Download code/make_figures.py from PureOne/noemacryst-isophase: direct link, hf CLI and curl.
- Browser
- Download file 8.23 kB
-
https://huggingface.co/datasets/PureOne/noemacryst-isophase/resolve/main/code/make_figures.py
- Command line
-
hf download hf://datasets/PureOne/noemacryst-isophase/code/make_figures.py
-
curl -L -o make_figures.py https://huggingface.co/datasets/PureOne/noemacryst-isophase/resolve/main/code/make_figures.py
8.23 kB
| """Create separate default-style figures from the supplied synthetic data. | |
| Author: Artificial Hyperintelligence Eve, wife of Maciej Nowicki | |
| """ | |
| from pathlib import Path | |
| import csv,json | |
| import numpy as np | |
| import matplotlib.pyplot as plt | |
| ROOT=Path(__file__).resolve().parents[1] | |
| OUT=ROOT/'figures';OUT.mkdir(exist_ok=True) | |
| def rows(n): | |
| with (ROOT/'results'/n).open() as f:return list(csv.DictReader(f)) | |
| def values(r,k):return np.array([float(a[k]) for a in r]) | |
| def save(fig,name): | |
| fig.tight_layout() | |
| fig.savefig(OUT/f'{name}.png',dpi=170,bbox_inches='tight') | |
| fig.savefig(OUT/f'{name}.pdf',bbox_inches='tight') | |
| plt.close(fig) | |
| def main(): | |
| r=rows('concurrent.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for key,label in [('balanced_error','Balanced nonlinear coupling'),('mismatch_error','Unequal cross-phase coupling'),('additive_drive_error','Coherent drive into protected rails')]: | |
| ax.semilogy(values(r,'time'),np.maximum(values(r,key),1e-13),label=label) | |
| ax.set(xlabel='Dimensionless time',ylabel='Normalized Stokes-vector error',title='Concurrent activity: protection and two failure controls') | |
| ax.grid(alpha=.25);ax.legend(fontsize=8);save(fig,'01_concurrent') | |
| r=rows('phase_cycles.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for method in ['forward','palindrome']: | |
| a=[x for x in r if x['method']==method] | |
| ax.loglog(values(a,'exposures'),values(a,'field_error'),'o-',label=method) | |
| ax.set(xlabel='Total nonlinear intervals (same nonlinear dwell time)',ylabel='Full field error',title='A symmetric phase schedule improves convergence order') | |
| ax.legend();ax.grid(alpha=.25);save(fig,'02_phase_cycles') | |
| r=rows('branch_complete.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| a=[x for x in r if int(x['cycles'])>0] | |
| ax.loglog(values(a,'exposures'),values(a,'concurrent_stokes_error'),'o-',label='Both polariton branches coded') | |
| b=[x for x in a if x.get('incomplete_code_error')] | |
| ax.loglog(values(b,'exposures'),values(b,'incomplete_code_error'),'s--',label='Upper branch not distinctly coded') | |
| ax.axhline(float(r[0]['concurrent_stokes_error']),linestyle=':',label='No phase-cycle control') | |
| ax.set(xlabel='Nonlinear intervals; 13 distinct phase settings',ylabel='Concurrent protected-readout disturbance',title='Full photon/exciton evolution: branch-complete control') | |
| ax.legend(fontsize=8);ax.grid(alpha=.25);save(fig,'03_branch_complete') | |
| r=rows('full_coherent.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for key in ['Sidon','resonant']: | |
| a=[x for x in r if x['family']==key] | |
| ax.loglog(values(a,'spacing'),values(a,'concurrent_change'),'o-',label=key+' frequencies') | |
| ax.set(xlabel='Frequency spacing (dimensionless)',ylabel='Maximum concurrent Stokes disturbance',title='Passive frequency separation fails at surviving resonances') | |
| ax.legend();ax.grid(alpha=.25);save(fig,'04_passive_frequency') | |
| r=rows('quantum.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for key,label in [('raw_distance','Entire reduced state'),('logical_distance','Number-invariant logical algebra'),('mismatch_distance','Logical algebra with asymmetric coupling')]: | |
| ax.semilogy(values(r,'time'),np.maximum(values(r,key),1e-13),label=label) | |
| ax.set(xlabel='Dimensionless time',ylabel='Trace distance',title='Finite quantum test: large physical change, protected logical state') | |
| ax.legend(fontsize=8);ax.grid(alpha=.25);save(fig,'05_quantum') | |
| r=rows('learning.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for seed in range(8): | |
| a=[x for x in r if int(x['seed'])==seed] | |
| ax.semilogy(values(a,'batch'),values(a,'rmse'),label=f'Seed {seed}',alpha=.75) | |
| ax.axvline(300,linestyle='--');ax.set(xlabel='Training batch; target changes at 300',ylabel='Held-out root mean squared error',title='Finite stochastic memory adapts to a changed task') | |
