{ "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" }