{
  "visual_id": "E45-doublet-exclusive",
  "title": "An independent outgoing doublet breakup calculation",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261002T004220697119Z-E28-doublet-exclusive"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261002T004220697119Z-E28-doublet-exclusive/results.json",
      "sha256": "c6137ff7551d47fa0cc154e61dd67a58f09b0e0ed2c974f232b94edabeb7779c"
    }
  ],
  "configurations": {
    "E28-doublet-exclusive": {
      "energies_MeV": [
        3.0,
        5.0
      ],
      "cutoffs_MeV": [
        600.0,
        1200.0
      ],
      "panels": [
        240,
        720
      ],
      "product_order": 64,
      "product_control_order": 96,
      "phase_orders": [
        80,
        160
      ],
      "contour_points": [
        176,
        256
      ],
      "contour_depths": [
        0.4,
        0.7
      ],
      "fit_binding_MeV": 8.4818,
      "fit_points": 256,
      "flux_relative_tolerance": 0.003,
      "grid_relative_tolerance": 0.003,
      "phase_relative_tolerance": 0.0003,
      "product_relative_tolerance": 0.0003,
      "elastic_absolute_tolerance_fm": 3e-05,
      "optical_absolute_tolerance_fm2": 3e-06,
      "point_component_relative_tolerance": 0.003,
      "reserved_q_fractions": [
        0.07,
        0.23,
        0.51,
        0.83,
        0.97
      ],
      "whole_run_timeout_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "blas_threads": 1,
      "scope": "Neutral LO doublet spectator l=0, S-wave pairs, equal kinetic nucleon masses; independent three-body outgoing flux. No charged, NLO or complete-wave result."
    }
  },
  "assumptions": {
    "E28-doublet-exclusive": [
      "Hammer-Konig Eqs3/5/6/8: same calibrated auxiliary-dibaryon H in source, kernel and outgoing D_i t_i.",
      "Explicit normalized Clebsch-Gordan tensors and nn charge multiplicity sqrt2 reproduce parent C independently.",
      "B=2pi gd b; gd\u00b2=8pi K\u00b2 gamma; final nnp factor1/2 gives sigma=4gamma/(3k)int dq q\u00b2p dx norm(b)\u00b2.",
      "Elastic/contour loss is a held-out comparator and never sets the outgoing normalization.",
      "Only neutral LO doublet spectator l0, S-wave NN interactions and equal kinetic masses; no physical truncation posterior."
    ]
  },
  "plotted_values": {
    "path": "E45-doublet-exclusive-data.json",
    "sha256": "fdf5d224cb5dfc8db0cc6568b906f4ac62148b8b7f36db2275616068ac006721"
  },
  "caption": "Explicit antisymmetric charge/spin amplitudes and the independently calibrated three-body force determine the neutral LO l=0 flux. Multiply pure-doublet values by 1/3 for an unpolarized cross section. The right panel compares a separately solved contour elastic loss; normalization was not fitted to it. Nearly coincident cutoff curves are not an EFT uncertainty band. Higher doublet waves, complete wave remainders and unscreened spin-complete charged flux remain unfinished.",
  "alt_text": "Pure doublet S-wave breakup rises from about five to nine and a half square femtometres; the independent flux comparison differs by less than two parts in ten million.",
  "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": "815552c9c7cbd8635a173445bf0089496bcb56fd29f39298d2b0a48bf25885d8",
    "png": "9aa8d6c7ad64144b57241ba8257a050c932996591aabc62f09c8e6558ef69715"
  }
}