec(t1) - self.c * t1) / self.h - t0 s = s + ck * t1 return s def a_op(sec): return (sec["H0"] - sec["E0"] * sp.identity(sec["M"], format="csr")).tocsr().astype(complex) def a_matvec(A0, gval): def mv(v): o = A0 @ v o[0] += gval * v[0] return o return mv def propagate_const(sec, g, chi0, dl, nstep, sel): """Exact evolution with constant source g from chi0; phi at k*dl, k = 1..nstep.""" D = sec["D"] ch = Cheb(-0.1 - abs(g), 4 * D * TF + 0.1 + abs(g), dl) mv = a_matvec(a_op(sec), g) b = np.zeros((sec["M"], 1), complex) b[0] = 1 / np.sqrt(sec["X"]) w = ch.apply(mv, b, ch.coef[:, 1:2])[:, 0] chi = chi0.astype(complex)[:, None] out = np.empty((len(sel), nstep)) for k in range(nstep): chi = ch.apply(mv, chi, ch.coef[:, 0:1]) chi[:, 0] += w out[:, k] = phi_from_chi(sec, sel, chi[sel], g)[:, 0] return out, chi[:, 0] # ---------------------------------------------------------------- scaling functions, helpers def gD(zeta, D): """Re Gamma(D/2, -i zeta)/Gamma(D/2): gradient ratio (8.9) for D = 1, 3.""" z = np.sqrt(np.asarray(zeta, float)) * np.exp(-1j * np.pi / 4) if D == 1: return erfc(z).real return (erfc(z) + 2 * z / np.sqrt(np.pi) * np.exp(-z * z)).real def zeta_star(eps, D): zz = np.linspace(1e-7, 5, 500001) bad = np.abs(1 - gD(zz, D)) > eps return float(zz[np.argmax(bad)]) def P_axis(u, rho, D): """Trigonometric factor P_D(u) of the axis front form (8.6).""" s = 0 for j in range(D): c = 2.0 ** (1 - D) * comb(D - 1, j) * np.exp(-1j * (D - 1 - 2 * j) * np.pi / 4) s = s + c * np.exp(-1j * (2 * j + 1) * u) / (2 * j + 1) return np.imag(1j ** (rho + 1) * s) def eta(z): w = np.sqrt(1 - z ** 2) return np.arctanh(w) - w def last_entry(lams, dev, eps): bad = np.where(np.abs(dev) > eps)[0] if len(bad) == 0: return float(lams[0]) return float(lams[min(bad[-1] + 1, len(lams) - 1)]) def powerfit(x, y): p = np.polyfit(np.log(x), np.log(y), 1) return float(p[0]), float(np.exp(p[1])) def grad(ph, lp, ds): """Central-difference gradient along the axis and its static value; ph rows are (d-1, d+1) pairs.""" G = np.array([(ph[2 * i + 1] - ph[2 * i]) / 2 for i in range(len(ds))]) Gst = np.array([(-lp[d + 1] + lp[d - 1]) / 2 for d in ds]) return G, Gst # ================================================================ item 1: front def front(sec, g, ds, dl, lam_max, p_f, eps_f, fit_min, label): D = sec["D"] sel = [sec["axis"](int(d)) for d in ds] v0 = np.zeros(sec["M"], complex) t0 = time.time() nst = int(round(lam_max / dl)) ph, _ = propagate_const(sec, g, v0, dl, nst, sel) lams = dl * np.arange(1, nst + 1) arr = np.array([lams[np.argmax(np.abs(ph[i]) >= 0.5 * eps_f * d ** -p_f)] for i, d in enumerate(ds)]) big = ds >= fit_min slope = np.polyfit(ds[big], arr[big], 1)[0] kap = [] for i, d in enumerate(ds): z = 2 * TF * lams / d # (8.5) at every order, in units 2 n g / t_f: t_f (e^{2|g| lam} - 1) / (2|g|) * e^{-rho eta} logb = np.log(TF * np.expm1(2 * abs(g) * lams) / (2 * abs(g))) - d * eta(np.minimum(z, 