{
  "visual_id": "E39-atomic-inclusive",
  "title": "Boost redistributes spectator probability across bound and continuum channels",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261001T195600924014Z-E29-atomic-inclusive"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261001T195600924014Z-E29-atomic-inclusive/results.json",
      "sha256": "9ddda6bd7c36da2273fad54bcad95b9fe366eaaa27ecc0abb9bca70b5dfb85f8"
    },
    {
      "path": "runs/20261001T195600924014Z-E29-atomic-inclusive/independent-controls.json",
      "sha256": "75babb6c0b2a415f204f453be94ab9f8fc30cefe6613babb31ff36c388223631"
    }
  ],
  "configurations": {
    "E29-atomic-inclusive": {
      "parent": "20260930T210506521193Z-E29-atomic-mass",
      "parent_manifest_sha256": "fba452cab296e1527ccfc6845a537a054325f968161b776ba80985b30eff969a",
      "lmax_refinement": [
        2,
        4,
        6
      ],
      "series_terms_refinement": [
        4,
        6,
        8
      ],
      "spectral_refinement": [
        [
          200,
          128
        ],
        [
          400,
          256
        ],
        [
          800,
          512
        ]
      ],
      "fixed_beta_controls": [
        0.0,
        0.1,
        0.35
      ],
      "case_indices": [
        4,
        6,
        7
      ],
      "gates": {
        "spectral_closure_absolute": 3e-06,
        "series_absolute": 1e-07,
        "response_relative": 2e-06,
        "zero_recoil_absolute": 1e-11,
        "independent_coulomb_absolute": 1e-08
      },
      "wall_limit_seconds": 600,
      "threads": 1,
      "scope": "Inclusive spectator recoil spectral and kinematic response. No corrected weak lifetime, QED/current corrections or plasma reaction network."
    }
  },
  "assumptions": {
    "E29-atomic-inclusive": [
      "Normalized correlated coalescence state and finite nuclear masses are inherited from the exact frozen parent. Nuclear model discrepancies and nn-only conditional changes remain.",
      "True hydrogenic nl bound states and delta(k)-normalized Coulomb continuum are summed with boost-generated angular channels. Spherical Bessel series truncation, angular truncation and spectral discretization are independently refined; no closure normalization is imposed.",
      "Reported MeV\u00b2 responses include neutrino momentum and the energy-delta Jacobian with a fixed allowed heavy-particle matrix element. They are not corrected rates or lifetimes; weak recoil/current normalization, radiative/QED, finite-size and hyperfine terms are missing.",
      "The final internal spectator Hamiltonian remains nonrelativistic with reduced mass. Exact two-body COM neutrino kinematics do not make the internal Hamiltonian relativistic.",
      "Free-electron capture on populated ions, screening/exchange and reacting-plasma kinetics remain outside this isolated atom calculation."
    ]
  },
  "plotted_values": {
    "path": "E39-atomic-inclusive-data.json",
    "sha256": "9d8bcddeb365facfea3880a3e6adf8a1ff13e32244a7b9f40cd91b6d820ee96d"
  },
  "caption": "The unitary operator exp(i\u03b2z) acts on the normalized inherited coalescence state; \u03b2 is in inverse Bohr radii and l-channel probabilities include all magnetic orientations. Bound states run to n=800; delta-k Coulomb continua use 512 points. Zero probabilities are omitted on the log axis. The maximum displayed normalization deficit is below 2e-7 and is not renormalized. \u03b2=0.35 is a spectral stress control. This is an atomic normalization and kinematics calculation, not a weak lifetime or a measured spectrum.",
  "alt_text": "Finite boosts populate higher angular waves in both the bound and continuum spectrum; the unboosted state has only l=0.",
  "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": "c38b05210c3c2c75f32a5cbc976c6c51650a9ec3e15cdbd513bf3adc5339415e",
    "png": "7866d85ded76c477e3126627653e7ed2248f487ba8b4c88b3d66e6798667620c"
  }
}