"""Full propagator checks of multistage photon survival and finite dwell. No physical measurements are represented by this script. """ from pathlib import Path import json import numpy as np from scipy.linalg import expm rng=np.random.default_rng(8102028) max_telescope=0.;max_two=0.;max_bound_violation=0. for case in range(250): b=rng.normal(size=3);x=rng.normal(size=3) U0=np.dot(b,b);n0=b/np.sqrt(U0) actual=n0.copy();ideal=n0.copy();rbound=0.;Uprev=U0 for j in range(12): n=b/np.linalg.norm(b);pulse=rng.normal();a=pulse*n b=b+np.cross(x,a);x=x+a U=np.dot(b,b);nn=b/np.sqrt(U);P=np.outer(nn,nn) gamma=rng.uniform(.2,2);dwell=rng.uniform(.01,2) M=expm(-gamma*U*(np.eye(3)-P)*dwell/2) actual=M@actual;ideal=P@ideal eps=np.exp(-gamma*U*dwell/2) rbound+=eps*np.sqrt(U0*(U-Uprev)/(Uprev*U)) Uprev=U theo=U0/U max_telescope=max(max_telescope,abs(np.dot(ideal,ideal)-theo)) max_bound_violation=max(max_bound_violation,abs(np.dot(actual,actual)-theo)-2*rbound) assert abs(np.dot(actual,actual)-theo)<=2*rbound+1e-12 for case in range(100): gamma=rng.uniform(.1,2);t1,t2=rng.uniform(0,3,size=2) n1=np.array([0.,1.,1.])/np.sqrt(2);n2=np.array([0.,1.,0.]) M1=expm(-gamma*2*(np.eye(3)-np.outer(n1,n1))*t1/2) M2=expm(-gamma*4*(np.eye(3)-np.outer(n2,n2))*t2/2) psi=M2@M1@np.array([0.,0.,1.]) e=np.exp(-gamma*t1) pred=((1-e)**2+(1+e)**2*np.exp(-4*gamma*t2))/4 err=abs(np.dot(psi,psi)-pred);max_two=max(max_two,err) assert err<1e-12 result={'seed':8102028,'multistage_histories':250,'stages_per_history':12,'two_stage_checks':100,'max_ideal_telescope_residual':max_telescope,'max_two_stage_residual':max_two,'maximum_error_bound_violation':max_bound_violation,'status':'all checks passed; exact formulas concern the defined loss protocol'} out=Path(__file__).resolve().parent/'results';out.mkdir(exist_ok=True) (out/'quantum_protocol_check.json').write_text(json.dumps(result,indent=2)+'\n') print(json.dumps(result,indent=2))