1 - 1e-12)) m = (z <= 0.95) & (logb > np.log(1e-9)) kap.append(float(np.max(np.abs(ph[i][m]) / np.exp(logb[m])))) win = [np.abs(2 * TF * lams - d) <= 3 * d ** (1 / 3) for d in ds] peak = np.array([np.max(np.abs(ph[i][win[i]])) for i in range(len(ds))]) pe, pc = powerfit(ds[big], peak[big]) res = dict(criterion=f"first lam with |delta rho| >= eps (n g/t) rho^-p, i.e. |phi| >= (eps/2) rho^-p; eps={eps_f}, p={p_f}", rho=ds.tolist(), arrival=arr.tolist(), arrival_times_2t_over_rho=(2 * TF * arr / ds).tolist(), speed_linear_fit=float(1 / slope), fit_min_rho=int(fit_min), max_ratio_to_kapteyn_bound_ahead=max(kap), front_peak_phi=peak.tolist(), front_peak_exponent=pe, front_peak_prefactor=pc) # axis front form (8.6): phi = (1/2) J_rho(u) (2/(pi u))^{(D-1)/2} P_D(u), u = 2 t_f lam pD = 1 / 3 + (D - 1) / 2 cD = 0.6749 * 2 ** (0.5 - D) * (2 / np.pi) ** ((D - 1) / 2) fd = {} for i, d in enumerate(ds): if d >= fit_min: u = 2 * TF * lams[win[i]] fr = 0.5 * jv(d, u) * (2 / (np.pi * u)) ** ((D - 1) / 2) * P_axis(u, int(d), D) fd[int(d)] = float(np.max(np.abs(ph[i][win[i]] - fr)) / np.max(np.abs(fr))) res["front_form_rel_dev"] = fd res["front_peak_times_rho_pD"] = (peak * ds ** pD).tolist() res["lower_bound_cD_over_2"] = cD / 2 if D == 1: res["front_peak_times_d13"] = (peak * ds ** (1 / 3)).tolist() ahead = {} for i, d in enumerate(ds): m = 2 * TF * lams <= 0.8 * d ahead[int(d)] = float(np.max(np.abs(ph[i][m]))) res["max_abs_phi_for_2tlam_le_0p8rho"] = ahead log(f"[{label}] front ({time.time() - t0:.0f}s):", res) return res # ================================================================ item 2 (i): formation, sudden def formation_sudden(sec, g, lp, ds, dl, lam_w, epsF, fit_min, label): D = sec["D"] sel = [sec["axis"](int(d + s)) for d in ds for s in (-1, 1)] v0 = np.zeros(sec["M"], complex) t0 = time.time() nst = int(lam_w / dl) ph, _ = propagate_const(sec, g, v0, dl, nst, sel) lams = dl * np.arange(1, nst + 1) G, Gst = grad(ph, lp, ds) zs = zeta_star(epsF, D) lf, coll = [], {} for i, d in enumerate(ds): ratio = G[i] / Gst[i] lf.append(last_entry(lams, 1 - ratio, epsF)) zeta = d ** 2 / (4 * TF * lams) m = zeta <= 0.5 coll[int(d)] = float(np.max(np.abs(ratio[m] - gD(zeta[m], D)))) lf = np.array(lf) big = ds >= fit_min a, c = powerfit(ds[big], lf[big]) res = dict(window_end=float(lam_w), eps=epsF, zeta_star=zs, d=ds.tolist(), lam_form=lf.tolist(), lam_form_pred=(ds ** 2 / (4 * TF * zs)).tolist(), fit_exponent=a, fit_min_d=int(fit_min), fit_prefactor=c, pred_prefactor=1 / (4 * TF * zs), max_dev_from_scaling_fn_zeta_le_0p5=coll) log(f"[{label}] formation sudden ({time.time() - t0:.0f}s):", res) return res # ================================================================ first order, sum rule, lambda-average def small_checks(sec, g, lp, S2, lams, rs, label, running=()): sel = [sec["axis"](int(r)) for r in rs] H = sec["H0"].toarray() H[0, 0] += g E, V = np.linalg.eigh(H) ph = sudden_dense(sec, g, lams, sel, eig=(E, V)) ph1, st = first_order_dense(sec, lams, sel) res = dict(L=sec["L"], D=sec["D"], g_s_over_t_f=g, sector_dim=sec["M"], S2=float(S2), static_sector_vs_fourier=float(np.max(np.abs(st + lp[rs]))), exact_vs_first_order_rel=float(np.max(np.abs(ph - ph1)) / abs(lp[0]))) a_ = V.T @ sec["c0"] davg = np.array([((a_ ** 2) @ (V[o] ** 2) - sec["c0"][o] ** 2) / sec["size"][o] * TF * sec["X"] / (2 * g) for o in sel]) res["infinite_lambda_average_vs_static_rel"] = float(np.max(np.abs(davg + lp[rs])) / abs(lp[0])) phs = sudden_dense(sec, g, lams[[0, len(lams) // 2, -1]], list(range(sec["M"])), eig=(E, V)) res["sum_rule_max_abs"] = float(np.max(np.abs((phs * sec["size"][:, None]).sum(axis=0)))) run = {} dE = E[:, None] - E[None, :] for cL in running: Lam = cL * sec["L"] ** 2 / TF x = -1j * dE * Lam K = np.where(np.abs(dE) > 1e-14, np.expm1(x) / np.where(np.abs(dE) > 1e-14, x, 1.0), 1.0) devs, devx = [], [] for o, r, da in zip(sel, rs, davg): w = a_ * V[o] avg = (np.einsum("i,ij,j->", w, K, w).real - sec["c0"][o] ** 2) / sec["size"][o] * TF * sec["X"] / (2 * g) devs.append(abs(avg + lp[r])) devx.append(abs(avg - da)) run[f"{cL}L^2/t"] = dict(max_dev_from_static_phi=float(max(devs)), max_dev_from_exact_average_phi=float(max(devx)), bound_S2_over_tLambda=float(S2 / (TF * Lam))) if running: res["running_average"] = run log(f"[{label}] small checks:", res) return res def remainder_check(L, D, g, lam_max, rs, label): """Exact evolution against first order at finite g; bounds (8.5)/(8.18) in units 2 n |g| / t_f: |phi - phi1| <= t_f (e^{2|g|lam} - 1 - 2|g|lam) B / (2|g|), |phi| <= t_f (e^{2|g|lam} - 1) B / (2|g|), B(r, lam) = max_{s <= lam} |U(r, s)| (running maximum on the grid).""" sec = sector(L, D) sel = [sec["axis"](int(r)) for r in rs] lams = np.linspace(lam_max / 4000, lam_max, 4000) ph = sudden_dense(sec, g, lams, sel) ph1, _ = first_order_dense(sec, lams, sel) E, V = np.linalg.eigh(sec["H0"].toarray()) W = V[sel, :] * V[0, :][None, :] / np.sqrt(sec["size"][sel])[:, None] B = np.maximum.accumulate(np.abs(W @ np.exp(-1j * np.outer(E, lams))), axis=1) x = 2 * abs(g) * lams b_rem = TF * (np.expm1(x) - x) * B / (2 * abs(g)) b_tot = TF * np.expm1(x) * B / (2 * abs(g)) m = b_rem > 1e-8 # ratios where the bound is above the round-off level of the dense evolution res = dict(L=L, D=D, g_s_over_t_f=g, lam_max=lam_max, max_abs_g_lam=float(abs(g) * lam_max), r=[int(r) for r in rs], max_ratio_remainder_to_bound_where_bound_gt_1em8=[float(np.max(np.abs(ph[i] - ph1[i])[m[i]] / b_rem[i][m[i]])) for i in range(len(rs))], max_excess_remainder_over_bound=[float(np.max(np.abs(ph[i] - ph1[i]) - b_rem[i])) for i in range(len(rs))], max_ratio_total_to_bound=[float(np.max(np.abs(ph[i]) / b_tot[i])) for i in range(len(rs))], max_excess_total_over_bound=[float(np.max(np.abs(ph[i]) - b_tot[i])) for i in range(len(rs))], max_abs_remainder_phi=[float(np.max(np.abs(ph[i] - ph1[i]))) for i in