Recorded data and provenance for the associated calculation.
| experiment_key | convex-count-quadratic-envelope |
|---|---|
| created_utc | 2026-10-12T08:20:24.787811+00:00 |
| evaluations | 257 |
View complete data
{
"experiment_key": "convex-count-quadratic-envelope",
"created_utc": "2026-10-12T08:20:24.787811+00:00",
"sources": {
"experiments/convex-count-envelope.py": "6650f29a11b56cf16794e50c809fb92cf6a25829453698095912b357307ad8d0",
"experiments/forward-count-action.py": "5f1dd9a03cf8e6b07a56d507791fed8ff859f10abf22bb755c60c3bd1ed6d909",
"experiments/inverse-current-radial.py": "52d9f1c981635192e06d96b11f0b1e4e5e2d1bf3d5ed420b59411fd45ef7be80",
"experiments/excited-shell-orientation-current.py": "508484d445dbb86da9f88a31642268b5a1dba8264588e6f48ebb6cc00cf9c264"
},
"evaluations": 257,
"conditions": {
"exact ground count derivatives start the all-shell strict-convexity proof at each maintained depth above two": 5,
"every maintained assignment belongs to the common strictly convex count chart": 14,
"the maximum over every admissible geometric tangent uniquely selects the maintained branch": 14,
"the selected envelope tangent preserves the complete stationary interaction value": 14,
"the finite geometric envelope has a strict open winner gap at each maintained state": 14,
"all competing tangent inequalities give a nonempty exact local scalar-ratio winner interval": 14,
"finite ratio displacements remain inside the exact affine winner chart": 28,
"independent variation of the actual envelope gives the complete preferred-time source": 14,
"every retained complete spatial block has an exactly Hermitian generator": 70,
"independent massive spatial block diagonalization agrees with the full linear spectrum": 70
},
"maximum_errors": {
"independent massive spatial block diagonalization agrees with the full linear spectrum": 2.3044629267895138e-16
},
"cases": [
{
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},
{
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{
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{
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{
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}
],
"limits": [
"the envelope is a specified effective constitutive action derived from geometric count tangents",
"the preferred-time realization has exact local quadratic dynamics and its existing Sobolev persistence argument applies",
"proper-current and responding-clock choices retain their current response and require separate persistence analysis",
"the strict convexity chart excludes the low depth-two tangents; every maintained massive depth-two assignment remains included",
"the global evolution at tied charts is unassigned; small-persistence neighborhoods stay inside their unique winner chart",
"no new sector-depth preference, localized particle, complete boost inertia or physical contact-source origin follows"
]
}