{
  "visual_id": "E68-fourbody-triplet",
  "title": "Authenticated neutron\u2013triton spin average",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261002T161505505732Z-E28-fourbody-triplet"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261002T161505505732Z-E28-fourbody-triplet/results.json",
      "sha256": "3ec33d86a8d0b5026d86960bf45a01d93cd72f44a0a3f4a1df991eb0efa08880"
    },
    {
      "path": "runs/20261002T161505505732Z-E28-fourbody-triplet/authenticated-unpolarized-elastic.json",
      "sha256": "75f9e015295f4374d4a0b86ca4751a4ecfed501f97ad8f72c9240778aaf6a6cc"
    }
  ],
  "configurations": {
    "E28-fourbody-triplet": {
      "model": "Fixed R2 Gaussian LO force, frozen-triton neutron relative L0 total J1 positive-parity continuum",
      "energies_MeV": [
        0.05,
        0.1,
        0.2
      ],
      "force_parent": "20260929T233754706450Z-E28-spin-complete",
      "singlet_parent": "20261002T051954553720Z-E28-fourbody-scattering",
      "singlet_manifest_sha256": "a722701a94e104217cd867a9dce1961a67724de83de90137dd76016ee487be78",
      "singlet_review": "20261002T061723976347Z-W05-fourbody-scattering-review",
      "target_backend": "20261002T051426816644Z-E28-fourbody-scattering-controls",
      "frozen_sources": [
        "public_fourbody.py",
        "public_spin_complete.py",
        "public_fourbody_scattering.py",
        "spin_channels.py"
      ],
      "target_dimensions": [
        48,
        64
      ],
      "relative_basis_dimensions": [
        12,
        16
      ],
      "relative_width_interval_fm": [
        0.4,
        10.0
      ],
      "target_overlap_loss_gate": 0.0001,
      "target_energy_error_gate_MeV": 0.02,
      "relative_phase_change_gate_radians": 0.0005,
      "continuum_quadrature_gate": 1e-07,
      "unitarity_gate": 1e-09,
      "coordinate_phase_gate_radians": 1e-06,
      "positive_norm_minimum": 1e-08,
      "free_metric_relative_cut": 1e-11,
      "exterior_radius_refinement_fm": [
        120.0,
        160.0
      ],
      "whole_job_timeout_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "threads": 1,
      "maximum_production_jobs": 3,
      "scope": "Same-force frozen-target single-channel J1 elastic continuum and authenticated J0/J1 unpolarized L0 average; not target polarization, full FY, rearrangement, breakup, or radiative formation.",
      "job": "target"
    }
  },
  "assumptions": {
    "E28-fourbody-triplet": [
      "Same pinned R2 pair and scalar3BF coefficients and saved compressed full-spin target; exact triplet coupling and all24 fermion permutations.",
      "Relative L0 and total J1; all three M projections give identical scalar-force norm/H weights.",
      "Exact direct local folding, finite-rank localized exchange; whole infinite-space norm orthogonalization with no Pauli-eigenvalue shifts.",
      "Outgoing spectral normalization fixed independently; real standing-wave ODE supplies a separate continuum comparator.",
      "Spin-averaged J0/J1 elastic sum only after authenticating identical targets, Hamiltonian, kinetic units and energies.",
      "No target polarization, higher orbital waves, rearrangement, breakup, radiative formation or full FY result."
