ouroboros-pasterski-research-program / references /run_sabrina_weyl_double_copy_shadow_involution.json
| { | |
| "kernel": "run_sabrina_weyl_double_copy_shadow_involution", | |
| "role": "post-computation assertion only", | |
| "schema": "ouroboros_scientific_reference_assertion_v1", | |
| "scientific_payload": { | |
| "claim_boundary": { | |
| "capabilities_removed": [], | |
| "full_shadow_kernel_normalization_claimed": false, | |
| "interacting_double_copy_claimed": false, | |
| "naive_self_shadow_substitution_allowed": false, | |
| "singular_state_physics_claimed": false | |
| }, | |
| "exact_checks": { | |
| "archive_hash_matches": true, | |
| "coefficient_table_present": true, | |
| "fixed_zero_exact": true, | |
| "gauge_pair_exchanged": true, | |
| "member_hash_matches": true, | |
| "pole_exchange_exact": true, | |
| "primary_double_copy_exact": true, | |
| "primary_shadow_curvatures_present": true, | |
| "removable_self_shadow_limits_exact": true, | |
| "scalar_pair_exchanged": true, | |
| "shadow_double_copy_exact": true, | |
| "source_blocks_match": true, | |
| "source_primary_weyl_exact": true, | |
| "source_shadow_weyl_exact": true, | |
| "tau_squared_identity": true, | |
| "weyl_double_copy_definition_present": true, | |
| "weyl_pair_exchanged": true | |
| }, | |
| "involution_certificate": { | |
| "checks": { | |
| "gauge_pair_exchanged": true, | |
| "primary_double_copy_exact": true, | |
| "scalar_pair_exchanged": true, | |
| "shadow_double_copy_exact": true, | |
| "source_primary_weyl_exact": true, | |
| "source_shadow_weyl_exact": true, | |
| "tau_squared_identity": true, | |
| "weyl_pair_exchanged": true | |
| }, | |
| "coefficients": { | |
| "gauge_primary": "Delta - 1", | |
| "gauge_shadow": "1 - Delta", | |
| "scalar_primary": "(2 - 2*Delta)/Delta", | |
| "scalar_shadow": "(2 - 2*Delta)/(Delta - 2)", | |
| "weyl_primary": "-Delta**2/2 + Delta/2", | |
| "weyl_shadow": "-Delta**2/2 + 3*Delta/2 - 1" | |
| }, | |
| "tau": "2-Delta" | |
| }, | |
| "paper": { | |
| "arxiv_id": "2012.15694", | |
| "title": "Shifting Spin on the Celestial Sphere" | |
| }, | |
| "result_version": "sabrina_weyl_double_copy_shadow_involution_v1", | |
| "scope": { | |
| "chirality_exchange_applied": true, | |
| "coefficient_level_only": true, | |
| "universal_shadow_spacetime_factor_stripped": "2/X^2" | |
| }, | |
| "singularity_certificate": { | |
| "fixed_zero_exact": true, | |
| "pole_exchange_exact": true, | |
| "reduced_primary_limit": "0", | |
| "reduced_shadow_limit": "0", | |
| "removable_limits_exact": true, | |
| "scalar_primary": { | |
| "pole": "Delta=0", | |
| "zero": "Delta=1" | |
| }, | |
| "scalar_shadow": { | |
| "pole": "Delta=2", | |
| "zero": "Delta=1" | |
| }, | |
| "self_shadow_point": 1, | |
| "unreduced_quotient_at_self_shadow": "0/0", | |
| "weyl_primary_zeros": [ | |
| 0, | |
| 1 | |
| ], | |
| "weyl_shadow_zeros": [ | |
| 1, | |
| 2 | |
| ] | |
| }, | |
| "source_evidence": { | |
| "archive_sha256": "ff00948d397a3aaaa36cec9a65f63477b16c6315c982669e63259b0a8961fc46", | |
| "block_hashes": { | |
| "primary_shadow_curvatures": "8acb82a9be540c4a2d8eead0630fbcb8fe0c15fcbd76c81abfa1fadfcebe7a80", | |
| "weyl_double_copy_definition": "5cbf0c6d34e0ca8ba5607901422b27778f4b6c966fb2dae1468294d2fa0dbed4", | |
| "weyl_double_copy_table": "774c827ab158f3d9fbae9dbc062ceb3638202c3dc36940d488f19f968db13490" | |
| }, | |
| "checks": { | |
| "archive_hash_matches": true, | |
| "coefficient_table_present": true, | |
| "member_hash_matches": true, | |
| "primary_shadow_curvatures_present": true, | |
| "source_blocks_match": true, | |
| "weyl_double_copy_definition_present": true | |
| }, | |
| "member_sha256": "17ed9a4bf99bf5a3a53a11d7da5c3000c4b99db7688432072e6703a597671794" | |
| }, | |
| "status": "complete", | |
| "theorem": { | |
| "divisor_exchange": "the scalar prefactor poles Delta=0 and Delta=2 are exchanged, while Delta=1 is fixed", | |
| "double_copy_equivariance": "C_P=f_P^2/S_P and C_S=f_S^2/S_S are preserved under tau", | |
| "involution": "tau(Delta)=2-Delta exchanges the stripped primary and shadow gauge, scalar, and Weyl double-copy coefficients", | |
| "self_shadow_boundary": "at Delta=1 the unreduced f^2/S quotient is 0/0; its reduced primary and shadow limits both equal zero" | |
| } | |
| }, | |
| "scientific_payload_sha256": "f6243bc6dfdd05769cab60b02d4e23c53ef9c0119f2ac7a10d54eda023956fee" | |
| } | |