{
  "visual_id": "E12-charged-threebody",
  "title": "Charged bound states and the extra NLO input",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T224825117361Z-E28-charged"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20260929T224825117361Z-E28-charged/charged-ordinary-renormalization.csv",
      "sha256": "3f35db5e1fe22411d88e5d5bcff41a0739c4a8cd7ddc7da9829dae52fa011c63"
    },
    {
      "path": "runs/20260929T224825117361Z-E28-charged/charged-source-benchmark.csv",
      "sha256": "758de566c83db3c5bc11de618b30e5081a6a769febab9142d62424f0e2355605"
    },
    {
      "path": "runs/20260929T224825117361Z-E28-charged/nn-only-fixed-force-diagnostic.csv",
      "sha256": "4b2a74d948165928eecdbee515ec51d134bf3b387df60a16ebc9a2fc3bee8c06"
    }
  ],
  "configurations": {
    "E28-charged": {
      "cutoffs_MeV": [
        300,
        600,
        1200,
        1800
      ],
      "points": [
        96,
        144
      ],
      "angles": [
        32,
        64
      ],
      "fitted_Btriton_MeV": 8.4818,
      "fitted_BHe3_MeV": 7.718043,
      "physical_inverse_ann_fm": -0.052910052910052914,
      "a_np_fm": -23.74,
      "aC_pp_fm": -7.8063,
      "ranges_fm": [
        1.765,
        2.73,
        2.794
      ],
      "nn_range_fm": 2.75,
      "source_curve_tolerance_MeV": 0.025
    }
  },
  "assumptions": {
    "E28-charged": [
      "Iterate all published O(alpha) Coulomb exchange diagrams and the Coulomb-resummed pp propagator at LO.",
      "Integrate the zero-photon-mass logarithmic singularity by subtraction; do not replace a diagonal infinity with an uncorrected finite value.",
      "Effective ranges, gauged range vertices and three-body corrections enter exactly once at NLO.",
      "Fit strong H and H1 to ordinary tritium, then fit the required charged Halpha to ordinary He3. The latter is a calibration, not a held-out prediction.",
      "Compare independently extracted published LO binding curves in their isospin-symmetric input convention separately from the physical nn-input calculation.",
      "An nn-only diagnostic leaves the npp sector unchanged. Holding H1 fixed away from its ordinary calibration does not determine the additional scattering-length-dependent NLO short-distance response; cutoff spread is exposed.",
      "No charged continuum scattering, four-body amplitudes, new weak currents or fundamental field trajectory is inferred."
    ]
  },
  "plotted_values": {
    "path": "E12-charged-threebody-data.json",
    "sha256": "6158e8777ab0bcb67ccc102c05f8f0fd2f7c552c0599b8fc64c5fcab111c277b"
  },
  "caption": "All O(alpha) three-body Coulomb kernels are iterated; the pp propagator resums Coulomb ladders. The logarithmic singularity is integrated at zero photon mass. The source curve comparison uses its isospin-symmetric convention and retains a 6\u201313-keV graphical/convention residual. The second panel instead uses the physical nn input. Fitting an NLO electromagnetic three-body term restores ordinary He3 binding by construction; it is not a prediction. The last panel holds the ordinary NLO strong term fixed in an nn-only variation and exposes unresolved cutoff dependence away from its calibration point. It is not a renormalized field response.",
  "alt_text": "The source helium-3 curve is approximately reproduced. Omitting the NLO electromagnetic force causes growing cutoff dependence. Fitting ordinary nuclear bindings does not fix the response away from the calibration point.",
  "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": "42699ddb686e021152c7f2de698234d53ccd11c02c50a72f31a17bad1015eebe",
    "png": "e6de5428ab9393c8613d2bce941a72ea0566c7cb192eff6b45bfbbf7e63c4c21"
  }
}