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| #!/usr/bin/env python3 | |
| """Standalone exact and truncated causal-return capsule verification. | |
| Run: python v5_dynamic_verify.py [--quick] [--output-prefix v5_dynamic] | |
| Requires NumPy and Matplotlib. No earlier ELYSIAEN modules are imported. | |
| This is a finite positive discrete-time system, not a measured optical device. | |
| The time index is explicitly an implemented state update; a steady radiance | |
| fixed point is not automatically identified with physical or game-frame time. | |
| """ | |
| from __future__ import annotations | |
| import os | |
| os.environ["OPENBLAS_NUM_THREADS"] = "1" | |
| os.environ["OMP_NUM_THREADS"] = "1" | |
| import argparse | |
| import json | |
| import platform | |
| from pathlib import Path | |
| import numpy as np | |
| SEED = 2026102553 | |
| def wnorm(x, weight): | |
| x = np.asarray(x) | |
| return float(np.max(np.abs(x)/weight.reshape((-1,)+(1,)*(x.ndim-1)), initial=0.)) | |
| def row_map(rng, rows, cols, out_weight, in_weight, budget): | |
| a = rng.uniform(.03, 1., (rows, cols)) | |
| a *= (budget*out_weight/(a@in_weight))[:, None] | |
| return a | |
| def precompute(U, D, V, W, OZ, OF, steps): | |
| K, F, J, Q = [], [], [], [] | |
| power = np.eye(D.shape[0]) | |
| for j in range(steps): | |
| K.append(U@power@V); F.append(U@power@W) | |
| J.append(OF@power@V); Q.append(OF@power@W) | |
| power = power@D | |
| return K, F, J, Q | |
| def initial_traces(U, D, OF, exterior0, steps): | |
| phi=[]; psi=[]; initial=exterior0.copy() | |
| for t in range(steps+1): | |
| phi.append(U@initial); psi.append(OF@initial); initial=D@initial | |
| return phi, psi | |
| def causal(K, F, J, Q, OZ, Bs, Ls, Rs, local_source, | |
| xi, z0, phi, psi, horizon, *, wrong_current_egress=False): | |
| """Exact when horizon>=steps; otherwise only last horizon impulses kept. | |
| Initial exterior traces phi/psi are compiled before this routine. | |
| A deployed capsule needs their declared initial-state basis or a budget | |
| for dropping them. No exterior-sized array is read in this evaluator. | |
| """ | |
| steps, k = len(Bs), len(z0) | |
| z = np.zeros((steps+1, k)); z[0] = z0 | |
| y = np.zeros((steps+1, OZ.shape[0])) | |
| for t in range(steps+1): | |
| incoming = phi[t].copy() | |
| y[t] = OZ@z[t]+psi[t] | |
| for j in range(min(t, horizon)): | |
| old = t-1-j | |
| egress = Rs[min(t, steps-1)] if wrong_current_egress else Rs[old] | |
| outgoing = egress@z[old] | |
| incoming += K[j]@outgoing+F[j]@xi[old] | |
| y[t] += J[j]@outgoing+Q[j]@xi[old] | |
| if t < steps: | |
| z[t+1] = Bs[t]@z[t]+local_source[t]+Ls[t]@incoming | |
| return z, y | |
| def full_oracle(U, D, V, W, OZ, OF, Bs, Ls, Rs, source, xi, z0, f0): | |
| steps, k, nf = len(Bs), len(z0), len(f0) | |
| states = np.zeros((steps+1, k+nf)); states[0] = np.r_[z0, f0] | |
| for t in range(steps): | |
| z, v = states[t, :k], states[t, k:] | |
| states[t+1, :k] = Bs[t]@z+Ls[t]@U@v+source[t] | |
| states[t+1, k:] = D@v+V@Rs[t]@z+W@xi[t] | |
| return states[:, :k], states[:, :k]@OZ.T+states[:, k:]@OF.T | |
| def trial(rng, number, steps): | |
| k = (2, 3, 4)[number % 3] | |
| nf = (7, 12, 20)[(number//3) % 3] | |
| delta = (.2, .6, .9)[(number//9) % 3] | |
| a = np.exp(rng.uniform(-.7, .7, k)) | |
| w = np.exp(rng.uniform(-.7, .7, nf)) | |
| D = row_map(rng, nf, nf, w, w, delta) | |
| U = row_map(rng, k, nf, a, w, .18*np.sqrt(1-delta)) | |
| V = row_map(rng, nf, k, w, a, .25*np.sqrt(1-delta)) | |
| W = rng.uniform(.001, .02, (nf, 2))*w[:, None] | |
| OZ = rng.uniform(-.5, .8, (3, k)) | |
