{
  "visual_id": "E83-atomic-vacuum-polarization",
  "title": "Static atomic energy correction and finite-basis control",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261003T064522393857Z-W07-atomic-VP-production"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261003T064522393857Z-W07-atomic-VP-production/results.json",
      "sha256": "f952453bdcf163d15c6c24a8c0c2e3a2099f05a4c90bf9ac9e53638c713f7ecd"
    },
    {
      "path": "runs/20261003T064522393857Z-W07-atomic-VP-production/order10.npz",
      "sha256": "de2981c8a2b56e8e46dfe252be1afddcbfb698f5873f393c7e0e8a00cd050372"
    }
  ],
  "configurations": {
    "W07-atomic-VP-production": {
      "stage": "preregistered_energy_production_and_separate_contact_diagnostic",
      "parent": "20260930T210506521193Z-E29-atomic-mass",
      "potential_source": "Frolov2111.05381v1Eq2/3, electrostatic potential multiplied by test charge",
      "charge_products": {
        "electron_nucleus": -2,
        "electron_electron": 1
      },
      "units": "ordinary a0,Hartree; on-shell alpha, electron loop",
      "loop_points": 64,
      "cosh_upper": 16,
      "threads": 1,
      "maximum_RSS_bytes": 3221225472,
      "whole_timeout_seconds": 600,
      "scope": "First-order static electronic vacuum-polarization atomic energy/contact component, not complete QED or inclusive weak rate",
      "basis_orders": [
        4,
        6,
        8,
        10
      ],
      "quadrature_relative_gate": 1e-07,
      "independent_relative_gate": 2e-10,
      "basis_energy_relative_gate": 0.0002,
      "finite_lambda_relative_gate": 0.0001,
      "contact_basis_relative_gate": 0.01,
      "benchmark_run": "20261003T062555526603Z-W07-atomic-VP-benchmark",
      "contact_acceptance": "Not admitted from Bohr-scale basis alone; independent ordinary hydrogenic short-range response required before asymmetrical basis extension.",
      "loop_refinements": [
        "cosh64/96",
        "sine96",
        "cosh_upper16/20",
        "radial14/17"
      ],
      "local_alpha_scales": [
        0.1,
        0.01
      ],
      "parent_isotopes": [
        "helion",
        "alpha particle"
      ],
      "daughter_mass_source": "same frozen ordinary triton CODATA mass; alpha is atomic control only",
      "hydrogen_contact_controls": {
        "loop_points": 160,
        "cosh_upper": 24,
        "basis_powers": [
          8,
          12,
          16,
          20,
          24
        ],
        "oracle_relative_gate": 0.0001,
        "resolvent_residual_gate": 1e-10,
        "realspace_Green_gate": 1e-12,
        "small_alpha_limit_gate": 0.004,
        "refined_subdivision": 2,
        "refined_decimal_digits": 60
      },
      "preserved_runs": [
        "20261003T063813341057Z-W07-atomic-VP-production",
        "20261003T064046220373Z-W07-atomic-VP-production",
        "20261003T064051568047Z-W07-atomic-VP-contact-resolution",
        "20261003T064258029914Z-W07-atomic-VP-production",
        "20261003T064338708175Z-W07-atomic-VP-production"
      ]
    }
  },
  "assumptions": {
    "W07-atomic-VP-production": [
      "First-order static electron-loop pair potentials; no complete QED, radiative recoil, finite size or weak lifetime.",
      "Ordinary helion/triton masses stay distinct from conditional nuclear-model trajectories.",
      "Both electron-nuclear and electron-electron vacuum-polarization terms retained."
    ]
  },
  "plotted_values": {
    "path": "E83-atomic-vacuum-polarization-data.json",
    "sha256": "75d50a5e7fe1a4aafec6ba5a76c3621d5159261db06e2b4a930c6997044f92d8"
  },
  "caption": "The left values are first-order corrections in the same finite-mass correlated helium-3 state, with two nuclear pairs and one electron pair. The right sequence need not be variational; it resolves this potential expectation, not omitted physical operators. Independent analytic polynomial moments and an infinite-loop integral reproduce the complete correction. The separate contact response fails its basis gate and has unresolved overlap conditioning. No complete QED threshold, corrected contact amplitude or weak lifetime follows.",
  "alt_text": "Nuclear attraction dominates the small repulsive electron contribution. The last relative energy-correction change is 5.49e-5, below the declared 2e-4 gate.",
  "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": "3b945d8f8916df2befd06cf4b155d58dddd25828415325327afcc668c0db5dd5",
    "png": "d4cb73d728011ce10fc89fea74cb24fa5bdf5424630f4e8fd74217f68cf64a16"
  }
}