{
  "schema": "classical-reconstruction-boyer-magnetic-population-audit/v1",
  "status": "TWO_BRANCH_COEFFICIENT_ONLY_POPULATION_DYNAMICS_UNDEFINED",
  "source": {
    "arxiv": "2606.08785",
    "path": "research/boyer-2026/magnetic/MagneticField.tex",
    "sha256": "411b892ca60f807b5e3d8788a7dd4a5a3097fa7b2de5556fa9debb53c30440ca"
  },
  "source_claims": {
    "orientation_random_without_B": true,
    "random_forces_reorient": true,
    "two_direction_claim": true,
    "resonant_configuration_time": true
  },
  "preserved_coefficient_status": "ZEEMAN_COEFFICIENT_MATCH_SELECTION_MECHANISM_PARTIAL",
  "preserved_total_separation_J_per_T": 1.85480201314e-23,
  "missing_population_dynamics": {
    "orientation_sde": "No explicit stochastic differential equation for the orbit-normal orientation under zero-point radiation plus B is derived.",
    "capture_rates": "No transition/capture rates into clockwise and counter-clockwise resonant branches are calculated.",
    "branch_weights": "No quantitative population weights are predicted from a generic initial orientation ensemble.",
    "beam_transport": "No apparatus-level Stern-Gerlach deflection distribution/width is propagated from the proposed orbital dynamics.",
    "finite_time_convergence": "No convergence-time distribution or survival probability is computed."
  },
  "verdict": "The source gives a physical orientation narrative and two resonant branch labels, but not an executable probability flow from a generic ensemble to two quantitative populations.",
  "promotion_rule": "Do not promote coefficient identity to Stern-Gerlach population reconstruction until branch capture, weights and beam distributions are generated from declared dynamics."
}