Torres R, Siegel T, Brugnera L, Procino I, Underwood Jonathan G, Altucci C, Velotta R, Springate E, Froud C, Turcu I C E, Ivanov M Yu, Smirnova O, Marangos J P
Blackett Laboratory, Imperial College London, Prince Consort Road, London SW7 2BW, UK.
Opt Express. 2010 Feb 1;18(3):3174-80. doi: 10.1364/OE.18.003174.
The emerging techniques of molecular spectroscopy by high order harmonic generation have hitherto been conducted only with Ti:Sapphire lasers which are restricted to molecules with high ionization potentials. In order to gain information on the molecular structure, a broad enough range of harmonics is required. This implies using high laser intensities which would saturate the ionization of most molecular systems of interest, e.g. organic molecules. Using a laser at 1300 nm, we are able to extend the technique to molecules with relatively low ionization potentials (approximately 11 eV), observing wide harmonic spectra reaching up to 60 eV. This energy range improves spatial resolution of the high harmonic spectroscopy to the point where interference minima in harmonic spectra of N(2)O and C(2)H(2) can be observed.
迄今为止,通过高次谐波产生的分子光谱新兴技术仅使用钛宝石激光器进行,而这种激光器仅限于用于具有高电离势的分子。为了获取有关分子结构的信息,需要足够宽的谐波范围。这意味着要使用高激光强度,而这会使大多数感兴趣的分子系统(例如有机分子)的电离达到饱和。使用波长为1300 nm的激光器,我们能够将该技术扩展到具有相对较低电离势(约11 eV)的分子,观察到高达60 eV的宽谐波光谱。这个能量范围将高谐波光谱的空间分辨率提高到可以观察到N₂O和C₂H₂谐波光谱中的干涉极小值的程度。