references/run_sabrina_late_time_two_cut_reconstruction.json

{
  "kernel": "run_sabrina_late_time_two_cut_reconstruction",
  "role": "post-computation assertion only",
  "schema": "ouroboros_scientific_reference_assertion_v1",
  "scientific_payload": {
    "claim_boundary": {
      "capabilities_removed": [],
      "cross_order_relation_origin_invariant_without_La_zero_claimed": false,
      "distinct_cuts_required": true,
      "global_modes_reconstructed": false,
      "intercepts_origin_invariant_claimed": false,
      "source_error_claimed": false,
      "sphere_operator_inversion_claimed": false,
      "sphere_operator_kernels_resolved": false
    },
    "classification": "late_time_two_cut_image_reconstruction_exact_with_origin_covariance",
    "exact_checks": {
      "all_30_rational_reconstructions_exact": true,
      "archive_hash_matches": true,
      "coincident_cuts_rejected": true,
      "context_hash_matches": true,
      "context_marker_unique": true,
      "equation_hash_matches": true,
      "equation_marker_unique": true,
      "fixed_origin_cross_order_residual_zero": true,
      "member_hash_matches": true,
      "origin_shift_minus_intercept_covariant": true,
      "origin_shift_zero_intercept_covariant": true,
      "shifted_residual_is_tau_La_over_two": true,
      "symbolic_F2_reconstruction_exact": true,
      "symbolic_LF2_reconstruction_exact": true,
      "symbolic_V1_reconstruction_exact": true,
      "symbolic_Y3_reconstruction_exact": true
    },
    "finite_exact_rows": [
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "-1"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "-1"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "-1"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-3",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "1/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "-1",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "1/2",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "2",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "2",
        "u2": "7/2"
      },
      {
        "reconstruction_exact": true,
        "u1": "2",
        "u2": "7/2"
      }
    ],
    "paper": {
      "arxiv_id": "1905.10052",
      "title": "Implications of Superrotations"
    },
    "result_version": "sabrina_late_time_two_cut_reconstruction_v1",
    "source_evidence": {
      "archive_sha256": "f6dbbd7baa6b7eb93cb06b6460877b26f09ba30bacd6b447641ccf6843828df6",
      "checks": {
        "archive_hash_matches": true,
        "context_hash_matches": true,
        "context_marker_unique": true,
        "equation_hash_matches": true,
        "equation_marker_unique": true,
        "member_hash_matches": true
      },
      "context_sha256": "ac3cfdbbe3f446d97cf5ce608da5c078c9d481be3e07a76bc44f67611471adf4",
      "equation_sha256": "04b21882801dbf4f2f657ec7e880d361534f652f9529bc0c293c67b5a546a073",
      "member_sha256": "7f18a6972ebb356c2f7c90ad69823468e11323b04d918ed05cb46aed28edf100"
    },
    "status": "complete",
    "theorem": {
      "fixed_origin_cross_order_relation": "slope(Hzero)+one_half L(intercept(Hminus))=0",
      "origin_invariance_extra_condition": "L(a)=0",
      "origin_shift_law": "under v=u-tau: slopes fixed, b'=b+tau a, d'=d+tau c",
      "recovered_images": {
        "F2": "F2",
        "LF2": "LF2",
        "V1": "V1",
        "Y3": "Y3"
      },
      "shifted_cross_order_residual": "L_a*tau/2",
      "source_form": "Hminus(u)=-u Y3-2F2; Hzero(u)=u LF2+2V1",
      "two_cut_intercept": "[u2 H(u1)-u1 H(u2)]/(u2-u1)",
      "two_cut_slope": "[H(u2)-H(u1)]/(u2-u1)"
    }
  },
  "scientific_payload_sha256": "db1fd19b1f87b4ae81f8df3e51fb7af41553eddcc0138d1b499afb0ace0a7614"
}