Vyas Shubham, Hadad Christopher M, Modarelli David A
Department of Chemistry, The Ohio State University, 100 West 18th Avenue, Columbus, Ohio 43210, USA.
J Phys Chem A. 2008 Jul 24;112(29):6533-49. doi: 10.1021/jp802094r. Epub 2008 Jul 1.
Computational investigations into the ground and singlet excited-state structures and the experimental ground-state absorption spectra of N-confused tetraphenylporphyrin tautomers 1e and 1i and N-confused porphines (NCP) 2e and 2i have been performed. Structural data for the ground state, performed at the B3LYP/6-31G(d), B3LYP/6-31+G(d)//B3LYP/6-31G(d), and B3LYP/6-311+G(d)//B3LYP/6-31G(d) levels, are consistent with those performed at lower levels of theory. Calculations of the gas-phase, ground-state absorption spectrum are qualitatively consistent with condensed phase experiments for predicting the relative intensities of the Q(0,0) and Soret bands. Inclusion of implicit solvation in the calculations substantially improves the correlation of the energy of the Soret band with experiment for both tautomers (1e, 435 nm predicted, 442 nm observed in DMAc; 1i, 435 nm predicted, 437 nm observed in CH2Cl2). The x- and y-polarized Q-band transitions were qualitatively reproduced for 1e in both the gas phase and with solvation, although the low-energy absorption band in 1i was predicted at substantially higher energy (646 nm in the gas phase and 655 nm with solvation) than observed experimentally (724 nm in CH2Cl2). Franck-Condon state and equilibrated singlet excited-state geometries were calculated for unsubstituted NCP tautomers 2e and 2i at the TD-B3LYP/SVP and TD-B3LYP/TZVP//TD-B3LYP/SVP levels. Electronic difference density plots were calculated from these geometries, thereby indicating the change of electron density in the singlet excited states. Adiabatic S1 and S2 geometries of these compounds were also calculated at the TD-B3LYP/SVP level, and the results indicate that while 2i is a more stable ground-state molecule by approximately 7.0 kcal mol-1, the energy difference for the S1 excited states is only approximately 1.0 kcal mol-1 and is 6.1 kcal mol-1 for the S2 excited states.
已对N-稠合四苯基卟啉互变异构体1e和1i以及N-稠合卟吩(NCP)2e和2i的基态和单重激发态结构以及实验基态吸收光谱进行了计算研究。在B3LYP/6-31G(d)、B3LYP/6-31+G(d)//B3LYP/6-31G(d)和B3LYP/6-311+G(d)//B3LYP/6-31G(d)水平上进行的基态结构数据与在较低理论水平上进行的结果一致。气相基态吸收光谱的计算在预测Q(0,0)和Soret带的相对强度方面与凝聚相实验定性一致。在计算中包含隐式溶剂化显著改善了两种互变异构体(1e,预测435 nm,在DMAc中观察到442 nm;1i,预测435 nm,在CH2Cl2中观察到437 nm)Soret带能量与实验的相关性。对于1e,在气相和有溶剂化的情况下都定性地再现了x和y偏振的Q带跃迁,尽管1i中的低能吸收带预测的能量(气相中646 nm,有溶剂化时655 nm)比实验观察到的(在CH2Cl2中724 nm)高得多。在TD-B3LYP/SVP和TD-B3LYP/TZVP//TD-B3LYP/SVP水平上计算了未取代NCP互变异构体2e和2i的弗兰克-康登态和平衡单重激发态几何结构。根据这些几何结构计算了电子差分密度图,从而表明单重激发态中电子密度的变化。还在TD-B3LYP/SVP水平上计算了这些化合物的绝热S1和S2几何结构,结果表明,虽然2i作为基态分子更稳定约7.0 kcal mol-1,但S1激发态能量差仅约1.0 kcal mol-1,S2激发态能量差为6.1 kcal mol-1。