Abstract

The objective of this paper is to establish explicit concentration inequalities for the Glauber dynamics related with continuum or discrete Gibbs measures. At first we establish the optimal transportation-information $W_1 I$-inequality for the $M/M/\infty$-queue associated with the Poisson measure, which improves several previous known results. Under the Dobrushin's uniqueness condition, we obtain some explicit $W_1 I$-inequalities for Gibbs measures both in the continuum and in the discrete lattice. Our method is a combination of Lipschitzian spectral gap, the Lyapunov test function approach and the tensorization technique.

Highlights

  • 1.1 Transportation-information inequalities W1ILet be a Polish space equipped with the Borel σ-field, and let d be a lower semi-continuous metric on the product space ×

  • 1/p d(x, y)pdπ(x, y), where the infimum is taken over all probability measures π on the product space × with marginal distributions μ and ν (say coupling of (μ, ν))

  • This infimum is finite once μ and ν belong to p 1 (

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Summary

Transportation-information inequalities W1I

Let be a Polish space equipped with the Borel σ-field , and let d be a lower semi-continuous metric on the product space × (which does not necessarily generate the topology of ). 1/p d(x, y)pdπ(x, y) , where the infimum is taken over all probability measures π on the product space × with marginal distributions μ and ν (say coupling of (μ, ν)). This infimum is finite once μ and ν belong to p 1. Given a family of bounded measurable functions g (say g ∈ b ), the following properties are equivalent:. Gao and the third named author [6] proved a tensorization result for the Wasserstein distance (see Lemma 4.2 below) and established the “dimension-free" transportation-information inequalities Wp I(p ≥ 1) for the discrete Gibbs measure, under the Dobrushin’s uniqueness condition ([3, 4])

Continuum Gibbs measure and generator of the Glauber dynamic
W1I-inequality for continuum Gibbs measure
W1I-inequality
Findings
W1I-inequality for the discrete spin system
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