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Comparison of molecular dynamics and moment based methods as toolsin the computation of time dependent correlation functions

机译:比较分子动力学和基于矩的方法作为计算时间相关函数的工具

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Methods, such as the continued fractions that are based on the exact moments (Taylor coefficients)provide powerful analytic techniques for calculating approximate dynamic correlation functions ofphysical properties. Owing to the practical difficulties associated with obtaining higher order exactmoments these methods have been largely eclipsed by molecular dynamics. In this paper we developthe formalism for extracting trajectory moments from a molecular dynamics trajectory and comparethe performance of the two methods. We begin by using the classical phase space analogs ofquantum wave functions to obtain matrix representations (transition matrices) of the Lie group oftime displacement operators. The group elements for small time displacements, which correspond toa step of the trajectory, are approximated by using Trotter's theorem. The method is applied to thelinear harmonic oscillator, the Morse oscillator and the Lennard-Jones potential and the resultingmoments compared to those obtained by the Taylor expansion of a truncated continued fraction. Wefind that in the case of the harmonic oscillator the results from the continued fraction are much betterthan those from molecular dynamics. In the latter two cases, while the truncated fraction performsbetter than molecular dynamics both methods produce poor quality higher order moments. However,we are able to show the criterion whereby the overall error introduced by the truncated continuedfraction is smaller than that introduced by molecular dynamics. From this work we conclude that themoment based methods produce good results, they are analytic in nature rather than numerical andshould not be rejected but can be used to complement molecular dynamics.
机译:诸如基于精确矩(泰勒系数)的连续分数之类的方法提供了强大的分析技术,可用于计算物理性质的近似动态相关函数。由于与获得高阶精确矩相关的实际困难,这些方法在很大程度上被分子动力学所掩盖。在本文中,我们开发了从分子动力学轨迹中提取轨迹矩的形式主义,并比较了这两种方法的性能。我们首先使用量子波函数的经典相空间类似物来获得时间位移算子的Lie组的矩阵表示(过渡矩阵)。通过使用Trotter定理来近似对应于轨迹步长的小时间位移的组元素。将该方法应用于线性谐波振荡器,莫尔斯振荡器和Lennard-Jones势,并将所得的矩与通过截断的连续分数的泰勒展开获得的矩进行比较。我们发现,在谐波振荡器的情况下,连续分数的结果要好于分子动力学的结果。在后两种情况下,虽然截短的部分的表现优于分子动力学,但这两种方法均产生了质量较差的高阶矩。然而,我们能够显示出这样的判据,即截断的连续分数引入的总误差小于分子动力学引入的总误差。从这项工作中,我们得出结论,基于矩的方法产生了良好的结果,它们本质上是分析性的,而不是数值的,不应被拒绝,但可以用于补充分子动力学。

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