{ "compound_identity": { "h": [ 0.02, 0.01, 0.005, 0.0025 ], "errors": [ 0.006243278576986646, 0.0015769036915523503, 0.00039623812080580946, 9.93015408996616e-05 ], "loglog_slope_expected_2": 1.9915686739147795 }, "predictions": { "P1_compound_identity_error_is_O_h2": { "observed_slope": 1.9915686739147795, "expected": 2.0 }, "P2_shortest_path_min_entry_scales_alpha3": { "observed_log_slope": 3.000328903279753, "expected": 3.0, "note": "For the bidirectional 6-cycle, the worst off-diagonal entries require three edges; the leading path term is (alpha*t)^3/3!." }, "P3_stronger_uniform_coupling_improves_projective_contraction": { "alphas": [ 0.05, 0.1, 0.2, 0.4, 0.8 ], "q_bounds": [ 0.9999573853840754, 0.9996603554483036, 0.9973244232616174, 0.9799237269249854, 0.8752531714166867 ], "q_at_alpha_0.05": 0.9999573853840754, "q_at_alpha_0.8": 0.8752531714166867 } }, "rows": [ { "alpha": 0.05, "min_P": 9.58951945520055e-06, "q_birkhoff_bound": 0.9999573853840754, "max_sampled_ratio": 0.9904368818740336, "path_minentry_at_t0.08": 1.9693227495635823e-08, "path_prediction_alpha3_t3_over_6": 1.0666666666666668e-08, "repeated_window_ratios": [ 0.8944291654498862, 0.8975874342752008, 0.9006513184643506, 0.9035844819373794, 0.9063929759773381 ] }, { "alpha": 0.1, "min_P": 7.680825185932804e-05, "q_birkhoff_bound": 0.9996603554483036, "max_sampled_ratio": 0.944372279716586, "path_minentry_at_t0.08": 1.5754771052248844e-07, "path_prediction_alpha3_t3_over_6": 8.533333333333334e-08, "repeated_window_ratios": [ 0.6886449585037385, 0.797978357156317, 0.8769247795188834, 0.8890655437792796, 0.8965605690316094 ] }, { "alpha": 0.2, "min_P": 0.0006174201745380509, "q_birkhoff_bound": 0.9973244232616174, "max_sampled_ratio": 0.8915108767982187, "path_minentry_at_t0.08": 1.260442183468729e-06, "path_prediction_alpha3_t3_over_6": 6.826666666666667e-07, "repeated_window_ratios": [ 0.6805728376856377, 0.8257056192834158, 0.8964865403937533, 0.8791229156627779, 0.8671507262264395 ] }, { "alpha": 0.4, "min_P": 0.0050348059863144735, "q_birkhoff_bound": 0.9799237269249854, "max_sampled_ratio": 0.8004953597589071, "path_minentry_at_t0.08": 1.0085473630854028e-05, "path_prediction_alpha3_t3_over_6": 5.461333333333334e-06, "repeated_window_ratios": [ 0.7738700322543988, 0.6876036475171393, 0.6977015394129747, 0.7319873434335363, 0.7234811407745301 ] }, { "alpha": 0.8, "min_P": 0.043452021571022015, "q_birkhoff_bound": 0.8752531714166867, "max_sampled_ratio": 0.6798605371956746, "path_minentry_at_t0.08": 8.074577006188443e-05, "path_prediction_alpha3_t3_over_6": 4.369066666666667e-05, "repeated_window_ratios": [ 0.19163812173118022, 0.4905163641804326, 0.5379220870005692, 0.5286077901331985, 0.5274295384889923 ] } ], "baseline_signed_generator": { "min_transition_entry": -0.1462517985915507, "valid_positive_output_sample_ratio_max": 2.491604424899665, "metzler_violation": 0.8 }, "interpretation": "Positive irreducible compound dynamics produced strictly positive finite-window transitions and geometric Hilbert contraction. The signed baseline has a negative transition entry, so the positive-cone theorem is unavailable." }