Jang Seogjoo J, Min Byeong Ki, Rhee Young Min
Department of Chemistry and Biochemistry, Queens College, City University of New York, 65-30 Kissena Boulevard, Queens, New York, New York 11367, United States.
Ph.D. Programs in Chemistry and Physics, Graduate Center of the City University of New York, New York, New York 10016, United States.
J Chem Theory Comput. 2025 Feb 25;21(4):1850-1864. doi: 10.1021/acs.jctc.4c00590. Epub 2025 Feb 13.
Starting from a general molecular Hamiltonian expressed in the basis of adiabatic electronic and nuclear position states, where a compact and complete expression for the nonadiabatic derivative coupling (NDC) Hamiltonian term is obtained, we provide a general analysis of the Fermi's golden rule (FGR) rate expression for nonadiabatic transitions between adiabatic states. We then consider a quasi-adiabatic approximation that uses crude adiabatic states and NDC couplings, both evaluated at the minimum potential energy configuration of the initial adiabatic state, for the definition of the zeroth and first-order terms of the Hamiltonian. Although the application of this approximation is rather limited, it allows deriving a general FGR rate expression without further approximation while accounting for non-Condon contribution to the FGR rate arising from momentum operators of NDC terms and its coupling with vibronic displacements. For a generic and widely used model where all nuclear degrees of freedom and environmental effects are represented as linearly coupled harmonic oscillators, we derive a closed-form FGR rate expression that requires only Fourier transform. The resulting rate expression includes quadratic contributions of NDC terms and their couplings to Franck-Condon modes, which require evaluation of two additional bath spectral densities in addition to the conventional one that appears in a typical FGR rate theory based on the Condon approximation. Model calculations for the case where nuclear vibrations consist of both a sharp high-frequency mode and an Ohmic bath spectral density illustrate new features and implications of the rate expression. We then apply our theoretical expression to the nonradiative decay from the first excited singlet state of azulene, which illustrates the utility and implications of our theoretical results.
从以绝热电子和核位置态为基表示的一般分子哈密顿量出发,在此基础上获得了非绝热导数耦合(NDC)哈密顿量项的紧凑且完整的表达式,我们对绝热态之间非绝热跃迁的费米黄金规则(FGR)速率表达式进行了一般性分析。然后,我们考虑一种准绝热近似,该近似使用在初始绝热态的最小势能构型处评估的粗略绝热态和NDC耦合来定义哈密顿量的零阶和一阶项。尽管这种近似的应用相当有限,但它允许在不做进一步近似的情况下推导一般的FGR速率表达式,同时考虑到NDC项的动量算符及其与振转位移的耦合对FGR速率产生的非康登贡献。对于一个通用且广泛使用的模型,其中所有核自由度和环境效应都表示为线性耦合的谐振子,我们推导了一个仅需傅里叶变换的封闭形式的FGR速率表达式。所得的速率表达式包括NDC项及其与弗兰克 - 康登模式耦合的二次贡献,这除了在基于康登近似的典型FGR速率理论中出现的常规浴谱密度外,还需要评估另外两个浴谱密度。核振动由一个尖锐的高频模式和一个欧姆浴谱密度组成的情况下的模型计算说明了该速率表达式的新特征和含义。然后,我们将我们的理论表达式应用于薁的第一激发单重态的非辐射衰变,这说明了我们理论结果的实用性和含义。