Department of Physics, Freie Universitaet Berlin, Berlin, Germany.
J Phys Chem A. 2012 Jan 26;116(3):1023-9. doi: 10.1021/jp211970j. Epub 2012 Jan 17.
We combine femtosecond polarization resolved VIS-pump IR-probe spectroscopy with DFT and TD-DFT calculations to identify and assign absorption bands to electronic transitions for corroles. These macrocycles and their corresponding metal complexes are receiving great attention because of their utility in many fields, while many of their spectroscopic features have not yet been fully described. Analysis of the perturbed free induction decay provides information about the bleaching signal at time zero and allows for determination of overlapping excited state and bleaching signal amplitudes. The S(0) → S(1) and S(0) → S(2) transitions in the Q-band of the hexacoordinated Al(tpfc)(py)(2) and Br(8)Al(tpfc)(py)(2) absorption spectra are explicitly assigned. Angles between these electronic transition dipole moments (tdms) with a single vibrational transition dipole moment of (53 ± 2)° and (34 ± 2)° when excited at 580 and 620 nm for hexacoordinated Al(tpfc)(py)(2) and (51 ± 2)° and (43 ± 2)° when excited at 590 and 640 nm for hexacoordinated Br(8)Al(tpfc)(py)(2) were determined. The relative angles between the two lowest electronic tdms are (90 ± 8)° and (94 ± 3)° for Al(tpfc)(py)(2) and Br(8)Al(tpfc)(py)(2), respectively. Angles are determined before time zero by polarization resolved perturbed free induction decay and after time zero by polarization resolved transients. Comparison of corrole's wave functions with those of porphine show that the reduced symmetry in the corrole molecules results in lifting of Q-band degeneracy and major reorientation of the electronic transition dipole moments within the molecular scaffold. This information is necessary in designing optimal corrole-based electron and energy transfer complexes.
我们结合飞秒极化分辨可见泵浦红外探测光谱学与 DFT 和 TD-DFT 计算,识别并分配电子跃迁的吸收带,以确定 Corrole 的吸收带。这些大环及其相应的金属配合物由于在许多领域的实用性而受到极大关注,尽管它们的许多光谱特征尚未得到充分描述。对受扰自由感应衰减的分析提供了关于零时漂白信号的信息,并允许确定重叠的激发态和漂白信号幅度。六配位 Al(tpfc)(py)(2)和 Br(8)Al(tpfc)(py)(2)吸收光谱的 Q 带中 S(0)→S(1)和 S(0)→S(2)跃迁被明确分配。在 580nm 和 620nm 激发时,这些电子跃迁偶极矩(t dms)与单个振动跃迁偶极矩之间的夹角为(53±2)°和(34±2)°,而在 590nm 和 640nm 激发时,夹角为(51±2)°和(43±2)°六配位 Br(8)Al(tpfc)(py)(2)。当用 580nm 和 620nm 激发六配位 Al(tpfc)(py)(2)时,两个最低电子 tdms 之间的相对角度分别为(90±8)°和(94±3)°,当用 590nm 和 640nm 激发六配位 Br(8)Al(tpfc)(py)(2)时,两个最低电子 tdms 之间的相对角度分别为(90±8)°和(94±3)°。在零时之前通过极化分辨受扰自由感应衰减确定角度,在零时之后通过极化分辨瞬态确定角度。Corrole 分子的波函数与 porphine 的波函数的比较表明,Corrole 分子的对称性降低导致 Q 带简并的消除和电子跃迁偶极矩在分子骨架内的主要重定向。在设计最佳的基于 Corrole 的电子和能量转移配合物时,这些信息是必要的。