Manuscript Oai365-A@1 · Oai365-A.tex · section · a3840e3d
Connection ledger
Hypothesis and connection ledgers › Connection ledger · lines 1706–1769
| Connection | Established mathematical interface | Non-transfer boundary |
|---|---|---|
| Connection | Established mathematical interface | Non-transfer boundary |
| XXII-A/B/C/F | Event-order specification, faithful generation, covariance audit; an explicit enriched pilot is supplied here. | The pilot is not a general quantum-to-spacetime theorem. The original finite futures remain finite. |
| 365-01/02 | Same-patch DN energy is the named inverse target. Gauge and diffeomorphism invariance are proved here. | The catalogue supplies neither the observation law nor a verified inverse theorem for use here. The target metric is Riemannian. |
| En08-A and Ito–Lourenço | Conditional classification after a proper homogeneous strictly convex cone is constructed. | Classification does not create event displacements, access, or physical units. |
| XXII-D and En08-B | Complete-channel and endpoint approximation certificates. | Geometry does not provide quantum wires, arrival topology, directional availability, or bounded-cost control. |
| En10-A/B | Calibrated source-weight inference and the need for a physical acceptance package. | A source weight is not a boundary energy form. The physical identification bridge is not automatic. |
| En09-A | Complete clock-conditioned extraction with separate covariance requirements. | A clock record is not a derived metric or autonomous time law. |
| VII-J and En05-A | Scheduled ancestry bounds actual influence for declared channel networks; geometric embedding is additional. | Scheduled reachability, influence, and supplied causal relation are not identified. |
| 365-03 | A documentary negative control for coefficient regularity. | No transfer from rough scalar conductivity to smooth Lorentz geometry or conventional quantum potentials is made. |
| XXII-E | Metric-jet and independent source interfaces. | Conformal cones, static inverse uniqueness, and conservation do not imply Einstein dynamics. |
The additional catalogue families numbered
095, 211, 212, 215, 243, 265, 280, 282, 283, and 290 remain
documentary comparison pointers from the supplied plan.
No theorem from any of them is used in this manuscript.
No result is inferred from the filenames
Conductivity.lean or 271-04, and no formal execution
is asserted.