Liu Xia, Tripathy Umakanta, Bhosale Sheshanath V, Langford Steven J, Steer Ronald P
Department of Chemistry, University of Saskatchewan, 110 Science Place Saskatoon, SK Canada S7N 5C9.
J Phys Chem A. 2008 Sep 25;112(38):8986-98. doi: 10.1021/jp804792x. Epub 2008 Aug 28.
The steady-state absorption, fluorescence, and excitation spectra and upper excited-state temporal fluorescence decay profiles of 11 tetrapyrroles in several fluid solvents are presented and analyzed to ascertain the factors that control their S2 population decay times. The S2 lifetimes, which vary by more than 2 orders of magnitude, are controlled exclusively by their rates of radiationless decay. The only important electronic relaxation path is S2-S1 internal conversion, the efficiency of which is near 1.0 in all compounds studied (except CdTPP where it is 0.69). The rate of S1 population rise equals the rate of S2 population decay in all cases. Among the compounds studied, only MgTPP exhibits S2-S1 decay behavior that corresponds to the weak coupling limit of radiationless transition theory; all zinc metalloporphyrins exhibit intermediate to strong coupling. Perdeuteration of ZnTPP produces no significant change in the rate of S2 decay or in the quantum yield of S2-S0 fluorescence, indicating that in-plane C-C and C-N vibrations are the accepting modes in S1 with the largest Franck-Condon factors. The initial vibrational energy content of the S2 states (0 < E(vib) < 3500 cm(-1) over the range of compounds) plays no significant role in determining their overall population decay rates in solution. The S2 population decay rates of these tetrapyrroles are controlled by two factors: the Franck-Condon factor, which is inversely proportional to the exponent of the S2-S1 electronic energy spacing and the S2-S1 coupling energy. The S2-S1 electronic energy spacing is determined in solution by the difference in the polarizabilities of the S2 and S1 states and can be controlled by varying the polarizability of the solvent. The S2-S1 coupling energy is influenced by the nature, location, and effect of the substituents, with beta-alkyl substitution and reduction of symmetry in the tetrapyrrole--for example by loss of planarity--increasing the interstate coupling energy.
本文给出并分析了11种四吡咯在几种流体溶剂中的稳态吸收光谱、荧光光谱、激发光谱以及上激发态时间分辨荧光衰减曲线,以确定控制其S2态布居衰减时间的因素。S2态寿命变化超过2个数量级,完全由无辐射衰减速率控制。唯一重要的电子弛豫路径是S2-S1内转换,在所研究的所有化合物中(除了CdTPP,其效率为0.69),该过程的效率接近1.0。在所有情况下,S1态布居增长速率等于S2态布居衰减速率。在所研究的化合物中,只有MgTPP的S2-S1衰减行为符合无辐射跃迁理论的弱耦合极限;所有锌金属卟啉都表现出中等至强耦合。ZnTPP的全氘代对S2衰减速率或S2-S0荧光量子产率没有显著影响,这表明面内C-C和C-N振动是S1态中具有最大弗兰克-康登因子的接受模式。S2态的初始振动能量含量(在化合物范围内0 < E(vib) < 3500 cm(-1))在决定其在溶液中的总体布居衰减速率方面没有显著作用。这些四吡咯的S2态布居衰减速率由两个因素控制:弗兰克-康登因子,它与S2-S1电子能量间距的指数成反比,以及S2-S1耦合能。S2-S1电子能量间距在溶液中由S2和S1态极化率的差异决定,并且可以通过改变溶剂的极化率来控制。S2-S1耦合能受取代基的性质、位置和效应影响,例如β-烷基取代以及四吡咯对称性的降低(例如通过平面性的丧失)会增加态间耦合能。