{
  "visual_id": "E02-bonn",
  "title": "The public Bonn tensor benchmark",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T203530228825Z-E25-Bonn"
  ],
  "claim_ids": [
    "C02"
  ],
  "input_files": [
    {
      "path": "runs/20260929T203530228825Z-E25-Bonn/tensor-threshold-scan.csv",
      "sha256": "6d7d5c30ed4a88673e598243893a868fc743fc7de8bc6254f6be4d2280ca7a85"
    },
    {
      "path": "runs/20260929T203530228825Z-E25-Bonn/Bonn-thresholds.csv",
      "sha256": "080b8f7d9284710878a1cf31c0c54f68e6670cc5f4686549d78158f580b9ba51"
    },
    {
      "path": "runs/20260929T203530228825Z-E25-Bonn/ordinary-Bonn-baselines.csv",
      "sha256": "ebdcaf2eb21e855fc0a4f3c5a61bad26cafcd13751c4b7b62060c927a19a37be"
    }
  ],
  "configurations": {
    "E25-Bonn": {
      "points": [
        80,
        128,
        192
      ],
      "tensor_angular_points": 128,
      "momentum_map_scale_MeV": 1000
    }
  },
  "assumptions": {
    "E25-Bonn": [
      "Machleidt source potential plus independently solved relativistic momentum-space Hamiltonian; no refitting.",
      "A/B/C parameters from Li--Machleidt Table 1. Scalar delta does not contribute to the tensor subtraction.",
      "Tensor operator from Wang et al. 2018 Table I/2024 Eq.1, with monopole vertices squared, upper-spinor projections and consistent LSJ D-wave phase.",
      "Threshold is determined from zero-energy infinite-volume scattering, not a positive discretized energy being called bound.",
      "Published lambda values correspond to a_t approximately -100 fm, not exactly infinite scattering length. Both are calculated separately.",
      "Any source-target residual is reported. Tensor quenching is a diagnostic Hamiltonian change, not a matched fundamental field."
    ]
  },
  "plotted_values": {
    "path": "E02-bonn-data.json",
    "sha256": "9f126fef160a99ccb3345342974a4472698770dbd0acfa6f09868f930565b454"
  },
  "caption": "The original potential core and published A/B/C parameters reproduce ordinary binding within several eV. The tensor operator is independently projected with a checked LSJ phase. Unitarity and finite negative scattering length are different targets. The right panel compares our exact a=\u2212100 fm points with source multipliers described only as approximately \u2212100 fm, without a precision budget. At those quoted multipliers our values are about \u2212116 fm. The plotted difference does not by itself establish a discrepancy with a precision source datum. These are Hamiltonian perturbations, not field predictions.",
  "alt_text": "Bonn A, B and C lose the shallow deuteron at tensor strengths about 0.430, 0.580 and 0.642. Reconstructed minus-100-fm points lie slightly below their source targets.",
  "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": "3f1d57be9140437e6ec47fd2bb9c89bda3e5f8e6bc4933b7da034a4596b76d07",
    "png": "14c4fab612317f97f72c7afb49097f2b4ed7aa456410a091b46fccb7c65ab4fe"
  }
}