English

Large Deviations for Empirical Measures of Self-Interacting Markov Chains

Probability 2025-07-15 v3 Optimization and Control

Abstract

Let Δo\Delta^o be a finite set and, for each probability measure mm on Δo\Delta^o, let G(m)G(m) be a transition probability kernel on Δo\Delta^o. Fix x0Δox_0 \in \Delta^o and consider the chain {Xn,  nN0}\{X_n, \; n \in \mathbb{N}_0\} of Δo\Delta^o-valued random variables such that X0=xX_0=x, and given X0,,XnX_0, \ldots , X_n, the conditional distribution of Xn+1X_{n+1} is G(Ln+1)(Xn,)G(L^{n+1})(X_n, \cdot), where Ln+1=1n+1i=0nδXiL^{n+1} = \frac{1}{n+1} \sum_{i=0}^{n} \delta_{X_i} is the empirical measure at instant nn. Under conditions on GG we establish a large deviation principle for the empirical measure sequence {Ln,  nN}\{L^n, \; n \in \mathbb{N}\}. As one application of this result we obtain large deviation asymptotics for the Aldous-Flannery-Palacios (1988) approximation scheme for quasistationary distributions of irreducible finite state Markov chains. The conditions on GG cover various other models of reinforced stochastic evolutions as well, including certain vertex reinforced and edge reinforced random walks and a variant of the PageRank algorithm. The particular case where G(m)G(m) does not depend on mm corresponds to the classical results of Donsker and Varadhan (1975) on large deviations of empirical measures of Markov processes. However, unlike this classical setting, for the general self-interacting models considered here, the rate function takes a very different form; it is typically non-convex and is given through a dynamical variational formula with an infinite horizon discounted objective function.

Keywords

Cite

@article{arxiv.2304.01384,
  title  = {Large Deviations for Empirical Measures of Self-Interacting Markov Chains},
  author = {Amarjit Budhiraja and Adam Waterbury and Pavlos Zoubouloglou},
  journal= {arXiv preprint arXiv:2304.01384},
  year   = {2025}
}

Comments

64 pages

R2 v1 2026-06-28T09:47:53.798Z