2020
DOI: 10.48550/arxiv.2006.10871
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A shape theorem and a variational formula for the quenched Lyapunov exponent of random walk in a random potential

Abstract: We prove a shape theorem and derive a variational formula for the limiting quenched Lyapunov exponent and the Green's function of random walk in a random potential on a square lattice of arbitrary dimension and with an arbitrary finite set of steps. The potential is a function of a stationary environment and the step of the walk. This potential is subject to a moment assumption whose strictness is tied to the mixing of the environment. Our setting includes directed and undirected polymers, random walk in stati… Show more

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Cited by 2 publications
(3 citation statements)
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“…potentials and the simple random walk on Z d in the present and aforementioned articles, let us finally refer results for models with various changes of our setting. In [8,17], the underlying space is Z d , but the potential is stationary and ergodic and each step of the random walk is in an arbitrary finite set. Under such a more general setting, [17] studied the quenched large deviation principle and [8] constructed the quenched Lyapunov exponent.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…potentials and the simple random walk on Z d in the present and aforementioned articles, let us finally refer results for models with various changes of our setting. In [8,17], the underlying space is Z d , but the potential is stationary and ergodic and each step of the random walk is in an arbitrary finite set. Under such a more general setting, [17] studied the quenched large deviation principle and [8] constructed the quenched Lyapunov exponent.…”
Section: Introductionmentioning
confidence: 99%
“…In [8,17], the underlying space is Z d , but the potential is stationary and ergodic and each step of the random walk is in an arbitrary finite set. Under such a more general setting, [17] studied the quenched large deviation principle and [8] constructed the quenched Lyapunov exponent. On the other hand, [18, Part II] treats a Brownian motion evolving in a Poissonian potential, which is a continuum version of our model.…”
Section: Introductionmentioning
confidence: 99%
“…The "cocycle" branch of [52,51,54,28] has also been developed for FPP [34,43] and bears connections to the formula of Krishnan. Meanwhile, the "entropy" branch led to an LPP formula [28,Thm.…”
mentioning
confidence: 99%