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单粒子水平上的守恒动力学。

Particle-conserving dynamics on the single-particle level.

机构信息

Institute for Theoretical Physics I, Friedrich-Alexander University Erlangen-Nürnberg Theoretical Physics II, University of Bayreuth, Universitätsstraße 30, 95447 Bayreuth, Germany.

Department of Physics, University of Fribourg, CH-1700 Fribourg, Switzerland.

出版信息

Phys Rev E. 2019 Jan;99(1-1):012605. doi: 10.1103/PhysRevE.99.012605.

Abstract

We generalize the particle-conserving dynamics method of de las Heras et al. [J. Phys.: Condens. Matter 28, 244024 (2016)JCOMEL0953-898410.1088/0953-8984/28/24/244024] to binary mixtures and apply this to hard rods in one dimension. Considering the case of one species consisting of only one particle enables us to address the tagged-particle dynamics. The time-evolution of the species-labeled density profiles is compared to exact Brownian dynamics and (grand-canonical) dynamical density functional theory. The particle-conserving dynamics yields improved results over the dynamical density functional theory and well reproduces the simulation data at short and intermediate times. However, the neglect of a strict particle order (due to the fundamental statistical assumption of ergodicity) leads to errors at long times for our one-dimensional setup. The isolated study of that error makes clear the fundamental limitations of (adiabatic) density-based theoretical approaches when applied to systems of any dimension for which particle caging is a dominant physical mechanism.

摘要

我们将 de las Heras 等人的粒子守恒动力学方法[J. Phys.: Condens. Matter 28, 244024 (2016)JCOMEL0953-898410.1088/0953-8984/28/24/244024]推广到二元混合物,并将其应用于一维硬棒。考虑到只有一种粒子的一种物质的情况,使我们能够解决标记粒子的动力学问题。与确切的布朗动力学和(巨正则)动态密度泛函理论相比,研究了物种标记密度分布的时间演化。在短时间和中间时间内,粒子守恒动力学比动态密度泛函理论产生了更好的结果,并很好地再现了模拟数据。然而,由于遍历性的基本统计假设,对严格的粒子顺序的忽略(due to the fundamental statistical assumption of ergodicity)导致我们在一维设置中长时间出现误差。对该误差的单独研究清楚地表明了(绝热)基于密度的理论方法在任何维度的系统中应用时的基本局限性,对于这些系统,粒子笼闭是主要的物理机制。

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