\section{Combining the local constructions} \label{sec-global} Fix an integer $r\ge6$ divisible by six, and put $k=r-1$ and $d=r-3$. We use the labelled frame family of the preceding section, with \[ \Delta=64r^8,\qquad \eta=\frac{r!}{2d!(\Delta+1)},\qquad \beta=(r-2)\eta. \] At each sufficiently large background size $M$, select exactly $\lfloor\eta M^d\rfloor$ labelled frames whose allowed sets of cyclic rows are pairwise disjoint. The selection is fixed before the modifications described below. Define \begin{equation}\label{eq-global-parameters} A=\left\lceil\frac{r^3}{\beta}\right\rceil,\quad Q_{ \mathrm{grid}}=rA,\quad W=r^2A,\quad H=rA^2,\quad G=W-r,\quad \rho=\frac{A\beta}{r},\quad E=10^{12}r^{22}W^4. \end{equation} The letter $Q_{\mathrm{grid}}$ denotes a grid width. It is unrelated to the row charge used in the assembly section. \subsection{Sets of active letters and fixed background letters} Take the $W$ control letters to be the pairs $(i,j)$ with $0\le i(2L+1)K$ ensures a gap longer than $2L+1$ between consecutive event times. Cut in this gap and regard the remaining components as ordinary intervals. The cut changes only where these intervals are written; the canonical times in \eqref{eq-event} remain unchanged. For a component whose first and last events are $f,e$, let $(v,j)$ be its forbidden pair. Choose the normal boundary $s\in[f-r+1,f]$ at which $v$ is mobile; the normal role action is a cycle on the $r$ roles. Set \[ P=2r\left\lceil\frac{e+1-s}{2r}\right\rceil. \] Replace the next $P$ normal batches by $P/2$ pairs of a permitted order and its reverse, using the order whose first target is different from $j$. Follow them by one normal cleanup batch. The local endpoint theorem shows that these $P+1$ batches end at exactly the normal literal state. Throughout the first $P$ batches, the letter $v$ is either mobile or in the first target slot. Thus it never occupies $j$ during any event batch. The inequalities \[ f-r+1\le s\le f,\qquad e+1\le s+P\le e+2r,\qquad s+P+1\le e+2r+1 \] put the entire replacement inside its merged interval. Different replacements are disjoint. Each restores its normal endpoint, so they can all be performed on the same cyclic walk. The joint-state containment proved earlier keeps every modified row inside the originally selected allowed set. If two modified candidates met, their unique shared letter would be stationary in both rows and would produce an event \eqref{eq-event}. The modification prevents that occupancy. This excludes collisions between two modifications as well as collisions with normal rows. Regard a batch starting at integer time $t$ as the unit interval $[t,t+1]$. The inequalities above put every changed batch inside the interval union. That union has total length at most $2LK\le5rK$, so at most $5rK$ batches change. A complete batch has at most $k(M+k)$ source rows. Comparing each changed batch with its normal version therefore changes the total row count by at most $10r^2KM$ when $M\ge r$. The short charge stays exactly $2(r-1)M$. There is also an untouched normal batch. Its full rows follow the literal successor $F$, which is the additional hypothesis needed in the connector construction. \subsection{Uniform counts} Let $B$ be the total number of source rows in the surviving modified contours, let $q$ be their total short charge, and let $c_{\mathrm{adv}}$ be the number of circles in the actual connector lists constructed in the assembly section. Put $D_{m,W}=\prod_{i=0}^{W-1}(m+i)$ and $c_r=2(r-1)/(r-2)$. \begin{proposition}\label{prop-global-counts} For every multiple $m$ of $r$ with $m\ge4E$, the construction has literal closure, pairwise distinct source cyclic classes above the chosen old cyclic order, and the safe connector lists of the assembly section. Its counts satisfy \[ \frac{B}{D_{m,W}}=\frac{\rho W}{m}(1+\theta),\qquad \frac{q+c_{\mathrm{adv}}}{D_{m,W}} =\frac{c_r\rho W}{m^2}(1+\epsilon),\qquad |\theta|,|\epsilon|\le\frac Em, \] and $c_{\mathrm{adv}}\le(r-1)q/m$. \end{proposition} \begin{proof} We first verify the size conditions used in the construction. The ceiling defining $A$ gives \[ \eta^{-1}=\frac{r-2}{\beta}\le\frac{r}{\beta} \le\frac{W}{r^4}\le W. \] Also $W\ge r^2\ge1$ and $G\le W$. The definition of $E$ implies $E\ge W^2$, $E\ge rW$, and $4E\ge38r^4$. Hence \[ M\ge m\ge38r^4,\qquad m\ge4W^2\ge G^2,\qquad G0$ under the present size bound. Averaging the relative row errors over the surviving contours gives a number $u$ such that \[ |u|\le\frac{2r+1040r^5W^2}{m}. \] Their short charges are all exactly $q_0$. Write $v=c_{\mathrm{adv}}/q$, so $0\le v\le(r-1)/m$. The two normalized counts now have the exact expressions \begin{align*} \frac{B}{D_{m,W}} &=\frac{H\beta}{m} \frac{\phi\psi t\mu^{d+2}(1+u)}{\chi},\\ \frac{q+c_{\mathrm{adv}}}{D_{m,W}} &=\frac{c_rH\beta}{m^2} \frac{\phi\psi t\mu^{d+1}(1+v)}{\chi}. \end{align*} The relative-error numerators, each to be divided by $m$, are bounded by \[ \begin{array}{lr} \text{rounding the selected frame count}&W\,,\\ \text{distinct guard positions}&W^2/2\,,\\ \text{guard-only deletion}&18r^2W^3\,,\\ \text{nearby incompatible events}&7\,118\,280r^{22}W^4\,,\\ \text{row count within a contour}&2r+1040r^5W^2\,,\\ \text{additional connector charge}&r\,,\\ \text{replacing powers of }M\text{ by powers of }m&2W^2\,,\\ \text{the product }D_{m,W}/m^W&W^2\,. \end{array} \] The first bound uses $d\ge3$ and $\eta^{-1}\le W/r^4$. The next three were proved in \eqref{eq-guard-count}, \eqref{eq-guard-loss}, and \eqref{eq-proximity-loss}. The row bound follows by dividing the displayed estimate for $N$ by $(r-2)M^2$. We use the product inequalities \[ \prod_i(1+u_i)\le\frac1{1-\sum_i u_i},\qquad \prod_i(1-u_i)\ge1-\sum_i u_i \quad(0\le u_i,\ \sum_i u_i<1). \] For the first inequality, use $1+u_i\le1/(1-u_i)$ and the second inequality. For the powers of $\mu$, there are at most $r$ equal factors $1+G/m$. Their deviations sum to at most $rG/m\le1/4$, so \[ 1\le\mu^{d+1}\le\mu^{d+2} \le\frac1{1-rG/m}\le1+\frac{2rG}{m} \le1+\frac{2W^2}{m}. \] For $\chi$, the deviations $i/m$ sum to at most $W^2/(2m)\le1/8$, which gives $1\le\chi\le1+W^2/m$ in the same way. The sum of the listed numerators is less than $9\cdot10^6r^{22}W^4$. Let $s$ be that sum divided by $m$. Then $s<1/1000$. To combine the estimates, let $s_0$ be the sum of the deviations allowed for the numerator factors in either exact expression, and let $s_1$ be the deviation allowed for $\chi$. Thus $s_0+s_1\le s$. The product inequalities give a numerator between $1-s_0$ and $1/(1-s_0)$, while $1\le\chi\le1+s_1$. The ratio is therefore at least \[ \frac{1-s_0}{1+s_1}\ge1-s_0-s_1\ge1-s \] and at most $1/(1-s_0)\le1/(1-s)\le1+2s$. In particular its deviation from one is at most $4s$. Since $36\cdot10^6<10^{12}$, each relative error is at most $E/m$. Finally $H\beta=\rho W$, as required. \end{proof} \begin{lemma}\label{lem-polynomial-width} The parameters in \eqref{eq-global-parameters} satisfy $r^2\le W\le352r^9$ and $r^2\le\rho