Boundaries recorded, not re-proved

The XI-G classes $\pm (k_1,k_2,0)$, $k_1+k_2=2\mathrm{d}t$, remain excluded. ${\mathcal{C}}_{3,\mathrm{D}}$ and ${{\Phi }^{(2)}}_{\mathrm{D}}$ are different, model-dependent insertions and supply no representative of the original class.

${{\mathcal{J}}^{\mathrm{D}}}_{g,{\sigma }_{\epsilon }}({\varphi }_m)=\varnothing$ stands. The slot $r_{\mathrm{D}}+r_g$ solves the gauge-fixed forcing equation with zero data; it is not an invariant coupled Einstein solution, and the Einstein row of Theorem thm:plateau is where that distinction appears.

No quantum retarded product of ${\mathcal{J}}_{\mathrm{D}}$: $Q_H{\mathcal{C}}_{3,\mathrm{D}}$ and $Q_H{{\Phi }^{(2)}}_{\mathrm{D}}$ are classes of classical insertions.

No loop, state, antibracket, master identity, interacting differential, or $\epsilon \to 0$ limit.

No identification with an X-track mixed map; the inverse is $-\mathcal{P}{E}_0^{\mathrm{R}}$, not $-4\mathcal{P}{E}_0^{\mathrm{R}}$; no triangle residue is subtracted; the initial surface is not moved; $J_3$ is not ramped a second time.