| OF = rng.uniform(-.2, .4, (3, nf)) | |
| Bbar = row_map(rng, k, k, a, a, (.4, .7)[number % 2]) | |
| Lbar = row_map(rng, k, k, a, a, .85) | |
| Rbar = row_map(rng, k, k, a, a, .9) | |
| H = np.linalg.solve(np.eye(nf)-D, np.eye(nf)) | |
| C = U@H@V | |
| Abar = Bbar+Lbar@C@Rbar | |
| q = float(np.max(Abar@a/a)) | |
| assert q < .9 | |
| # A single upper family, not individual reduced stability, bounds every | |
| # delayed word. This criterion is sufficient and need not be necessary. | |
| full_upper = np.block([[Bbar, Lbar@U], [V@Rbar, D]]) | |
| full_radius=float(max(abs(np.linalg.eigvals(full_upper)))) | |
| assert full_radius < 1 | |
| rate_records=[] | |
| for gamma in ((delta+full_radius)/2,(full_radius+1)/2): | |
| rate_return=Bbar/gamma+(Lbar@U@np.linalg.solve(gamma*np.eye(nf)-D,V)@Rbar)/gamma | |
| local_rate_radius=float(max(abs(np.linalg.eigvals(rate_return)))) | |
| assert (full_radius<gamma)==(local_rate_radius<1) | |
| rate_records.append({'gamma':gamma,'full_radius':full_radius, | |
| 'rate_return_radius':local_rate_radius, | |
| 'admitted':bool(local_rate_radius<1)}) | |
| Bs, Ls, Rs, sources, xis = [], [], [], [], [] | |
| local_upper = .12*a | |
| for t in range(steps): | |
| Bs.append(Bbar*rng.uniform(.3, 1., (k, k))) | |
| Ls.append(Lbar*rng.uniform(.2, 1., (k, k))) | |
| Rs.append(Rbar*rng.uniform(.2, 1., (k, k))) | |
| # Abrupt changes and smooth variation both stay in fixed envelopes. | |
| xis.append(np.array([.4+.3*np.sin(t/7.)**2, .8 if t >= steps//3 else .1])) | |
| sources.append(local_upper*rng.uniform(.1, 1., k)) | |
| z0 = rng.uniform(0, .1, k)*a | |
| exterior0 = np.zeros(nf) if number%2==0 else rng.uniform(0,.1,nf)*w | |
| K, F, J, Q = precompute(U, D, V, W, OZ, OF, steps) | |
| phi,psi=initial_traces(U,D,OF,exterior0,steps) | |
| exact_z, exact_y = full_oracle(U, D, V, W, OZ, OF, Bs, Ls, Rs, sources, xis, z0, exterior0) | |
| memory_z, memory_y = causal(K, F, J, Q, OZ, Bs, Ls, Rs, sources, xis, z0, phi,psi, steps) | |
| exact_error = max(wnorm((exact_z-memory_z).T, a), float(np.max(abs(exact_y-memory_y)))) | |
| assert exact_error < 2e-11 | |
| forcing_upper = local_upper+Lbar@U@H@W@np.ones(2)+Lbar@U@(wnorm(exterior0,w)*w) | |
| z_budget = max(wnorm(z0, a), wnorm(forcing_upper, a)/(1-q)) | |
| zbar = z_budget*a | |
| assert np.max(exact_z-zbar) <= 1e-11 | |
| full_output_gain = (abs(OZ)+abs(OF)@H@V@Rbar)@a | |
| records = [] | |
| for h in (0, 1, 2, 4, 8, 16): | |
| approximate_z, approximate_y = causal(K, F, J, Q, OZ, Bs, Ls, Rs, sources, xis, z0, phi,psi, h) | |
| assert np.max(approximate_z-zbar) <= 2e-11 | |
| assert np.max(approximate_z-exact_z) <= 2e-11 | |
| tail_power = np.linalg.matrix_power(D, h) | |
| exterior_drive = V@Rbar@zbar+W@np.ones(2) | |
| incoming_tail = Lbar@U@tail_power@H@exterior_drive | |
| local_bound = wnorm(incoming_tail, a)/(1-q) | |
| output_tail = abs(OF)@tail_power@H@exterior_drive | |
| output_bound = full_output_gain*local_bound+output_tail | |
| local_error = wnorm((exact_z-approximate_z).T, a) | |
| output_error = np.max(abs(exact_y-approximate_y), axis=0) | |
| assert local_error <= local_bound+2e-10*max(1., local_bound) | |
| assert np.all(output_error <= output_bound+2e-10*np.maximum(1., output_bound)) | |
| records.append({"horizon": h, "local_error": local_error, | |
| "local_uniform_bound": local_bound, | |
| "maximum_output_error": float(max(output_error)), | |
| "maximum_output_uniform_bound": float(max(output_bound)), | |
| "local_error_to_bound": local_error/local_bound if local_bound else 0., | |
