Institute for Mathematical Physics Boundaries and Harmonic Functions for Random Walks with Random Transition Probabilities Boundaries and Harmonic Functions for Random Walks with Random Transition Probabilities
Institute for Mathematical Physics Boundaries and Harmonic Functions for Random Walks with Random Transition Probabilities Boundaries and Harmonic Functions for Random Walks with Random Transition Probabilities
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数学物理研究所 具有随机转移概率的随机游走的边界和调和函数 具有随机转移概率的随机游走的边界和调和函数
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A. S
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V. Kaimanovich;Y. Kifer;Zion Rubshtein;Ben;Typeset By;A. S
The usual random walk on a group (homogeneous both in time and in space) is determined by a probability measure on the group. In a random walk with random transition probabilities this single measure is replaced with a stationary sequence of measures , so that the resulting (random) Markov chains are still space homogeneous, but no longer time homogeneous. We study various notions of measure theoretical boundaries associated with this model, establish an analogue of the Poisson formula for (random) bounded harmonic functions, and identify these boundaries for several classes of groups. Random walks on groups were intensively studied during the last 40 years (see, for instance, [Ka96] and the references therein). Their importance is due to numerous applications, in particular, to the description of boundaries and spaces of harmonic functions and to the study of ergodic properties of group actions. Such random walks are Markov chains which are homogeneous both in time and space and can be also represented as products of independent identically distributed (i.i.d.) group elements. In the particular important case of products of random matrices additional tools such as Lyapunov exponents can be employed. A random walk on a group G is determined by a Markov operator P = P (µ) which consists in the (right) convolution with a fixed probability measure µ on G, so that the operator P is invariant with respect to the action of the group on itself by left translations. There are two models for further " randomization " of these " ordinary " random walks. The first model is usually referred to as random walks in random environment (RWRE) and consists in considering a probability measure λ on the space of all Markov operators on G. In this model the individual operators (environments) are not group invariant, although the group structure is taken into account by requiring the measure λ to be quasi-invariant with respect to the action of G on the space of environments (more specifically, λ is usually assumed to be either translation invariant or stationary with respect to the " moving environment " chain, see, for instance, [Kal81], [KMo84], [KSi00]). One chooses a random environment according to the distribution λ, and then runs a time (but not space!) homogeneous Markov chain in this environment. The other model which we call random walks with random transition probabilities (RWRTP) is opposite to RWRE in the sense that here one …