Nascimento Daniel R, Biasin Elisa, Poulter Benjamin I, Khalil Munira, Sokaras Dimosthenis, Govind Niranjan
Physical and Computational Sciences Directorate, Pacific Northwest National Laboratory, Richland, Washington 99352, United States.
Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, United States.
J Chem Theory Comput. 2021 May 11;17(5):3031-3038. doi: 10.1021/acs.jctc.1c00144. Epub 2021 Apr 28.
We present a time-dependent density functional theory (TDDFT) approach to compute the light-matter couplings between two different manifolds of excited states relative to a common ground state in the context of 4d transition metal systems. These quantities are the necessary ingredients to solve the Kramers-Heisenberg (KH) equation for resonant inelastic X-ray scattering (RIXS) and several other types of two-photon spectroscopies. The procedure is based on the pseudo-wavefunction approach, where the solutions of a TDDFT calculation can be used to construct excited-state wavefunctions, and on the restricted energy window approach, where a manifold of excited states can be rigorously defined based on the energies of the occupied molecular orbitals involved in the excitation process. Thus, the present approach bypasses the need to solve the costly TDDFT quadratic-response equations. We illustrate the applicability of the method to 4d transition metal molecular complexes by calculating the 2p4d RIXS maps of three representative ruthenium complexes and comparing them to experimental results. The method can capture all the experimental features in all three complexes to allow the assignment of the experimental peaks, with relative energies correct to within ∼0.6 eV at the cost of two independent TDDFT calculations.
我们提出了一种含时密度泛函理论(TDDFT)方法,用于在4d过渡金属体系的背景下,计算相对于共同基态的两个不同激发态流形之间的光与物质耦合。这些量是求解用于共振非弹性X射线散射(RIXS)和其他几种双光子光谱学的克莱默斯 - 海森堡(KH)方程的必要要素。该过程基于伪波函数方法(其中TDDFT计算的解可用于构建激发态波函数)和受限能量窗口方法(其中可基于激发过程中涉及的占据分子轨道的能量严格定义激发态流形)。因此,本方法无需求解代价高昂的TDDFT二次响应方程。我们通过计算三种代表性钌配合物的2p4d RIXS图谱并将其与实验结果进行比较,说明了该方法对4d过渡金属分子配合物的适用性。该方法能够捕捉所有三种配合物中的所有实验特征,以便对实验峰进行归属,相对能量的误差在约0.6 eV以内,代价是进行两次独立的TDDFT计算。