{
  "visual_id": "E05-abundances",
  "title": "Abundance histories depend on reaction amplitudes",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T201633081739Z-E30-source-BBN",
    "20260929T213258904696Z-E30-STM-BBN",
    "20260929T203401050040Z-E30-likelihood",
    "20260929T223004324566Z-E28-response-consistency"
  ],
  "claim_ids": [
    "C02",
    "C10",
    "C14"
  ],
  "input_files": [
    {
      "path": "runs/20260929T201633081739Z-E30-source-BBN/abundances.csv",
      "sha256": "a38b22b37eec6d274e8a79b2c53d669f18734c68ede88b437f486f72d16cbd1a"
    },
    {
      "path": "runs/20260929T213258904696Z-E30-STM-BBN/abundances.csv",
      "sha256": "ea533f480e4213b69f74f093a8fc64d6965fe31ff6c350a63e9540535fffc9d1"
    },
    {
      "path": "runs/20260929T203401050040Z-E30-likelihood/conditional-likelihoods.csv",
      "sha256": "57f7dd2487511a480365d0b1084ebfa2910374b38c1f350541496b5b86ba2b95"
    },
    {
      "path": "runs/20260929T223004324566Z-E28-response-consistency/results.json",
      "sha256": "8b6be765020fd19afdca002068a8e0391374d67d4f4628d484674df6c0f4eb8b"
    }
  ],
  "configurations": {
    "E30-source-BBN": {
      "cases": [
        {
          "spin_Bnn_MeV": 0.1,
          "source_rate_scale": 0.0,
          "label": "standard-recovery"
        },
        {
          "spin_Bnn_MeV": 0.1,
          "source_rate_scale": 1.0,
          "label": "B0.1"
        },
        {
          "spin_Bnn_MeV": 2.0,
          "source_rate_scale": 1.0,
          "label": "B2.0"
        },
        {
          "spin_Bnn_MeV": 2.5,
          "source_rate_scale": 1.0,
          "label": "B2.5"
        },
        {
          "spin_Bnn_MeV": 3.0,
          "source_rate_scale": 1.0,
          "label": "B3.0"
        },
        {
          "spin_Bnn_MeV": 3.2,
          "source_rate_scale": 1.0,
          "label": "B3.2"
        },
        {
          "spin_Bnn_MeV": 2.5,
          "source_rate_scale": 0.2,
          "label": "B2.5-scale0.2"
        },
        {
          "spin_Bnn_MeV": 2.5,
          "source_rate_scale": 5.0,
          "label": "B2.5-scale5.0"
        },
        {
          "spin_Bnn_MeV": 3.2,
          "source_rate_scale": 1.0,
          "vacuum_weak_only": true,
          "label": "B3.2-vacuum-weak"
        },
        {
          "spin_Bnn_MeV": 2.5,
          "source_rate_scale": 1.0,
          "public_tolerance_scale": 0.1,
          "public_solver": "Radau",
          "label": "B2.5-refined"
        }
      ]
    },
    "E30-STM-BBN": {
      "Bnn_MeV": 2.5,
      "cutoffs_MeV": [
        600,
        1200
      ],
      "parent": "20260929T201633081739Z-E30-source-BBN",
      "temperatures_MeV": [
        5e-05,
        2.0
      ],
      "temperature_points": 600
    },
    "E30-likelihood": {
      "parent": "20260929T201633081739Z-E30-source-BBN",
      "observables": [
        "He4/H number ratio",
        "log10(D/H)"
      ],
      "observed": [
        0.08146,
        -4.5974
      ],
      "observation_covariance": [
        [
          3.364e-07,
          0.0
        ],
        [
          0.0,
          2.704e-05
        ]
      ],
      "nuisances": [
        "npdg",
        "dpHe3g",
        "ddHe3n",
        "ddtp",
        "tpag",
        "tdan",
        "taLi7g",
        "He3ntp",
        "He3dap",
        "He3aBe7g",
        "Be7nLi7p",
        "Li7paa",
        "tau_n",
        "omega_b"
      ],
      "tau_n_s": [
        878.4,
        0.5
      ],
      "omega_b": [
        0.0223,
        0.0002
      ],
      "networks": [
        "standard-recovery",
        "B2.5"
      ],
      "workers": 3
    },
    "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": {
    "E30-source-BBN": [
      "Actual standard PRyMordial background, four reversible strong transfer channels and all crossed nn/d thermal weak channels.",
      "Strong reference data are evaluated; hypothetical channel transfer amplitudes remain the explicit Eq.15 analogy, with factor-five controls.",
      "No invented nn radiative capture or source-exact historical Kneller limit is claimed. Reverse rates use one rest-mass and spin table.",
      "Published abundances can be tested conditionally on this nuclear closure; no universal constraint on post-BBN or unobserved phases.",
      "Baryon energy release divided by radiation is suppressed by eta. This fixed background omits higher-order nuclear heat feedback."
