B5: exclusions, the jet, and the classical ledger

The following boundaries remain explicit.

X-track comparison. No X-E or X-F inverse, density switch, or mixed-tree prescription is imported. No field map is identified with $k_{\mathrm{mix}}$. The reciprocity constraint mentioned in the production brief is a constraint on a proposed identification, not a permission to remove ramp derivatives from a new action.

The X-G manuscript is not among the supplied dependencies. Its numerical reciprocity witness is therefore not rederived or used as a premise of any theorem here.

original coupled jet. The original empty fixed-input Einstein jet ${\mathcal{J}}_g({\varphi }_m)=\varnothing$ is retained as the predecessor result for its original action, as cited by XI-B and XI-E. A new action requires its own coupled equation and conservation analysis.

The statement “no jet repair is claimed” in XII-A is not a decision about a model that XII-A never defines. This manuscript does not turn it into one. The changed jet is unresolved.

original ledger. The classical ledger $-I+I+0=0$ belongs to the original XI-F response and its stated coefficient comparison. It is not recomputed here, not promoted to a quantum relation, and not used as the plateau law of an undefined changed response.

quantum constructions. No second graviton line, fish graph, triangle subtraction, ${\mathsf{T}}_2$, reflected residue, ghost loop, state, or expectation value is formed. No interacting differential, master equation, or interacting BRST class is claimed.

width. The ramp width remains $\epsilon >0$ throughout. No limiting argument is used to suppress the layer terms. Smoothness at fixed width does not identify the new model with a sharp insertion.

additional readout. No X-Enter record, cone token, conical current, or independent readout is assigned to the kernel. None is a premise of this audit.