Abstract

We consider a specific random graph which serves as a disordered medium for a particle performing biased random walk. Take a two-sided infinite horizontal ladder and pick a random spanning tree with a certain edge weight c for the (vertical) rungs. Now take a random walk on that spanning tree with a bias beta >1 to the right. In contrast to other random graphs considered in the literature (random percolation clusters, Galton–Watson trees) this one allows for an explicit analysis based on a decomposition of the graph into independent pieces. We give an explicit formula for the speed of the biased random walk as a function of both the bias beta and the edge weight c. We conclude that the speed is a continuous, unimodal function of beta that is positive if and only if beta < beta _c^{(1)} for an explicit critical value beta _c^{(1)} depending on c. In particular, the phase transition at beta _c^{(1)} is of second order. We show that another second order phase transition takes place at another critical value beta _c^{(2)}<beta _c^{(1)} that is also explicitly known: For beta <beta _c^{(2)} the times the walker spends in traps have second moments and (after subtracting the linear speed) the position fulfills a central limit theorem. We see that beta _c^{(2)} is smaller than the value of beta which achieves the maximal value of the speed. Finally, concerning linear response, we confirm the Einstein relation for the unbiased model (beta =1) by proving a central limit theorem and computing the variance.

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