{
  "visual_id": "V22",
  "title": "Validate the continuum method before extending the nuclear claim",
  "classification": "new_simulation",
  "status": "validated_within_scope",
  "experiment_ids": [
    "E18-surrogate"
  ],
  "run_ids": [
    "20260927T155225274142Z-E18-surrogate"
  ],
  "model_ids": [
    "Minnesota-NN-1S0-continuum-method-benchmark"
  ],
  "claim_ids": [
    "C02"
  ],
  "input_files": [
    {
      "path": "runs/20260927T155225274142Z-E18-surrogate/heldout-validation.csv",
      "sha256": "1181890a72119becbaf0e863423fd3cfe66f53488c4e52caab898fa23ef09754"
    },
    {
      "path": "runs/20260927T155225274142Z-E18-surrogate/continuum-poles.csv",
      "sha256": "dd3ad7cfd4a34a6a1b4491ef53d14ff968eaa9058bbab1287f27d14a6886b1d4"
    },
    {
      "path": "runs/20260927T155225274142Z-E18-surrogate/results.json",
      "sha256": "847273bb1df85c10fcb91860214e3fbcf7e1aa2ceaa255ee0c28e13c04d80ea0"
    }
  ],
  "plotted_values": {
    "path": "V22-data.json",
    "sha256": "7cc752500b4a0302f844780628c3ddfed83263a2ff9dd139642be8e295da7f60"
  },
  "source_ids": [
    "E18-scattering-EC"
  ],
  "units": "Explicit axis labels and unit-bearing source columns; normalized quantities are defined in the caption.",
  "transformations": [
    "Saved numerical outputs only; physical interpolation, selection and normalization are described by the generator and caption."
  ],
  "uncertainty_type": "Numerical controls, published errors, and declared model/nuisance scenarios remain distinct; no biological threshold.",
  "validity_limits": [
    "A component calculation does not establish an observationally allowed complete history."
  ],
  "caption": "Minnesota NN singlet-S benchmark, with 256 reserved direct scattering calculations. Two actively selected basis states substantially reduce the error. Pole continuation distinguishes bound and virtual sheets through outgoing boundary conditions; these are not finite-box eigenvalues. The benchmark lacks a field-to-Hamiltonian map and does not compute alpha\u2013alpha or Hoyle regimes. Basis disagreement is a heuristic uncertainty indicator.",
  "alt_text": "The error distribution shifts strongly downward with two extra basis states. A separate continuum pole crosses zero momentum as attraction changes, moving between virtual and bound sheets.",
  "render_command": "uv run --offline --frozen python run.py full render",
  "generator_sha256": "fa75ece843491c857348bd38d22cfeeae732a8bb9caa8c1921182f783c2cc6a4",
  "extension_generator_sha256": "4cef7f7e2f45594db1c8eb981fb50ae736aad43e6708d1f12826d99b57a40cce",
  "output_sha256": {
    "svg": "9858269085fdc970a39ad8cfa250b27286a62ee491ddc997efb05fdad598f873",
    "png": "bb43eefacfac71a2125acfbe568496c3b53a2cb297f6399604ef5d311328a15f"
  }
}