← 研踪 PaperTrailarXiv:2605.05877 · v2
Understanding Simulated Annealing: from Weak Poincaré Inequalities to a Discrete Optimal Transport Framework
首次提交 2026-05-07 16:44
版本更新 2026-11-08 19:28
雷达观测 2026-11-10 12:16
摘要
Simulated annealing follows a path of distributions from an easy initial law to a target. Standard analyses require rapid mixing at every fixed temperature, which can fail for multimodal targets even when annealing succeeds. Motivated by the continuous optimal-transport analysis of annealed Langevin dynamics by Guo, Tao, and Chen (ICLR 2025), we develop a discrete optimal-transport framework for finite-state annealing. The discrete action of the path integrates the minimum electrical energy needed to route the demand $-\partial_sπ_s$ through the chain's transition capacities. Like a path-dependent inverse conductance, it penalizes a bottleneck only when the path must move mass across it. We also introduce weak action, which leaves an $\varepsilon$ amount of this motion unrouted. Up to initialization error, action $\mathcal A$ gives reverse-KL error at most $\mathcal A/(4T)$ after $T$ expected updates, while weak action gives TV error at most $\varepsilon+\sqrt{\mathcal A^{w}_\varepsilon/(8T)}$. Paralleling canonical paths and Poincaré inequalities, we develop flow and spectral bounds, showing that pathwise (weak) Poincaré inequalities imply (weak) action bounds. We also show that a weak Poincaré inequality yields a genuine one after removing a small amount of mass. As a pathwise analogue of chain decomposition, we obtain a componentwise algorithm for mixtures with phase weights supplied at initialization. Applications include mean-field Ising and Potts models and bipartite spin systems. For every fixed $δ>0$, we give a polynomial-time single-site annealing sampler for uniform independent sets in $(d,D)$-biregular bipartite graphs with $D/d\geq1+δ$ and large $D$. To our knowledge, this is the first polynomial-time sampler requiring only a fixed multiplicative degree imbalance, strictly extending the $D\geq7d\log d$ regime of Cannon and Perkins (SODA 2020).
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Understanding Simulated Annealing: from Weak Poincaré Inequalities to a Discrete Optimal Transport Framework
Simulated annealing follows a path of distributions from an easy initial law to a target. Standard analyses require rapid mixing at every fixed temperature, which can fail for multimodal targets even when annealing succeeds. Motivated by the continuous optimal-transport analysis of annealed Langevin dynamics by Guo, Tao, and Chen (ICLR 2025), we develop a discrete optimal-transport framework for finite-state annealing. The discrete action of the path integrates the minimum electrical energy needed to route the demand $-\partial_sπ_s$ through the chain's transition capacities. Like a path-dependent inverse conductance, it penalizes a bottleneck only when the path must move mass across it. We also introduce weak action, which leaves an $\varepsilon$ amount of this motion unrouted. Up to initialization error, action $\mathcal A$ gives reverse-KL error at most $\mathcal A/(4T)$ after $T$ expected updates, while weak action gives TV error at most $\varepsilon+\sqrt{\mathcal A^{w}_\varepsilon/(8T)}$. Paralleling canonical paths and Poincaré inequalities, we develop flow and spectral bounds, showing that pathwise (weak) Poincaré inequalities imply (weak) action bounds. We also show that a weak Poincaré inequality yields a genuine one after removing a small amount of mass. As a pathwise analogue of chain decomposition, we obtain a componentwise algorithm for mixtures with phase weights supplied at initialization. Applications include mean-field Ising and Potts models and bipartite spin systems. For every fixed $δ>0$, we give a polynomial-time single-site annealing sampler for uniform independent sets in $(d,D)$-biregular bipartite graphs with $D/d\geq1+δ$ and large $D$. To our knowledge, this is the first polynomial-time sampler requiring only a fixed multiplicative degree imbalance, strictly extending the $D\geq7d\log d$ regime of Cannon and Perkins (SODA 2020).
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