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作 者:严运安[1,2]
机构地区:[1]贵州师范学院,贵州省纳米材料模拟与计算重点实验室,贵州550018 [2]北京计算科学研究中心,北京100094
出 处:《Chinese Journal of Chemical Physics》2017年第3期277-286,I0001,共11页化学物理学报(英文)
基 金:This work is supported by the National Natural Science Foundation of China (No.21373064), the Program for Innovative Research Team of Guizhou Province (No.QKTD[2014]4021), and the Natural Sci- entific Foundation from Guizhou Provincial Department of Education (No.ZDXK[2014]IS). All the calculations were performed at Guizhou Provincial High- Performance Computing Center of Condensed Mate- rials and Molecular Simulation in Guizhou Education University.
摘 要:A wide range of quantum systems are time-invariant and the corresponding dynamics is dic- tated by linear differential equations with constant coefficients. Although simple in math- ematical concept, the integration of these equations is usually complicated in practice for complex systems, where both the computational time and the memory storage become limit- ing factors. For this reason, low-storage Runge-Kutta methods become increasingly popular for the time integration. This work suggests a series of s-stage sth-order explicit Runge- Kutta methods specific for autonomous linear equations, which only requires two times of the memory storage for the state vector. We also introduce a 13-stage eighth-order scheme for autonomous linear equations, which has optimized stability region and is reduced to a fifth-order method for general equations. These methods exhibit significant performance improvements over the previous general-purpose low-stage schemes. As an example, we ap- ply the integrator to simulate the non-Markovian exciton dynamics in a 15-site linear chain consisting of perylene-bisimide derivatives.
关 键 词:Low-storage Runge-Kutta Autonomous linear differential equation Time-dependent dynamics Time-invariant Hamiltonian
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