Biophysics Program, Stanford University, Stanford, California 94305, United States.
Department of Chemistry and The PULSE Institute, Stanford University, Stanford, California 94305, United States.
J Chem Theory Comput. 2020 Sep 8;16(9):5499-5511. doi: 10.1021/acs.jctc.0c00644. Epub 2020 Aug 20.
The study of photoinduced dynamics in chemical systems necessitates accurate and computationally efficient electronic structure methods, especially as the systems of interest grow larger. The linear response hole-hole Tamm-Dancoff approximated (-TDA) density functional theory method was recently proposed to satisfy such demands. The -electron electronic states are obtained by means of double annihilations on a doubly anionic ( + 2)-electron reference state, allowing for the ground and excited states to be formed on the same footing and thus enabling the correct description of conical intersections. Dynamic electron correlation effects are incorporated by means of the exchange-correlation functional. The accuracy afforded by the simultaneous treatment of static and dynamic correlation in addition to the relatively low computational cost, comparable to that of time-dependent density functional theory (TDDFT), makes it a promising electronic structure method for on-the-fly generation of potential energy surfaces in nonadiabatic dynamics simulations of photochemical systems, particularly those for which the nπ* and ππ* electronic excitations are most relevant. Here, we apply the -TDA method to nonadiabatic dynamics simulations of prototypical photochemical processes. First, we demonstrate the ability of -TDA to adequately describe conical intersection geometries. We next examine its ability to describe the ultrafast excited state dynamics of photoexcited ethylene through an multiple spawning (AIMS) dynamics simulation. Finally, we present an alternative variant of the -TDA method, which uses orbitals from a fractional occupation number Kohn-Sham (FON-KS) calculation applied to an ensemble with -electrons. The resulting method is termed floating occupation molecular orbital -TDA (FOMO--TDA). This scheme allows us to combine -TDA with global hybrid functionals and allows us to avoid unbound valence orbitals that may result from an ( + 2)-electron self-consistent field (SCF) procedure. FOMO--TDA-BHLYP faithfully reproduces the nonadiabatic dynamics of -azobenzene (TAB) and is used to characterize the excited state decay pathways from the first (nπ*) excited state.
化学体系中光诱导动力学的研究需要准确且计算效率高的电子结构方法,特别是当感兴趣的体系变得更大时。最近提出了线性响应空穴-空穴 Tamm-Dancoff 近似(-TDA)密度泛函理论方法来满足这些需求。-电子电子态是通过在双阴离子(+2)-电子参考态上进行双重湮灭获得的,允许在相同的基础上形成基态和激发态,从而能够正确描述锥形交叉。通过交换相关泛函纳入动态电子相关效应。由于同时处理静态和动态相关以及相对较低的计算成本(与时间依赖密度泛函理论(TDDFT)相当)而提供的准确性,使其成为在非绝热动力学模拟中生成光化学体系势能面的有前途的电子结构方法,特别是对于那些最相关的 nπ和ππ电子激发。在这里,我们将-TDA 方法应用于典型光化学反应过程的非绝热动力学模拟。首先,我们证明了-TDA 能够充分描述锥形交叉几何形状的能力。接下来,我们通过多次产生(AIMS)动力学模拟检查其描述光激发乙烯超快激发态动力学的能力。最后,我们提出了-TDA 方法的另一种变体,该方法使用分数占据数 Kohn-Sham(FON-KS)计算的轨道应用于具有-电子的集合。所得方法称为浮动占据分子轨道-TDA(FOMO--TDA)。该方案允许我们将-TDA 与全局杂化泛函结合使用,并避免可能由(+2)-电子自洽场(SCF)过程引起的未结合价轨道。FOMO--TDA-BHLYP 忠实地再现了 -偶氮苯(TAB)的非绝热动力学,并用于表征从第一(nπ*)激发态的激发态衰减途径。