Within this work the Even-Lavie valve was successfully employed as a new pulsed helium droplet source and was used for the electronic spectroscopy of various organic molecules doped into the droplets. udThe detailed characterization of the pulsed helium droplet beam revealed a significantly different dependence of the droplet size on the stagnation conditions as compared to a continuous helium droplet beam. The combined investigation of Rayleigh-scattering from the droplets and laser induced fluorescence (LIF) from molecules doped into the droplets revealed a bimodal droplet size distribution. LIF from dopant molecules inside helium droplets could only be observed from the leading fraction of the droplet pulses. The size of these droplets can be varied between 10000 and 1000000 helium atoms per droplet. The other fraction of the droplet pulses carries very large droplets not useful for doping with molecules. Variations of the stagnation conditions mainly affect the relative abundance of the two fractions. udThe optimum signal is almost constant from single shot up to 500 Hz operation and the density of the droplets is about 20 times higher than in the continuous droplet beam.ududThe electronic spectra of the anthracene-derivatives Anthracene, 9,10-Dichloroanthracene, 9-Chloroanthracene, 9-Cyanonanthracene, 9-Phenylanthracene, 9-Methylanthracene, 1-Methylanthracene and 2-Methylanthracene, the charge transfer molecules Phenylpyrrole and Fluorazene, and the Pyrromethene Dyes BDP, 8-PhPM, PM546, PM567, and PM650, doped into the pulsed helium droplet beam were recorded and compared to the corresponding spectra of the isolated molecules in a supersonic jet. Thereby, significant differences which could not be reduced to the lower temperature in the helium droplets, and which are consequently attributed to the interaction between the helium environment and the embedded molecules, could be observed.udThe perturbations of the electronic transitions are reflected by substantial line broadening, the occurrence of a fine structure of electronic transitions (zero phonon lines accompanied by phonon wings), and in rare cases a multiplet splitting of zero phonon lines.udThe broadening of molecular transitions is counterintuitive to what is expected for sub-Kelvin temperature and was attributed to a damping of the electronically excited state by the helium environment which occurs if the electronic excitation induces a significant nuclear rearrangement. Broad electronic spectra could also be observed due to the dominance of phonon wings over pure molecular transitions. udBoth broadening effects reflect a strong perturbation of the electronic transitions of the dopant species by the helium droplet. This result deduced from a larger systematic investigation is of importance for planning photochemical experiments in helium droplets and contributes to the understanding of the solvation of molecules in superfluid helium droplets.
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机译:在这项工作中,Even-Lavie阀被成功用作新的脉冲氦气滴源,并用于电子光谱分析了掺入液滴中的各种有机分子。脉冲氦滴束的详细表征表明,与连续氦滴束相比,滴滴大小对停滞条件的依赖性显着不同。液滴的瑞利散射和掺杂到液滴中的分子的激光诱导荧光(LIF)的组合研究显示出双峰液滴尺寸分布。只能从液滴脉冲的前导部分观察到氦液滴内部的掺杂剂分子产生的LIF。这些液滴的大小可以在每个液滴10000至1000000氦原子之间变化。液滴脉冲的其他部分携带着非常大的液滴,这些液滴对掺杂分子没有用。停滞条件的变化主要影响两个部分的相对丰度。 ud从单次发射到高达500 Hz的操作,最佳信号几乎是恒定的,液滴的密度比连续液滴束的密度高约20倍。 ud ud蒽衍生物蒽的电子光谱为9,10-二氯蒽,9-氯蒽,9-氰基蒽,9-苯基蒽,9-甲基蒽,1-甲基蒽和2-甲基蒽,电荷转移分子苯基吡咯和芴基,以及吡咯亚甲基染料BDP,8-PhPM和PM546,PM567,记录了掺入脉冲氦液滴束中的,并与超音速射流中分离的分子的相应光谱进行了比较。因此,可以观察到无法降低到氦液滴中较低温度的显着差异,并因此归因于氦环境与包埋分子之间的相互作用。 ud电子跃迁的扰动反映为线变宽,出现电子跃迁的精细结构(零声子线伴有声子翼),在极少数情况下零声子线会多重分裂。 ud分子跃迁的变宽与亚开尔文的预期相反温度的升高归因于氦气环境对电子激发态的阻尼,这在电子激发引起明显的核重排时会发生。由于声子翼在纯分子跃迁上的优势,也可以观察到宽广的电子光谱。 ud这两种展宽效应都反映了氦液滴对掺杂物物种电子跃迁的强烈干扰。从较大的系统研究中得出的结果对于计划氦滴中的光化学实验具有重要意义,并且有助于理解超流体氦滴中分子的溶剂化作用。
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