    ]
  },
  "plotted_values": {
    "path": "E68-fourbody-triplet-data.json",
    "sha256": "c5dc9d0e3c43d10947fb457a2b4bbe544d253c7a9d921e2e7bbfb90a9c3c04ad"
  },
  "caption": "The same LO Gaussian pair/three-body force, compressed triton, relative basis and threshold supply both pure spin channels. The unpolarized average is one quarter J=0 plus three quarters J=1. An independent finite-element boundary map and an initial-spin density trace verify continuum normalization and weights. This remains a frozen-target L=0 elastic approximation without polarization, higher orbital waves or reaction channels.",
  "alt_text": "The spin-averaged cross section lies between the two pure-channel values and decreases over the three tested energies.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
    "src/metastable/render.py": "ff4837be5102588b6614aeb2b7880b10c0a0c20a155e2eb7b409014a47a3de01",
    "src/metastable/spin_report.py": "dd5c64c5c658938948672a7dc767aa02c34dde012c3fc4aedfc3642f88796847",
    "src/metastable/continuation_report.py": "f9bbce6d0e201a9f55c826d6e9c47ab901e51a71b4a1f962b52eb08a63ba5fe9",
    "src/metastable/refinement_report.py": "4539c0ec814603105ab3a2b5cc82ce291c0151113b5bd3916cdc235aadb9bfb0",
    "src/metastable/atomic_mass_report.py": "46dd1cdb56a5a02cafe001a1f6a7fb201e149461850df41e012f77a580c3694b",
    "src/metastable/closure_report.py": "b34a03a9e0058eed65722df542dbb92691dd138787e2078b43ee9f18e221f75c",
    "src/metastable/october_report.py": "f93e7f89e43165d8d25e2184b9b32e6e21c3e1ffe66020d35944f263aaecb726",
    "src/metastable/october_followup_report.py": "925d905ff3bddf97a7ace2f68a4a28e7dfea2238c4f81d891dda2a9e70c6d4f6",
    "src/metastable/october_dynamics_report.py": "6b8d84c0ce0d78f52d064c68697f0d9c885cdc736e215b54eba46821dbe59a33",
    "src/metastable/october_calibration_report.py": "f714ef7ccfaa26e847c6135054f53528b3ff1d7096e7d113cffeea333e77e3d2",
    "src/metastable/october_interface_report.py": "2fc8826a33c952d7898154f84830748c26842c9a165d14aa7b7fb9721fac00bd",
    "src/metastable/october_checkpoint8_report.py": "f3b54f23510b9bfeffc5ff04e6df54e967228f43ba25a15e12e34f898cdfe0af",
    "src/metastable/october_checkpoint9_report.py": "4bd987aac59964ccb4768a95e0cb6f7d1fdccbeffe9483860da7b431f2224ae4",
    "src/metastable/october_checkpoint10_report.py": "9da673d773b63298e041914447ffd97065c1cf2b8966c90fc4ebcbee25a0ed63",
    "src/metastable/october_checkpoint11_report.py": "5f01064f02f4c76d0059d348a763b285c92c3677e6cb0ba0bbf7faa1a4b98248",
    "src/metastable/october_checkpoint12_report.py": "46022030652e3a1e274dfd27b36dfab25d90a97fde439b1da44d6f1fdc5140b5",
    "src/metastable/october_checkpoint13_report.py": "997c59be3af1b6b7be95fd4314e0f3b98c562629901a639572284045a65980c2",
    "src/metastable/october_checkpoint14_report.py": "d84de7d8516d8a4d8e21b5f9f279476f3035f719c1c8ab03b7ac1e44bf822240",
    "src/metastable/october_checkpoint15_report.py": "1f6e17b9549dc31fbb58ba578c4d8ed8e219b4ad30810df0a9d7d2d00e63efdc",
    "src/metastable/october_checkpoint16_report.py": "74cb8aac45d1d5ce0e6eb6678e9b6cdf98cd46fd6e264a513b612ab763fcd034",
    "src/metastable/october_checkpoint17_report.py": "9daceb74e91f6f8db0f7d89929226d46c464c284d06d0694f525fecf0c736bf6",
    "src/metastable/october_checkpoint18_report.py": "f33f88e316cae93af87cef75d8df41ce82970c8f8bc466dd7a094a92c5f00f8b",
    "src/metastable/october_checkpoint19_report.py": "ce2250507145354b6478cafaaff98c2b8ae2795c3c309f0d903a920365a77090",
    "src/metastable/october_checkpoint20_report.py": "e2ea0a8a374036254008cf6de8f10352dfb2585c4ccb18c1e850c017e6128294",
    "src/metastable/october_checkpoint21_report.py": "596b873676167227b2c92d358fcdbc0614908a5a9daad1da6227b81fce203eec",
    "src/metastable/publication_files.py": "e68bd0ee4e849a72fa828f0cfcf34cb6b1b9f2a8bbdbb3d51085054915039607"
  },
  "command": "python run.py full public-report",
  "output_sha256": {
    "svg": "d627d2b1fa851eea4a6850178b8d7a94695d8b6bb229e286c96a73c8168385a6",
    "png": "1197efd429d546725766eb715ba1e96858c4ef5865830c7dd80512445d79f041"
  }
}