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MeanField/experiments/plateau_supplemental_cases_2026-09-17.json

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[
{
"id": "n1_J0p10_onset_between_bounds",
"arguments": [
"--index",
"1",
"--angular-momentum",
"0.1",
"--no-central",
"--max-newton",
"0",
"--probe-state",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/captures/n1_J0p10_capture/capture_2/physical_base.txt",
"--probe-direction",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/captures/n1_J0p10_capture/capture_2/normalized_direction.txt",
"--replay-candidate",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/supplemental_inputs/n1_J0p10_onset_between_bounds.txt",
"--surface-trace"
],
"notes": "Candidate at alpha=0.073032369116392076, strictly between exact sampled closure and pressure h boundaries. No new Newton/Krylov solve. Surface carrier and boundary-coefficient contributions are inspected without preparing extra trials."
},
{
"id": "n1_J0p10_late_surface_trace",
"arguments": [
"--index",
"1",
"--angular-momentum",
"0.1",
"--no-central",
"--max-newton",
"0",
"--probe-state",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/captures/n1_J0p10_capture/capture_11/physical_base.txt",
"--probe-direction",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/captures/n1_J0p10_capture/capture_11/normalized_direction.txt",
"--replay-candidate",
"/Users/tboudreaux/.codex/.chatgpt-projects/g-p-6a6b3f2194ec8191bebcd59075897f1d/diagnostics/pressure_shape_2026-09-17/captures/n1_J0p10_capture/capture_11/normalized_candidate.txt",
"--surface-trace"
],
"notes": "Exact late candidate replay plus surface carrier and limiting-point boundary-coefficient contributions. No new Newton/Krylov solve."
}
]