Kimura Akihiro
Department of Physics, Graduate School of Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan.
J Chem Phys. 2024 Sep 28;161(12). doi: 10.1063/5.0227158.
According to many reports, the various structures of photosynthetic light-harvesting/reaction-center complexes and their molecular-dynamics simulations necessitate a numerically efficient and quality-conserved theory of excitation energy transfer and exciton relaxation in large pigment systems. Although exciton dynamics depend on various parameters, such as exciton coupling strength, exciton-phonon coupling, site energy values for each pigment, and temperature, classifying the transition mechanism for any Hamiltonian into perturbatively delocalized or localized theories is challenging. In this study, perturbative quantum master equations of a reduced density matrix for any orthogonal transformation similar to the coherent modified Redfield theory are derived. Our approach qualitatively conserves the dynamics of relevant perturbative approximations in each limiting case. As an application, any orthogonal transformation of a relevant system is optimized using the average of the square of interactions between orthogonal state transitions. The numerical results for two pigment systems are compared with the limiting formalisms of the modified Redfield and Förster theory.
根据许多报道,光合光捕获/反应中心复合物的各种结构及其分子动力学模拟需要一种在数值上高效且能保持质量的理论,用于描述大色素系统中的激发能转移和激子弛豫。尽管激子动力学取决于各种参数,如激子耦合强度、激子 - 声子耦合、每种色素的位点能量值以及温度,但将任何哈密顿量的跃迁机制分类为微扰离域或局域理论都具有挑战性。在本研究中,我们推导了与相干修正的雷德菲尔德理论类似的、针对任何正交变换的约化密度矩阵的微扰量子主方程。我们的方法在每个极限情况下定性地保留了相关微扰近似的动力学。作为应用,使用正交态跃迁之间相互作用平方的平均值对相关系统的任何正交变换进行优化。将两个色素系统的数值结果与修正的雷德菲尔德理论和福斯特理论的极限形式进行了比较。