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Probing the tails of the ground state energy distribution for the directed polymer in a random medium of dimension $d=1,2,3$ via a Monte-Carlo procedure in the disorder

机译:探讨基态能量分布的尾部   定向聚合物在一个尺寸为$ d = 1,2,3 $的随机介质中通过monte-Carlo   这种疾病的程序

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摘要

In order to probe with high precision the tails of the ground-state energydistribution of disordered spin systems, K\"orner, Katzgraber and Hartmann\cite{Ko_Ka_Ha} have recently proposed an importance-sampling Monte-CarloMarkov chain in the disorder. In this paper, we combine their Monte-Carloprocedure in the disorder with exact transfer matrix calculations in eachsample to measure the negative tail of ground state energy distribution$P_d(E_0)$ for the directed polymer in a random medium of dimension $d=1,2,3$.In $d=1$, we check the validity of the algorithm by a direct comparison withthe exact result, namely the Tracy-Widom distribution. In dimensions $d=2$ and$d=3$, we measure the negative tail up to ten standard deviations, whichcorrespond to probabilities of order $P_d(E_0) \sim 10^{-22}$. Our results arein agreement with Zhang's argument, stating that the negative tail exponent$\eta(d)$ of the asymptotic behavior $\ln P_d (E_0) \sim - | E_0 |^{\eta(d)}$as $E_0 \to -\infty$ is directly related to the fluctuation exponent$\theta(d)$ (which governs the fluctuations $\Delta E_0(L) \sim L^{\theta(d)}$of the ground state energy $E_0$ for polymers of length $L$) via the simpleformula $\eta(d)=1/(1-\theta(d))$. Along the paper, we comment on thesimilarities and differences with spin-glasses.
机译:为了高精度地探测无序自旋系统的基态能量分布的尾巴,Korner,Katzgraber和Hartmann \ cite {Ko_Ka_Ha}最近提出了对该疾病进行重要性采样的Monte-CarloMarkov链。在本文中,我们将无序中的蒙特卡洛过程与每个样本中的精确传递矩阵计算相结合,以测量尺寸为$ d = 1,2的随机介质中定向聚合物的基态能量分布的负尾$ P_d(E_0)$ ,3 $。在$ d = 1 $中,我们通过与精确结果(即Tracy-Widom分布)的直接比较来检查算法的有效性。在维度$ d = 2 $和$ d = 3 $中,我们测量了负尾部最多10个标准差,这对应于阶次$ P_d(E_0)\ sim 10 ^ {-22} $的概率。我们的结果与Zhang的观点一致,指出负尾部指数$ \ eta(d)$为渐近行为$ \ ln P_d(E_0)\ sim-| E_0 | ^ {\ eta(d)} $ as $ E_0 \ to-\ infty $是可怕的与波动指数$ \ theta(d)$(决定长度为$的聚合物的基态能量$ E_0 $的波动$ \ Delta E_0(L)\ sim L ^ {\ theta(d)} $ L $)通过简单公式$ \ eta(d)= 1 /(1- \ theta(d))$。在本文中,我们评论了自旋玻璃的异同。

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  • 作者

    Monthus, Cecile; Garel, Thomas;

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  • 年度 2006
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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