Abstract

We investigate the number Vp(n)V_p(n) of distinct sites visited by an nn-step resetting random walker on a dd-dimensional hypercubic lattice with resetting probability pp. In the case p=0p=0, we recover the well-known result that the average number of distinct sites grows for large nn as ⟨V0(n)⟩∼nd/2\langle V_0(n)\rangle\sim n^{d/2} for d<2d<2 and as ⟨V0(n)⟩∼n\langle V_0(n)\rangle\sim n for d>2d>2. For p>0p>0, we show that ⟨Vp(n)⟩\langle V_p(n)\rangle grows extremely slowly as ∼[log⁡(n)]d\sim \left[\log(n)\right]^d. We observe that the recurrence-transience transition at d=2d=2 for standard random walks (without resetting) disappears in the presence of resetting. In the limit p→0p\to 0, we compute the exact crossover scaling function between the two regimes. In the one-dimensional case, we derive analytically the full distribution of Vp(n)V_p(n) in the limit of large nn. Moreover, for a one-dimensional random walker, we introduce a new observable, which we call imbalance, that measures how much the visited region is symmetric around the starting position. We analytically compute the full distribution of the imbalance both for p=0p=0 and for p>0p>0. Our theoretical results are verified by extensive numerical simulations.

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