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Pure rotational coherent anti-Stokes Raman scattering spectroscopy of nitric oxide: Determination of Raman tensor invariants

机译:一氧化氮的纯旋转相干抗斯托克斯拉曼散射光谱:拉曼张量不变的测定

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Coherent anti-Stokes Raman scattering (CARS) measurements of the pure rotational Raman spectrum of nitric oxide were performed. Measurements were performed in a room-temperature gas cell using a dual-broadband pure rotational CARS configuration. In this configuration, a broadband dye laser was used to generate the pump and Stokes beams, and the 355-nm third-harmonic beam from a Nd:YAG laser was used as the probe beam. The Raman spectrum of NO is of significant theoretical interest because of the spin splitting in the ground electronic level of NO. A detailed model of the pure rotational Raman spectrum of NO was developed based on an irreducible tensor analysis using Hund's case (a) wave functions as basis states for the analysis. The pure rotational Raman polarizability tensor element eta v=0 alpha<^>q=02 eta v=0 in the molecular frame was determined for NO based on fitting pure rotational CARS spectra of mixtures of NO and nitrogen (N-2). In addition to the pure rotational CARS spectrum featuring (2)pi(1/2)->(2)pi(1/2) and (2)pi(3/2)->(2)pi(3/2) transitions, there is an electronic Raman transition at 121 cm(-1) between the spin split (2)pi(1/2) and (2)pi(3/2) ground electronic levels that has been the subject of previous theoretical interest, but the value of the tensor invariant eta v=0 alpha<^>q=22 eta v=0 that contributes to the intensity of the electronic Raman transitions has not been quantitatively determined. Analysis of our pure rotational CARS spectra indicates that the magnitude of this term is much smaller than indicated in previous work, but the analysis is complicated by the weakness of the electronic Raman transitions compared with pure rotational transitions in the same spectral region. Future experiments to more definitively determine the magnitude and sign of the eta v=0 alpha<^>q=22 eta v=0 polarizability tensor element are proposed.
机译:进行一氧化氮旋转拉曼光谱的相干反斯托克斯拉曼散射(汽车)测量。使用双宽带纯旋转汽车配置在室温气室中进行测量。在这种配置中,使用宽带染料激光器产生泵和斯托克梁,并且来自Nd:YAG激光器的355nm三谐波束作为探针光束。由于在地面电子电平的旋转分裂,NO的拉曼光谱是显着的理论兴趣。基于使用HUND的案例(A)波函数作为分析的基本态,基于不可缩小的张量分析开发了纯旋转拉曼光谱的详细模型。在分子框架中确定纯旋转拉曼极化性张量元件ETA v = 0α<^ = 02ηv = 0,不基于嵌合NO和氮气混合物的配合纯旋转轿厢光谱(N-2)。除了纯旋转汽车谱具有(2)PI(1/2) - >(2)PI(1/2)和(2)PI(3/2) - >(2)PI(3/2)过渡,在旋转分裂(2)PI(1/2)和(2)PI(3/2)地面电子水平之间存在121cm(-1)的电子拉曼过渡,这是先前理论兴趣的主题但是,尚未定量地确定有助于电子拉曼转换的强度的张量不变的ETA v = 0 alpha <^> q = 22 eta v = 0的值。我们纯旋转汽车光谱的分析表明,该术语的大小远小于先前的工作中所示,但是通过相同光谱区域中的纯旋转转换相比,通过电子拉曼转换的弱点复杂。提出了未来的实验,更明确地确定ETA v = 0 alpha q = 22 eTa v = 0偏振张量元件的幅度和标志。

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