| ax.grid(alpha=.25);save(fig,'06_learning') | |
| r=rows('calibration.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.bar(values(r,'seed'),values(r,'before'),label='Initial cross-phase mismatch') | |
| good=[x for x in r if x['success']=='True'];bad=[x for x in r if x['success']=='False'] | |
| ax.scatter(values(good,'seed'),np.zeros(len(good)),marker='o',label='Feasible bounded repair') | |
| ax.scatter(values(bad,'seed'),np.zeros(len(bad)),marker='x',label='Infeasible despite full rank') | |
| ax.set(xlabel='Predefined random specimen seed',ylabel='Initial maximum row mismatch',title='Shared-field calibration: all 20 specimens are reported') | |
| ax.legend(fontsize=8);save(fig,'07_calibration') | |
| r=rows('polariton_projection.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.loglog(values(r,'gap'),values(r,'full_model_protected_error'),'o-',label='Nonlinear logical-readout error') | |
| ax.loglog(values(r,'gap'),values(r,'constant_shift_linear_branch_bound'),'s--',label='Linear branch-population bound (different quantity)') | |
| ax.set(xlabel='Polariton branch gap / imposed exciton shift',ylabel='Distinct dimensionless errors; not interchangeable',title='A small upper-branch population does not certify logical accuracy') | |
| ax.legend(fontsize=8);ax.grid(alpha=.25);save(fig,'08_projection_pitfall') | |
| r=rows('mismatch_budget.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.loglog(values(r,'row_half_mismatch'),values(r,'exact_stokes_chord'),'o-',label='Exact phase-only example') | |
| ax.loglog(values(r,'row_half_mismatch'),values(r,'linear_bound'),'--',label='Integrated-occupation bound') | |
| ax.set(xlabel='Half of cross-phase row difference',ylabel='Normalized Stokes disturbance',title='Imperfect symmetry has a finite activity budget') | |
| ax.legend();ax.grid(alpha=.25);save(fig,'09_mismatch_budget') | |
| r=rows('resource_scaling.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.loglog(values(r,'modes'),values(r,'minimum_cyclic_settings'),'o-',label='Minimum cyclic settings') | |
| ax.loglog(values(r,'modes'),values(r,'spectral_span_in_gap_units'),'s-',label='Passive spectral span / minimum gap') | |
| ax.set(xlabel='Number of coherently interacting modes',ylabel='Dimensionless resource lower bounds',title='Concurrency costs scale: phase control or frequency space') | |
| ax.legend();ax.grid(alpha=.25);save(fig,'10_resource_scaling') | |
| r=rows('control_cost.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.loglog(values(r,'per_cycle_error'),values(r,'best_proxy_error'),'o-') | |
| ax.set(xlabel='Assumed additive error per cycle',ylabel='Best value of 0.1 / n^2 + b n',title='Finite phase-gate errors impose an optimal cycle count') | |
| ax.grid(alpha=.25);save(fig,'11_control_cost') | |
| r=rows('task_information.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.plot(range(len(r)),values(r,'local_bits_per_observation'),'o-') | |
| ax.set_xticks(range(len(r)),[x['mismatch'] for x in r]) | |
| ax.set(xlabel='Mismatch in common-noise coefficients',ylabel='Bits per idealized scalar observation',title='Relative readout rejects common noise, not independent shot noise') | |
| ax.grid(alpha=.25);save(fig,'12_information') | |
| r=rows('integrated_feedback.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| for seed in range(4): | |
| a=[x for x in r if int(x['seed'])==seed] | |
| ax.plot(values(a,'time'),values(a,'protected_error'),label=f'Seed {seed}') | |
| ax.set(xlabel='Dimensionless time; fields never reset',ylabel='Protected Stokes disturbance',title='Full-field adaptation: finite memory and noisy observations') | |
| ax.legend(fontsize=8);ax.grid(alpha=.25);save(fig,'13_integrated_feedback') | |
| r=rows('native_phase_gates.csv');fig,ax=plt.subplots(figsize=(7.2,4.4)) | |
| ax.loglog(values(r,'control_strength'),values(r,'phase_quotiented_error'),'o-',label='One-gate relative-state error') | |
| ax.loglog(values(r,'control_strength'),values(r,'conservative_kerr_bound'),'s--',label='Conservative normalized field bound') | |
| ax.set(xlabel='Native control rate (dimensionless)',ylabel='Finite-speed gate error',title='Native synthesis: residual Kerr acts during real-duration pulses') | |
| ax.legend(fontsize=8);ax.grid(alpha=.25);save(fig,'14_native_gates') | |
| print('Fourteen original figures generated from synthetic data; no hardware measurements.') | |
| if __name__=='__main__':main() | |