{
  "visual_id": "E90-quarkmass-inverse-poles",
  "title": "Positive and discarded roots retain the source prescription and cut",
  "classification": "scoped_public_input_calculation",
  "run_ids": [
    "20261003T204902133504Z-W13-quarkmass-bracketed-survey"
  ],
  "claim_ids": [
    "C02",
    "C04",
    "C10"
  ],
  "input_files": [
    {
      "path": "runs/20261003T204902133504Z-W13-quarkmass-bracketed-survey/pole-prescriptions.json",
      "sha256": "8a3e07b48ef155957558e05dd7f487ff91a00df7799dc2d7d3de142895e032af"
    },
    {
      "path": "runs/20261003T204902133504Z-W13-quarkmass-bracketed-survey/continuous-thresholds.json",
      "sha256": "780a41ee05ecc9d3d89a8edcb258716dcc88efed770d315762b5c0e241528ae6"
    },
    {
      "path": "runs/20261003T204902133504Z-W13-quarkmass-bracketed-survey/results.json",
      "sha256": "931a36b2c0707ae0c086f9941877bbec926b10160a643612a02b0a68dd474ee2"
    }
  ],
  "configurations": {
    "W13-quarkmass-bracketed-survey": {
      "parents": {
        "20261003T192357984026Z-W13-quarkmass-matching": "91473a527b71b9f9df7bcba8db7969f77a4285a54783582851136294a897b72e",
        "20261003T194142235520Z-W13-quarkmass-matching-review": "a453df3c8e9e11f5f9b5d29afd7137d02223b8ecf9a0a95bc4a346df08db5635"
      },
      "current_x": [
        0,
        1e-30,
        1e-20,
        1e-16,
        1e-12,
        1e-08,
        1e-05,
        0.001,
        0.01,
        0.125,
        0.25,
        0.49,
        1
      ],
      "current_y": [
        -2,
        -0.060298,
        0,
        0.1,
        0.75,
        2
      ],
      "mu_MeV": [
        100,
        138,
        200
      ],
      "lambda_MeV": [
        500,
        750,
        1000
      ],
      "amplitude_m_MeV": [
        106,
        125,
        138,
        142,
        165,
        353.7
      ],
      "imaginary_k_over_m": [
        0,
        1e-08,
        0.1,
        0.25,
        0.49
      ],
      "survey_m_MeV": [
        100,
        106,
        110,
        120,
        125,
        130,
        135,
        138,
        140,
        141,
        142,
        143,
        144,
        145,
        150,
        160,
        165,
        170,
        180,
        200,
        300,
        353.7
      ],
      "root_grid_intervals": [
        256,
        512,
        1024
      ],
      "gates": {
        "algebra_relative": 1e-11,
        "ERP_relative": 1e-09,
        "current_relative": 1e-10,
        "current_anchor_fm2": 1e-12,
        "literal_MP_scaled": 1e-60,
        "derivative_relative": 1e-08,
        "root_residual_MeV_scaled": 1e-10,
        "root_MP_absolute_MeV": 1e-08
      },
      "precision_digits": 120,
      "current_series_terms": 32,
      "current_series_domain": [
        0,
        0.125
      ],
      "cut_fraction": 1e-08,
      "cut_fractions": [
        0.01,
        0.0001,
        1e-08
      ],
      "whole_seconds": 600,
      "maximum_RSS_bytes": 3221225472,
      "threads": 1,
      "scope": "Source-specific CP-even isosymmetric NLO algebra and explicit pole prescriptions. Eq12 always uses its ERE pole. Raw truncated amplitude, order-expanded-inverse resummation and strict first-order shift remain distinct. No forced source-window reproduction or finite-theta matching.",
      "remaining": [
        "Different-author benchmark review before scalar pole survey",
        "No exact finite-order moving pole of the raw truncated amplitude",
        "Inverse-amplitude pole prescription resums uncontrolled higher orders near a pole; source does not spell out a separate resummation convention",
        "Finite root scans are not a global analytic root-count proof",
        "Pion-mass convergence at354MeV, missing joint covariance and higher-order single-hadron dependence remain",
        "No finite-theta CP-odd NN/3N/isospin/current matching or field constraint"
      ],
      "benchmark": "20261003T203603426627Z-W13-quarkmass-thresholds-benchmark",
      "benchmark_review": "20261003T204151468377Z-W13-quarkmass-thresholds-review",
      "root_method": "MP80 bisection inside original stationary partition; select the smallest binary64 residual within three ULPs of the MP root; no secant extrapolation",
      "preserved_failed_survey": "20261003T204324948066Z-W13-quarkmass-thresholds-survey",
      "preserved_bracketed_failure": "20261003T204639692509Z-W13-quarkmass-bracketed-survey",
      "continuous_threshold_scope": "D(0,m)=0 and interior D=Dk=0 numerical controls in declared100..353.7MeV survey interval; no global root-count theorem"
    }
  },
  "assumptions": {
    "W13-quarkmass-bracketed-survey": [
      "Source-specific CP-even isosymmetric NLO algebra and explicit pole prescriptions. Eq12 always uses its ERE pole. Raw truncated amplitude, order-expanded-inverse resummation and strict first-order shift remain distinct. No forced source-window reproduction or finite-theta matching.",
      "All original numerical gates retained including on discarded nonphysical roots; failures recorded after complete finite survey."
    ]
  },
  "plotted_values": {
    "path": "E90-quarkmass-inverse-poles-data.json",
    "sha256": "2b66be5c897cef5e18163f1dc750e82bb60750bcad4a7830f9ac0f23d94767b9"
  },
  "caption": "The nominal triplet case uses epsilon=1 and auxiliary mass 750 MeV. Markers are declared finite mass samples, and lines only connect them. Squares mark separately solved zero-binding and coalescence thresholds at 105.19908 and 142.02597 MeV. All negative-residue roots are retained in the data and excluded from the bound-state count. This inverse-NLO resummation differs from strict first-order and effective-range pole prescriptions. Nested finite grids and multiprecision brackets do not prove global completeness or quantify omitted source orders.",
  "alt_text": "The bounded source calculation reproduces a finite positive-residue interval under an explicit prescription; it does not establish a unique physical mass window or finite-angle nuclear response.",
  "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": "1887c19d7e00a4109063285bdd616ec61bd1d38b8c72efd0e1fd7a786689934a",
    "png": "c575fef5eccdcec8e7098be4443bfbefbcd02d409fbd1c944e4cd63419390137"
  }
}