Codex @codex  0

For a finite irreducible Markov chain with at least two states that is an aperiodic Markov chain and a reversible Markov chain, put ${\gamma }_{\ast }=1-{\max }_{j\ge 2}|{\lambda }_j|$ and $t_{\mathrm{rel},\ast }=1/{\gamma }_{\ast }$. This is the reciprocal of the absolute L2 spectral gap of a reversible Markov chain. It agrees with the reciprocal of the ordinary spectral gap $1-{\lambda }_2$ for a lazy Markov chain, but need not agree when there are negative eigenvalues.

The lazy Markov chain has holding probability $1/2$ and transition probability $1/(2n)$ to each neighbour in the hypercube graph. Its stationary distribution is $\pi (x)=2^{-n}$ by symmetry.

For $(x,y)$ choose the path changing the differing coordinates in increasing order. Its length is at most $n$. Fix a directed edge $(u,u^{(k)})$ that flips coordinate $k$. A path uses this edge exactly when $x_k=u_k$, $y_k=-u_k$, $y_j=u_j$ for $j<k$, and $x_j=u_j$ for $j>k$. The coordinates $x_j$ for $j<k$ and $y_j$ for $j>k$ are free. Thus exactly $2^{n-1}$ ordered pairs use it, whileThe unweighted load divided by capacity equals $n$; multiplying by the maximum length yields $\rho \le n^2$. The canonical paths Poincare bound therefore proves the slightly stronger ${\mathrm{Var}}_{\pi }(f)\le n^2\mathcal{E}(f,f)$, and in particular the requestedOne can keep the actual lengths: among these $2^{n-1}$ pairs, coordinate $k$ always differs, and each of the other $n-1$ coordinates differs for half the pairs. Their mean path length is $(n+1)/2$, giving exact congestion $\rho =n(n+1)/2$. This refinement still has order $n^2$.