Non-identifications retained

$Q_H{{\Phi }^{(2)}}_{\mathrm{D}}$ is not a quantum retarded product of ${\mathcal{J}}_{\mathrm{D}}$. No Hadamard line is contracted against ${\mathcal{J}}_{\mathrm{D}}$.

The original detected XI-G classes with $\pm (k_1,k_2,0)$ and $k_1+k_2=2\mathrm{d}t$ remain excluded. ${{\Phi }^{(2)}}_{\mathrm{D}}$ is not a representative of those classes.

${{\mathcal{J}}^{\mathrm{D}}}_{g,{\sigma }_{\epsilon }}({\varphi }_m)=\varnothing$ stands. The slot $r_{\mathrm{D}}+r_g$ solves a gauge-fixed forcing equation, not the invariant coupled Einstein equation.

The inverse coefficient is $-1$, not $-4$. No X-track mixed map, reciprocity test, or triangle residue is imported.

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

The local pairing hypothesis $A\gamma =0$ near $S_{\xi }$ does not decide XI-G's global Einstein-subshell representative question.

No cone, token, conical readout, or Enter record is used.