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Brownian motion in dynamically disordered media - art. no. 051111

机译:动态混乱的媒体中的布朗运动-艺术。没有。 051111

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The motion of Brownian test particles in a model random potential with time dependent correlations is investigated using four methods: renormalized perturbation, perturbation using Martin, Siggia, and Rose functional formalism (MSR), the Edwards variational method on the MSR functional, and renormalization group with the MSR function. The disorder averaged one-particle propagators determined by the renormalized perturbation expansion and MSR perturbation expansion are identical to the second and possibly higher order, and the two-particle propagators determined by these perturbation methods are identical at the first and possibly higher order. The one-particle propagator determined by the Edwards method is identical to the perturbation expansions at the first order, but the second-order analogue of the Edwards method has a more complex expression, which reduces to the second-order perturbation expression with additional higher-order terms. The diffusion constant and two-particle correlations are calculated from these propagators and are used to determine the effects of the random potential on the Brownian particles. Generally, the diffusion rate decreases with the disorder strength and increases with the temporal decay rate. The two competing mechanisms result in an enhancement of the diffusion constant for weak potentials with fast temporal fluctuations. The system exhibits two-particle correlations that are inherently non-Gaussian and indicate clustering behavior. The diffusion constant is also determined from a simple one-loop renormalization group calculation. In the static limit, the diffusion constant calculated by the renormalization group recovers the results of Deem and Chandler [M.W. Deem and D. Chandler, J. Stat. Phys. 76, 911 (1994)]. [References: 73]
机译:使用四种方法研究模型随机势中具有时间依赖性的布朗测试粒子的运动:重新归一化扰动,使用Martin,Siggia和Rose功能形式主义(MSR)进行扰动,针对MSR函数的Edwards变分方法以及重新归一化组具有MSR功能。由重新归一化的扰动展开和MSR扰动展开确定的无序平均单粒子传播子与第二阶和可能更高阶相同,而由这些扰动方法确定的两粒子传播子在第一阶和可能更高阶上相同。爱德华兹方法确定的单粒子传播子与一阶扰动展开相同,但爱德华兹方法的二阶类似物具有更复杂的表达式,这会降低为二阶扰动表达式,并具有更高的订单条款。从这些传播子计算出扩散常数和两粒子的相关性,并用于确定随机势对布朗粒子的影响。通常,扩散率随无序强度而减小,随时间衰减率而增大。两种竞争机制导致具有快速时间波动的弱势的扩散常数增加。该系统展现出两个粒子相关性,它们固有地是非高斯的,并指示聚类行为。扩散常数还可以通过简单的单回路重归一化组计算来确定。在静态极限中,由重归一化组计算的扩散常数恢复了Deem和Chandler的结果。 Deem和D. Chandler,J。Stat。物理76,911(1994)]。 [参考:73]

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