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  "numerical_controls": {
    "relative_Q2_change_256_to_384": 6.016019451182686e-05,
    "relative_Q2_change_192_to_384": 0.00017279493871491525,
    "relative_green_flux_difference_at_384": 2.3315204092488884e-05,
    "maximum_relative_source_method_difference_from_flux": 0.0037438179691551277,
    "maximum_relative_source_quadrature_change": 0.0003929472838479775
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  "cassini": {
    "central_s_minus2": 1.6e-27,
    "one_sigma_s_minus2": 1.8e-27,
    "source": "https://arxiv.org/abs/2602.17884v2"
  },
  "comparison": {
    "selected_local_Q2": 2.3581489185629482e-26,
    "observational_upper_two_sigma": 5.1999999999999996e-27,
    "fractional_reduction_to_upper_two_sigma": 0.7794880569642366,
    "interpretation": "Comparison with the quoted observational band; no combined likelihood or complete theoretical uncertainty"
  },
  "source_sha256": "61e26c5144694ff333bc6616dab72ce8ebd9a76515d66f9202481e2a0bbd3c49",
  "input_sha256": {
    "rust/src/main.rs": "2dab4dfbb87656a33e64a69855a811e69ed344ad9c053c47387b81e911057a3b",
    "outputs/dark_summary.json": "63b02654dc975a055537e5e695e7f3f814845e361fb6f89f677d9bd439f0a9c4",
    "outputs/dark_solar_summary.json": "4733f713630a0e65bc18a5dc11c32bf15cbbb90fbc1021c1741cdb5cfbbe0d5a",
    "outputs/dark_lattice_bands.csv": "77793f80fb338a66b95254601d7aa5dbc2948eb9f25b0a1bf8a05cc02a5e60aa",
    "outputs/dark_lattice_controls.csv": "f81628727f2df1f290f766cd83c8318af28c0a35654f54ed3392d1c660fad539",
    "outputs/dark_solar_table_w450.csv": "c86de970b610bdabe60a21a3c07270f78510b7eb07f489a74abfac5601f399c4"
  },
  "dependencies_sha256": {
    "dark_solar_report.py": "a91222576f43c8299d47db1d04370a2cfd6657153e210a677d76c7e9e3a35821",
    "dark_solar_green_check.py": "2208372c0b72f73670ede656cb683b2c8690fafab2f57b9a0a22fd45c2969ca0",
    "dark_band_report.py": "22d648a83dc43aac735b2879af73cb4e1c83b2e2815711d018b21670549571dc"
  },
  "limitations": [
    "The new gravity solutions remain local AQUAL, not the nonlocal eight-band field equation",
    "Large mu floors are counterfactual diagnostics and alter the microscopic local law",
    "Poisson-source budgets depend on interpolated second derivatives and finite-domain boundaries",
    "The source budget is not a bound on the backreaction from a nonlocal modification",
    "The very small saddle region is not resolved to microscopic length scales",
    "The separate Cassini relativistic light-propagation/PPN test has no LQ8 metric prediction"
  ]
}