ouroboros-pasterski-research-program / references /run_sabrina_ads_radiation_spectral_commutator.json
| { | |
| "kernel": "run_sabrina_ads_radiation_spectral_commutator", | |
| "role": "post-computation assertion only", | |
| "schema": "ouroboros_scientific_reference_assertion_v1", | |
| "scientific_payload": { | |
| "claim_boundary": { | |
| "capabilities_removed": [], | |
| "cotton_cft_dictionary_constructed": false, | |
| "flat_limit_rederived": false, | |
| "local_cut_criterion_constructed": false, | |
| "physical_ads_radiation_criterion_rigorously_proved": false | |
| }, | |
| "exact_checks": { | |
| "archive_hash_matches": true, | |
| "commutator_form_unique": true, | |
| "cotton_alone_insufficient_stated": true, | |
| "member_hash_matches": true, | |
| "misaligned_pair_detected": true, | |
| "nonzero_commuting_counterexample": true, | |
| "rational_witnesses_all_pass": true, | |
| "source_blocks_match": true, | |
| "super_poynting_label_unique": true, | |
| "symbolic_identity_exact": true, | |
| "two_exact_solution_classes_present": true | |
| }, | |
| "paper": { | |
| "arxiv_id": "2404.02146", | |
| "title": "Radiation in Holography" | |
| }, | |
| "result_version": "sabrina_ads_radiation_spectral_commutator_v1", | |
| "source_evidence": { | |
| "archive_sha256": "1a1275f84b2989c1956ca93f60d06baee3e055215413dbb77fba34ba28e0fbf2", | |
| "block_hashes": { | |
| "ads_cft_consequence": "8e347f43f7d95be26e202ab50962119cc31c340723e94a7c8b27c02fda833d92", | |
| "exact_solution_contrast": "c91f230530dc24dcd3655ee27a14e1be008e3ef9f1678b267ce7830d0fbbf632", | |
| "radiation_criterion": "4061b04e420a9bda4964f1db07018893583601f910aefd40fd70cdbb2fe63816" | |
| }, | |
| "checks": { | |
| "archive_hash_matches": true, | |
| "commutator_form_unique": true, | |
| "cotton_alone_insufficient_stated": true, | |
| "member_hash_matches": true, | |
| "source_blocks_match": true, | |
| "super_poynting_label_unique": true, | |
| "two_exact_solution_classes_present": true | |
| }, | |
| "member_sha256": "3cc6daa2e0d3520d63eb64da653fd87b39e0ef362decbd75503fd58e8cc15f3e" | |
| }, | |
| "spectral_certificate": { | |
| "identity": "||[C,T]||_F^2 = 2 sum_{i<j} (c_i-c_j)^2 T_ij^2", | |
| "misaligned_pair": { | |
| "commutator_nonzero": true, | |
| "frobenius_norm_squared": "18" | |
| }, | |
| "nonzero_commuting_pair": { | |
| "both_nonzero": true, | |
| "commutator_zero": true, | |
| "degenerate_block_mixing_nonzero": true | |
| }, | |
| "rational_witness_count": 96, | |
| "rational_witness_failures": [], | |
| "selection_rules": { | |
| "coordinate_free": "real symmetric C and T commute if and only if they are simultaneously orthogonally diagonalizable", | |
| "degenerate_spectrum": "stress may mix vectors only within equal-Cotton-eigenvalue blocks", | |
| "distinct_spectrum": "zero commutator forces every off-diagonal stress component to vanish in the Cotton eigenbasis" | |
| }, | |
| "symbolic_lhs": "2*c1**2*t12**2 + 2*c1**2*t13**2 - 4*c1*c2*t12**2 - 4*c1*c3*t13**2 + 2*c2**2*t12**2 + 2*c2**2*t23**2 - 4*c2*c3*t23**2 + 2*c3**2*t13**2 + 2*c3**2*t23**2", | |
| "symbolic_residual": "0", | |
| "symbolic_rhs": "2*c1**2*t12**2 + 2*c1**2*t13**2 - 4*c1*c2*t12**2 - 4*c1*c3*t13**2 + 2*c2**2*t12**2 + 2*c2**2*t23**2 - 4*c2*c3*t23**2 + 2*c3**2*t13**2 + 2*c3**2*t23**2" | |
| }, | |
| "status": "complete", | |
| "theorem": { | |
| "interpretation": "the criterion measures eigenframe misalignment, weighted by Cotton eigenvalue gaps", | |
| "no_radiation_algebraic_condition": "the proposed super-Poynting criterion vanishes exactly when Cotton-York and stress commute", | |
| "nonzero_not_sufficient": "nonzero Cotton-York and nonzero stress are necessary but not sufficient for a nonzero commutator", | |
| "spectral_identity": "||[C,T]||_F^2 = 2 sum_{i<j} (c_i-c_j)^2 T_ij^2" | |
| } | |
| }, | |
| "scientific_payload_sha256": "241d637afce046d817e7a3107063956a87e7581ccc4ccb9230959c16a846ff1d" | |
| } | |