The fifth pass: one identification, three refusals, four candidate displays

coefficients (D0.14). XIV-H, lines 653–665 Hq: the ${q^{L,I,J}}_{\alpha \beta }$ are the coefficients of the actual differentiated source, including ramp derivatives, with $|\alpha |+|\beta |\le 2$. The undifferentiated source is XII-C's density-weighted cubic XIICsource, not a displayed polynomial. Expanding it is a calculation, not a located display; it is not performed here.

factor (D0.14). The record reports a normalization line $\square {E_0}^{\mathrm{R}}=\mathrm{id}$ in XIV-I (locator not returned) alongside (eq:R). XII-D sets $v_f=E^{\mathrm{A}}f$ and does not display $E^{\mathrm{A}}$. No XIV text declares ${E^{\mathrm{A}}}_m$ to be the advanced inverse of $\square +m^2$. Lemma lem:advanced constructs that inverse and proves its uniqueness; the identification remains a candidate.

stress (D0.12). XIII-C and XIV-J display Jstress

and the record reports the vertex as $-\frac{1}{2}\int g{\gamma }_{\mu \nu }{T_0}^{\mu \nu }$ (locator not returned). XIV-J does not display the normalization of $T^{\mu \nu }(\varphi ,\psi )$ in (eq:hess); Lemma lem:polar shows the factor is two-valued.

replacement (D0.11). XII-A, Definition def:admissible, lines 518–528 XIIAhad, defines an admissible $H^{\prime }$ by four clauses: the same shell equations in both slots, the same graded antisymmetric part $i\Delta$, a smooth difference $H^{\prime }-H$, and vanishing unless $|A|+|B|$ is even and the ghost numbers sum to zero. No manuscript equates a XIV object with this $H^{\prime }$ (F3).

sets (D0.9, D0.17). XIII-C, lines 603–620 XIIICvertex: the ${\Delta }_I$ are the connected collision subsets of the cycle-vertex table, for instance $\{y,u,v\}$ and $\{y,v\}$ on $B_1$. $D_{\Gamma }$, $w_{\Gamma }$, $S_{\Gamma /I}$ remain roles.