{
  "created_at": "2026-10-11T16:01:30.159622+00:00",
  "sources": {
    "experiments/spatial-source-saturation-checks.py": "56bd144519dbd066da32c8950845465d3b461fb12306f8d13476535cef542f2e",
    "experiments/spatial-band-curvature-checks.py": "1adbe50fbe865da9b237fe8d3dd424ee43dcb951fc8f8c01a31a3e4b9330f657"
  },
  "conditions": {
    "ground-plus-first-shell exact overlap deficit": 1,
    "equal ground polarization leaves a strict first-shell separation": 1,
    "zonal kernel is ambient monogenic scalar component": 18,
    "zonal kernel is ambient monogenic vector component": 18,
    "positive zonal shells have physical orthogonal norms": 6,
    "negative zonal shells have physical orthogonal norms": 6,
    "both Dirac signs are explicitly retained": 6,
    "kernel agrees with independently projected polynomial modes": 18,
    "all spatial polarization overlap singular values agree": 18,
    "two-point contact nonzero eigenvalues from independent frames": 18,
    "distinct points cannot saturate an excited cumulative band": 12,
    "ground-plus-first-shell overlap bounds every larger band": 12,
    "bright spatial field has canonical unit norm": 28,
    "complete cubic source Parseval identity across both Dirac signs": 28,
    "full source leakage fraction is admissible": 28,
    "smooth bright self-density strictly misses full contact saturation": 26,
    "independent quadrature refinement": 56,
    "two-point width correction agrees with existing spatial quantum metric": 14
  },
  "max_relative_errors": {
    "positive zonal shells have physical orthogonal norms": 3.552713678800501e-15,
    "negative zonal shells have physical orthogonal norms": 3.907985046680551e-15,
    "both Dirac signs are explicitly retained": 8.526512829121202e-14,
    "kernel agrees with independently projected polynomial modes": 5.169511351229718e-16,
    "all spatial polarization overlap singular values agree": 4.440892098500626e-16,
    "two-point contact nonzero eigenvalues from independent frames": 1.4509034919170382e-15,
    "bright spatial field has canonical unit norm": 1.2361356382939448e-10,
    "complete cubic source Parseval identity across both Dirac signs": 3.46965969635089e-10,
    "independent quadrature refinement": 3.373000610241917e-10,
    "two-point width correction agrees with existing spatial quantum metric": 8.815436955550327e-05
  },
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    {
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      "sphere_radius": "R; all angles dimensionless, physical separation R times angle",
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  ],
  "family_comparisons": [
    {
      "depth": 2,
      "low": "W",
      "high": "Higgs",
      "within_sector_ratio_available": true,
      "quartic_ratio_relative_to_simplex": -7.33772518335396e-05
    },
    {
      "depth": 3,
      "low": "down",
      "high": "strange",
      "within_sector_ratio_available": true,
      "quartic_ratio_relative_to_simplex": -0.6523750000000009
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    {
      "depth": 4,
      "low": "up",
      "high": "top",
      "within_sector_ratio_available": true,
      "quartic_ratio_relative_to_simplex": -0.26076838839790073
    },
    {
      "depth": 5,
      "low": "nu1",
      "high": "nu3",
      "within_sector_ratio_available": true,
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    {
      "depth": 6,
      "low": "electron",
      "high": "muon",
      "within_sector_ratio_available": true,
      "quartic_ratio_relative_to_simplex": -0.04524596409199011
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    {
      "depth": 10,
      "low": "tau",
      "high": "tau",
      "within_sector_ratio_available": false,
      "quartic_ratio_relative_to_simplex": 0.0
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  ],
  "scope": "Actual positive spherical Dirac bands; density self-contact is a classical comparison, not electron position probability or a Lorentz-scalar master derivation."
}
