{
  "visual_id": "E98-conversion-regulator-cluster",
  "title": "A matched three-body limit does not repair the separated-dimer prescription",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261004T202054925963Z-W05-fourbody-conversion-benchmark"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261004T202054925963Z-W05-fourbody-conversion-benchmark/results.json",
      "sha256": "8c1f9f66435a66ca956bab34d62e7ec4536cfa3f5aacd16302652cda7e0b1f2f"
    }
  ],
  "configurations": {
    "W05-fourbody-conversion-benchmark": {
      "cutoff_MeV": 1200.0,
      "H": -1.912525083123017,
      "Bd_MeV": 2.2245663699998204,
      "Bnn_MeV": 2.5,
      "mass_n_MeV": 939.56542194,
      "negative_binding_MeV": [
        5.0,
        8.4818,
        11.767153560055796,
        20.0
      ],
      "spectator_orders": [
        24,
        48
      ],
      "pair_cutoff_ratios": [
        2,
        4,
        16,
        128,
        2048
      ],
      "angular_orders": [
        256,
        512
      ],
      "operator_gate": 1e-10,
      "spin_gate": 1e-11,
      "whole_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "frozen_inputs": {
        "src/metastable/public_stm_attached_contact.py": "f2d7f72ed8d414114d245624d5105a9994fdb7a458778eddf27921cceaa0bbbf",
        "src/metastable/public_fourbody_projection.py": "05b398f7f8e91612e65fce5f85f28e8de24d80f995c98b99f50c9021cef5de5e",
        "src/metastable/spin_fewbody.py": "9a80e2f94c6c10089cc6da3ac2b75602a989e3e1dbc5843d0f8d7ae31d2cb9ca",
        "src/metastable/spin_channels.py": "68dbaa8b4c0df6050ca2a7c6432902e34b80beeef7c9402dcd79b0c4080a1af6",
        "reports/fourbody-conversion-regulator-plan-20261004.md": "7c944dd1779ede916132332b528a6dab6764fb0c8e02941f1e2d4a05199410e6",
        "reports/stm-attached-contact-findings.md": "01911fa8cc81402b9f9c1515033023146929860334c6547754023f9e001d8559",
        "reports/fourbody-projection-findings.md": "c8a73eb7190bc1894a7a0cd140c80a4203886f3d252a3b88017d8b84bde12609",
        "data/raw/E28-Hammer/paper.pdf": "7fb2fd6435ae37650ffeb769f16da12c0c0338b1d464d24411b8ad300e8532c1",
        "data/derived/spin-sources/E28-Hammer.txt": "04f698e0ad63807e51154315da8bae6fd24cabc0512778df04d980ed4bec8951"
      },
      "parents": [
        {
          "id": "20261003T012657182307Z-E28-STM-fourbody-operator",
          "sha256": "ef32f797173a01fb1d113fc4a6a1f05c007f86fd0ee93e1b527341f626a58e7b"
        },
        {
          "id": "20261003T192457580506Z-W05-STM-attached-contact",
          "sha256": "21562b12b883288ee40d9aaef007c78f228fa2dd24416dfae8f473dfe7faa492"
        },
        {
          "id": "20261003T223509360913Z-W05-fourbody-projection-benchmark",
          "sha256": "1ba43b041b3e64f3b11d051e3fab103c6c296ae10c7485c55f13fde3910af734"
        },
        {
          "id": "20261004T201927550051Z-W05-fourbody-conversion-benchmark",
          "sha256": "2e1ac6f3b71748471736c73d02131c965f11e6f77016a865b2c617968c8188e5"
        }
      ],
      "scope": "New conversion Hamiltonian method only: N3 complete limiting STM comparison and N4 separated np-triplet+nn-singlet dimer cluster obstruction. Finite R differs from parent; no matched N4 action, amplitude, force refit, or global physical claim.",
      "preliminary_run_role": "All preliminary344 checks passed; final adds preregistered independent MP80 angular contractions and rigorous finite-R matrix-error bounds; no gates changed."
    }
  },
  "assumptions": {
    "W05-fourbody-conversion-benchmark": [
      "New conversion Hamiltonian method only: N3 complete limiting STM comparison and N4 separated np-triplet+nn-singlet dimer cluster obstruction. Finite R differs from parent; no matched N4 action, amplitude, force refit, or global physical claim."
    ]
  },
  "plotted_values": {
    "path": "E98-conversion-regulator-cluster-data.json",
    "sha256": "01288691be7979e27b702363a68310d43204088a8444f0f4fd412f684858fa68"
  },
  "caption": "All points use the new conversion-regulated Hermitian model, the inherited 1200 MeV spectator cutoff and Bnn=2.5 MeV. The left panel takes the maximum over all eight declared negative-energy/grid supports. The right panel evaluates the original deuteron and dineutron product state after spatial separation at finite cutoffs, then varies the pair cutoff at fixed spectator cutoff. Its growing energy defect is not an eigenvalue, binding prediction or new threshold. Independent angular-log matrices and high-precision dimer integrals reproduce both trends; finite-regulator matching remains inexact.",
  "alt_text": "As the pair cutoff rises, the three-body matrix difference falls while the separated product-state defect grows. The tested four-body cluster completion is rejected.",
  "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": "b06551822debed40d482a803719acc9ec628fd33d1db67d4236e10a9eb88797a",
    "png": "bf90096a814fdf898fc6ce80c6e70f8654875b3d864d1701d4c399c9a074d300"
  }
}
