{
  "visual_id": "E11-binding-consistency",
  "title": "One rate does not define a consistent nuclear network",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T223004324566Z-E28-response-consistency"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20260929T223004324566Z-E28-response-consistency/transfer-bound-state-consistency.csv",
      "sha256": "bb7ff17208987ede9e874c7dd9988c8014c302372fd1110f72d5a3ca1f9f1b7e"
    }
  ],
  "configurations": {
    "E28-response-consistency": {
      "transfer_network_run": "20260929T213258904696Z-E30-STM-BBN",
      "Bnn_MeV": [
        0.1,
        0.5,
        2.0,
        2.5,
        3.2
      ],
      "cutoffs_MeV": [
        600,
        1200
      ],
      "points": [
        144,
        192
      ],
      "ordinary_Btriton_MeV": 8.4818,
      "fixed_BHe3_for_Q_illustration_MeV": 7.718043
    }
  },
  "assumptions": {
    "E28-response-consistency": [
      "Use exactly the neutral LO three-body family behind the solved p+nn to n+d transfer amplitude.",
      "Fit H only to ordinary tritium, then keep it fixed as the nn inverse length changes. Do not retune hypothetical tritium to its ordinary binding.",
      "Follow the ordinary triton pole branch below all dimer thresholds, excluding regulator-induced deep branches.",
      "For the Q-value illustration only, hold He3 binding and particle masses fixed; charged He3 response is not derived.",
      "The audit tests consistency of a single-rate BBN substitution. It supplies no complete updated abundance network or field prediction."
    ]
  },
  "plotted_values": {
    "path": "E11-binding-consistency-data.json",
    "sha256": "346488430de7c7401345165e2bd0c27927ac9cf3fb4f59e774aaff19f1749cbe"
  },
  "caption": "The same neutral LO force used in the solved transfer amplitude is fitted only to ordinary tritium. Keeping that force fixed as nn becomes bound shifts the triton pole; the BBN rate-substitution experiment instead retains ordinary tritium. At Bnn=2.5 MeV the mismatch is about 3.285 MeV, much larger than the cutoff and quadrature differences. Those differences do not measure omitted EFT orders. The right-hand panel holds helium-3 binding and particle masses fixed solely to display weak Q values. It does not calculate a charged three-body response or any lifetime. No phase-dependent counterterm is refitted to conceal the mismatch.",
  "alt_text": "The calculated tritium binding rises while the rate-substitution network holds it fixed. Under a fixed helium-3 illustration, the displayed tritium beta channel closes and electron capture opens.",
  "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": "d67a5d38a7831bb454acfe8e7b20eba380696286c85c8d038bb4b0b3c832f27a",
    "png": "8a05b7c8160319a25f7686288d595c81f3ab7d9390f0e05093c2f0eee8efa02c"
  }
}