\section{Calibration of the finite certificates}\label{app:certificates} We verify the central-interval routine and choose the finite calculation's parameters. The purpose of the calibration is to ensure that a failed certificate identifies a coordinate whose short interval gives a high density throughout its middle half. \subsection{The central-interval test} For the one-coordinate list $[A_i,B_i]$, $1\le i\le N$, take $u$ to be the $N/4$-th upper endpoint in sorted order and $v$ to be the $3N/4$-th lower endpoint. The alphabet size $S$ is divisible by four, and the queried coordinate is interior, so $N/4$ is an integer. Return \texttt{FAIL} if $u\ge v$ or fewer than $N/4$ list intervals lie wholly in $[u,v]$. Otherwise return $[u,v]$. At least $N/4$ intervals end at or below $u$, and at least $N/4$ begin at or above $v$. On success, at least $N/4$ intervals also lie wholly inside $[u,v]$. Enclosure certifies mass at least $1/4$ in each of the three regions. The true distribution is continuous and supported on $(\ell_x,r_x)$, so these masses imply $\ell_x0$, degree at most $k$, and directed paths of at most $2H$ vertices. If any coordinate involved in a comparison has interval width at least $w_*$, comparison certification succeeds. If $W_x\ge w_*$, then \textnormal{\texttt{CentralInterval}}$(D,x)$ succeeds. \end{lemma} \begin{proof}[Proof of Lemma~\ref{lem:certificate-success}] Calibrate both routines using Theorem~\ref{thm:local} with \begin{equation}\label{eq:estimator-coupling-parameters} d=k,\qquad h=2H,\qquad \alpha=\frac\eta2,\qquad \delta=\frac{\eta w_*}{8(B+1)}. \end{equation} These parameters are fixed for the interaction. They do not depend on the queried widths. Suppose one queried coordinate $x$ has $W_x\ge w_*$. If the computed intervals overlap and both have width at most $\delta$, the enclosed positions differ by at most $2\delta$. Lemma~\ref{lem:gap} therefore bounds the unresolved fraction by \[ 1-p-q\le\alpha+\Prb(|X_x-X_y|\le2\delta) \le\alpha+\frac{4(B+1)\delta}{w_*}=\eta. \] Thus $\max(p,q)\ge(1-\eta)/2>1/2-\eta$, so comparison certification succeeds. For a threshold $c$, an unresolved interval contains $c$. If its width is at most $\delta$, its enclosed position is within $\delta$ of $c$, giving the stronger bound \begin{equation}\label{eq:threshold-unresolved} \alpha+\frac{2(B+1)\delta}{w_*}=\frac{3\eta}{4}. \end{equation} It remains to show that \texttt{CentralInterval} succeeds when $W_x\ge w_*$. By \eqref{eq:threshold-unresolved}, at most a fraction $\tau=3\eta/4$ of its intervals contain any fixed real number. This bound applies in particular to the selected endpoints $u$ and $v$. An interval extending below $u$ either ends strictly below $u$ or contains $u$. By the rank defining $u$, fewer than $N/4$ intervals end strictly below it. Thus at most $(1/4+\tau)N$ intervals extend below $u$. Similarly, at most $N/4$ intervals begin strictly above $v$, so at most $(1/4+\tau)N$ extend above $v$. At least $(1/2-2\tau)N\ge N/4$ intervals therefore lie wholly inside $[u,v]$, since $\eta<1/32$. Enclosure gives this interval mass at least $1/4$. Continuity forces $u