Statistics of low energy excitations for the directed polymer in a $1+d$ random medium ($d=1,2,3$)

Details Statistics of low energy excitations for the directed polymer in a $1+d$ random medium ($d=1,2,3$) Statistics of low energy excitations for the directed polymer in a $1+d$ random medium ($d=1,2,3$)

2006-02-08

arxiv.org/abs/cond-mat/0602200v1

Phys. Rev. E 73, 056106 (2006)

Physics

Condensed Matter

Disordered Systems and Neural Networks

15 pages, 25 figures

Scientific paper

10.1103/PhysRevE.73.056106

We consider a directed polymer of length $L$ in a random medium of space dimension $d=1,2,3$. The statistics of low energy excitations as a function of their size $l$ is numerically evaluated. These excitations can be divided into bulk and boundary excitations, with respective densities $\rho^{bulk}_L(E=0,l)$ and $\rho^{boundary}_L(E=0,l)$. We find that both densities follow the scaling behavior $\rho^{bulk,boundary}_L(E=0,l) = L^{-1-\theta_d} R^{bulk,boundary}(x=l/L)$, where $\theta_d$ is the exponent governing the energy fluctuations at zero temperature (with the well-known exact value $\theta_1=1/3$ in one dimension). In the limit $x=l/L \to 0$, both scaling functions $R^{bulk}(x)$ and $R^{boundary}(x)$ behave as $R^{bulk,boundary}(x) \sim x^{-1-\theta_d}$, leading to the droplet power law $\rho^{bulk,boundary}_L(E=0,l)\sim l^{-1-\theta_d} $ in the regime $1 \ll l \ll L$. Beyond their common singularity near $x \to 0$, the two scaling functions $R^{bulk,boundary}(x)$ are very different : whereas $R^{bulk}(x)$ decays monotonically for $0

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