#!/usr/bin/env python3 """Finite nonabelian operator-module checks and conservative coding certificates. All matrix tests are finite-dimensional illustrations of the accompanying proofs. Certificate plots evaluate stated sufficient bounds for explicitly chosen norm budgets; they are not device measurements or decoder benchmarks. Requires Python 3.10+, NumPy, SciPy, Matplotlib. """ from __future__ import annotations import argparse import csv import itertools import json import math from pathlib import Path import numpy as np from scipy.linalg import expm, svd from scipy.special import gammaln SEED=20261104 TOL=3e-10 I2=np.eye(2,dtype=complex) X=np.array([[0,1],[1,0]],complex) Y=np.array([[0,-1j],[1j,0]],complex) Z=np.diag([1,-1]).astype(complex) SINGLE=[I2,X,Y,Z] def kron(ops:list[np.ndarray])->np.ndarray: a=np.ones((1,1),complex) for op in ops:a=np.kron(a,op) return a def onsite(op:np.ndarray,j:int,n:int)->np.ndarray: return kron([op if k==j else I2 for k in range(n)]) def paulis(n:int)->list[tuple[tuple[int,...],int,np.ndarray]]: return [(label,sum(a!=0 for a in label),kron([SINGLE[a] for a in label])) for label in itertools.product(range(4),repeat=n)] def collective_algebra(n:int)->list[np.ndarray]: """Permutation-invariant Pauli sums form a basis of collective SU(2) algebra.""" groups={} for label,weight,op in paulis(n): counts=tuple(label.count(j) for j in (1,2,3)) groups[counts]=groups.get(counts,np.zeros_like(op))+op answer=[op/np.linalg.norm(op,'fro') for op in groups.values()] assert len(answer)==math.comb(n+3,3) gram=np.array([[np.vdot(a,b) for b in answer] for a in answer]) assert np.linalg.norm(gram-np.eye(len(answer)))np.ndarray: algebra=collective_algebra(n) columns=np.column_stack([(p@a).reshape(-1) for label,w,p in paulis(n) if w<=s for a in algebra]) u,singular,_=svd(columns,full_matrices=False) rank=int(np.sum(singular>1e-10*singular[0])) return u[:,:rank] def model_hamiltonians(r:int)->tuple[np.ndarray,np.ndarray,float]: """r survivors, one erased physical qubit, then a shared bath qubit.""" n=r+1 j=[sum((onsite(op/2,k,n) for k in range(n)),np.zeros((2**n,2**n),complex)) for op in (X,Y,Z)] h0=.71*np.kron(j[0],X)+.53*np.kron(j[1],Z)+.39*np.kron(j[2],Y) h0+=np.kron(np.eye(2**n),.21*X-.17*Y+.13*Z) # An explicit erased-site flip demonstrates that E is not assumed inert. h0+=.27*np.kron(onsite(X,r,n),Y)+.19*np.kron(onsite(Z,r,n),X) h1=np.zeros_like(h0) budget=0.0 for k in range(r): amplitude=.018*(k+1)/r bath=(.43+.03*k)*SINGLE[1+k%3]+.17*SINGLE[1+(k+1)%3] term=amplitude*np.kron(onsite(SINGLE[1+k%3],k,n),bath) h1+=term budget+=amplitude*np.linalg.norm(bath,2) assert np.linalg.norm(h0-h0.conj().T)list[np.ndarray]: """Exact constant-H interaction-Dyson coefficients via block exponential. The (0,k) block of exp(I tensor A + shift tensor B) is the coefficient of lambda^k in exp(A+lambda B), with A=-itH0 and B=-itH1. """ d=len(h0) shift=np.diag(np.ones(order),1) generator=np.kron(np.eye(order+1),-1j*duration*h0) generator+=np.kron(shift,-1j*duration*h1) big=expm(generator) return [big[:d,k*d:(k+1)*d] for k in range(order+1)] def coefficient_blocks(op:np.ndarray,d_r:int,d_eb:int)->np.ndarray: return op.reshape(d_r,d_eb,d_r,d_eb).transpose(0,2,1,3).reshape(d_r*d_r,d_eb*d_eb) def projection_checks()->tuple[list[dict],list[np.ndarray],float,float]: r=4 h0,h1,local_budget=model_hamiltonians(r) duration=.83 exact=expm(-1j*duration*(h0+h1)) coeff=dyson_coefficients(h0,h1,duration,2) d_r,d_eb=2**r,4 rows=[] approximations=[] a=duration*local_budget for s in (0,1,2): approximation=sum(coeff[:s+1],np.zeros_like(h0)) approximations.append(approximation) blocks=coefficient_blocks(approximation,d_r,d_eb) q=orthogonal_module_basis(r,s) module_error=np.linalg.norm(blocks-q@(q.conj().T@blocks),'fro')/np.linalg.norm(blocks,'fro') raw=np.column_stack([p.reshape(-1)/math.sqrt(d_r) for _,w,p in paulis(r) if w<=s]) raw_error=np.linalg.norm(blocks-raw@(raw.conj().T@blocks),'fro')/np.linalg.norm(blocks,'fro') tau=math.exp(a+(s+1)*math.log(a)-gammaln(s+2)) actual_tail=float(np.linalg.norm(exact-approximation,2)) assert module_error1e-3 rows.append({"surviving_qubits":r,"erased_qubits":1,"bath_dimension":2, "joint_dimension":len(h0),"Dyson_order_s":s, "collective_algebra_dimension":math.comb(r+3,3), "module_dimension_numerical":q.shape[1], "module_dimension_upper_bound":sum(math.comb(r,w)*3**w for w in range(s+1))*math.comb(r+3,3), "relative_Frobenius_module_projection_error":float(module_error), "relative_Frobenius_raw_Pauli_projection_error":float(raw_error), "actual_operator_tail_norm":actual_tail,"safe_Dyson_tail_tau":tau, "integrated_residual_budget_a":a, "erased_site_flip_in_baseline":True}) return rows,approximations,a,duration def choi(kraus:list[np.ndarray])->np.ndarray: size=kraus[0].size out=np.zeros((size,size),complex) for k in kraus: v=k.reshape(-1,order='F') out+=np.outer(v,v.conj()) return out def psd_sqrt(a:np.ndarray)->np.ndarray: eig,u=np.linalg.eigh((a+a.conj().T)/2) assert eig[0]>=-TOL return (u*np.sqrt(np.maximum(eig,0)))@u.conj().T def amplitude_kraus(joint:np.ndarray,r:int)->tuple[list[np.ndarray],np.ndarray]: """Bath initially |0>; E input unrestricted; E output and bath discarded.""" d_r,d_a=2**r,2**(r+1) v=joint[:,np.arange(d_a)*2] ks=[] for e_out in range(2): for b in range(2): ks.append(v[(np.arange(d_r)*2+e_out)*2+b,:]) return ks,v def canonical_kraus(dictionary:list[np.ndarray],r:int,complete:bool)->list[np.ndarray]: d_r,d_a,m=2**r,2**(r+1),len(dictionary) erase=[] for e in range(2): k=np.zeros((d_r,d_a),complex) for a in range(d_r):k[a,a*2+e]=1 erase.append(k) result=[a@k/math.sqrt(m) for a in dictionary for k in erase] if complete: deficit=np.eye(d_r)-sum((a.conj().T@a for a in dictionary),np.zeros((d_r,d_r),complex))/m completion=psd_sqrt(deficit) result.extend(completion@k for k in erase) trace=sum((k.conj().T@k for k in result),np.zeros((d_a,d_a),complex)) assert np.linalg.norm(trace-np.eye(d_a))tuple[float,float]: matrix=np.column_stack([a.reshape(-1,order='F') for a in dictionary]) inverse=np.linalg.inv(matrix) duals=[inverse[i].conj().reshape(dictionary[0].shape,order='F') for i in range(len(dictionary))] gram=np.array([[np.trace(d.conj().T@a) for a in dictionary] for d in duals]) assert np.linalg.norm(gram-np.eye(len(dictionary)))list[dict]: r=2 d=2**r h0,h1,budget=model_hamiltonians(r) duration=.71 coefficients=dyson_coefficients(h0,h1,duration,1) approximate=coefficients[0]+coefficients[1] exact=expm(-1j*duration*(h0+h1)) a=duration*budget tau=math.exp(a+2*math.log(a)-gammaln(3)) assert np.linalg.norm(exact-approximate,2)<=tau+TOL approx_ks,v=amplitude_kraus(approximate,r) vnorm=float(np.linalg.norm(v,2)) assert vnorm<=1+tau+TOL jpsi=choi(approx_ks) pauli=[p for _,_,p in paulis(r)] units=[] for aindex in range(d): for bindex in range(d): e=np.zeros((d,d),complex);e[aindex,bindex]=1;units.append(e) nonorthogonal=[] for i,p in enumerate(pauli): aop=p+.21*pauli[(i+1)%len(pauli)] nonorthogonal.append(aop/np.linalg.norm(aop,2)) cases=[('orthonormal_unitary_Paulis',pauli,False,'m*v^2'), ('matrix_unit_Auerbach_basis',units,True,'m^2*c^2*v^2'), ('nonorthogonal_contraction_dictionary',nonorthogonal,True,'m^2*c^2*v^2')] rows=[] for name,dictionary,complete,formula in cases: m=len(dictionary) c,offdiag=dual_coordinate_norm(dictionary) if name!