Recorded data and provenance for the associated calculation.
| experiment | two-channel-tau-test |
|---|---|
| created_utc | 2026-09-24T10:51:24.407745+00:00 |
| source_report | experiments/results/light-tau-branch-batch-20260924T102749_642908Z.json |
| identity | (1+x/b^4)/((1+x)(1+x/C^4))=A/(1+x)+B/(1+x/C^4) |
| conditional_action | sum_i [D_i(R) q_i^2/2 - J_i q_i + beta_i q_i k] + F0(k); D_i=1+(R/L_i)^4, J_i=beta_i=sqrt(gamma*w_i) |
| elimination | F_eff=F0-gamma*sum(w_i/D_i)/2+gamma*sum(w_i/D_i)*k-gamma*sum(w_i/D_i)*k^2/2 |
| scope | Exact positive-channel decomposition and necessary current-curvature and radial-stress tests. Channel stiffness powers, source amplitudes, direct current curvature, and stress-balancing field action are not derived from the master field; frequency stationary points alone are not complete energy stationary states. |
View complete data
{
"experiment": "two-channel-tau-test",
"created_utc": "2026-09-24T10:51:24.407745+00:00",
"source_report": "experiments/results/light-tau-branch-batch-20260924T102749_642908Z.json",
"identity": "(1+x/b^4)/((1+x)(1+x/C^4))=A/(1+x)+B/(1+x/C^4)",
"conditional_action": "sum_i [D_i(R) q_i^2/2 - J_i q_i + beta_i q_i k] + F0(k); D_i=1+(R/L_i)^4, J_i=beta_i=sqrt(gamma*w_i)",
"elimination": "F_eff=F0-gamma*sum(w_i/D_i)/2+gamma*sum(w_i/D_i)*k-gamma*sum(w_i/D_i)*k^2/2",
"scope": "Exact positive-channel decomposition and necessary current-curvature and radial-stress tests. Channel stiffness powers, source amplitudes, direct current curvature, and stress-balancing field action are not derived from the master field; frequency stationary points alone are not complete energy stationary states.",
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"sources": {
"experiments/two-channel-tau-test.py": "0801379e27c9d71cb38110217c53acf095e559929e85c4a669cdc74fbf3d32c2",
"experiments/results/light-tau-branch-batch-20260924T102749_642908Z.json": "f76f1eafaacb1214f4673ef0a491ddc921c50e713f26168fd986d32147301901"
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}