Belletête Michel, Durocher Gilles, Hamel Sébastien, Côte Michel, Wakim Salem, Leclerc Mario
Département de Chimie, Université de Montréal, Montréal, Quebec H3C 3J7, Canada.
J Chem Phys. 2005 Mar 8;122(10):104303. doi: 10.1063/1.1857477.
The molecular structure of three ladder oligo(p-aniline)s, 5,11-diethyl-6,12-dimethylindolo[3,2-b]carbazole (DIMER 2P), 14-ethyl-5,8-dihydro-diindolo[3,2-b:2',3'-h]carbazole (TRIMER 2P), and 5,8,14-triethyl-diindolo[3,2-b:2',3'-h]carbazole (TRIMER 3P) were investigated by first principles calculations at the Hartree-Fock (HF6-31G*) and density functional theory (DFTB3LYP6-31G*) levels. It is found that the agreement between theoretical and x-ray geometrical parameters is good and rather similar for both theoretical methods. The nature and the energy of the first two singlet-singlet electronic transitions have been obtained by Zerner intermediate neglect of differential overlap/spectroscopy semiempirical calculations performed on the HF6-31G* and DFTB3LYP6-31G* optimized geometries, as well as time-dependent density functional theory (TDDFT) calculations performed on the DFTB3LYP6-31G* optimized structures. For all the compounds and for all the theoretical approaches, it is observed that the S(1)<--S(0) electronic transition (pipi*) is weakly allowed and polarized along the short axis (y) of the molecule. On the other hand, the S(2)<--S(0) electronic transition of each oligomer possesses a much larger oscillator strength and is polarized along the long (x) molecular axis. It is found that TDDFT calculations provide the best overall agreement between the energies and the corresponding optical transitions obtained from the absorption bands (0-0 peaks) measured in dichloromethane as well as providing a good evaluation of the bathochromic shifts caused by the increase in the conjugation length or by the presence of extra alkyl chains on the nitrogen atoms in TRIMER 3P compared to TRIMER 2P.
通过在哈特里-福克(HF6-31G*)和密度泛函理论(DFTB3LYP6-31G*)水平上的第一性原理计算,研究了三种梯形低聚对苯胺、5,11-二乙基-6,12-二甲基吲哚并[3,2-b]咔唑(二聚体2P)、14-乙基-5,8-二氢-二吲哚并[3,2-b:2',3'-h]咔唑(三聚体2P)和5,8,14-三乙基-二吲哚并[3,2-b:2',3'-h]咔唑(三聚体3P)的分子结构。结果发现,两种理论方法的理论几何参数与X射线几何参数之间的一致性都很好且相当相似。通过对HF6-31G和DFTB3LYP6-31G优化几何结构进行泽纳微分重叠忽略/光谱半经验计算,以及对DFTB3LYP6-31G优化结构进行含时密度泛函理论(TDDFT)计算,得到了前两个单重态-单重态电子跃迁的性质和能量。对于所有化合物和所有理论方法,都观察到S(1)<--S(0)电子跃迁(ππ)微弱允许且沿分子短轴(y)极化。另一方面,每种低聚物的S(2)<--S(0)电子跃迁具有大得多的振子强度且沿分子长轴(x)极化。结果发现,TDDFT计算在能量与从二氯甲烷中测量的吸收带(0-0峰)获得的相应光学跃迁之间提供了最佳的总体一致性,并且对三聚体3P与三聚体2P相比共轭长度增加或氮原子上存在额外烷基链引起的红移提供了良好的评估。