='nonorthogonal_contraction_dictionary':assert abs(c-1)1 and offdiag>1 canonical=canonical_kraus(dictionary,r,complete) jphi=choi(canonical) factor=m*vnorm**2 if formula=='m*v^2' else m*m*c*c*vnorm**2 diff=factor*jphi-jpsi minimum=float(np.linalg.eigvalsh((diff+diff.conj().T)/2)[0]) assert minimum>=-TOL safe_factor=m*(1+tau)**2 if formula=='m*v^2' else m*m*c*c*(1+tau)**2 rows.append({"dictionary":name,"surviving_qubits":r,"input_physical_qubits":r+1, "dictionary_size_m":m,"maximum_basis_operator_norm":max(float(np.linalg.norm(op,2)) for op in dictionary), "maximum_dual_coordinate_norm_c":c,"HS_offdiagonal_Gram_norm":offdiag, "approximate_amplitude_operator_norm_v":vnorm,"safe_tail_tau":tau, "CP_domination_formula":formula,"tested_CP_domination_factor":factor, "safe_factor_using_1_plus_tau":safe_factor, "minimum_unnormalized_Choi_domination_eigenvalue":minimum, "canonical_channel_completed":complete,"Choi_dimension":len(jpsi), "arbitrary_erased_site_flip_present":True}) return rows def h2(q:float)->float: if q<=0 or q>=1:return 0.0 return -q*math.log2(q)-(1-q)*math.log2(1-q) def log_collective_algebra_dimension(n:int,b:int)->float: full,rem=divmod(n,b) out=full*math.log2(math.comb(b+3,3)) if rem:out+=math.log2(math.comb(rem+3,3)) return out def log2_one_plus_exp2(x:float)->float: if x>50:return x+math.log1p(2**(-x))/math.log(2) return math.log2(1+2**x) def finite_certificate_rows()->list[dict]: """Conservative m^2 CP bound, full input dimension 2^N. User-facing curves assert only the assumed per-site residual budget; they do not measure or infer it for an experimental platform. """ rows=[] p,target=.1,.01 for nu in (1,2,3): for beta in (.25,.5,1.): for amplitude in (.001,.01): for exponent in range(4,13): n=10**exponent b=max(2,int(math.ceil(math.sqrt(n)))) epsilon=amplitude*(b/n)**(beta/nu) a=n*epsilon s=int(math.ceil(math.e**2*a+4*math.log(n))) logtau=a+(s+1)*math.log(a)-gammaln(s+2) tau=math.exp(logtau) if logtau>-745 else 0.0 tail_error_log=logtau+math.log(2+tau) tail_ok=tail_error_log<=math.log(target/4) cutoff_ok=s<=n/2 q=s/n pauli_log=n*h2(q)+s*math.log2(3) if cutoff_ok else 2*n alg_log=log_collective_algebra_dimension(n,b) logm=pauli_log+alg_log # Using the upper dimension estimate is conservative even # when it exceeds the full operator-space dimension. eta=math.sqrt(math.log(4/target)/(2*n)) u=n*(p+eta) logm1=log2_one_plus_exp2(logm) correction=2*math.log2(target/(2*(1+tau)**2)) logical_bound=n-2*u-4*logm-logm1-1+correction logical=max(0,int(math.floor(logical_bound))-32) if tail_ok and cutoff_ok else 0 if logical: logcoding=(2*logm+u+.5*(1+logical+logm1-n))*math.log(2)+2*math.log1p(tau) assert logcoding<=math.log(target/2)+1e-9 rows.append({"N":n,"nu":nu,"Holder_beta":beta,"residual_amplitude":amplitude, "cell_qubits_b":b,"erasure_probability_p":p,"target_error":target, "per_site_residual_epsilon":epsilon,"Dyson_order_s":s, "support_fraction_s_over_N":q,"log_safe_tail_tau":float(logtau), "tail_budget_passes":bool(tail_ok),"entropy_envelope_applicable":bool(cutoff_ok), "log2_Pauli_ball_upper_bound":pauli_log, "log2_collective_algebra_dimension":alg_log, "log2_operator_module_dimension_upper_bound":logm, "erasure_slack_eta":eta,"erasure_cutoff_u":u, "logical_qubits_certified":logical,"certified_rate":logical/n, "interpretation":"Sufficient bound for an assumed residual norm budget; no implemented decoder"}) # Independent small-size verification of both exact dimension counts. for n in (4,8,16,32): for s in range(n//2+1): exact=sum(math.comb(n,w)*3**w for w in range(s+1)) assert math.log2(exact)<=n*h2(s/n)+s*math.log2(3)+TOL return rows def write_csv(path:Path,rows:list[dict])->None: with path.open('w',newline='') as f: writer=csv.DictWriter(f,fieldnames=list(rows[0]));writer.writeheader();writer.writerows(rows) def plots(output:Path,projection:list[dict],certificates:list[dict])->None: 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(1,2,figsize=(9,3.8),layout='constrained') orders=[r['Dyson_order_s'] for r in projection] axes[0].semilogy(orders,[max(r['relative_Frobenius_module_projection_error'],1e-17) for r in