#!/usr/bin/env python3 """Generate exact tables and explicitly labeled model illustrations. Run from any working directory. No network access is required. Figures are not experimental physical data; CSV/JSON values follow the manuscript's formulas. """ from __future__ import annotations import csv import json import math import sys from pathlib import Path ROOT = Path(__file__).resolve().parents[1] sys.path.insert(0, str(ROOT / 'src')) import numpy as np import sympy as sp import matplotlib matplotlib.use('Agg') import matplotlib.pyplot as plt from noulith import TwistedAlgebra from noulith.protocols import root_profile from noulith.geometry import line_arrangement_generators def write_csv(name: str, rows: list[dict]) -> None: with (ROOT / 'data' / name).open('w', newline='', encoding='utf-8') as file: writer = csv.DictWriter(file, fieldnames=list(rows[0])) writer.writeheader() writer.writerows(rows) def save(fig, name: str) -> None: fig.tight_layout() fig.savefig(ROOT / 'figures' / f'{name}.pdf', bbox_inches='tight') fig.savefig(ROOT / 'figures' / f'{name}.png', dpi=180, bbox_inches='tight') plt.close(fig) def main() -> None: (ROOT / 'data').mkdir(exist_ok=True) (ROOT / 'figures').mkdir(exist_ok=True) gap_rows = [] for p in range(2, 17): m = 2 while math.comb(m, 2) < p + 1: m += 1 gap_rows.append(dict(p=p, channels=m, state_dimension=2**m, length_J=p*p, length_K=p*(p+1)//2, length_gap=p*(p-1)//2, minimal_protocols_J=2**m+1, minimal_protocols_K=2**m+p, protocol_gap=p-1)) write_csv('arc_blind_family.csv', gap_rows) fig, ax = plt.subplots(figsize=(6.6, 3.9)) ax.plot([r['p'] for r in gap_rows], [r['length_J'] for r in gap_rows], 'o-', label=r'$\dim R/(a^p,b^p)=p^2$') ax.plot([r['p'] for r in gap_rows], [r['length_K'] for r in gap_rows], 's-', label=r'$\dim R/(a,b)^p=p(p+1)/2$') ax.set(xlabel='Power p', ylabel='Local algebra length', title='Equal arc orders, different analytic defects') ax.legend(); ax.grid(True, alpha=.25) save(fig, 'arc_blind_lengths') root_rows = [] for ell in range(2, 8): for d in range(0, 25): for r in range(1, 9): root_rows.append(dict(root_order=ell, degree=d, blocks=r, exponent=int(root_profile(d, r, ell)))) write_csv('root_budget_profiles.csv', root_rows) fig, ax = plt.subplots(figsize=(6.6, 3.9)) degrees = list(range(25)) for r in (1, 2, 3, 5): ax.step(degrees, [root_profile(d,r,3) for d in degrees], where='mid', label=f'{r} block(s)') ax.set(xlabel='Complement degree d', ylabel='Vanishing exponent', title='Third-root resonance: block budget versus order') ax.set_xticks(range(0,25,3)); ax.legend(); ax.grid(True, alpha=.25) save(fig, 'root_budget_profiles') jet_rows=[] m, ell = 12, 3 grid=[] for k in range(5): gridrow=[] for r in range(1,7): threshold=min(m, r*(ell-1)+ell*k) rank=sum(math.comb(m,d) for d in range(threshold+1)) jet_rows.append(dict(channels=m, root_order=ell, blocks=r, jet_order=k, rank=rank, dimension=2**m)) gridrow.append(rank/(2**m)) grid.append(gridrow) for r in range(1,5): for k in range(3): rank=sum(math.comb(8,d) for d in range(min(8,2*r+3*k)+1)) jet_rows.append(dict(channels=8,root_order=3,blocks=r,jet_order=k,rank=rank,dimension=256)) write_csv('root_jet_visibility.csv',jet_rows) fig, ax = plt.subplots(figsize=(6.6, 3.9)) im=ax.imshow(np.array(grid),origin='lower',aspect='auto',extent=(.5,6.5,-.5,4.5),vmin=0,vmax=1) ax.set(xlabel='Block budget r',ylabel='Parameter jet order k',title='Visible constant-state fraction: m = 12, root order 3') fig.colorbar(im,ax=ax,label='Visible fraction') save(fig,'jet_visibility') hilbert_rows=[] for m in range(4,11): for degree in range(8): value = 1 if degree==0 else (m-1 if degree==1 else m) hilbert_rows.append(dict(channels=m,degree=degree,hilbert_function=value)) write_csv('branch_hilbert_functions.csv',hilbert_rows) fig,ax=plt.subplots(figsize=(6.6,3.9)) for m in (4,6,8): ax.plot(range(8), [1,m-1]+[m]*6,'o-',label=f'{m} branches') ax.set(xlabel='Degree',ylabel='Graded dimension',title='Exact second-deficit branch-ring Hilbert