Manuscript I-B@1 · I-B-v1.tex · section · 5357688f
Corrections to the proposed architecture
Scope, provenance, and necessary corrections › Corrections to the proposed architecture · lines 139–192
{}1.16
| Potential identification | Correction used here |
|---|---|
| The product defect is a worldline | After adjoining , the full defect has coordinates and is a worldsheet. Fixing gives one worldline. |
| Clock outcome equals the time of one fixed event | For distinct calibrated labels, exact event-time agreement forces a deterministic clock outcome. Nontrivial history conditioning instead refers to different labelled events. |
| Changing the clock basis changes time coordinates | A general basis change changes the observable. Coordinate relabelling is a much more restrictive operation. |
| Scheduled past lies in metric future | An ancestor of an output lies in its metric past; equivalently, the output lies in the ancestor's metric future. |
| A lapse jet supplies a cosmological metric | A spatial metric and shift are also required. The exact background and the formal perturbation parameter remain distinct. |
| Spatially constant metric components imply flatness | Spacetime-constant components imply flatness. Time-dependent, spatially homogeneous metrics need not be flat. |
| Enter consumes the geometric time axis | Enter consumes a finite clock encoding. The classical manifold, coordinate, and future cone remain present. |
| Exact null transport follows on a fixed lattice | Our exact result uses a declared target-adapted chain. It is not an exact-attainment claim for a previously fixed lattice. |
These corrections restrict the theorem to a coherent, nonempty model; they are not additional emergence assumptions.
boundaries.
Throughout this paper, “XV-B is not opened” means that the inherited
downstream admission exit is not activated by this construction.
It does not deny the existence of a technical manuscript bearing that
identifier. XVI-N is not discharged; O.1 remains
NOT_CLOSED for the purposes of this release; no inherited
quantum coefficient is admitted; and no compilation, numerical
execution, physical implementation, or machine verification is asserted.
The narrower internal-amplitude advance in XIV-I is not withdrawn, but
it is not the full joint characteristic map absent at I3/J2
CheungXIVIJ,CheungStops.