| "output_error_to_componentwise_bound": float(np.max(output_error/output_bound))}) | |
| wrong_z, wrong_y = causal(K, F, J, Q, OZ, Bs, Ls, Rs, sources, xis, z0, phi,psi, steps, wrong_current_egress=True) | |
| wrong_error = wnorm((wrong_z-exact_z).T, a) | |
| # Compute an a-priori scalar horizon from ||D||<=delta. The matrix-tail | |
| # certificate above is generally sharper and retains propagation shape. | |
| alpha = float(np.max(U@w/a)); ell = float(np.max(Lbar@a/a)) | |
| drive_norm = wnorm(V@Rbar@zbar+W@np.ones(2), w) | |
| prefactor = ell*alpha*drive_norm/((1-delta)*(1-q)) | |
| target = .001 | |
| required_h = max(0, int(np.ceil(np.log(target/prefactor)/np.log(delta)))) if prefactor>target else 0 | |
| assert prefactor*delta**required_h <= target+1e-12 | |
| return {"local_states": k, "exterior_states": nf, "steps": steps, | |
| "exterior_contraction_delta": delta, "upper_return_witness_q": q, | |
| "initial_exterior_is_zero":bool(np.all(exterior0==0)), | |
| "rate_threshold_checks":rate_records, | |
| "exact_causal_maximum_error": exact_error, | |
| "wrong_current_egress_error": wrong_error, | |
| "scalar_horizon_for_local_error_0_001": required_h, | |
| "retained_kernel_scalars_per_history_step": k*k+k*2+3*k+3*2, | |
| "records": records}, (exact_z, memory_z, records) | |
| def counterexamples(): | |
| # Stable reference with coupling .5. Every reduced closure is zero, but | |
| # the actual switched exterior carries a delayed amplifying path. | |
| U=V=np.array([[.5]]); D=np.zeros((1,1)); W=np.zeros((1,1)) | |
| OZ=np.array([[1.]]); OF=np.array([[1.]]) | |
| steps=16 | |
| Bs=[np.zeros((1,1)) for _ in range(steps)] | |
| Ls=[np.array([[4. if t%2==0 else 0.]]) for t in range(steps)] | |
| Rs=[np.array([[0. if t%2==0 else 4.]]) for t in range(steps)] | |
| zero=[np.zeros(1) for _ in range(steps)] | |
| K,F,J,Q=precompute(U,D,V,W,OZ,OF,steps) | |
| phi,psi=initial_traces(U,D,OF,np.ones(1),steps) | |
| z,y=full_oracle(U,D,V,W,OZ,OF,Bs,Ls,Rs,zero,zero,np.zeros(1),np.ones(1)) | |
| causal_z,causal_y=causal(K,F,J,Q,OZ,Bs,Ls,Rs,zero,zero,np.zeros(1),phi,psi,steps) | |
| wrong_z,wrong_y=causal(K,F,J,Q,OZ,Bs,Ls,Rs,zero,zero,np.zeros(1),phi,psi,steps,wrong_current_egress=True) | |
| assert np.max(abs(y-causal_y))==0 | |
| assert y[-1,0]==65536. and wrong_y[-1,0]==0 | |
| # A fixed stable world is still not in equilibrium immediately. | |
| fixed=np.array([[.1,.2],[.2,.8]]); source=np.array([.3,.1]) | |
| equilibrium=np.linalg.solve(np.eye(2)-fixed,source) | |
| return {"switching": {"reference_couplings": .5, | |
| "reference_spectral_radius": .5, | |
| "each_reduced_closure": 0., "two_step_full_gain": 4., | |
| "steps": steps, "final_full_output": float(y[-1,0]), | |
| "final_exact_causal_output": float(causal_y[-1,0]), | |
| "final_wrong_current_egress_output": float(wrong_y[-1,0]), | |
| "common_upper_reduced_return": 4., | |
| "correct_envelope_admission_rejects": True}, | |
| "equilibrium_is_not_first_update": {"equilibrium_local_state":float(equilibrium[0]), | |
| "first_dynamic_local_state_from_zero":.3, | |
| "absolute_difference":float(equilibrium[0]-.3)}} | |
| def main(): | |
| parser=argparse.ArgumentParser(description=__doc__) | |
| parser.add_argument("--quick",action="store_true") | |
| parser.add_argument("--output-prefix",default="v5_dynamic") | |
| args=parser.parse_args() | |
| rng=np.random.default_rng(SEED) | |
| ncases=12 if args.quick else 81 | |
| steps=32 if args.quick else 96 | |
| records=[]; example=None | |
| for number in range(ncases): | |
| record,figuredata=trial(rng,number,steps) | |
| records.append(record) | |
