Documentary comparisons and component ledger

The outline describes III and VI as classical quotient or Einstein–scalar jet constructions, IV Model 3 as a metric-valued prescribed-inverse comparison, and Em02-E as a classical relational-lapse comparison on an installed background. Those are documentary descriptions of distinct models. No unsupplied theorem or identification is imported CheungClassicalComparisons,CheungXIXE.

In particular, a classical Einstein–scalar jet theorem can already contain the gravitational equations among its premises. A prescribed inverse on Minkowski space already fixes its background and comparison operator. Neither is an operational derivation from ${\mathcal{P}}_{3q}$.

The supplied source and response records in XVI-B and XVI-D likewise do not supply the present source or metric extraction maps. Their smooth source-response domains are not, by notation alone, the event carrier or comparison domain of this programme CheungXVIBD.

{}1.13 {@{}p{.25}p{.67}@{}} Component & Role and boundary
Component & Role and boundary

XXII-A & Faithful generation, selection target, and the constant conformal ambiguity. No field dynamics is inherited CheungXXIIA.

XXII-B & Ledger syntax, source-boundary warnings, reference stability, tolerance, and refinement tests CheungXXIIB.

XXII-C & Frozen process class and component order. The identifiers do not supply derivatives, Hamiltonians, or a local metric field CheungXXIIC.

XXII-D & Compatible transport contract, calibration separation, quantum transmission obstruction, and tests F1–F6 CheungXXIID.

En08-A; En08-B & Scheduler obstruction and prescribed-boundary approximation. Neither supplies the metric-jet or source rule needed here CheungEn08A,CheungEn08B.

VII-J & Three-relation discipline. A supplied geometric embedding is a separate certificate CheungVIIJ.

XIX-C; XIX-D & Refinement, interpolation, finite-coverage, and proof-transfer discipline. No native dynamics comparison is inherited CheungXIXC,CheungXIXD.

Oai265-A–B & Static records do not instantiate recovery or a gravitational dictionary; channel certificates require their own access and statistical assumptions CheungOai265A,CheungOai265B.

Oai282-B & A separately specified free-scalar stress-class and Ward benchmark, not stress-energy extraction for process data or Einstein dynamics CheungOai282B.

En07-A; En07-B & Channel/cost separation and conditional endpoint-recovery scope, respectively. Neither provides energy-momentum accounting here CheungEn07A,CheungEn07B.

III, IV, VI; VIII-A/B/C; Em02-E & Documentary classical, geometric, and lapse comparisons only. No operational correspondence theorem is supplied CheungClassicalComparisons,CheungXXIIA.