{
  "visual_id": "E31-charged-partial-waves",
  "title": "Charged doublet P, D and F waves below breakup",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20260930T205654839089Z-E28-pd-partial-waves"
  ],
  "claim_ids": [
    "C02",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20260930T205654839089Z-E28-pd-partial-waves/higher-pd-zero-screen.csv",
      "sha256": "412798818e96522609913bc87e8b262112671ecbe338f3a3bf9d35a950f1078d"
    },
    {
      "path": "runs/20260930T205654839089Z-E28-pd-partial-waves/screened-higher-pd-phases.csv",
      "sha256": "048c56f9ab7cd35265bc24f3d475afc6859b1e786c7638a39dee74741c8c5a20"
    },
    {
      "path": "runs/20260930T205654839089Z-E28-pd-partial-waves/neutral-higher-wave-controls.csv",
      "sha256": "bd821d1244b414b46eea9216b6f1ab96d0c65057afcd9aac3caee506cd2bc30f"
    },
    {
      "path": "runs/20260930T205654839089Z-E28-pd-partial-waves/results.json",
      "sha256": "141f29b4cdd94361b10f54b55ca8a72a08e296cfad7bd18a934c8a8d1f0f5791"
    }
  ],
  "configurations": {
    "E28-pd-partial-waves": {
      "parent": "20260929T224825117361Z-E28-charged",
      "ell": [
        1,
        2,
        3
      ],
      "cutoffs_MeV": [
        600,
        1200
      ],
      "k_MeV": [
        20,
        35,
        50
      ],
      "screen_MeV": [
        1.0,
        0.5,
        0.25,
        0.125
      ],
      "quadrature_per_interval": [
        32,
        48
      ],
      "angular_points": 48,
      "grid_tolerance_degrees": 0.025,
      "screen_window_tolerance_degrees": 0.06,
      "angular_tolerance_degrees": 0.01
    }
  },
  "assumptions": {
    "E28-pd-partial-waves": [
      "Project the pre-S-wave angular kernels of Konig et al. Eqs 33,65-67 with P_l; neutral exchange follows Gabbiani et al. Eqs 3.2-3.3, including its (-1)^l convention.",
      "Doublet spin only, spectator l=1,2,3; NN interactions remain S wave. Spin-orbit/tensor forces and independent NN higher partial waves are absent.",
      "All single-photon exchanges are iterated at LO and the pp pair is Coulomb resummed. The box keeps the published expansion through linear photon mass; omitted O(lambda\u00b2) terms vanish in screening limit.",
      "NLO has a single effective-range and gauged-range insertion. Momentum-independent three-body forces project to zero for l>0; no higher-wave phase is fitted.",
      "Only energies below three-body breakup. The real on-shell pole is treated by PV subtraction plus its outgoing residue.",
      "Subtract the independently solved pure composite-deuteron Coulomb phase at each l and photon mass; screened full phases themselves have no unscreened limit.",
      "Neutral limits, l=0 old-solver recovery, reciprocity, direct angular integrals, grid/angular/screening changes, LO and perturbative NLO unitarity test conventions.",
      "Screening extrapolation and two cutoffs are numerical/regulator diagnostics, not an EFT truncation posterior. No exclusive breakup or charged above-breakup amplitude or finite-field rate is supplied."
    ]
  },
  "plotted_values": {
    "path": "E31-charged-partial-waves-data.json",
    "sha256": "9ef93c48b51ba69bed2b4c9dea1a1c7dd55e4d72225bf2a72e7c2abcbc189a41"
  },
  "caption": "These ordinary-background doublet amplitudes extend spectator l=1,2,3 while keeping pair S-wave interactions. Angular projection is applied to the source kernels before their S-wave average; it is a new equation extension, not a published higher-wave table. LO iterates the one-photon kernels, while NLO is one perturbative insertion. A separate composite-deuteron Coulomb amplitude defines the subtraction convention. Linear zero-screen intercepts use the three smallest photon masses; the window/grid comparisons are numerical diagnostics, not an EFT truncation uncertainty. All momenta remain below breakup. Charged quartet waves, charged breakup, doublet/higher-wave exclusive neutral flux and finite-field matching remain unfinished.",
  "alt_text": "Charged doublet P, D and F phases differ between LO and a strict NLO insertion. Screening and momentum-grid changes are displayed separately, along with the neutral-channel control; none is a phase-transition observable.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
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    "src/metastable/continuation_report.py": "f9bbce6d0e201a9f55c826d6e9c47ab901e51a71b4a1f962b52eb08a63ba5fe9",
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    "src/metastable/atomic_mass_report.py": "46dd1cdb56a5a02cafe001a1f6a7fb201e149461850df41e012f77a580c3694b",
    "src/metastable/closure_report.py": "b34a03a9e0058eed65722df542dbb92691dd138787e2078b43ee9f18e221f75c",
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    "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",
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    "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": "6e934e80f308976c391be65e98d40053f696a2b1d305f1f8299477ddf5278bd8",
    "png": "3646453c92b334e97fa828a37ab4aa957dc11a563f00c99f76d700c4d8f38693"
  }
}