Manuscript II-B@1 · II-B-v1.tex · section · bfd2eb3c

Corrections table

Non-identifications and absence of geometric reconstruction › Corrections table · lines 2292–2373

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Potential identification	Correction in II-B
Potential identification	Correction in II-B
A finite fit is a global identity	The certificate concerns one three-label family. Global constant-coefficient membership remains undecided here.
Action and response equivalence coincide	Evaluation descends to action classes but can have a nontrivial kernel; the response quotient is a different quotient.
A clock record is already a contact label	The map $δ$ is additional declared data, with an explicit nonuniqueness counterexample.
One random readout gives several times of one event	Distinct exact event-time labels force a deterministic outcome. The stochastic construction uses history labels.
Enter destroys the time axis	It consumes finite quantum names. $M, g, T$ , and the causal relation remain present.
A clock basis change is a coordinate transformation	It generally changes the pointer observable and instrument, not the geometry.
Three labels need a three-dimensional qubit factor	The model uses two clock qubits and specifies all four outcomes; the fourth maps to the blind label.
Flat-space labels are conical scattering states	They remain auxiliary vertex labels interpreted in a declared local frame; no global scattering bridge is constructed.
A table probe measures the gravitational tree	The probe is controlled by the computed table. A field–apparatus matching theorem would be additional.
A contact fit is a mixture of channels	The valid operational identity uses centered instrument differences, not a non-normalized positive mixture.
The residual response is a stress tensor	No tensor-valued source map or variational matter action is supplied by the finite table instrument.
Weighting preserves the old quotient	A nonconstant density weight can turn a divergence into a nonzero response term; a switched problem needs a new contract.
A joint output formula delivers the clock record remotely	Remote use of $k$ requires a causal classical wire or local record-controlled processing before departure.
A scheduled cone is the exact influence region	It is an upper bound for complete channels, not necessarily a minimal region and not a postselection theorem.
Exact null transport is a microscopic Hamiltonian model	The proof is a finite endpoint-channel and causal-dependency certificate on a target-adapted chain.
Increasing the number of registers gives a field continuum limit	Each experiment is finite; no field algebra, convergence theorem, or detector scaling limit follows from the register count.