Department of Chemistry, University of Cambridge, Cambridge CB2 1EW, United Kingdom.
J Chem Phys. 2010 Dec 28;133(24):244105. doi: 10.1063/1.3507878.
We present a plane wave basis set implementation for the calculation of electronic coupling matrix elements of electron transfer reactions within the framework of constrained density functional theory (CDFT). Following the work of Wu and Van Voorhis [J. Chem. Phys. 125, 164105 (2006)], the diabatic wavefunctions are approximated by the Kohn-Sham determinants obtained from CDFT calculations, and the coupling matrix element calculated by an efficient integration scheme. Our results for intermolecular electron transfer in small systems agree very well with high-level ab initio calculations based on generalized Mulliken-Hush theory, and with previous local basis set CDFT calculations. The effect of thermal fluctuations on the coupling matrix element is demonstrated for intramolecular electron transfer in the tetrathiafulvalene-diquinone (Q-TTF-Q(-)) anion. Sampling the electronic coupling along density functional based molecular dynamics trajectories, we find that thermal fluctuations, in particular the slow bending motion of the molecule, can lead to changes in the instantaneous electron transfer rate by more than an order of magnitude. The thermal average, (<|H(ab)|(2)>)(1/2)=6.7 mH, is significantly higher than the value obtained for the minimum energy structure, |H(ab)|=3.8 mH. While CDFT in combination with generalized gradient approximation (GGA) functionals describes the intermolecular electron transfer in the studied systems well, exact exchange is required for Q-TTF-Q(-) in order to obtain coupling matrix elements in agreement with experiment (3.9 mH). The implementation presented opens up the possibility to compute electronic coupling matrix elements for extended systems where donor, acceptor, and the environment are treated at the quantum mechanical (QM) level.
我们提出了一种平面波基组方法,用于在约束密度泛函理论(CDFT)框架内计算电子转移反应的电子耦合矩阵元。继 Wu 和 Van Voorhis 的工作[J. Chem. Phys. 125, 164105 (2006)]之后,非绝热波函数由 CDFT 计算得到的 Kohn-Sham 行列式近似,并且通过有效的积分方案计算耦合矩阵元。我们在小体系中对分子间电子转移的结果与基于广义 Mulliken-Hush 理论的高精度从头算非常吻合,并且与以前的局部基组 CDFT 计算结果一致。对于四硫富瓦烯-二醌(Q-TTF-Q(-))阴离子中的分子内电子转移,我们展示了热涨落对耦合矩阵元的影响。沿着基于密度泛函的分子动力学轨迹对电子耦合进行采样,我们发现热涨落,特别是分子的缓慢弯曲运动,可以导致瞬时电子转移率的变化超过一个数量级。热平均值((<|H(ab)|(2)>)(1/2)=6.7 mH)明显高于最小能量结构(|H(ab)|=3.8 mH)的结果。虽然 CDFT 与广义梯度近似(GGA)泛函相结合可以很好地描述所研究体系中的分子间电子转移,但为了获得与实验相符的耦合矩阵元(3.9 mH),需要对 Q-TTF-Q(-)进行精确交换。所提出的实现方法为扩展系统中电子耦合矩阵元的计算开辟了可能性,其中供体、受体和环境都在量子力学(QM)水平上进行处理。