{
  "visual_id": "E54-charged-threebody",
  "title": "A coupled screened charged three-body outgoing-flux calculation",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261002T034622487037Z-E28-charged-threebody"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261002T034622487037Z-E28-charged-threebody/refinement-synthesis.json",
      "sha256": "4ef332219e66d5389e69384b32cf2204c6e1cc8c9c73724f1ccfe9bc2b402470"
    },
    {
      "path": "runs/20261002T034622487037Z-E28-charged-threebody/results.json",
      "sha256": "42267c4659073ae012039f377e5c4a35a266a9d6d7976650b5977f4bd8faa8e1"
    }
  ],
  "configurations": {
    "E28-charged-threebody": {
      "model": "Equal-mass LO quartet, total orbital L0, zero-range np triplet and finite-screen pp Coulomb pair l1/spectator l1",
      "energies_MeV": [
        5.0
      ],
      "cutoff_MeV": 600.0,
      "screen_radius_fm": 2.0,
      "screen_power": 4,
      "pp_pair_ell": 1,
      "pp_radial_ranks": [
        12,
        24
      ],
      "spectator_panels": [
        120,
        240
      ],
      "product_orders": [
        24,
        40
      ],
      "angular_orders": [
        24,
        40
      ],
      "phase_orders": [
        60,
        100
      ],
      "pair_phase_absolute_gate_radians": 2e-05,
      "pair_source_relative_gate": 0.0005,
      "threebody_flux_balance_relative_gate": 0.003,
      "spectator_grid_relative_gate": 0.003,
      "radial_rank_relative_gate": 0.003,
      "phase_quadrature_relative_gate": 0.0003,
      "angular_product_relative_gate": 0.001,
      "neutral_amplitude_absolute_gate_fm": 1e-06,
      "neutral_flux_relative_gate": 1e-06,
      "max_sequential_production_jobs": 4,
      "whole_job_timeout_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "threads": 1,
      "scope": "Finite-screen finite-partial-wave charged Hamiltonian pilot; no unscreened full pd breakup, higher pp waves, doublet or 3BF claim.",
      "job": "quadrature"
    }
  },
  "assumptions": {
    "E28-charged-threebody": [
      "Same neutral np pole/equal mass and cutoff; add explicitly finite-screen pp Coulomb l1, total orbitalL0; no quartet3BF.",
      "Screened pp operator is iterated off shell via radial free-resolvent Nystrom matrix at positive and negative pair energies.",
      "Reciprocal Jacobi cross kernels and explicit proton antisymmetry; coupled equation solved with exact pp-block elimination.",
      "Outgoing three-body amplitude includes pp component, unchanged deuteron residue and identical-proton1/2; optical loss held out.",
      "FiniteR2fm, finite pp angular basis and rank are declared model/numerical limitations; no unscreened full pd breakup."
    ]
  },
  "plotted_values": {
    "path": "E54-charged-threebody-data.json",
    "sha256": "0d9bc14be3e0c968bf462fafefe11f8182459b94c3a90fd2045703a84529f73d"
  },
  "caption": "Actual off-shell pp Coulomb scattering and reciprocal npS/ppP Faddeev components supply the outgoing amplitude, including antisymmetric proton exchange. The normalization is not fitted to elastic loss. The failed coarse comparison is shown as a refinement control, never accepted evidence. The final finite-screen model passes unchanged numerical gates; pp higher odd waves, screening removal, spin-doublet channels and corresponding three-body forces are absent. This is not full unscreened proton\u2013deuteron breakup or an EFT error estimate.",
  "alt_text": "Grid refinement reduces the flux-balance discrepancy from0.477percent to0.061percent, below the fixed0.3percent gate; rank and quadrature refinements give small further changes.",
  "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": "8bac9f146c542980273d086c421ab4d66a7efe91d5271d5f88b6a5aaf6c26cf4",
    "png": "4def40102b1158dd1b8b445c70a72c4cacbaceebca2c40bbf8de329fea6569b0"
  }
}