首页> 外文期刊>The Journal of Chemical Physics >Rovibronic bands of the (A)over-tilde -(X)over-tilde transition of CH3OO and CD3OO detected with cavity ringdown absorption near 1.2-1.4 mu m
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Rovibronic bands of the (A)over-tilde -(X)over-tilde transition of CH3OO and CD3OO detected with cavity ringdown absorption near 1.2-1.4 mu m

机译:检测到CH3OO和CD3OO的(A)倾斜度<-(X)倾斜度过渡的Robrbronic带,腔衰荡吸收在1.2-1.4μm附近

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We have recorded several rovibronic bands of CH3OO and CD3OO in their (A) over tilde <-(K) over tilde transitions in the range of 1.18-1.40 mu m with the cavity ringdown technique. While the electronic origins for these species have been reported previously, many newly observed rovibronic bands are described here. The experimental vibrational frequencies (given as nu in the unit cm(-1) in this paper) for the COO bending (nu(8)) and COO symmetric stretching (nu(7)) modes in the (A) over tilde state are 378 and 887 cm(-1) for CH3OO, and 348 and 824 cm(-1) for CD3OO, respectively. In addition, two other vibrational frequencies were observed for the (A) over tilde state of CD3OO, namely, nu(5) (954 cm(-1)) and nu(6) (971 cm(-1)). These experimental vibrational frequencies for the A state of both CH3OO and CD3OO are in good agreement with predictions from quantum-chemical calculations at the UB3LYP/aug-cc-pVTZ level. The enhanced activity of the nu(5) vibrational mode in CD3OO is rationalized by mode mixing with the nu(7) mode, as supported by calculations of multidimensional Franck-Condon factors. In addition, many hot bands involving the methyl torsional mode (nu(12)) are observed for both normal and deuterated methyl peroxy. These bands include the "typical" sequence transitions and some "atypical" ones due to the nature of the eigenvalues and eigenfunctions which are a consequence of the low, but very different, torsional barriers in the (X) over tilde and (A) over tilde states. In addition, the 12(2)(2) band in CH3OO and the 12(3)(3) band in CD3OO show quite different structures than the origin bands, an effect which results from tunneling splittings comparable to the rotational contour. (C) 2007 American Institute of Physics.
机译:我们已经用腔衰荡技术记录了CH3OO和CD3OO的几个电波带,它们在(A)的波浪线<-(K)上的波浪线过渡范围为1.18-1.40μm。尽管先前已经报道了这些物种的电子起源,但此处描述了许多新观察到的电子振动带。在波浪线状态下(A)的COO弯曲(nu(8))和COO对称拉伸(nu(7))模式的实验振动频率(在本文中,单位为cm(-1)中的nu)为CH3OO分别为378和887 cm(-1),CD300为348和824 cm(-1)。此外,对于CDAOO的(A)超过波浪状态,还观察到另外两个振动频率,即nu(5)(954 cm(-1))和nu(6)(971 cm(-1))。 CH3OO和CD3OO处于A状态的这些实验振动频率与UB3LYP / aug-cc-pVTZ水平的量子化学计算预测相符。 CD3OO中nu(5)振动模式的增强活动是通过与nu(7)模式进行模式混合来实现的,这是多维弗兰克-康登因子的计算所支持的。此外,对于正常和氘代甲基过氧均观察到许多涉及甲基扭转模式的热带(nu(12))。由于特征值和特征函数的性质,这些谱带包括“典型”序列跃迁和一些“非典型”序列跃迁,这是(X)跨越波浪号和(A)跨越低而又非常不同的扭转势垒的结果波浪号状态。此外,CH3OO中的12(2)(2)波段和CD300中的12(3)(3)波段显示出与原始波段完全不同的结构,这种效应是由与旋转轮廓相当的隧道裂隙产生的。 (C)2007美国物理研究所。

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