Studzinski Harald, Zhang Song, Wang Yanmei, Temps Friedrich
Institut für Physikalische Chemie, Christian-Albrechts-Universität zu Kiel, Olshausenstr. 40, D-24098 Kiel, Germany.
J Chem Phys. 2008 Apr 28;128(16):164314. doi: 10.1063/1.2907859.
The fast nonradiative decay dynamics of the lowest two excited pipi() electronic states (S(2) and S(3)) of hexafluorobenzene have been investigated by using femtosecond time-resolved time-of-flight mass spectrometry. The molecules were excited at wavelengths between 265 nm > or = lambda(pump) > or = 217 nm and probed by four- and three-photon ionization at lambda(probe)=775 nm. The observed temporal profiles exhibit two exponential decay times (tau(1)=0.54-0.1 ps and tau(2)=493-4.67 ps, depending on the excitation wavelength) and a superimposed coherent oscillation with vibrational frequency nu(osc)=97 cm(-1) and damping time tau(D) that is two to three times longer than the respective tau(1). The first decay component (tau(1)) is assigned to rapid radiationless transfer from the excited optically bright pipi() electronic state (S(2) or S(3), respectively) through a conical intersection (CI) to the lower-lying optically dark pisigma() state (S(1)) of the molecule; the second component (tau(2)) is attributed to the subsequent slower relaxation from the S(1) state back to the electronic ground state (S(0)). tau(2) dramatically decreases with increasing vibronic excitation energy up to the CI connecting the pisigma() with the S(0) state. The coherent oscillation is identified as nuclear motion along the out-of-plane vibration nu(16a) (notation as for benzene), which has e(2u) symmetry and acts as coupling mode between the pipi() and pisigma() states.
通过飞秒时间分辨飞行时间质谱法研究了六氟苯最低的两个激发ππ电子态(S₂和S₃)的快速无辐射衰变动力学。分子在265 nm≥λ(泵浦)≥217 nm之间的波长处被激发,并在λ(探测)=775 nm处通过四光子和三光子电离进行探测。观察到的时间分布呈现出两个指数衰变时间(τ₁=0.54 - 0.1 ps和τ₂=493 - 4.67 ps,取决于激发波长)以及一个叠加的相干振荡,其振动频率ν(振荡)=97 cm⁻¹,阻尼时间τ(D)比相应的τ₁长两到三倍。第一个衰变分量(τ₁)被归因于从激发的光学明亮的ππ电子态(分别为S₂或S₃)通过锥形交叉点(CI)快速无辐射转移到分子的较低光学暗的πσ态(S₁);第二个分量(τ₂)归因于随后从S₁态回到电子基态(S₀)的较慢弛豫。随着振动激发能量增加直至连接πσ与S₀态的CI,τ₂显著减小。相干振荡被确定为沿着面外振动ν₁₆a(苯的标记)的核运动,其具有e₂u对称性,并作为ππ和πσ态之间的耦合模式。