Department of Chemistry, Faculty of Art and Sciences, Ondokuz Mayıs University, 55139 Samsun, Turkey.
J Chem Phys. 2011 Feb 14;134(6):064325. doi: 10.1063/1.3535595.
We have measured electronic and Raman scattering spectra of 1,1',3,3'-tetraethyl-5,5',6,6'-tetrachloro-benzimidazolocarbocyanine iodide (TTBC) in various environments, and we have calculated the ground state geometric and spectroscopic properties of the TTBC cation in the gas and solution phases (e.g., bond distances, bond angles, charge distributions, and Raman vibrational frequencies) using density functional theory. Our structure calculations have shown that the ground state equilibrium structure of a cis-conformer lies ∼200 cm(-1) above that of a trans-conformer and both conformers have C(2) symmetry. Calculated electronic transitions indicate that the difference between the first transitions of the two conformers is about 130 cm(-1). Raman spectral assignments of monomeric- and aggregated-TTBC cations have been aided by density functional calculations at the same level of the theory. Vibrational mode analyses of the calculated Raman spectra reveal that the observed Raman bands above 700 cm(-1) are mainly associated with the in-plane deformation of the benzimidazolo moieties, while bands below 700 cm(-1) are associated with out-of-plane deformations of the benzimidazolo moieties. We have also found that for the nonresonance excited experimental Raman spectrum of aggregated-TTBC cation, the Raman bands in the higher-frequency region are enhanced compared with those in the nonresonance spectrum of the monomeric cation. For the experimental Raman spectrum of the aggregate under resonance excitation, however, we find new Raman features below 600 cm(-1), in addition to a significantly enhanced Raman peak at 671 cm(-1) that are associated with out-of-plane distortions. Also, time-dependent density functional theory calculations suggest that the experimentally observed electronic transition at ∼515 nm (i.e., 2.41 eV) in the absorption spectrum of the monomeric-TTBC cation predominantly results from the π → π∗ transition. Calculations are further interpreted as indicating that the observed shoulder in the absorption spectrum of TTBC in methanol at 494 nm (i.e., 2.51 eV) likely results from the ν(") = 0 → ν' = 1 transition and is not due to another electronic transition of the trans-conformer-despite the fact that measured and calculated NMR results (not provided here) support the prospect that the shoulder might be attributable to the 0-0 band of the cis-conformer.
我们已经测量了 1,1',3,3'-四乙基-5,5',6,6'-四氯苯并咪唑并咔啉碘化物(TTBC)在各种环境中的电子和拉曼散射光谱,并使用密度泛函理论计算了 TTBC 阳离子在气相和溶液相中的基态几何和光谱性质(例如,键距、键角、电荷分布和拉曼振动频率)。我们的结构计算表明,顺式构象的基态平衡结构比反式构象高约 200cm(-1),并且两种构象都具有 C(2)对称性。计算得到的电子跃迁表明,两种构象的第一跃迁之间的差异约为 130cm(-1)。通过密度泛函理论计算,对单体和聚集态 TTBC 阳离子的拉曼光谱进行了辅助分析。对计算拉曼光谱的振动模式分析表明,观察到的高于 700cm(-1)的拉曼带主要与苯并咪唑部分的面内变形有关,而低于 700cm(-1)的带与苯并咪唑部分的面外变形有关。我们还发现,对于聚集态 TTBC 阳离子的非共振激发实验拉曼光谱,高频区域的拉曼带与单体阳离子的非共振光谱相比得到增强。然而,对于共振激发下的聚集态实验拉曼光谱,我们发现除了在 671cm(-1)处的拉曼峰显著增强外,还存在低于 600cm(-1)的新拉曼特征,这与面外变形有关。此外,时变密度泛函理论计算表明,单体 TTBC 阳离子吸收光谱中观察到的约 515nm(即 2.41eV)的电子跃迁主要来自 π→π∗跃迁。计算结果进一步表明,甲醇中 TTBC 吸收光谱在 494nm(即 2.51eV)处的肩峰可能是由于 ν(")=0→ν'=1 跃迁的结果,而不是反式构象的另一个电子跃迁的结果-尽管测量和计算的 NMR 结果(此处未提供)支持该肩峰可能归因于顺式构象的 0-0 带的观点。