A finite ergodic Markov chain exhibits cutoff if its distance to equilibrium remains close to its initial value over a certain number of iterations and then abruptly drops to near 0 on a much shorter time scale. Originally discovered in the context of card shuffling (Aldous-Diaconis, 1986), this remarkable phenomenon is now rigorously established for many reversible chains. Here we consider the non-reversible case of random walks on sparse directed graphs, for which even the equilibrium measure is far from being understood. We work under the configuration model, allowing both the in-degrees and the out-degrees to be freely specified. We establish the cutoff phenomenon, determine its precise window and prove that the cutoff profile approaches a universal shape. We also provide a detailed description of the equilibrium measure.
Motivated by applications to real-world networks (see, e.g., the survey by Cooper @cite_17 and the references therein), the mixing properties of random walks on large but finite random graphs have recently become the subject of many investigations. The attention has been mostly restricted to the undirected setting, where the in-degree distribution is reversible. In particular, Frieze and Cooper have studied the (i.e., the expected time needed for the chain to visit all states) of various random graphs @cite_28 @cite_14 @cite_34 @cite_33 , and analyzed the precise component structures induced by the walk on random regular graphs @cite_15 . Bounds for the mixing time on the largest component of the popular Erd os--Renyi model have also been obtained by various authors, in both the critical and super-critical connectivity regime @cite_18 @cite_1 @cite_5 @cite_13 .
@cite_18 @cite_14 @cite_33 @cite_28 @cite_1 @cite_5 @cite_15 @cite_34 @cite_13 @cite_17
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We identify the scaling limit for the sizes of the largest components at criticality for inhomogeneous random graphs with weights that have finite third moments. We show that the sizes of the (rescaled) components converge to the excursion lengths of an inhomogeneous Brownian motion, which extends results of Aldous (1997) for the critical behavior of Erdos-Renyi random graphs. We rely heavily on martingale convergence techniques, and concentration properties of (super)martingales. This paper is part of a programme initiated in van der Hofstad (2009) to study the near-critical behavior in inhomogeneous random graphs of so-called rank-1. In this article we present a study of the mixing time of a random walk on the largest component of a supercritical random graph, also known as the giant component. We identify local obstructions that slow down the random walk, when the average degree d is at most O( @math ), proving that the mixing time in this case is Θ((n-d)2) asymptotically almost surely. As the average degree grows these become negligible and it is the diameter of the largest component that takes over, yielding mixing time Θ(n-d) a.a.s.. We proved these results during the 2003–04 academic year. Similar results but for constant d were later proved independently by in [3]. © 2008 Wiley Periodicals, Inc. Random Struct. Alg., 2008 Most of this work was completed while the author was a research fellow at the School of Computer Science, McGill University. Suppose that G is a finite, connected graph and X is a lazy random walk on G . The lamplighter chain X ? associated with X is the random walk on the wreath product G ? =Z 2 ?G , the graph whose vertices consist of pairs (f - ,x) where f is a labeling of the vertices of G by elements of Z 2 = 0,1 and x is a vertex in G . There is an edge between (f - ,x) and (g - ,y) in G ? if and only if x is adjacent to y in G and f z =g z for all z?x,y . In each step, X ? moves from a configuration (f - ,x) by updating x to y using the transition rule of X and then sampling both f x and f y according to the uniform distribution on Z 2 ; f z for z?x,y remains unchanged. We give matching upper and lower bounds on the uniform mixing time of X ? provided G satisfies mild hypotheses. In particular, when G is the hypercube Z d 2 , we show that the uniform mixing time of X ? is T(d2 d ) . More generally, we show that when G is a torus Z d n for d=3 , the uniform mixing time of X ? is T(dn d ) uniformly in n and d . A critical ingredient for our proof is a concentration estimate for the local time of the random walk in a subset of vertices. The percolation phase transition and the mechanism of the emergence of the giant component through the critical scaling window for random graph models, has been a topic of great interest in many dierent communities ranging from statistical physics, combinatorics, computer science, social networks and probability theory. The last few years have witnessed an explosion of models which couple random aggregation rules, that specify how one adds edges to existing congurations, and choice, wherein one selects from a ‘limited’ set of edges at random to use in the conguration. These models exhibit fascinating new phenomenon, ranging from delaying or speeding up the emergence of the giant component, to percolation", where the diameter of the scaling window is several orders of magnitude smaller than that for standard random graph models. While an intense study of such models has ensued, understanding the actual emergence of the giant component and merging dynamics in the critical scaling window has remained impenetrable to a rigorous analysis. In this work we take an important step in the analysis of such models by studying one of the standard examples of such processes, namely the Bohman-Frieze model, and provide rst results on the asymptotic dynamics, through the critical scaling window, that lead to the emergence of the giant component for such models. We identify the scaling window and show that through this window, the component sizes properly rescaled converge to the standard multiplicative coalescent. Proofs hinge on a careful analysis of certain innite-type branching processes with types taking values in the space of RCLL paths, and stochastic analytic techniques to estimate susceptibility functions of the components all the way through the scaling window where these functions explode. Previous approaches for analyzing random graphs at criticality have relied largely on classical breadth-rst search techniques that exploit asymptotic connections with Brownian excursions. For dynamic random graph models evolving via general Markovian rules, such approaches fail and we develop a quite dierent set of tools that can potentially be used for the study of critical dynamics for all bounded size rules.