Recorded data and provenance for the associated calculation.
| version | 20261022-scoped-correction |
|---|---|
| scope | Supplied projected-force law, fixed nuclear geometry and specified preparations; no directional-force derivation, nuclear alignment dynamics or polarization selection. |
| status | pass |
View complete data
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"parameters": {
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"dt": 0.004,
"duration": 400.0,
"seed": 1
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"counterexamples": {
"roundness_fourth_moments_exact": [
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"scope": "Supplied projected-force law, fixed nuclear geometry and specified preparations; no directional-force derivation, nuclear alignment dynamics or polarization selection.",
"sources": {
"experiments/nuclear_depth_orbit_dimension_checks.py": "b8b2b19e78b6031c8cd420068e8ef6012ad6c90c30d5717c9f120a2df04d1e55"
},
"checks": [
{
"name": "C1 stated single-center preparations keep unit radius",
"ok": true
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{
"name": "C2 stated L=2,3,4 and long irrational run have diagonal second moments near 1/4",
"ok": true
},
{
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{
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{
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"ok": true
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{
"name": "C6 aligned restricted frequencies match doubled single-center law",
"ok": true
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{
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"ok": true
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{
"name": "C8 seeded finite trajectories respect their conserved-energy radius bounds",
"ok": true
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{
"name": "C9 spread is preparation-dependent: shared plane sees 1; private difference sees 1/2 each",
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{
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{
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{
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"ok": true
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{
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},
{
"name": "C14 energy-coordinate propagator agrees with two half steps",
"ok": true
},
{
"name": "C15 aligned propagation agrees with analytical gyro solution",
"ok": true
},
{
"name": "C16 finite runs conserve the complete quadratic energy",
"ok": true
},
{
"name": "C17 sampled stiffness matches analytic 2k,2k,2k,k(1-cos phi),k(1+cos phi)",
"ok": true
},
{
"name": "C18 independent uniform axes in R7 have E|cos|=5/16 and E cos^2=1/7",
"ok": true
}
],
"status": "pass"
}