Department of Chemistry, Stanford University, Stanford, California 94305, USA.
J Chem Phys. 2013 Jul 7;139(1):014104. doi: 10.1063/1.4812355.
The quantum-classical Liouville equation offers a rigorous approach to nonadiabatic quantum dynamics based on surface hopping type trajectories. However, in practice the applicability of this approach has been limited to short times owing to unfavorable numerical scaling. In this paper we show that this problem can be alleviated by combining it with a formally exact generalized quantum master equation treatment. This allows dramatic improvements in the efficiency of the approach in nonadiabatic regimes, making it computationally tractable to treat the quantum dynamics of complex systems for long times. We demonstrate our approach by applying it to a model of condensed phase charge transfer where our method is shown to be numerically exact in regimes where fewest-switches surface hopping and mean field approaches fail to obtain either the correct rates or long-time populations.
量子经典刘维尔方程为非绝热量子动力学提供了一种基于表面跳跃型轨迹的严格方法。然而,由于数值比例的不利影响,这种方法在实践中的应用一直局限于短时间。在本文中,我们表明,通过将其与形式上精确的广义量子主方程处理相结合,可以缓解这个问题。这使得在非绝热区域中该方法的效率显著提高,从而使得长时间处理复杂系统的量子动力学在计算上变得可行。我们通过将其应用于凝聚相电荷转移的模型来证明我们的方法,在那里,我们的方法在少数切换表面跳跃和平均场方法无法获得正确的速率或长时间群体的区域中被证明是数值精确的。