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首页> 外文期刊>The Journal of Chemical Physics >PHASE SPACE DISTRIBUTION FUNCTION FORMULATION OF THE METHOD OF REACTIVE FLUX - MEMORY FRICTION
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PHASE SPACE DISTRIBUTION FUNCTION FORMULATION OF THE METHOD OF REACTIVE FLUX - MEMORY FRICTION

机译:反应堆记忆摩擦法的相空间分布函数公式。

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The Grote-Hynes transmission coefficient for the rate of barrier crossing in the presence of memory friction is rederived here using the method of reactive flux. By combining the methodology developed in an earlier paper [D. J. Tanner and D. Kohen, J. Chem. Phys. 100, 4932 (1994)] with the non-Markovian Fokker-Planck equation of Adelman [S. Adelman, J. Chem. Phys. 64, 124 (1976)] we are able to obtain not only the asymptotic rate constant but the behavior of the rate constant at all times. The salient features of the time dependent rate constant, k(t), are interpreted in terms of the time evolution of the representative distribution functions that originate at the top of the barrier. The short time behavior of the rate constant is very different in the dynamic and static limits, with close analogies to the stochastic theory of spectral line shapes. The dependence of the ''plateau time''-the time for the rate constant to reach its steady state value-on the memory kernel is explored numerically, and analytical expressions are obtained in the dynamic and static limits. (C) 1995 American Institute of Physics. [References: 27]
机译:在此,使用电抗通量的方法重新求出了存在记忆摩擦时屏障越过速率的Grote-Hynes传输系数。通过结合早期论文中开发的方法[D。 J. Tanner和D. Kohen,J。Chem。物理100,4932(1994)],其中包含Adelman的非马尔可夫Fokker-Planck方程[S.阿德尔曼,化学杂志。物理64,124(1976)],我们不仅可以获得渐近速率常数,而且还可以始终获得速率常数的行为。与时间相关的速率常数k(t)的显着特征是根据代表分布函数的时间演化来解释的,该分布函数起源于屏障的顶部。速率常数的短时行为在动态和静态极限上有很大不同,与频谱线形状的随机理论非常相似。通过数值研究“平稳时间”(速率常数达到其稳态值的时间)对内存内核的依赖性,并在动态和静态极限下获得解析表达式。 (C)1995年美国物理研究所。 [参考:27]

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