{
  "visual_id": "E15-trinucleon-weak",
  "title": "Binding energies and weak currents must agree",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260930T005525250915Z-E29-trinucleon-weak"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20260930T005525250915Z-E29-trinucleon-weak/trinucleon-weak-currents.csv",
      "sha256": "c97a88fa203fe6f627a168d62b18b762d62bb417c10d846b35e93ec83f65a01d"
    }
  ],
  "configurations": {
    "E29-trinucleon-weak": {
      "parents": [
        "20260929T233754706450Z-E28-spin-complete",
        "20260930T005420065273Z-E28-threshold-refinement"
      ],
      "gA": 1.2756,
      "tau_n_s": 878.4,
      "current": "sum_i tau_i+ and sum_i sigma_i tau_i+",
      "phase_space": "allowed heavy-nucleus, point Coulomb; nuclear masses",
      "refinement": "Truncate both states to min(N_initial,N_final)-128 spin/spatial basis functions"
    }
  },
  "assumptions": {
    "E29-trinucleon-weak": [
      "No weak datum is fitted. The current acts on fully antisymmetrized spin-isospin wavefunctions from the separate local Gaussian LO family.",
      "The full fixed-charge S=1/2 internal space is included. Earlier fixed-seed currents forced |F|=|GT|/sqrt(3) and are retained only as restricted controls.",
      "B(F)=|<F>|^2 and B(GT)=3|<sigma_z tau+>|^2 for J=1/2 states. Explicit SU(4) algebra is checked independently.",
      "Ordinary neutron lifetime fixes a common leading weak normalization; missing two-body axial, radiative, recoil and atomic corrections prevent precision lifetimes.",
      "Both independently predicted and empirical nuclear Q values are reported, never silently replacing the former by the latter.",
      "A bound-state beta-plus channel is evaluated if He3 becomes heavier than tritium plus a positron. Plasma electron capture and other competing channels are not absolute-stability claims.",
      "An nn-only perturbation holds the other pair and three-body forces fixed. It is not a field-matched trajectory."
    ]
  },
  "plotted_values": {
    "path": "E15-trinucleon-weak-data.json",
    "sha256": "a0b61e1b78a2c4b2d6b04d491e26e973ad3a34f2bbda754020e603abe5dcaadb"
  },
  "caption": "Fermi and Gamow\u2013Teller operators act on the independently solved antisymmetric trinucleon states; no weak observable is fitted. The exact SU(4) limit and basis refinements are checked. Rates use neutron normalization and an allowed point-Coulomb phase-space integral, including positron repulsion. Ordinary binding errors can exceed the measured 19-keV tritium Q value, so a calculation with the empirical Q is stored separately as a current check. The right panel uses the model\u2019s own masses. Higher-order axial currents, atomic corrections and plasma electron capture remain outside this impulse approximation.",
  "alt_text": "One-body weak matrix elements change modestly across regulators while binding errors can reverse a small decay energy. In the nn-only diagnostic, helium-3 beta-plus decay opens as tritium becomes more strongly bound.",
  "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": "e2817bc85afe05ed0f38496d790a21ae307750ffdd45757784c47a78df16a817",
    "png": "2b73684820b3c55f7ae82ae8d75e3ac276de01697ebc2842d4b497d891e81024"
  }
}