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A simplified relativistic time-dependent density-functional theory formalism for the calculations of excitation energies including spin-orbit coupling effect

机译:简化的相对论时变密度函数理论形式,用于计算包括自旋轨道耦合效应在内的激发能

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In the present work we have proposed an approximate time-dependent density-functional theory (TDDFT) formalism to deal with the influence of spin-orbit coupling effect on the excitation energies for closed-shell systems. In this formalism scalar relativistic TDDFT calculations are first performed to determine the lowest single-group excited states and the spin-orbit coupling operator is applied to these single-group excited states to obtain the excitation energies with spin-orbit coupling effects included. The computational effort of the present method is much smaller than that of the two-component TDDFT formalism and this method can be applied to medium-size systems containing heavy elements. The compositions of the double-group excited states in terms of single-group singlet and triplet excited states are obtained automatically from the calculations. The calculated excitation energies based on the present formalism show that this formalism affords reasonable excitation energies for transitions not involving 5p and 6p orbitals. For transitions involving 5p orbitals, one can still obtain acceptable results for excitations with a small truncation error, while the formalism will fail for transitions involving 6p orbitals, especially 6p(1/2) spinors. (c) 2005 American Institute of Physics.
机译:在当前的工作中,我们提出了一种近似于时间的密度泛函理论(TDDFT)形式,以处理自旋轨道耦合效应对闭壳系统的激发能的影响。在这种形式主义中,首先进行标量相对论TDDFT计算以确定最低的单组激发态,并将自旋轨道耦合算子应用于这些单组激发态以获得具有自旋轨道耦合效应的激发能。本方法的计算工作量比两分量TDDFT形式主义的计算工作量小得多,并且该方法可以应用于包含重元素的中型系统。从计算中自动获得根据单组单重态和三重态激发态的双组激发态的组成。基于当前形式主义计算的激发能表明,该形式主义为不涉及5p和6p轨道的跃迁提供了合理的激发能。对于涉及5p轨道的跃迁,对于截断误差很小的激发,人们仍然可以获得可接受的结果,而对于涉及6p轨道,尤其是6p(1/2)旋子的跃迁,形式主义将失败。 (c)2005年美国物理研究所。

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