Department of Physics, Chemistry and Pharmacy, University of Southern Denmark, Odense, Denmark.
J Chem Phys. 2013 Nov 14;139(18):184308. doi: 10.1063/1.4826533.
Charge transfer excitations can be described within Time-Dependent Density Functional Theory (TD-DFT), not only by means of the Coulomb Attenuated Method (CAM) but also with a combination of wave function theory and TD-DFT based on range separation. The latter approach enables a rigorous formulation of multi-determinantal TD-DFT schemes where excitation classes, which are absent in conventional TD-DFT spectra (like for example double excitations), can be addressed. This paper investigates the combination of both the long-range Multi-Configuration Self-Consistent Field (MCSCF) and Second Order Polarization Propagator Approximation (SOPPA) ansätze with a short-range DFT (srDFT) description. We find that the combinations of SOPPA or MCSCF with TD-DFT yield better results than could be expected from the pure wave function schemes. For the Time-Dependent MCSCF short-range DFT ansatz (TD-MC-srDFT) excitation energies calculated over a larger benchmark set of molecules with predominantly single reference character yield good agreement with their reference values, and are in general comparable to the CAM-B3LYP functional. The SOPPA-srDFT scheme is tested for a subset of molecules used for benchmarking TD-MC-srDFT and performs slightly better against the reference data for this small subset. Beyond the proof-of-principle calculations comprising the first part of this contribution, we additionally studied the low-lying singlet excited states (S1 and S2) of the retinal chromophore. The chromophore displays multireference character in the ground state and both excited states exhibit considerable double excitation character, which in turn cannot be described within standard TD-DFT, due to the adiabatic approximation. However, a TD-MC-srDFT approach can account for the multireference character, and excitation energies are obtained with accuracy comparable to CASPT2, although using a much smaller active space.
电荷转移激发可以在含时密度泛函理论(TD-DFT)中描述,不仅可以使用库仑衰减方法(CAM),还可以结合波函数理论和基于范围分离的 TD-DFT。后一种方法可以严格制定多行列式 TD-DFT 方案,其中可以解决常规 TD-DFT 光谱中不存在的激发类(例如双激发)。本文研究了长程多组态自洽场(MCSCF)和二阶极化传播子逼近(SOPPA)方法与短程 DFT(srDFT)描述的组合。我们发现,SOPPA 或 MCSCF 与 TD-DFT 的组合产生的结果优于纯波函数方案所预期的结果。对于时间相关的 MCSCF 短程 DFT 方法(TD-MC-srDFT),在具有主要单参考特征的更大分子基准集上计算的激发能与它们的参考值吻合得很好,并且通常与 CAM-B3LYP 函数相当。SOPPA-srDFT 方案在用于基准 TD-MC-srDFT 的分子子集上进行了测试,并且针对该小子集的参考数据,它的性能略好。除了包含本研究贡献的第一部分的原理证明计算之外,我们还研究了视黄醛发色团的低能单重激发态(S1 和 S2)。发色团在基态中具有多参考特征,两个激发态都表现出相当大的双激发特征,由于绝热近似,这在标准 TD-DFT 中无法描述。然而,TD-MC-srDFT 方法可以解释多参考特征,并且可以获得与 CASPT2 相当的精度的激发能,尽管使用的活性空间要小得多。