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苯二聚体的电子态:简单中的复杂性。

Electronic states of the benzene dimer: a simple case of complexity.

机构信息

Department of Chemistry, University of Southern California, Los Angeles, California 90089-0482, USA.

出版信息

J Phys Chem A. 2012 Jan 12;116(1):653-62. doi: 10.1021/jp209190e. Epub 2011 Dec 9.

Abstract

Electronic structure calculations of the excited states of the benzene dimer using equation-of-motion coupled-cluster method are reported. The calculations reveal large density of electronic states, including multiple valence, Rydberg, and mixed Rydberg-valence states. The calculations of the oscillator strengths for the transitions between the excimer state (i.e., the lowest excited state of the dimer, 1(1)B(1g)) and other excited states allowed us to identify the target state responsible for the excimer absorption as the E(1u) state of a mixed Rydberg-valence character at 3.04 eV above the excimer (1(1)B(1g)). Although at D(6h) the 1(1)B(1g) → E(1u) transition is symmetry-forbidden, small geometric displacements (to D(2h)) that have a negligible effect on the excitation energy split this degenerate state into the dark (4B(3u)) and bright (4B(2u)) components (oscillator strength of 0.3 au). The excitation energy for this transition depends strongly on the dimer structure, which explains the broad character of the experimentally observed excimer absorption spectrum.

摘要

使用运动方程耦合簇方法对苯二聚体的激发态的电子结构进行了计算。计算揭示了大量的电子态,包括多个价态、里德堡态和混合里德堡-价态。对激子态(即二聚体的最低激发态,1(1)B(1g))与其他允许的激发态之间跃迁的振子强度的计算使我们能够确定负责激子吸收的目标态为混合里德堡-价态的 E(1u)态,其位于激子上方 3.04 eV。尽管在 D(6h)点,1(1)B(1g)→E(1u)跃迁是对称禁阻的,但小的几何位移(至 D(2h))对激发能的分裂影响很小,从而将这个简并态分裂为暗(4B(3u))和亮(4B(2u))分量(振子强度为 0.3 au)。这个跃迁的激发能强烈依赖于二聚体结构,这解释了实验观测到的激子吸收光谱的宽特征。

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