{
  "visual_id": "E04-reaction-controls",
  "title": "Weak conversion and strong-rate controls",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T193546300964Z-E26-thermal",
    "20260929T194839837161Z-E29-source-rates"
  ],
  "claim_ids": [
    "C02"
  ],
  "input_files": [
    {
      "path": "runs/20260929T193546300964Z-E26-thermal/thermal-weak-rates.csv",
      "sha256": "15e6f01a7df83de9b3f96514a0ae1a4b052ce76d5c9ef80f443c8ca93f7e7b26"
    },
    {
      "path": "runs/20260929T194839837161Z-E29-source-rates/held-out-analogy-control.csv",
      "sha256": "d9ffa107bb9e5dd3877551112093d7643c92612c91f91f651445609d8647034b"
    }
  ],
  "configurations": {
    "E26-thermal": {
      "temperatures_MeV": [
        0.001,
        0.001099671260166408,
        0.0012092768804359741,
        0.0013298070309991303,
        0.0014623505735569615,
        0.0016081048980284532,
        0.001768386739694722,
        0.0019446440745016582,
        0.0021384691999823766,
        0.002351613119971668,
        0.002586001363063102,
        0.0028437513777116495,
        0.003127191661128125,
        0.0034388827947746474,
        0.0037816405764944114,
        0.004158561458250031,
        0.004573050519273265,
        0.0050288522273338725,
        0.005530084266022886,
        0.006081274733643806,
        0.00668740304976422,
        0.0073539449389749,
        0.008086921898236897,
        0.008892955594701487,
        0.009779327685429282,
        0.010754045599416258,
        0.011825914876197084,
        0.01300461871452831,
        0.01430080544978899,
        0.015726184750364084,
        0.017293633402042617,
        0.01901731163608008,
        0.02091279105182546,
        0.02299719528955767,
        0.02528935472436085,
        0.027809976578533197,
        0.03058183198931387,
        0.033629961721886134,
        0.03698190238605456,
        0.04066793520022369,
        0.044721359549995794,
        0.04917879381269887,
        0.05408050616547448,
        0.059470778365424484,
        0.06539830578818345,
        0.07191663733883974,
        0.07908465920933244,
        0.08696712685255747,
        0.09563524997900368,
        0.10516733586074035,
        0.11564949675432419,
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        0.16912010791025994,
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        0.2045130365127145,
        0.2248971085823953,
        0.24731288680258387,
        0.2719628738855896,
        0.29906975624424414,
        0.328878415726768,
        0.36165814186378675,
        0.3977050646127915,
        0.4373448295773111,
        0.4809355398685446,
        0.5288709911860535,
        0.5815842293430247,
        0.6395514623745525,
        0.7032963625706931,
        0.773394797298565,
        0.8504800313514556,
        0.9352484478226213,
        1.0284658391857777,
        1.1309743254155264,
        1.243699961645545,
        1.3676611040916682,
        1.5039776098170654,
        1.6538809534495926,
        1.8187253522451339,
        2.0
      ],
      "quadrature_points": [
        96,
        160
      ]
    },
    "E29-source-rates": {
      "bindings_MeV": [
        0.1,
        2.0,
        2.5,
        3.0,
        3.5
      ],
      "radius_fm": 1.4,
      "strong_rate_multiplier_envelope": [
        0.2,
        1.0,
        5.0
      ]
    }
  },
  "assumptions": {
    "E26-thermal": [
      "All four Kneller Eq.16 crossings and inverses, with electron mass, Fermi-Dirac populations and final-state Pauli blocking.",
      "B(GT)=6 times previously calculated radial overlap; reverse nuclear spin average gives B(GT)/3.",
      "Point-Coulomb Fermi factor for electron/deuteron channels, zero chemical potentials; optional decoupled-neutrino temperature.",
      "Heavy-nucleus Born limit: the equilibrium ratio is exp(-delta/T)/3; finite-mass translational and recoil corrections are higher order.",
      "Ordinary neutron lifetime normalizes the one-body current. Two-body axial and finite-field response uncertainties remain separate."
    ],
    "E29-source-rates": [
      "Historical ENDF/B-IV MAT1146 MT103 is acquired; DD/DT analogues use frozen ENDF/B-VIII.1 evaluated reference cross sections.",
      "Kneller Eq.15 kinematic/statistical/Coulomb factors are implemented; source analog amplitudes are assumptions for hypothetical channels.",
      "The modern DT reference retains its resonance. This is a declared updated analogue experiment, not the unrecovered Chulick nonresonant historical table.",
      "Below each reference table first energy the reduced Eq.15 amplitude is held constant; raw ENDF data are never extrapolated silently.",
      "Both He3+nn exit channels are present. Q values come from one mass table, including Q(He3+nn->alpha+n)=20.58-Bnn MeV, correcting source Eq.6a.",
      "No unmeasured allowed nn electromagnetic operator is invented or equated to ordinary np capture."
    ]
  },
  "plotted_values": {
    "path": "E04-reaction-controls-data.json",
    "sha256": "25cd23b267fbb2fa9e036f2177fce41eaf713d4b43259f68893fe69cc32f64cc"
  },
  "caption": "The four crossed weak processes include electron mass, Fermi factors, neutrino occupations and Pauli blocking in the heavy-nucleus allowed approximation. Equal temperatures satisfy detailed balance including the spin factor. A closed vacuum beta channel can still convert thermally. The historical strong-rate analogy underpredicts an independently evaluated DD comparison by roughly fourfold; it has no precision status for a hypothetical reaction.",
  "alt_text": "Weak rates rise with temperature even for a 3.2-MeV dineutron whose displayed vacuum beta decay is closed. A reserved strong-reaction analogy gives only about a quarter of the evaluated cross section.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
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    "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",
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    "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": "8833f3f91af4d239fb6ccf70c9989618cd30a97088954ae70436f8e0467a7574",
    "png": "e58f7ac44f311152169c57ab467f1784678ef06ed3d0c7bfcf81794b56d48462"
  }
}