{
  "visual_id": "E10-coupled-transition",
  "title": "A source nuclear Hamiltonian crossing its threshold",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260929T220308671706Z-E32-coupled",
    "20260929T220837446601Z-E32-continuum-check"
  ],
  "claim_ids": [
    "C02",
    "C06"
  ],
  "input_files": [
    {
      "path": "runs/20260929T220308671706Z-E32-coupled/coupled-transition-results.csv",
      "sha256": "999cc7717a2720de663dbf9ea69490d29cfab2ab411edef084c644d2e0eb5c89"
    },
    {
      "path": "runs/20260929T220308671706Z-E32-coupled/excursion-04.npz",
      "sha256": "8d87eb7d48450e937e5af06823418ba455bca6478d22fd2cf948b4c742b6f994"
    },
    {
      "path": "runs/20260929T220837446601Z-E32-continuum-check/results.json",
      "sha256": "80fed4f3fb53066c271679e7dd22a33f281a1be5d34997c10561444804b35395"
    }
  ],
  "configurations": {
    "E32-coupled": {
      "source_run": "20260929T203530228825Z-E25-Bonn",
      "cases": [
        {
          "points": 192,
          "tau": 0.02,
          "dt": 0.002,
          "hold": 1.0
        },
        {
          "points": 192,
          "tau": 0.2,
          "dt": 0.002,
          "hold": 1.0
        },
        {
          "points": 192,
          "tau": 2.0,
          "dt": 0.002,
          "hold": 1.0
        },
        {
          "points": 128,
          "tau": 0.2,
          "dt": 0.0005,
          "hold": 1.0
        },
        {
          "points": 192,
          "tau": 0.2,
          "dt": 0.0005,
          "hold": 1.0
        },
        {
          "points": 256,
          "tau": 0.2,
          "dt": 0.0005,
          "hold": 1.0
        },
        {
          "points": 256,
          "tau": 2.0,
          "dt": 0.001,
          "hold": 1.0
        },
        {
          "points": 192,
          "tau": 0.0002,
          "dt": 1e-05,
          "hold": 1.0
        },
        {
          "points": 192,
          "tau": 0.2,
          "dt": 0.002,
          "hold": 0.0,
          "low": 1.0
        },
        {
          "points": 80,
          "tau": 0.2,
          "dt": 0.0005,
          "hold": 1.0
        }
      ]
    },
    "E32-continuum-check": {
      "parent_run": "20260929T220308671706Z-E32-coupled",
      "points": 256,
      "tau": 0.02,
      "hold": 1.0,
      "dt": [
        0.0001,
        5e-05
      ]
    }
  },
  "assumptions": {
    "E32-coupled": [
      "Reuse source Bonn B relativistic S/D Hamiltonian and independently projected tensor operator without refitting.",
      "Excursion from lambda=1 to .4, below the previously verified infinite-volume threshold .57957, and back to 1.",
      "Prescribed homogeneous histories and closed-system quantum work; neither an allowed cosmic wall nor field backreaction is supplied.",
      "All quadrature continuum states are propagated. Return projection uses the exact bound subspace of the final Hamiltonian.",
      "No absorber, irreversible decay, thermal capture rate or hysteresis is inferred. Finite-time continuum quadrature is explicitly refined.",
      "The published tensor-subtraction residual from E25-Bonn remains; no precision reproduction beyond that scope."
    ],
    "E32-continuum-check": [
      "Reuse frozen independently constructed Bonn B 256-point operators from the parent calculation.",
      "Reserve the fastest plotted passage for combined continuum/time refinement.",
      "This numerical check retains the same prescribed tensor trajectory and all physical limitations."
    ]
  },
  "plotted_values": {
    "path": "E10-coupled-transition-data.json",
    "sha256": "20d6d925c392671fbbf47c0ce9e71f98ac6a6dda160a7c471379989cb55d86a4"
  },
  "caption": "Bonn B follows a prescribed smooth excursion from tensor multiplier 1 to 0.4 and back, holding for \u210f/MeV between ramps. The minimum lies below its verified infinite-volume binding threshold. The complete S/D Hamiltonian and its quadrature continuum are propagated, with time, momentum-grid, sudden-limit and independent ODE controls. Nuclear energy change is checked against the supplied work. The final projector measures returned binding; intermediate overlap with the original deuteron is not an instantaneous bound fraction. Passage times are diagnostic, not derived from a viable field. No irreversibility, hysteresis or thermal capture rate is claimed.",
  "alt_text": "Only part of the initial deuteron returns to the bound state after the interaction is restored. The external work agrees with the nuclear energy change.",
  "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": "b5799e15bd11e3b708a43dd8a749aab0428f54ca6c10ec32cd426aea67d8508c",
    "png": "008c07a9667111e667f7b4d77d14659535f4255a6890f87abcd236492e373b51"
  }
}