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Monte Carlo Wavefunction Approach to Singlet Fission Dynamics of Molecular Aggregates

机译:蒙特卡洛波函数法研究分子聚集体的单重态裂变动力学

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摘要

We have developed a Monte Carlo wavefunction (MCWF) approach to the singlet fission (SF) dynamics of linear aggregate models composed of monomers with weak diradical character. As an example, the SF dynamics for a pentacene dimer model is investigated by considering the intermolecular electronic coupling and the vibronic coupling. By comparing with the results by the quantum master equation (QME) approach, we clarify the dependences of the MCWF results on the time step (Δt) and the number of MC trajectories (MC). The SF dynamics by the MCWF approach is found to quantitatively (within an error of 0.02% for SF rate and of 0.005% for double-triplet (TT) yield) reproduce that by the QME approach when using a sufficiently small Δt (~0.03 fs) and a sufficiently large MC (~105). The computational time (treq) in the MCWF approach also exhibits dramatic reduction with increasing the size of aggregates (N-mers) as compared to that in the QME approach, e.g., ~34 times faster at the 20-mer, and the size-dependence of treq shows significant reduction from N5.15 (QME) to N3.09 (MCWF). These results demonstrate the promising high performance of the MCWF approach to the SF dynamics in extended multiradical molecular aggregates including a large number of quantum dissipation, e.g., vibronic coupling, modes.
机译:我们已经开发了一种蒙特卡罗波函数(MCWF)方法,用于由具有弱双自由基特性的单体组成的线性聚集体模型的单线裂变(SF)动力学。例如,并五苯二聚体模型的SF动力学通过考虑分子间电子耦合和振动耦合来研究。通过与量子主方程(QME)方法的结果进行比较,我们阐明了MCWF结果对时间步长(Δt)和MC轨迹数(MC)的依赖性。当使用足够小的Δt(〜0.03 fs)时,发现MCWF方法的SF动力学在定量上(SF率的误差为0.02%,双三联体(TT)产率的误差为0.005%)与QME方法相同。 )和足够大的MC(〜10 5 )。与QME方法相比,MCWF方法的计算时间(treq)随聚集体(N-mers)尺寸的增加而显着减少,例如20 mer时约34倍,尺寸- treq依赖性从N 5.15 (QME)显着降低到N 3.09 (MCWF)。这些结果证明了MCWF方法在扩展的多自由基分子聚集体中的SF动力学方面有希望的高性能,包括大量的量子耗散(例如,振动耦合)模式。

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