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随机介质中弹性弦的弛豫动力学

Relaxation dynamics of an elastic string in random media.

作者信息

Noh Jae Dong, Park Hyunggyu

机构信息

Department of Physics, University of Seoul, Seoul 130-743, Korea.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Oct;80(4 Pt 1):040102. doi: 10.1103/PhysRevE.80.040102. Epub 2009 Oct 8.

Abstract

We investigate numerically the relaxation dynamics of an elastic string in two-dimensional random media by thermal fluctuations starting from a flat configuration. Measuring spatial fluctuations of its mean position, we find that the correlation length grows in time asymptotically as xi approximately (ln t)1/chi . This implies that the relaxation dynamics is driven by thermal activations over random energy barriers which scale as EB(l) approximately l;chi with a length scale l . Numerical data strongly suggest that the energy barrier exponent chi is identical to the energy fluctuation exponent chi=1/3 . We also find that there exists a long transient regime, where the correlation length follows a power-law dynamics as xi approximately t1/z with a nonuniversal dynamic exponent z . The origin of the transient scaling behavior is discussed in the context of the relaxation dynamics on finite ramified clusters of disorder.

摘要

我们从平坦构型出发,通过热涨落对二维随机介质中弹性弦的弛豫动力学进行了数值研究。通过测量其平均位置的空间涨落,我们发现关联长度随时间渐近增长,即$\xi\approx(\ln t)^{1/\chi}$。这意味着弛豫动力学是由跨越随机能量势垒的热激活驱动的,这些势垒的尺度为$E_B(l)\approx l^{\chi}$,其中$l$为长度尺度。数值数据强烈表明,能量势垒指数$\chi$与能量涨落指数$\chi = 1/3$相同。我们还发现存在一个长的瞬态区域,其中关联长度遵循幂律动力学,即$\xi\approx t^{1/z}$,其中$z$为非普适动力学指数。我们在无序有限分支簇上的弛豫动力学背景下讨论了瞬态标度行为的起源。

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