    ],
    "E30-STM-BBN": [
      "Replace only p+nn <-> n+d by the actually solved neutral LO three-body amplitude; retain the other three declared evaluated-analogue transfers.",
      "Ordinary triton calibration fixes H once per cutoff. The alternative-phase three-body response is explicitly held fixed, not inferred.",
      "A zero and unitarity-saturating above-breakup S-wave contribution bracket the unresolved S-wave thermal tail at every temperature.",
      "All reverse rates use the same mass/spin table. Equal nucleon masses are used only in the LO amplitude and its thermal speed.",
      "Higher partial waves, charged NLO terms and larger-nucleus correlations are outside this conditional network.",
      "Independent energy interpolation, momentum quadrature and thermal quadrature controls precede abundance interpretation."
    ],
    "E30-likelihood": [
      "LBT 2026 Eq.2 and Cooke 2018 Eq.9 are independent published summary likelihoods; original line-flux/spectral likelihoods are not reconstructed.",
      "Use actual final He4/H and D/H number ratios. LBT uses Y=4y/(1+4y), not a rest-mass-weighted CMB helium fraction.",
      "PRyMordial lognormal nuclear-rate nuisances are independent across reactions and perfectly correlated across temperatures within a reaction, as in the source model.",
      "Central one-sigma finite differences compute the abundance covariance separately in each network; curvature and independent combined-nuisance runs test local linearity.",
      "Neutron lifetime and BBN-independent Planck baryon priors match the frozen PRyMordial publication. They are conditional on its ordinary recombination/cosmological model.",
      "The uncertain hypothetical transfer amplitude is not covered by ordinary-rate errors. Factor-five scenarios remain separate, with no invented nuisance probability.",
      "No continuous Bnn exclusion limit, universal bound, or constraint on a region outside our primordial history is inferred from a sparse conditional grid."
    ],
    "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": "E05-abundances-data.json",
    "sha256": "d489bdb8de97171d933178e2bb2193426643dac903b8808758d5b125943d43c2"
  },
  "caption": "Actual PRyMordial integrations retain fixed ordinary masses except Bnn. New transfer rates are explicit closures. Replacing one analogy by a solved LO amplitude has cutoff/refinement and above-breakup S-wave tail controls, but is a sensitivity test: that same force also shifts tritium binding, which this network leaves fixed. It is not a matched nuclear Hamiltonian. The likelihood uses LBT 2026 He4/H and Cooke 2018 log(D/H), with ordinary-rate, neutron-lifetime and stated baryon-prior covariance recomputed for ordinary BBN and the fixed-binding analogue model. Connected binding points are a guide, not an interpolated exclusion limit. Hypothetical-amplitude uncertainty is not included in those covariance bars.",
  "alt_text": "Weak binding changes abundances little. Stronger binding shifts helium and deuterium strongly, with additional variation from the formation model. The conditional 2.5-MeV analogue model fits the two abundance summaries worse than ordinary BBN.",
  "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": "fa88d973656974279bca3e8a0ded5786dc1772d1c4854a9e31620fec1de7a3b3",
    "png": "c5d8628e0df2839ed7dcdd21f47c1c3aed94e74a9873c7c8c991559cb4dcbd1a"
  }
}