417 research outputs found

    Maximal Displacement for Bridges of Random Walks in a Random Environment

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    It is well known that the distribution of simple random walks on Z\bf{Z} conditioned on returning to the origin after 2n2n steps does not depend on p=P(S1=1)p= P(S_1 = 1), the probability of moving to the right. Moreover, conditioned on {S2n=0}\{S_{2n}=0\} the maximal displacement maxk2nSk\max_{k\leq 2n} |S_k| converges in distribution when scaled by n\sqrt{n} (diffusive scaling). We consider the analogous problem for transient random walks in random environments on Z\bf{Z}. We show that under the quenched law PωP_\omega (conditioned on the environment ω\omega), the maximal displacement of the random walk when conditioned to return to the origin at time 2n2n is no longer necessarily of the order n\sqrt{n}. If the environment is nestling (both positive and negative local drifts exist) then the maximal displacement conditioned on returning to the origin at time 2n2n is of order nκ/(κ+1)n^{\kappa/(\kappa+1)}, where the constant κ>0\kappa>0 depends on the law on environment. On the other hand, if the environment is marginally nestling or non-nestling (only non-negative local drifts) then the maximal displacement conditioned on returning to the origin at time 2n2n is at least n1εn^{1-\varepsilon} and at most n/(lnn)2εn/(\ln n)^{2-\varepsilon} for any ε>0\varepsilon>0. As a consequence of our proofs, we obtain precise rates of decay for Pω(X2n=0)P_\omega(X_{2n}=0). In particular, for certain non-nestling environments we show that Pω(X2n=0)=exp{CnCn/(lnn)2+o(n/(lnn)2)}P_\omega(X_{2n}=0) = \exp\{-Cn -C'n/(\ln n)^2 + o(n/(\ln n)^2) \} with explicit constants C,C>0C,C'>0.Comment: Revised version, 19 pages, 1 figure To appear in: AIHP Prob. & Sta

    Routing on trees

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    We consider three different schemes for signal routing on a tree. The vertices of the tree represent transceivers that can transmit and receive signals, and are equipped with i.i.d. weights representing the strength of the transceivers. The edges of the tree are also equipped with i.i.d. weights, representing the costs for passing the edges. For each one of our schemes, we derive sharp conditions on the distributions of the vertex weights and the edge weights that determine when the root can transmit a signal over arbitrarily large distances

    Annealed deviations of random walk in random scenery

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    Let (Zn)nN(Z_n)_{n\in\N} be a dd-dimensional {\it random walk in random scenery}, i.e., Zn=k=0n1Y(Sk)Z_n=\sum_{k=0}^{n-1}Y(S_k) with (Sk)kN0(S_k)_{k\in\N_0} a random walk in Zd\Z^d and (Y(z))zZd(Y(z))_{z\in\Z^d} an i.i.d. scenery, independent of the walk. The walker's steps have mean zero and finite variance. We identify the speed and the rate of the logarithmic decay of (1nZn>bn)\P(\frac 1n Z_n>b_n) for various choices of sequences (bn)n(b_n)_n in [1,)[1,\infty). Depending on (bn)n(b_n)_n and the upper tails of the scenery, we identify different regimes for the speed of decay and different variational formulas for the rate functions. In contrast to recent work \cite{AC02} by A. Asselah and F. Castell, we consider sceneries {\it unbounded} to infinity. It turns out that there are interesting connections to large deviation properties of self-intersections of the walk, which have been studied recently by X. Chen \cite{C03}.Comment: 32 pages, revise
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