{
  "visual_id": "E88-quarkmass-current-matching",
  "title": "Source scattering and current matching at declared pion masses",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261003T192357984026Z-W13-quarkmass-matching"
  ],
  "claim_ids": [
    "C02",
    "C04",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261003T192357984026Z-W13-quarkmass-matching/central-ERP.csv",
      "sha256": "43f3c276822338b059e7a9fb44dd44c00a27b6686fc55eb7a6a8cf6fcf15062e"
    },
    {
      "path": "runs/20261003T192357984026Z-W13-quarkmass-matching/current-matching.csv",
      "sha256": "b7567e7eebd927c25f0f408a340e7862ff7aed375c7d34e08e5ed45d88f3a01e"
    },
    {
      "path": "runs/20261003T192357984026Z-W13-quarkmass-matching/results.json",
      "sha256": "b9187a23f86cdcf47f879f061e7112adcf110af6c51efdb7f0ced66f305deae6"
    }
  ],
  "configurations": {
    "W13-quarkmass-matching": {
      "M_MeV": 938.92,
      "f_MeV": 132.0,
      "gA": 1.25,
      "HC_MeV_fm": 197.3269804,
      "m_physical_MeV": 138.0,
      "m_lattice_MeV": 353.7,
      "m_lattice_error_MeV": 2.1,
      "LGT_physical_fm2": -4.513,
      "kappa_physical": 2.35,
      "alpha": 0.0072992700729927005,
      "cold_speed_m_s": 2200.0,
      "c_m_s": 299792458.0,
      "channels": [
        {
          "channel": "3S1",
          "a_physical_fm": 5.423,
          "a_physical_error_fm": 0.005,
          "r_physical_fm": 1.764,
          "r_physical_error_fm": 0.002,
          "a_lattice_fm": 0.63,
          "a_lattice_error_fm": 0.74
        },
        {
          "channel": "1S0",
          "a_physical_fm": -23.714,
          "a_physical_error_fm": 0.003,
          "r_physical_fm": 2.73,
          "r_physical_error_fm": 0.03,
          "a_lattice_fm": 0.63,
          "a_lattice_error_fm": 0.5
        }
      ],
      "mu_MeV": [
        100.0,
        138.0,
        200.0
      ],
      "lambda_MeV": [
        500.0,
        750.0,
        1000.0
      ],
      "m_supports_MeV": [
        100.0,
        106.0,
        110.0,
        120.0,
        125.0,
        130.0,
        135.0,
        138.0,
        140.0,
        142.0,
        145.0,
        150.0,
        165.0,
        180.0,
        200.0,
        300.0,
        353.7
      ],
      "current_m_supports_MeV": [
        125.0,
        130.0,
        135.0,
        138.0,
        140.0,
        141.0
      ],
      "sources": [
        "data/raw/W13-Chen-quarkmass-20261003/paper.pdf",
        "data/raw/W13-Chen-quarkmass-20261003/paper.pdf.provenance.json",
        "data/raw/W13-KSW-1998-20261003/paper.pdf",
        "data/raw/W13-KSW-1998-20261003/paper.pdf.provenance.json",
        "data/raw/W13-Chen-current-1999-20261003/paper.pdf",
        "data/raw/W13-Chen-current-1999-20261003/paper.pdf.provenance.json",
        "data/raw/W13-KSW-counting-1998-20261003/paper.pdf",
        "data/raw/W13-KSW-counting-1998-20261003/paper.pdf.provenance.json"
      ],
      "source_sha256": {
        "data/raw/W13-Chen-quarkmass-20261003/paper.pdf": "493d15d727c240036bdf7355a9f6ef9d87b9075ef397470f6158fc42849cf454",
        "data/raw/W13-Chen-quarkmass-20261003/paper.pdf.provenance.json": "121905b8f8a7b649a9feadf7987deba6a0a42e87b553da3c63cce49029ffb3fa",
        "data/raw/W13-KSW-1998-20261003/paper.pdf": "d0d7d5c42ea812e3138e3cd351997703e8e54b28a2f952a842497148506a147f",
        "data/raw/W13-KSW-1998-20261003/paper.pdf.provenance.json": "3724ce53944c764de2fa974ef7dbe4973a3933480c8b181d314e62fa2e1f4069",
        "data/raw/W13-Chen-current-1999-20261003/paper.pdf": "d58b3eb8499c95a49e7aa6d63faea45397c64950b570eed1281346e045564440",
        "data/raw/W13-Chen-current-1999-20261003/paper.pdf.provenance.json": "fea51d87c6d832ffa569ab71005586360ad272cba25b3448b123a0a8005be9f4",
