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Normal modes and frequencies from covariances in molecular dynamics or monte carlo simulations

机译:分子动力学或蒙特卡洛模拟中协方差的正常模式和频率

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We propose a simple method to obtain normal modes (NMs) and their characteristic frequencies from molecular dynamics or Monte Carlo simulations at any temperature.The resulting NM are consistent with the vibrational density of states (DOS) (every feature of the DOS can be attributed to one or few NMs).At low temperatures they coincide with the ones obtained from the Hessian matrix.We define the NMs (rho_i) by imposing the condition that their velocities be uncorrelated to each other: denotes time averate and delta_(ij) is Kroneker's delta.With this definition the modes are the eigenvectors of the matrix K_(ij)~(upsilon)=1/2[i,j=1,3 N(N being the number of atoms);m are masses and v atomic velocities].The eigenvalues of K_(ij)~(upsilon),lambda_i~(upsilon),represent the kinetic energy in each NM.The ratio between the eigenvalues (lambda_i~(upsilon)) and those obtained using positions (lambda_i~r),accelerations (lambda_i~a) in K_(ij)~v instead of velocities are a very good approximation to the mode frequencies:2piupsilon_iapprox(lambda_i~v/lambda_i~x)~(1/2)approx(lambda_i~a/lambda_i~x~(1/4)).We demonstrate the new method using with two cases:an isolated water molecular and a crystalline polymer.
机译:我们提出了一种简单的方法来从任何温度下的分子动力学或蒙特卡洛模拟中获得正态模(NMs)及其特征频率,所得的NM与状态振动密度(DOS)一致(DOS的所有特征都可以归因于DOS)到一个或几个NMs)。在低温下,它们与从Hessian矩阵获得的温度重合。我们通过施加条件使它们的速度彼此不相关来定义NMs(rho_i):表示时间平均,而delta_(ij)是克朗克的增量。在此定义下,众数是矩阵K_(ij)〜(upsilon)= 1/2 [i,j = 1,3 N(N是原子数); m是质量和v的原子速度] .K_(ij)〜(upsilon),lambda_i〜(upsilon)的特征值,代表每个NM的动能。特征值(lambda_i〜(upsilon))与使用位置(lambda_i〜r)获得的特征值之比,加速度(lambda_i〜a)用K_(ij)〜v代替速度是模式频率的一个很好的近似值:2piupsilon_iapprox(lambda_i〜v / lambda_i〜x)〜(1/2)approx(lambda_i〜a / lambda_i〜x〜(1/4) ))。我们用两种情况演示了新方法:分离的水分子和结晶聚合物。

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