{
  "visual_id": "E96-quartet-spin-mixture",
  "title": "Coherent finite-wave predictions supply both spin sectors of four neutral breakup cases",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261004T041239868634Z-W02-quartet-bin-synthesis"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261004T041239868634Z-W02-quartet-bin-synthesis/results.json",
      "sha256": "b415907b2d278c01ec91cb11f7d02069c1e77454d147a6710aa9e862f12962ab"
    }
  ],
  "configurations": {
    "W02-quartet-bin-synthesis": {
      "parents": [
        "20261004T040435217983Z-W02-quartet-bin-production",
        "20261004T040638249443Z-W02-quartet-bin-production",
        "20261004T040805960046Z-W02-quartet-bin-production",
        "20261004T041126535728Z-W02-quartet-bin-production"
      ],
      "review": "20261004T040112550769Z-W02-quartet-bin-review",
      "cases": [
        [
          3.0,
          600.0
        ],
        [
          5.0,
          600.0
        ],
        [
          3.0,
          1200.0
        ],
        [
          5.0,
          1200.0
        ]
      ],
      "whole_seconds": 600,
      "maximum_RSS_bytes": 3221225472
    }
  },
  "assumptions": {
    "W02-quartet-bin-synthesis": [
      "No new numerical kernels, amplitudes, extrapolation, or optical normalization",
      "Finite quartet l0..4 plus incoherent doublet/quartet spin mixture only",
      "Observed differences are not rigorous error bounds; independent production review remains required"
    ]
  },
  "plotted_values": {
    "path": "E96-quartet-spin-mixture-data.json",
    "sha256": "def0611e8aede818e004544d20561aba8e0e3a2f7b44536311b6726c4ecf7244"
  },
  "caption": "Strict interior ideal centre-of-mass bins at Ecm=3 and 5 MeV, with cutoffs 600 and 1200 MeV. Doublet and quartet use the same neutral LO kinetic masses, two-body inputs and calibrated doublet three-body convention. Partial waves l=0 through 4 interfere coherently within each spin sector; orthogonal incoming spin sectors contribute incoherently with weights 1/3 and 2/3. The bin coordinates and all raw reserved points are supplied in the linked production report. Small grid/product/quadrature changes are observed numerical comparisons, not confidence intervals or rigorous omitted-wave bounds.",
  "alt_text": "These four finite neutral LO predictions do not complete the infinite-wave, continuous endpoint, charged-channel, higher-order or detector problem.",
  "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": "d2aecfa474bf48f2fc40c997d40f93fea69a6829fb57241cf82556bffe0c230e",
    "png": "7cc1895cb06bbe2f4cdbfeda37b41b85764d70febaeb0d5fa47e9cfe89e28942"
  }
}