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CAN IMAGINARY INSTANTANEOUS NORMAL MODE FREQUENCIES PREDICT BARRIERS TO SELF-DIFFUSION

机译:能否以瞬时的正常模式频率预测障碍物的自扩散

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We discuss whether or not local information on the potential energy surface embodied by the distribution of unstable instantaneous normal modes can be used to predict the hopping rates and barrier heights for Zwanzig's model of self-diffusion [R. Zwanzig, J. Chem. Phys. 79, 4507 (1983)] in simple liquids, Results from a set of simulations of Lennard-Jones particles done at multiple temperatures and densities are presented. These simulations show that the theories which predict diffusive barrier heights from the distribution of imaginary frequencies are questionable. This discrepancy is due to the presence of imaginary frequency instantaneous normal modes which persist into the solid phase. Model systems are used to show that imaginary frequency instantaneous normal modes (and even those at the top of the barrier along that mode) are not necessarily indicators of diffusive barrier crossing as used in Zwanzig's model. These false barriers are shown to be the cause of all of the imaginary frequency zero-force modes in the solid as a ell as many of the imaginary frequency modes in the high-density super-cooled liquid. We therefore dispute their utility as predictors of barrier heights or hopping rates in related Liquid systems. We also show that attempts to separate the modes that are truly diffusive from those with false barriers using a frequency cutoff or local information on the potential energy surface are not successful at removing all of the non-barrier modes. (C) 1997 American Institute of Physics. [References: 29]
机译:我们讨论了是否可以使用Z瞬时的自扩散模型[R. R. S。,。,。 Zwanzig,J.Chem。物理79,4507(1983)],在简单的液体中,给出了在多个温度和密度下进行的一组Lennard-Jones粒子模拟的结果。这些模拟表明,根据虚数频率的分布预测扩散势垒高度的理论是有疑问的。这种差异是由于存在于固相中的虚频瞬时法线模式所致。模型系统用于显示虚频瞬时法向模态(甚至那些沿该模态位于障碍物顶部的频率)不一定是Zwanzig模型中使用的扩散性障碍物穿越的指标。这些错误的障碍被证明是导致固体中所有虚数频率零力模式的原因,与高密度过冷液体中的许多虚数频率模式一样。因此,我们怀疑它们在相关液体系统中作为屏障高度或跳跃率的预测指标的效用。我们还表明,尝试使用频率截止或势能面上的局部信息将真正具有扩散性的模式与具有虚假障碍的模式分离,并不能成功消除所有非障碍模式。 (C)1997美国物理研究所。 [参考:29]

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