{
  "visual_id": "E52-ordinary-weak-capture",
  "title": "Ordinary weak-current recoil and a separate muon benchmark",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261002T033607509184Z-E29-ordinary-weak-capture"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261002T033607509184Z-E29-ordinary-weak-capture/results.json",
      "sha256": "39bb3f2ddff13b6e6c66e65af8e17d4ce2c53eca47575a0cefa796ffc36e9cd6"
    }
  ],
  "configurations": {
    "E29-ordinary-weak-capture": {
      "completed_component": "Ordinary continuum electron-proton capture with exact tree-level point-current recoil, external-state and spin normalization, plus a separately labelled published muonic-hydrogen spin/radiative benchmark.",
      "remaining": [
        "Electronic capture QED inclusive radiative correction with a specified photon prescription",
        "Electronic finite-size and momentum-dependent form factors including induced pseudoscalar contribution",
        "Atomic incident-electron screening and exchange from a matched antisymmetrized bound-continuum Hamiltonian",
        "Atomic hyperfine populations and trinucleon recoil-current operators",
        "Unconditional atomic capture lifetimes and phase-dependent plasma population coupling"
      ],
      "electron_energies_total_MeV": [
        1.3,
        1.4,
        2.0,
        3.0,
        5.0,
        12.0
      ],
      "angular_orders": [
        16,
        32
      ],
      "electron_current": {
        "f": 1.0,
        "g": 1.26,
        "f2": 3.706,
        "gp": 0.0,
        "form_factors": "constant, Vogel-Beacom1999 benchmark convention; induced pseudoscalar excluded",
        "source": "W07-VogelBeacom-20261002 Eq4; current sign and q=pn-pp fixed independently by W07-MuonRadiative-20261002 Eq6"
      },
      "muon_benchmark": {
        "mass_MeV": 105.6583755,
        "f": 0.976,
        "g": 1.247,
        "f2": 3.583,
        "gp": 8.2,
        "GF_MeV_minus2": 1.166371e-11,
        "Vud": 0.9738,
        "finite_size_contact_factor": 0.995,
        "radiative_rate_factor": 1.028,
        "published_tree_singlet_s_inverse": 692.3,
        "published_corrected_singlet_s_inverse": 711.5,
        "source": "W07-MuonRadiative-20261002 Eqs6-13,25-26; muon mass E26-CODATA"
      },
      "parents": [
        "20261001T195600924014Z-E29-atomic-inclusive",
        "20260930T210506521193Z-E29-atomic-mass"
      ],
      "primary_inputs": [
        "data/raw/W07-VogelBeacom-20261002/paper.pdf",
        "data/raw/W07-VogelBeacom-20261002/paper.pdf.provenance.json",
        "data/raw/W07-MuonRadiative-20261002/paper.pdf",
        "data/raw/W07-MuonRadiative-20261002/paper.pdf.provenance.json",
        "data/raw/E26-CODATA/constants.txt",
        "data/raw/E26-CODATA/constants.txt.provenance.json"
      ],
      "relative_gates": {
        "spinor_trace": 3e-12,
        "invariant_no_magnetism": 3e-12,
        "lab_cm": 1e-09,
        "angular_refinement": 1e-11,
        "spin_mixture": 3e-12,
        "published_rest_formula": 3e-12,
        "muon_tree_reproduction": 0.0005,
        "muon_corrected_reproduction": 0.0005,
        "heavy_mass_limit": 3e-06
      },
      "resources": {
        "whole_job_timeout_seconds": 600,
        "maximum_RSS_bytes": 3221225472,
        "threads": 1,
        "max_jobs": 4
      }
    }
  },
  "assumptions": {
    "E29-ordinary-weak-capture": [
      "Ordinary electron capture only; nuclei retain physical proton/neutron masses. No conditional shifted-mass atomic lifetime supplied.",
      "Electron continuum result is sigma v/(GF^2 |Vud|^2), not a neutron-lifetime-normalized prediction. Constant f1,g1,f2 with gp=0 is a declared current truncation.",
      "Muon benchmark reproduces published form factors, finite-size contact and radiative factor for muonic hydrogen only; no factor transferred to electrons.",
      "Canonical initial spin singlet/triplet are coherent spin preparations for the continuum. They do not determine atomic hyperfine populations."
    ]
  },
  "plotted_values": {
    "path": "E52-ordinary-weak-capture-data.json",
    "sha256": "64a89db6acb17fa90aff6c89f015ed9a016973db6d3ac2ff1707b52286910038"
  },
  "caption": "Electronic rates use a constant point-current f1/g1/f2 benchmark with no induced pseudoscalar, atomic wavefunction or QED correction. Exact tree-level recoil includes currents and external-state normalization, not only the phase-space Jacobian. The muon panel separately uses the published finite-q current, finite-size contact and rounded1.028 radiative factor; it reproduces a source calculation rather than computing new loops. None of those muon corrections is borrowed for the electron/trinucleon atomic lifetime.",
  "alt_text": "The electronic current correction grows to about4.9percent at12MeV. The separate muon singlet rate is much larger than its triplet rate.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
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  },
  "command": "python run.py full public-report",
  "output_sha256": {
    "svg": "2888c59bba1ff33d8e93ae7290e49f465a30ba5f4e0287052e0863e40960c0f1",
    "png": "5ac50fc3a9aba4cb7d2b420fc9e39490ac72a23bbe8f57689d4a21058c402955"
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}