| if number==18 or example is None: example=figuredata | |
| negatives=counterexamples() | |
| all_windows=[item for row in records for item in row['records']] | |
| result={"title":"ELYSIAEN exact causal return capsules and finite-memory bounds", | |
| "date":"2026-10-25","seed":SEED,"python":platform.python_version(), | |
| "numpy":np.__version__,"random_switched_worlds":ncases, | |
| "steps_per_world":steps,"finite_horizons_per_world":6, | |
| "exact_causal_comparisons":ncases,"local_tail_certificates":len(all_windows), | |
| "rate_threshold_equivalence_checks":2*ncases, | |
| "nonzero_initial_exterior_cases":sum(not r['initial_exterior_is_zero'] for r in records), | |
| "componentwise_output_tail_certificates":len(all_windows)*3, | |
| "certificate_violations":0, | |
| "maximum_exact_causal_error":max(r['exact_causal_maximum_error'] for r in records), | |
| "maximum_wrong_current_egress_error":max(r['wrong_current_egress_error'] for r in records), | |
| "maximum_local_error_to_uniform_bound":max(r['local_error_to_bound'] for r in all_windows), | |
| "maximum_output_error_to_componentwise_bound":max(r['output_error_to_componentwise_bound'] for r in all_windows), | |
| "maximum_scalar_horizon_for_local_error_0_001":max(r['scalar_horizon_for_local_error_0_001'] for r in records), | |
| "negative_controls":negatives,"records":records, | |
| "scope":"Exact positive discrete-time dynamics; fixed exterior and supplied common upper family. CPU double-precision tests within declared tolerances, not outward-rounded proof, physical photonic timing, hardware energy or universal game dynamics."} | |
| prefix=Path(args.output_prefix); prefix.parent.mkdir(parents=True,exist_ok=True) | |
| prefix.with_name(prefix.name+'_results.json').write_text(json.dumps(result,indent=2)+'\n') | |
| import matplotlib | |
| matplotlib.use('Agg') | |
| import matplotlib.pyplot as plt | |
| plt.rcParams.update({'font.size':10,'axes.spines.top':False,'axes.spines.right':False}) | |
| fig,axes=plt.subplots(1,3,figsize=(13,3.7),constrained_layout=True) | |
| zs,zm,rs=example | |
| axes[0].plot(zs[:,0],color='#6b51b8',label='Full carried state') | |
| axes[0].plot(zm[:,0],'--',color='#27a9b8',label='Exact causal capsule') | |
| axes[0].set(xlabel='Implemented update',ylabel='Local state',title='History preserves chronology');axes[0].legend(fontsize=8) | |
| axes[1].semilogy([r['horizon'] for r in rs],[max(r['local_error'],1e-16) for r in rs],'o-',color='#6b51b8',label='Actual local error') | |
| axes[1].semilogy([r['horizon'] for r in rs],[r['local_uniform_bound'] for r in rs],'s--',color='#27a9b8',label='Uniform tail bound') | |
| axes[1].set(xlabel='Retained history length',ylabel='Weighted maximum error',title='Certified memory truncation');axes[1].legend(fontsize=8) | |
| eta=[];h=[] | |
| for row in records:eta.append(row['exterior_contraction_delta']);h.append(row['scalar_horizon_for_local_error_0_001']) | |
| axes[2].scatter(eta,h,color='#6b51b8',alpha=.45) | |
| axes[2].set(xlabel='Exterior contraction bound',ylabel='Sufficient history length',title='Near-critical memory costs more') | |
| fig.suptitle('ELYSIAEN / causal return capsules — finite numerical model',fontsize=12) | |
| fig.savefig(prefix.with_suffix('.png'),dpi=170);plt.close(fig) | |
| print(json.dumps({k:result[k] for k in ['random_switched_worlds','exact_causal_comparisons','local_tail_certificates','componentwise_output_tail_certificates','certificate_violations','maximum_exact_causal_error','maximum_scalar_horizon_for_local_error_0_001']},indent=2)) | |
| if __name__=='__main__':main() | |