        "data/raw/W13-KSW-counting-1998-20261003/paper.pdf": "a581ad14af495639984454b2af5f2e1b3f0a8dc49545cbd778ae0aca69412b66",
        "data/raw/W13-KSW-counting-1998-20261003/paper.pdf.provenance.json": "ef94607b1d94316c056b153c561c37f65af02144d37ef81e907fb73814a57f15"
      },
      "primary_conventions": {
        "gamma": "HC/a_phys fixed LO inside loops",
        "gamma_bar": "Distinct reparameterized Eq10 intercept, visibly barred in PDF p7",
        "f_gA": "9804032 p7 Eq2.18 text: f132MeV andgA1.25; KSW9802075 p13 f132MeV",
        "current": "1012.0453 Eq12, physical LGT\u22124.513fm\u00b2;9907042 Eq17/18 sameRG invariant normalization",
        "pole": "2010 ERE small root remains distinct from1999 quoted bound pole; no replacement to fit cold normalization"
      },
      "gates": {
        "algebra_relative": 1e-11,
        "primary_amplitude_ERP_relative": 1e-09,
        "current_MP_relative": 1e-10,
        "current_anchor_fm2": 1e-12,
        "one_over_v_relative": 1e-06
      },
      "scope": "Fixed-order source-specific CP-even isosymmetric quark-mass continuation; primary-normalized ordinary inputs and explicit sensitivity scenarios. Not a matched finite-theta Hamiltonian or a statistical posterior.",
      "remaining": [
        "Different-author independent review",
        "Unknown convergence radius in pion mass;354MeV lattice input may lie outside common chiral regime",
        "No lattice/ordinary joint covariance or Gaussian inverse-a propagation across zero",
        "No finite-theta CP-odd NN/3N/isospin/current matching to cyclic axion action",
        "Weak current requires its own ordinary normalization and source coupling convention; not inferred from magnetic normalization",
        "Higher-order M,f,gA mass dependence and omitted ERE shape terms are not fitted"
      ],
      "whole_run_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "threads": 1
    }
  },
  "assumptions": {
    "W13-quarkmass-matching": [
      "Fixed-order source-specific CP-even isosymmetric quark-mass continuation; primary-normalized ordinary inputs and explicit sensitivity scenarios. Not a matched finite-theta Hamiltonian or a statistical posterior."
    ]
  },
  "plotted_values": {
    "path": "E88-quarkmass-current-matching-data.json",
    "sha256": "b422894188af44aa3b369b257abb490d17e7494adca455b9dcdf760356136e7b"
  },
  "caption": "The central curves use the source ordinary scattering lengths/effective ranges and its lattice scattering anchors at 353.7 MeV. The current is normalized to LGT=\u22124.513 fm\u00b2 at 138 MeV and uses the source small effective-range pole and single-nucleon coupling. Lines connect declared samples, without a confidence band. The lattice triplet interval crosses zero and no joint covariance is supplied. Unknown mass-expansion errors, full-amplitude poles and finite-angle nuclear matching remain separate. This figure neither inserts a cyclic-field angle nor predicts a lifetime.",
  "alt_text": "Matching fixes this leading source-order current continuation. It does not fix every higher-order, weak or finite-angle response.",
  "generator": "src/metastable/public_report.py",
  "generator_sha256": "9e263878b7237d781a41d94693004412279b5cfa808ccd6e335b7b07269910d4",
  "generator_dependencies_sha256": {
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    "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",
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    "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": "1f00af328af99761104eb6580b87696ae5f7b623c72feb73488425299d8ba49a",
    "png": "f30c22b79077e243331eb2548a99d7978009622f5a9e2169aa10d214dd010d09"
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}