Manuscript III-B@1 · III-B-v1.tex · section · d2c98f62
Corrections to the proposed transfer
Release, corrections, and remaining emergence obligations › Corrections to the proposed transfer · lines 2405–2475
{}1.12
| Potential overstatement | Corrected statement |
|---|---|
| Potential overstatement | Corrected statement |
| Local flatness gives a global conical Cauchy theorem | The punctured product has noncompact causal diamonds. The positive results use a supported regular laboratory. |
| The chart Newton kernel is the conical inverse | It is an auxiliary prescription on declared compact sources, not a global cone boundary condition. |
| The product and tangency obstructions are equivalent | They test different transformations on different equation spaces. |
| Off-shell cancellation proves descent on an unchanged shell | The transformation must first preserve that shell and be constant on its declared equivalence classes. |
| Retarded gauges are residual wave gauges | A past-trivial homogeneous wave is zero. Nonzero residual waves generally have nonzero Cauchy data. |
| Zero scalar data can be fixed under every residual gauge | The homogeneous subtraction term must be retained. |
| The model is full Einstein–scalar linearization | Its metric equation remains vacuum linearized gravity. |
| An exact compact repair exhausts all compact observables | The displayed exact family vanishes, but the explicit compact coupled pair is nonzero. |
| The residual is the descended continuum field | The theorem constructs a finite evaluation encoding only. |
| A random clock code is the time of one fixed event | Exact event-time calibration with distinct labels is deterministic. The multi-outcome model uses history calibration. |
| Enter consumes the fourth geometric dimension | It consumes a finite clock factor. The supplied time coordinate and spacetime remain. |
| A clock basis change moves a geometric point | It changes the reading instrument, not the coordinates. |
| A remote controlled probe may use an available joint-state label | It requires an explicit causal classical record wire. |
| An exact SWAP chain is a microscopic propagation model | The proof certifies complete endpoint channels and causal tick-boundary dependencies, not a within-tick Hamiltonian. |
| Classical lapse formulas are clock-record identities | Their backgrounds, rods, inverse maps, and quantum obligations remain distinct. |