range(len(rs))]) log(f"[{label}] finite-coupling bounds (8.5), (8.18):", res) return res def integrator_checks(): """Chebyshev propagation against dense diagonalization.""" sec = sector(16, 3) g = 1e-3 sel = [sec["axis"](d) for d in range(9)] lams = 0.05 * np.arange(1, 401) ph, _ = propagate_const(sec, g, np.zeros(sec["M"], complex), 0.05, 400, sel) ph_big, _ = propagate_const(sec, g, np.zeros(sec["M"], complex), 2.0, 10, sel) ref = sudden_dense(sec, g, lams, sel) res = dict(cube_L=16, cheb_vs_dense_step_0p05=float(np.max(np.abs(ph - ref))), cheb_vs_dense_step_2=float(np.max(np.abs(ph_big - ref[:, 39::40])))) log("[integrator checks]", res) return res if __name__ == "__main__": T0 = time.time() RES["integrator_checks"] = integrator_checks() # ---------------- finite coupling: bounds (8.18) and (8.5) at every order RES["finite_coupling"] = dict( ring_L256_pos=remainder_check(256, 1, 0.02, 50.0, np.array([0, 4, 16, 64, 120]), "ring L=256, g=+0.02"), ring_L256_neg=remainder_check(256, 1, -0.02, 50.0, np.array([0, 4, 16, 64, 120]), "ring L=256, g=-0.02"), cube_L16_pos=remainder_check(16, 3, 0.05, 20.0, np.array([0, 2, 5, 8]), "cube L=16, g=+0.05")) # ---------------- ring L = 1024 (dense): first order, sum rule, lambda-average sec = sector(1024, 1) lp, S2 = lam_plus_axis(1024, 1, 512) RES["ring_L1024"] = small_checks(sec, 1e-5, lp, S2, np.linspace(1, 2000, 2000), np.array([0, 8, 64, 256]), "ring L=1024", running=(1.0, 4.0, 16.0)) # ---------------- ring L = 16384: front, and sudden formation before the wrap time L = 16384 sec = sector(L, 1) lp, S2 = lam_plus_axis(L, 1, 64) RES["ring_L16384"] = dict(L=L, g_s_over_t_f=1e-5, sector_dim=sec["M"]) RES["ring_L16384"]["front"] = front(sec, 1e-5, np.array([16, 24, 32, 48, 64, 96, 128, 160, 192, 256, 320, 384]), 0.02, 205.0, 0.5, 0.1, 64, "ring L=16384") RES["ring_L16384"]["formation_sudden"] = formation_sudden(sec, 1e-5, lp, np.array([6, 8, 12, 16, 24, 32, 40]), 0.5, 0.45 * L / TF, 0.2, 12, "ring L=16384") # ---------------- cube L = 32 (dense): first order, sum rule, lambda-average sec = sector(32, 3) lp, S2 = lam_plus_axis(32, 3, 16) RES["cube_L32"] = small_checks(sec, 1e-3, lp, S2, np.linspace(0.1, 300, 3000), np.arange(0, 17), "cube L=32", running=(1.0, 4.0)) # ---------------- cube L = 160: front, and sudden formation before the wrap time L = 160 sec = sector(L, 3) lp, S2 = lam_plus_axis(L, 3, 16) RES["cube_L160"] = dict(L=L, g_s_over_t_f=1e-3, sector_dim=sec["M"]) RES["cube_L160"]["front"] = front(sec, 1e-3, np.array([6, 8, 10, 12, 16, 20, 24, 32, 40, 48, 56, 64]), 0.05, 38.0, 1.5, 0.1, 12, "cube L=160") RES["cube_L160"]["formation_sudden"] = formation_sudden(sec, 1e-3, lp, np.array([3, 4, 5, 6, 7, 8, 9]), 0.1, 0.45 * L / TF, 0.1, 4, "cube L=160") log(f"total time {time.time() - T0:.0f}s") (OUT / "check_front_formation.json").write_text(json.dumps(RES, indent=1)) (OUT / "check_front_formation.log").write_text("\n".join(LOG) + "\n")