Richardson Jeremy O, Thoss Michael
Institut für Theoretische Physik und Interdisziplinäres Zentrum für Molekulare Materialien, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Staudtstraße 7/B2, 91058 Erlangen, Germany.
J Chem Phys. 2014 Aug 21;141(7):074106. doi: 10.1063/1.4892865.
There is currently much interest in the development of improved trajectory-based methods for the simulation of nonadiabatic processes in complex systems. An important goal for such methods is the accurate calculation of the rate constant over a wide range of electronic coupling strengths and it is often the nonadiabatic, weak-coupling limit, which being far from the Born-Oppenheimer regime, provides the greatest challenge to current methods. We show that in this limit there is an inherent sign problem impeding further development which originates from the use of the usual quantum flux correlation functions, which can be very oscillatory at short times. From linear response theory, we derive a modified flux correlation function for the calculation of nonadiabatic reaction rates, which still rigorously gives the correct result in the long-time limit regardless of electronic coupling strength, but unlike the usual formalism is not oscillatory in the weak-coupling regime. In particular, a trajectory simulation of the modified correlation function is naturally initialized in a region localized about the crossing of the potential energy surfaces. In the weak-coupling limit, a simple link can be found between the dynamics initialized from this transition-state region and an generalized quantum golden-rule transition-state theory, which is equivalent to Marcus theory in the classical harmonic limit. This new correlation function formalism thus provides a platform on which a wide variety of dynamical simulation methods can be built aiding the development of accurate nonadiabatic rate theories applicable to complex systems.
目前,人们对开发改进的基于轨迹的方法以模拟复杂系统中的非绝热过程非常感兴趣。此类方法的一个重要目标是在广泛的电子耦合强度范围内准确计算速率常数,而往往是远离玻恩 - 奥本海默体系的非绝热弱耦合极限对当前方法构成了最大挑战。我们表明,在此极限下存在一个阻碍进一步发展的固有符号问题,它源于使用通常的量子通量相关函数,该函数在短时间内可能会有非常剧烈的振荡。从线性响应理论出发,我们推导了一种用于计算非绝热反应速率的修正通量相关函数,无论电子耦合强度如何,它在长时间极限下仍能严格给出正确结果,但与通常的形式主义不同,在弱耦合区域它不会振荡。特别是,修正相关函数的轨迹模拟自然地在围绕势能面交叉点的局部区域初始化。在弱耦合极限下,可以在从这个过渡态区域初始化的动力学与广义量子黄金规则过渡态理论之间找到一个简单的联系,该理论在经典谐波极限下等同于马库斯理论。这种新的相关函数形式主义因此提供了一个平台,可以在此基础上构建各种动力学模拟方法,有助于开发适用于复杂系统的精确非绝热速率理论。