functions') ax.set_xticks(range(8)); ax.legend(); ax.grid(True,alpha=.25) save(fig,'branch_hilbert') # Geometric illustration of the exact normal form in three log-coordinates. fig=plt.figure(figsize=(6.3,4.5)) ax=fig.add_subplot(projection='3d') ts=np.linspace(-1,1,101) for direction,label in (([1,0,0],'channel 2 outlier'),([0,1,0],'channel 3 outlier'), ([0,0,1],'channel 4 outlier'),([1,1,1],'channel 1 outlier')): a=np.outer(ts,np.array(direction,dtype=float)) ax.plot(a[:,0],a[:,1],a[:,2],label=label) ax.set(xlabel=r'$z_2$',ylabel=r'$z_3$',zlabel=r'$z_4$',title='Four-channel resonance germ in logarithmic coordinates') ax.legend(loc='upper left',fontsize=7) save(fig,'four_branch_geometry') # Numerical illustration only; exact valuation claims have independent tests. import mpmath as mp mp.mp.dps=65 zeta=mp.exp(2*mp.pi*1j/3) def qfac(d,q): return mp.fprod(mp.fsum(q**j for j in range(k)) for k in range(1,d+1)) detuning_rows=[] figureseries=[] for composition in ((6,),(2,4),(2,2,2)): values=[] for exponent in np.linspace(-5,-1,41): t=mp.mpf(str(10**float(exponent))) value=abs(mp.fprod(qfac(d,zeta*(1+t)) for d in composition)) values.append(float(value)) detuning_rows.append(dict(composition='+'.join(map(str,composition)),t=float(t),amplitude=float(value), predicted_order=sum(d//3 for d in composition))) figureseries.append((composition, values)) write_csv('detuning_amplitudes.csv',detuning_rows) fig,ax=plt.subplots(figsize=(6.6,3.9)) ts=np.logspace(-5,-1,41) for composition,values in figureseries: ax.loglog(ts,values,label=' + '.join(map(str,composition))+f' ; order {sum(d//3 for d in composition)}') ax.set(xlabel='Detuning t',ylabel='Normalized isolated coefficient magnitude',title='Depth six: the cost of restricting block changes') ax.legend(); ax.grid(True,which='both',alpha=.25) save(fig,'detuning_amplitudes') A,B,C=sp.symbols('A B C') algebra=TwistedAlgebra(3,{(0,1):-1+A,(0,2):-1+B,(1,2):-1+C}) triple=sp.expand(algebra.shuffle_table()[-1]) z=sp.symbols('z2:5') certificate=dict(triple_shuffle=str(triple), expected_triple='A*B*C - A*C + A - B + C', four_branch_ideal=[str(x) for x in line_arrangement_generators(z)], definitions='Illustrations of proved abstract-model formulas; not physical experiments.', exactness={'tables':'integer arithmetic except detuning_amplitudes.csv', 'detuning':'65-digit mpmath evaluation exported as binary64 decimal values'}) assert sp.expand(triple-(A*B*C-A*C+A-B+C))==0 (ROOT/'data'/'symbolic_certificates.json').write_text(json.dumps(certificate,indent=2)+'\n') # Exact full-state ranks, distinct from the scalar branch curve. strata=[] for m in range(4,13): n=2**m for stratum,loss in [('outside_stars',0),('generic_single_star',1), ('nonzero_outlier_branch',2),('nonzero_two_star_intersection',2),('exterior_origin',m+1)]: strata.append(dict(channels=m,blocks=m-2,stratum=stratum,rank=n-loss,state_dimension=n)) write_csv('full_state_rank_strata.csv',strata) # Editable TeX tables are generated from exact data, not handwritten values. arc=[r'\begin{center}',r'\begin{tabular}{rrrrrrr}',r'\toprule', r'$p$ & $m$ & $2^m$ & $\dim R/J_p$ & $\dim R/K_p$ & $N(J_p)$ & $N(K_p)$\\',r'\midrule'] for row in gap_rows[:7]: keys=['p','channels','state_dimension','length_J','length_K','minimal_protocols_J','minimal_protocols_K'] arc.append(' & '.join(str(row[key]) for key in keys)+r'\\') arc += [r'\bottomrule',r'\end{tabular}',r'\end{center}'] (ROOT/'manuscript'/'generated_arc_table.tex').write_text('\n'.join(arc)+'\n') jet=[r'\begin{center}',r'\begin{tabular}{rrrr}',r'\toprule', r'Blocks $r$ & Jet $k=0$ & Jet $k=1$ & Jet $k=2$\\',r'\midrule'] for r in range(1,5): counts=[next(row['rank'] for row in jet_rows if row['channels']==8 and row['blocks']==r and row['jet_order']==k) for k in range(3)] jet.append(' & '.join(map(str,[r]+counts))+r'\\') jet += [r'\bottomrule',r'\end{tabular}',r'\end{center}'] (ROOT/'manuscript'/'generated_jet_table.tex').write_text('\n'.join(jet)+'\n') print('Generated six figures, six CSV tables, two TeX tables, and symbolic_certificates.json.') if __name__=='__main__': main()