projection], marker='o',color='#267882',label='Collective operator module') axes[0].semilogy(orders,[r['relative_Frobenius_raw_Pauli_projection_error'] for r in projection], marker='o',color='#a66c55',label='Raw weight ≤s Pauli span') axes[0].set(xlabel='Interaction-Dyson order s',ylabel='Relative projection residual', title='Four survivors, one erased site, shared bath',xticks=orders) axes[0].legend(frameon=False,fontsize=8) axes[1].semilogy(orders,[r['actual_operator_tail_norm'] for r in projection],marker='o', color='#267882',label='Exact unitary minus truncation') axes[1].semilogy(orders,[r['safe_Dyson_tail_tau'] for r in projection],marker='o', color='#9174b3',label='Proved tail upper bound') axes[1].set(xlabel='Interaction-Dyson order s',ylabel='Operator norm',title='Finite matrix tail check',xticks=orders) axes[1].legend(frameon=False,fontsize=8) for ax in axes:ax.grid(alpha=.16) for ext in ('png','pdf'):fig.savefig(output/f'nonabelian_module_checks.{ext}',dpi=220) plt.close(fig) fig,axes=plt.subplots(1,2,figsize=(9,3.8),layout='constrained') for nu,color in [(1,'#267882'),(2,'#9174b3'),(3,'#a66c55')]: chosen=[r for r in certificates if r['nu']==nu and r['Holder_beta']==.5 and r['residual_amplitude']==.001] axes[0].plot([r['N'] for r in chosen],[r['certified_rate'] for r in chosen],marker='o', color=color,label=f'Dimension {nu}') for beta,color in [(.25,'#a66c55'),(.5,'#9174b3'),(1.,'#267882')]: chosen=[r for r in certificates if r['nu']==2 and r['Holder_beta']==beta and r['residual_amplitude']==.001] axes[1].plot([r['N'] for r in chosen],[r['certified_rate'] for r in chosen],marker='o', color=color,label=f'Hölder β={beta:g}') for ax in axes: ax.axhline(.8,color='#354052',linestyle='--',linewidth=1) ax.set(xscale='log',xlabel='Physical qubits N',ylabel='Sufficient certified rate',ylim=(-.02,.83)) ax.legend(frameon=False,fontsize=8);ax.grid(alpha=.16) axes[0].set_title('Hölder β=1/2') axes[1].set_title('Spatial dimension 2') fig.suptitle('Generic nonabelian bound: p=0.1, target error=0.01, residual amplitude=0.001',fontsize=10) for ext in ('png','pdf'):fig.savefig(output/f'nonabelian_finite_certificates.{ext}',dpi=220) plt.close(fig) def main()->None: parser=argparse.ArgumentParser(description=__doc__) parser.add_argument('--output-dir',type=Path,default=Path(__file__).resolve().parents[1]/'results'/'nonabelian') parser.add_argument('--no-plot',action='store_true') args=parser.parse_args();args.output_dir.mkdir(parents=True,exist_ok=True) projection,_,_,_=projection_checks() cp=cp_domination_checks();certificates=finite_certificate_rows() result={'seed':SEED,'numerical_tolerance':TOL, 'status':'Finite matrix checks and analytic certificate evaluations, not proofs or novelty certification', 'Dyson_operator_module_checks':projection,'generic_CP_domination_checks':cp, 'finite_nonabelian_rate_certificates':certificates} (args.output_dir/'nonabelian_verification.json').write_text(json.dumps(result,indent=2)+'\n') write_csv(args.output_dir/'Dyson_module_checks.csv',projection) write_csv(args.output_dir/'generic_CP_checks.csv',cp) write_csv(args.output_dir/'finite_certificates.csv',certificates) if not args.no_plot:plots(args.output_dir,projection,certificates) print(json.dumps({'all_assertions_passed':True, 'module_dimensions':[r['module_dimension_numerical'] for r in projection], 'maximum_module_projection_residual':max(r['relative_Frobenius_module_projection_error'] for r in projection), 'raw_Pauli_projection_residuals':[r['relative_Frobenius_raw_Pauli_projection_error'] for r in projection], 'minimum_CP_domination_eigenvalue':min(r['minimum_unnormalized_Choi_domination_eigenvalue'] for r in cp), 'certificate_rows':len(certificates),'positive_certificates':sum(r['logical_qubits_certified']>0 for r in certificates)},indent=2)) if __name__=='__main__':main()