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  "strict_comparison": {
    "late_total_energy_ratio_excited_over_cone": 1.922943411767418,
    "late_theta_mean_separation_deg": 91.91011152887322,
    "late_theta_span_ratio_excited_over_cone": 1078.272893655554,
    "stationary_120_200_theta_slope_cone_deg_s": -0.00011674405540057217,
    "stationary_120_200_theta_slope_excited_deg_s": -0.00010858751126836493,
    "stationary_120_200_power_closure_cone_W": 7.615524739930529e-10,
    "stationary_120_200_power_closure_excited_W": -1.7627416329233213e-08
  },
  "scientific_interpretation": "A 0.396% change in one transverse rate kick sends the same damped, psidd=0 system to either the regular A/P cone or a persistent large-angle, average-A/P attractor with about 1.92 times the late total energy. This directly visualizes multistability and sensitive basin selection, rather than a change in forcing or sustained external spin injection.",
  "interpretation_caveat": "This is a local bracket on one precisely defined one-dimensional kick slice. The exploratory slice alternates among cone, AP-large-angle, and parallel high-speed attractors; it is not a globally monotone energy threshold. Nearby outcomes may be phase-sensitive or have a fractal/riddled basin boundary."
}