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Non-linear Log-Sobolev inequalities for the Potts semigroup and applications to reconstruction problems

11 May 2020
Yuzhou Gu
Yury Polyanskiy
ArXiv (abs)PDFHTML
Abstract

Consider a Markov process with state space [k][k][k], which jumps continuously to a new state chosen uniformly at random and regardless of the previous state. The collection of transition kernels (indexed by time t≥0t\ge 0t≥0) is the Potts semigroup. Diaconis and Saloff-Coste computed the maximum of the ratio of the relative entropy and the Dirichlet form obtaining the constant α2\alpha_2α2​ in the 222-log-Sobolev inequality (222-LSI). In this paper, we obtain the best possible non-linear inequality relating entropy and the Dirichlet form (i.e., ppp-NLSI, p≥1p\ge1p≥1). As an example, we show α1=1+1+o(1)log⁡k\alpha_1 = 1+\frac{1+o(1)}{\log k}α1​=1+logk1+o(1)​. The more precise NLSIs have been shown by Polyanskiy and Samorodnitsky to imply various geometric and Fourier-analytic results. Beyond the Potts semigroup, we also analyze Potts channels -- Markov transition matrices [k]×[k][k]\times [k][k]×[k] constant on and off diagonal. (Potts semigroup corresponds to a (ferromagnetic) subset of matrices with positive second eigenvalue). By integrating the 111-NLSI we obtain the new strong data processing inequality (SDPI), which in turn allows us to improve results on reconstruction thresholds for Potts models on trees. A special case is the problem of reconstructing color of the root of a kkk-colored tree given knowledge of colors of all the leaves. We show that to have a non-trivial reconstruction probability the branching number of the tree should be at least \frac{\log k}{\log k - \log(k-1)} = (1-o(1))k\log k. This extends previous results (of Sly and Bhatnagar et al.) to general trees, and avoids the need for any specialized arguments. Similarly, we improve the state-of-the-art on reconstruction threshold for the stochastic block model with kkk balanced groups, for all k≥3k\ge 3k≥3. These improvements advocate information-theoretic methods as a useful complement to the conventional techniques originating from the statistical physics.

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