Institute of Theoretical and Computational Chemistry, Heinrich-Heine-Universität Düsseldorf, Universitätsstr. 1, 40225 Düsseldorf, Germany.
Chemphyschem. 2011 Jul 11;12(10):1872-9. doi: 10.1002/cphc.201001068. Epub 2011 Apr 6.
Herein, the low-lying electronic states of various isomers and rotamers of 1,6-diphenyl-1,3,5-hexatriene (DPH) are studied by a combination of density functional theory and multireference configuration interaction. Starting from the all-trans nuclear arrangement, trans-cis isomerization pathways in the electronic ground state and in the first excited triplet state were determined. Further, spin-orbit coupling calculations were carried out at selected points where singlet-triplet energy gaps are small. The calculations reveal that the primarily excited, optically bright 1(1)B(u) state undergoes a curve crossing with the optically dark multiconfigurational 2(1)A(g) state upon geometry relaxation in the excited state. The strong vibronic coupling of the two singlets in the neighborhood of the conical intersection provides a conclusive explanation for the experimentally observed fast equilibration of the states and the appearance of delayed fluorescence. With regard to the trans-cis isomerization of the central CC bond, the perpendicular conformation is found to represent a maximum on the energy profile not only of the electronic ground state, but also of the low-lying excited states. The lack of a strong driving force along the torsional coordinate explains the low tendency of DPH for isomerization. Finally, the results of our spin-orbit coupling calculations suggest that the intramolecular formation of DPH molecules in the T(1)(1(3)B(u)) state proceeds from the 1(1)B(u) state and involves intermediately the T(2)(1(3)A(g)) state.
在此,通过密度泛函理论和多参考组态相互作用的组合,研究了 1,6-二苯基-1,3,5-己三烯(DPH)的各种异构体和旋转异构体的低电子态。从全反式核排列开始,确定了电子基态和第一激发三重态中的顺式-反式异构化途径。此外,在 singlet-triplet 能隙较小的选定点进行了自旋轨道耦合计算。计算表明,在激发态下,主要激发的光学亮态 1(1)B(u)态在几何弛豫时与光学暗多组态 2(1)A(g)态发生曲线交叉。两个单线态在锥形交叉附近的强烈振子耦合为实验观察到的状态快速平衡和延迟荧光的出现提供了一个决定性的解释。对于中央 CC 键的顺反异构化,垂直构象不仅在电子基态,而且在低能激发态的能量曲线上都代表了一个最大值。扭转坐标上没有强烈的驱动力解释了 DPH 异构化的低趋势。最后,我们的自旋轨道耦合计算结果表明,T(1)(1(3)B(u))态中 DPH 分子的分子内形成从 1(1)B(u)态开始,并涉及 T(2)(1(3)A(g))态。