{
  "visual_id": "E38-exclusive-partial",
  "title": "Independent exclusive quartet breakup through spectator l=4",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261001T193548336872Z-E28-exclusive-partial"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261001T193548336872Z-E28-exclusive-partial/exclusive-partial-flux.csv",
      "sha256": "ed885a2a986ff67b0162f791b5d99f65d2d3f7c35f743619200e9c36250151ac"
    },
    {
      "path": "runs/20261001T193548336872Z-E28-exclusive-partial/results.json",
      "sha256": "5979b8d935dd7967b172291fad2ae35dbec8d3bc295a722669055faea5a2cc50"
    }
  ],
  "configurations": {
    "E28-exclusive-partial": {
      "energies_MeV": [
        3.0,
        5.0
      ],
      "ell": [
        0,
        1,
        2,
        3,
        4
      ],
      "cutoffs_MeV": [
        600,
        1200
      ],
      "panels": [
        240,
        720
      ],
      "product_orders": [
        64,
        96
      ],
      "phase_orders": [
        80,
        160
      ],
      "relative_flux_gate": 0.003,
      "elastic_amplitude_gate_fm": 3e-05,
      "own_optical_gate_fm2": 3e-06
    }
  },
  "assumptions": {
    "E28-exclusive-partial": [
      "Extension of frozen quartet l0; same dimer residue, plane-wave measure, equal kinetic masses, pair S-wave forces and neutron antisymmetry.",
      "Addition theorem orientation average: (2l+1)[|A1|\u00b2+|A2|\u00b2\u22122Re(A1 A2*)P_l(qhat1.qhat2)]. Cross-l terms vanish only in the fully integrated orientation average.",
      "No elastic loss is an input to flux. Pure quartet requires unpolarized weight2/3.",
      "Differential spectra and rigorous infinite-wave remainder not established; cutoff sensitivity is not EFT uncertainty; no doublet or charged flux."
    ]
  },
  "plotted_values": {
    "path": "E38-exclusive-partial-data.json",
    "sha256": "2e9325693bffc6cdf1e3cbed52b4633b690e33df4a6aa730db3d05938caceb8b"
  },
  "caption": "Orientation-integrated single-wave flux follows the Legendre addition theorem and an independently normalized dimer residue and three-body phase space. Elastic loss is used only as a separate comparator. Pair forces remain S wave; spectator l=0\u20264 are shown at two energies and cutoffs. Cutoff differences and numerical discrepancies are not EFT error bars. Multiply pure-quartet cross sections by 2/3 for their unpolarized contribution. This quartet component supplies no rigorous infinite-wave bound or validated coherent differential spectrum. The subsequent doublet S-wave component has separate evidence; charged three-body breakup remains unfinished.",
  "alt_text": "The spectator l=1 wave is much larger than l=0 at both sampled collision energies. All displayed independently integrated fluxes agree closely with the separate contour-loss calculation.",
  "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": "bb81e5d5b562b944e791fce9ecd62195c6d66e58e1fb223f776360f5d500852e",
    "png": "bf55b2390bc13a44e9c742ead2eb1af06c6788b50763c7aba9a8c08a47c11d63"
  }
}