{
  "visual_id": "E30-neutral-breakup",
  "title": "Neutral higher partial waves across three-body breakup",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260930T195637530757Z-E28-neutral-breakup"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20260930T195637530757Z-E28-neutral-breakup/partial-amplitudes.csv",
      "sha256": "9b916079d07a599ed6998e5a396d8c025fda43fa7f40d7f2e04f4a38b142f7f8"
    },
    {
      "path": "runs/20260930T195637530757Z-E28-neutral-breakup/inclusive-cross-sections.csv",
      "sha256": "2f728dfe87033d2f5003fb3d14e1f62f2d1c3348f20eeb2f33bb9be2082e61db"
    },
    {
      "path": "runs/20260930T195637530757Z-E28-neutral-breakup/results.json",
      "sha256": "e83890c7b98edc3c9fa78013816f2669ebf38326164d66f4501eb425e3aba7af"
    }
  ],
  "configurations": {
    "E28-neutral-breakup": {
      "energies_MeV": [
        0.5,
        1.0,
        2.0,
        2.2235663699998205,
        2.2255663699998203,
        2.3,
        3.0,
        5.0,
        10.0
      ],
      "ell": [
        0,
        1,
        2,
        3,
        4
      ],
      "cutoffs_MeV": [
        600,
        1200
      ],
      "points": [
        176,
        256
      ],
      "contour_depths": [
        0.4,
        0.7
      ],
      "amplitude_tolerance_fm": 2e-05,
      "elastic_unitarity_tolerance": 2e-06,
      "positivity_tolerance": 2e-06
    }
  },
  "assumptions": {
    "E28-neutral-breakup": [
      "Primary partial-wave equations: Gabbiani, Bedaque and Griesshammer nucl-th/9911034, Eqs 3.2-3.4; charge-resolved doublet recoupling retained from Hammer-Konig.",
      "LO pair interactions remain S wave; spectator orbital waves l=0 through 4 are solved, not NN P-wave forces or tensor mixing.",
      "H is fitted once to ordinary triton at each real cutoff; only l=0 doublet receives this force. No observable here is fitted.",
      "q=x-i*d*x*(1-x/Lambda) keeps both cutoff endpoints fixed; physical outgoing pair square root and exchange log continue on lower contour.",
      "Inclusive breakup uses 1-|S|^2. Optical balance is an algebraic normalization check, NOT an independent integrated exclusive breakup-flux test.",
      "Conjugation, independent angular integrals, independent below-threshold PV amplitudes, grids and contour depths test numerical conventions.",
      "No charged breakup, exclusive final-state distributions, finite-field response, NLO error posterior, thermally extrapolated rates or full E28/E29 completion claimed."
    ]
  },
  "plotted_values": {
    "path": "E30-neutral-breakup-data.json",
    "sha256": "1e7c4c33466c30718de6f65bd35d8880c12a87a76e7c2bd95bde8243a2d83a93"
  },
  "caption": "LO STM amplitudes retain pair S-wave forces and extend spectator l=0 through 4. A lower complex contour avoids outgoing poles and cuts while preserving the real regulator endpoint. Independent below-threshold principal-value amplitudes, conjugation, angular projections, grids and contour depths pass. Inclusive breakup comes from elastic loss 1\u2212|S|\u00b2; optical balance is an algebraic normalization check, not an independent integrated exclusive three-body flux. Two cutoffs and the last retained wave diagnose sensitivity, not a complete EFT uncertainty or partial-wave bound. The later quartet l=0 exclusive calculation supplies one independent flux control; doublet/higher-wave exclusive distributions, charged breakup, thermal rates and finite-field matching remain unfinished.",
  "alt_text": "Neutral partial-wave amplitudes become absorptive above deuteron breakup. Inclusive loss rises continuously; higher spectator waves contribute at 10 MeV, with small displayed cutoff differences.",
  "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": "aca48c9d70eff154c0e11cc680b593c5d028c43601f18a1d86486117d8be3bd1",
    "png": "77ba5f57455089921701ae5b02215081ecbb7e2d602291f56d6e50edd5c71c33"
  }
}