Mondal Jahur A, Ghosh Hirendra N, Mukherjee T, Palit Dipak K
Radiation & Photochemistry Division, Bhabha Atomic Research Centre, Mumbai- 400085, India.
J Phys Chem A. 2006 Nov 9;110(44):12103-12. doi: 10.1021/jp062543m.
Ultrafast relaxation dynamics of the S2 and S1 states of 4,4'-bis(N,N-dimethylamino)thiobenzophenone (Michler's thione, MT) have been investigated in different kinds of solvents, using steady-state absorption and emission as well as femtosecond transient absorption and fluorescence up-conversion spectroscopic techniques. Steady-state fluorescence measurements, following photoexcitation to the S2 state of MT, reveal weak fluorescence from the S2 state (phi F approximately 10(-3) in nonpolar and 10(-4) in polar solvents) but much weaker fluorescence from the S1 state. Yield of fluorescence from the S2 state is reduced in polar solvents because of reduced energy gap between the S2 and S1 states, Delta E(S2-S1), as well as interaction with the solvent molecules. Occurrence of S2-fluorescence in polar solvents, despite small energy gap, suggests that symmetry allowed S2(1A1) --> S0 (1A1) radiative and symmetry forbidden S2(1A1) --> S1 (1A2) nonradiative transitions are the factors responsible for the S2 fluorescence in MT. Lifetime of the S2 state is shorter (varying in the range 0.28-3.5 ps in different solvents) than that predicted from the Delta E(S2-S1) value and this can be attributed to its flexible molecular structure, which promotes an efficient intramolecular radiationless deactivation pathways. The lifetime of the S1 state (approximately 1.9-6.5 ps) is also very short because of small energy difference between the S1 and T1 states (Delta E(S1-T1) approximately 300 cm(-1)) in cyclohexane and hydrogen-bonding interaction as well as the presence of the isoenergetic T1(pipi*) state to enhance the rate of the intersystem crossing process from the S1(npi*) state in protic solvents.
采用稳态吸收和发射以及飞秒瞬态吸收和荧光上转换光谱技术,研究了4,4'-双(N,N-二甲基氨基)硫代二苯甲酮(米氏硫酮,MT)的S2和S1态在不同溶剂中的超快弛豫动力学。对MT的S2态进行光激发后的稳态荧光测量表明,S2态发出的荧光较弱(在非极性溶剂中φF约为10^(-3),在极性溶剂中为10^(-4)),而S1态发出的荧光则弱得多。由于S2和S1态之间的能隙减小、ΔE(S2 - S1)以及与溶剂分子的相互作用,极性溶剂中S2态的荧光产率降低。尽管能隙较小,但极性溶剂中仍出现S2荧光,这表明对称性允许的S2(1A1)→S0(1A1)辐射跃迁和对称性禁阻的S2(1A1)→S1(1A2)非辐射跃迁是MT中S2荧光产生的原因。S2态的寿命比根据ΔE(S2 - S1)值预测的要短(在不同溶剂中变化范围为0.28 - 3.5 ps),这可归因于其灵活的分子结构,该结构促进了有效的分子内无辐射失活途径。S1态的寿命(约1.9 - 6.5 ps)也非常短,这是因为在环己烷中S1和T1态之间的能量差较小(ΔE(S1 - T1)约为300 cm^(-1))以及氢键相互作用,并且在质子溶剂中存在等能量的T1(ππ*)态以提高从S1(nπ*)态的系间窜越过程的速率。