Manian Anjay, Shaw Robert A, Lyskov Igor, Russo Salvy P
ARC Centre of Excellence in Exciton Science, School of Science, RMIT University, Melbourne, 3000, Australia.
Department of Chemistry, University of Sheffield, Sheffield S3 7HF, United Kingdom.
J Chem Theory Comput. 2022 Mar 8;18(3):1838-1848. doi: 10.1021/acs.jctc.2c00070. Epub 2022 Feb 23.
Ab initio treatments of interexcited state internal conversion (IC) are more often than not missing from exciton dynamic descriptions, because of their inherent complexity. Here, we define "interexcited state IC" as a same-spin nonradiative transition between states and , where ≠ ≠ 0. Competing directly with multiexciton processes such as singlet fission or triplet photoupconversion, inclusion of this mechanism in the narrative of molecular photophysics would allow for strategic synthesis of chromophores for more efficient photon-harvesting applications. Herein, we present a robust formalism which can model these rates using density functional theory (DFT)-based methods within the Franck-Condon and Herzberg-Teller regime. Using an unsubstituted diketo-pyrrolopyrrole (DPP) core as a case study, we illustrate the exciton dynamics along the first four excited states for both singlet and triplet manifolds, showing ultrafast same-spin transfer mechanisms due to all excited states, excluding the first triplet level, being in close energetic proximity (within 0.8 eV of each other). The resulting electron same-spin rates outcompete the electron spin-flipping intersystem crossing (ISC) rates, with excitons firmly obeying Kasha's rule as they cascade down from the high-lying excited states toward the lower states. Furthermore, we calculated that only the first singlet excited state displayed a reasonable probability of triplet exciton generation, of ∼40%, with a near-zero chance of the exciton reverting to the singlet manifold once the electron-hole pair are of parallel spin.
由于其固有的复杂性,激子动力学描述中往往缺少对激发态间内转换(IC)的从头算处理。在这里,我们将“激发态间IC”定义为态(i)和态(j)之间的同自旋非辐射跃迁,其中(i\neq j\neq0)。这种机制与诸如单线态裂变或三线态光上转换等多激子过程直接竞争,将其纳入分子光物理的描述中,有助于为更高效的光子捕获应用进行发色团的策略性合成。在此,我们提出一种稳健的形式体系,它可以在弗兰克 - 康登和赫兹伯格 - 泰勒区域内,使用基于密度泛函理论(DFT)的方法对这些速率进行建模。以未取代的二酮吡咯并吡咯(DPP)核为例,我们说明了单线态和三线态多重态中前四个激发态的激子动力学,表明除了第一个三线态能级外,所有激发态由于能量接近(彼此相差在0.8 eV以内)而呈现超快的同自旋转移机制。由此产生的电子同自旋速率超过了电子自旋翻转系间窜越(ISC)速率,激子从高能激发态向低能态级联时严格遵循卡沙规则。此外,我们计算得出只有第一个单线态激发态显示出约40%的三线态激子产生的合理概率,并且一旦电子 - 空穴对具有平行自旋,激子回到单线态多重态的概率几乎为零。