Documentary comparisons and the sibling contract

All entries below are version-qualified comparisons. They are not premises of the spectral, contact, Ward, CTP, or residual proofs. A reported source theorem retains its own hypotheses and is not independently verified by this manuscript.

{@{}P{.47}P{.47}@{}} Comparison used & Conclusion not imported
Comparison used & Conclusion not imported

XVIII-A, v2 SiblingXVIIIA. The sibling contract separates witness recovery, kernel admission, normalization, and ultraviolet matching. & Its conditional assembly and matching theorems are not premises of this spectral calculation. This benchmark does not discharge the original relational target's gates.

I, v2 CheungI. Destructive-readout semantics distinguish a classical record from a surviving measured quantum name. & No measurement uniqueness or field instrument is imported from a positive vacuum pairing.

VII-E, v1 CheungVIIE. Observation boundaries retain complete records, spectators, residual instruments, and continuations. & The spectral detector is not such a boundary or a scheduled apparatus realization.

Hawk04-A, v1 CheungHawk04A. Complete preservation and recovery through one declared output are different tasks. & No complete-access inverse or radiation decoder is constructed by the stress response.

Hawk04-B, v2 CheungHawk04B. Classical readout is distinguished from quantum return. & The CTP kernels are neither a classical-output channel nor a quantum-return register.

XVII-A, v1 CheungXVIIA. The separately identified finite-matrix bounded-effect reconstruction remains a different benchmark. & No reconstruction map, boundary CFT, entanglement wedge, Page curve, or metric identification is transferred.

VII-H, v1 CheungVIIH. A free massless Wick-square response has its own one-parameter contact freedom and invariant detector. & Its $\hslash {\delta }_0$ contact and insertion are not this massive two-stress classification. No massless connecting theorem is supplied.

XVI-B, v1 CheungXVIB. Late source agreement is not response agreement; source, response, and class kernel remain separate. & The preparation product rule does not identify ${\sigma }_{\epsilon }h$ with the companion cubic source.

XII-C, v1 CheungXIIC. The cubic-only density freeze retains actual preparation derivatives. & No cubic density, source array, or coupled Einstein jet is imported into the linear external-source model.

X-A-conv, v1 CheungXAconv. One fixed switched convolution has its own first-order covariance defect. & No successful ultraviolet-regulator identification, universal convolution no-go, or shared source law.