{
  "timestamp": "2026-09-12T13:29:34.545000+00:00",
  "scope": "Reciprocal retained/normal field evolution and its adiabatic limit.\n\nAll spinor components are evolved. The single momentum and two coefficient\ndirections define a finite mode control, not a spatially localized particle.\nThe orthogonal occupied fast columns are explicit spectator modes of the\nsame conditional field decomposition, with their full canonical norm.\n",
  "parameters": {
    "separations": [
      32.0,
      64.0
    ],
    "duration": 20.0,
    "rtol": 2e-12,
    "atol": 2e-14
  },
  "common_parameters": {
    "real_depth": 6,
    "active_coefficient_directions": 2,
    "spinor_components": 8,
    "momentum": 0.35,
    "base_epsilon": 0.8,
    "base_coupling": 0.6,
    "fast_occupied_columns": 2
  },
  "cases": [
    {
      "separation": 32.0,
      "epsilon": 25.6,
      "coupling": 19.2,
      "occupation_per_fast_mode": 0.03125,
      "slow_norm": 1.0,
      "fast_norm": 0.0625,
      "maximum_slow_norm_drift": 1.3322676295501878e-15,
      "maximum_fast_norm_drift": 1.7951889974554547e-12,
      "maximum_gram_error": 1.2730192994280534e-12,
      "maximum_energy_drift": 4.6705750378350785e-11,
      "maximum_adiabatic_slow_error": 0.0003806552132169424,
      "final_adiabatic_slow_error": 0.0003806552132169424,
      "maximum_projector_error": 0.006528419024577824,
      "maximum_negative_fraction": 1.065506374068844e-05,
      "rhs_evaluations": 30797
    },
    {
      "separation": 64.0,
      "epsilon": 51.2,
      "coupling": 38.4,
      "occupation_per_fast_mode": 0.015625,
      "slow_norm": 1.0,
      "fast_norm": 0.03125,
      "maximum_slow_norm_drift": 1.7763568394002505e-15,
      "maximum_fast_norm_drift": 1.6283155379603897e-12,
      "maximum_gram_error": 1.1534319912122598e-12,
      "maximum_energy_drift": 8.474376755884805e-11,
      "maximum_adiabatic_slow_error": 9.359916613568095e-05,
      "final_adiabatic_slow_error": 8.882387442764643e-05,
      "maximum_projector_error": 0.0032605348200135864,
      "maximum_negative_fraction": 2.6577718280620325e-06,
      "rhs_evaluations": 60041
    }
  ],
  "raw_data": "experiments/results/dirac-current-reciprocal-flow-20260912T132934_545000Z.npz",
  "source_sha256": {
    "experiments/dirac_current_reciprocal_flow.py": "3baa36767956dbdeeca7e519ced6b71c36a8b5741810aeb009411da20f697f47",
    "experiments/dirac_current_reduction.py": "e9a907c42f83662ade7a9ce8baba55a3c0e880c99ac5480b578beb6e381738e9",
    "experiments/spatial_dirac_mode_checks.py": "116a9f6d0f3cbcf9ee2fbe7a762e09c113194a07591191dd6663f5bcb8364552"
  },
  "dataset": {
    "path": "experiments/results/dirac-current-reciprocal-flow-20260912T132934_545000Z.npz",
    "sha256": "4364b269e4952c33110d6fd7676fd93481ab8c3edb47bbd474e084de54372577"
  },
  "publication_provenance": {
    "original_report_sha256": "4b614f9938a97bc4863c34ac822b33edcb2a4d962cdf760c51fd30ada7421a43",
    "changes": "Local file locations are replaced with portable artifact references. Calculation values and source-code fingerprints are unchanged."
  }
}