Kushnarenko Alexander, Miloglyadov Eduard, Quack Martin, Seyfang Georg
ETH Zurich, Lab. für Physikalische Chemie, HCI E235, Vladimir-Prelog-Weg 1-5/10, 8093 Zurich, Switzerland.
Phys Chem Chem Phys. 2018 Apr 25;20(16):10949-10959. doi: 10.1039/c7cp08561c.
From the analysis of high resolution overtone spectra it is well established that intramolecular vibrational energy redistribution (IVR) from an initially excited CH-stretching vibration is strongly influenced by its chemical environment. Due to a pronounced Fermi resonance between the CH-stretching and CH-bending vibrations a vibrational energy redistribution on the subpicosecond time scale (∼100 fs) is found for alkyl (sp3) CH-chromophores, whereas this doorway for energy flow is blocked for the acetylenic (sp) CH-stretching vibration because of the much lower CH-bending frequency. From the analysis of the high resolution spectra lifetimes for the initial CH-vibrational excitation of 10-100 ps or longer have been derived. In the present work we have investigated the IVR process for HCCCH2Br, HCCCH2Cl, and HCCCH2I after excitation of the first overtone of the CH-stretching vibration of the CH2X- and the CCH-group by time resolved femtosecond pump-probe experiments in a hollow waveguide. For HCCCH2Br and HCCCH2Cl a clearly different IVR behavior was found for the two different chemical environments. For the excitation of the alkyl CH-chromophore very fast initial relaxation times were found together with a slower relaxation process with τ2 = 15-40 ps, whereas for the acetylenic CH-stretching vibration a relaxation time τ3 = 70-200 ps has been determined. For HCCCH2I also for the excitation of the CCH-group a relatively fast relaxation process with a time constant τ2 = 6 ps could be identified which might result from a not yet identified strong vibrational coupling between the excited first overtone of the acetylenic CH-stretching vibrations with a combination state including the CI-stretching vibration.
通过对高分辨率泛音光谱的分析,已充分证实,从最初激发的C-H伸缩振动进行的分子内振动能量重新分布(IVR)受到其化学环境的强烈影响。由于C-H伸缩振动和C-H弯曲振动之间存在明显的费米共振,对于烷基(sp3)C-H发色团,在亚皮秒时间尺度(约100飞秒)上发现了振动能量重新分布,而对于炔属(sp)C-H伸缩振动,由于C-H弯曲频率低得多,这种能量流动通道被阻断。通过对高分辨率光谱的分析,得出了最初C-H振动激发的寿命为10-100皮秒或更长。在本工作中,我们通过在空心波导中进行的时间分辨飞秒泵浦-探测实验,研究了CH2X-和CCH基团的C-H伸缩振动的第一泛音激发后,HCCCH2Br、HCCCH2Cl和HCCCH2I的IVR过程。对于HCCCH2Br和HCCCH2Cl,在两种不同的化学环境中发现了明显不同的IVR行为。对于烷基C-H发色团的激发,发现了非常快的初始弛豫时间以及τ2 = 15-40皮秒的较慢弛豫过程,而对于炔属C-H伸缩振动,确定了弛豫时间τ3 = 70-200皮秒。对于HCCCH2I,对于CCH基团的激发,也可以识别出具有时间常数τ2 = 6皮秒的相对快速的弛豫过程,这可能是由于炔属C-H伸缩振动的激发第一泛音与包括C-I伸缩振动的组合态之间尚未确定的强振动耦合所致。