首页> 外文期刊>The Journal of Chemical Physics >Fluorescence excitation and emission spectroscopy of the (A)over-cap(1)A '' - (X)over-cap(1)A ' system of CHBr
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Fluorescence excitation and emission spectroscopy of the (A)over-cap(1)A '' - (X)over-cap(1)A ' system of CHBr

机译:CHBr的(A)上限(1)A''<-(X)上限(1)A'系统的荧光激发和发射光谱

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We report fluorescence excitation and emission spectra of CHBr in the 450-750 nm region. A total of 30 cold bands involving the pure bending levels 2(0)(n) with n=2-8 and combination bands 2(0)(n)3(0)(1)(n=1-8), 2(0)(n)3(0)(2)(n=1-6), 2(0)(n)3(0)(3)(n=1-2), 1(0)(1)2(0)(n)(n=5-7), 1(0)(1)2(0)(n)3(0)(1)(n=4-6), and 1(0)(1)2(0)(n)3(0)(2)(n=5) in the A (1)A(')<- X (1)A(') system were observed, in addition to a number of hot bands. The majority of these are reported and/or rotationally analyzed here for the first time. Spectra were measured under jet-cooled conditions using a pulsed discharge source, and rotational analysis yielded band origins and rotational constants for both bromine isotopomers (CH Br-79,CH Br-81). The derived A (1)A(') vibrational intervals are combined with results of [Yu J. Chem. Phys. 115, 5433 (2001)] to derive barriers to linearity for the 2(n), 2(n)3(1), and 2(n)3(2) progressions. The A (1)A(') state C-H stretching frequency is determined here for the first time, and the observed nu(3) dependence of the Br-79-Br-81 isotope splitting in the A (1)A(') state is in good agreement with theoretical expectations. Our dispersed fluorescence spectra probe the vibrational structure of the X (1)A(') state up to similar to 9000 cm(-1) above the vibrationless level; the total number of levels observed is more than twice that previously reported. As first reported by [Chen J. Mol. Spectrosc. 209, 254 (2001)], these spectra reveal numerous perturbations due to spin-orbit interaction with the low-lying a (3)A(') state. The results of a Dunham expansion fit of the ground state vibrational term energies, and comparisons with previous experimental and theoretical studies, are reported. Our results lead to several revised assignments, including the X (1)A(') C-H stretching fundamental. Globally, the vibrational frequencies of X (1)A('), a (3)A('), and A (1)A(') are in excellent agreement with theoretical predictions. (c) 2006 American Institute of Physics.
机译:我们报告在450-750 nm区域CHBr的荧光激发和发射光谱。总共30个冷带,其中n = 2-8的纯弯曲水平2(0)(n)和组合带2(0)(n)3(0)(1)(n = 1-8),2 (0)(n)3(0)(2)(n = 1-6),2(0)(n)3(0)(3)(n = 1-2),1(0)(1) 2(0)(n)(n = 5-7),1(0)(1)2(0)(n)3(0)(1)(n = 4-6)和1(0)(除了数字之外,还观察到A(1)A(')<-X(1)A(')系统中的1)2(0)(n)3(0)(2)(n = 5)乐队。其中大多数是首次报告和/或旋转分析。在使用脉冲放电源的射流冷却条件下测量光谱,旋转分析得出两种溴代异构体(CH Br-79,CH Br-81)的谱带起源和旋转常数。导出的A(1)A(')振动间隔与[Yu J. Chem。物理115,5433(2001)]得出2(n),2(n)3(1)和2(n)3(2)进行线性度的障碍。首次确定A(1)A(')状态CH的拉伸频率,并观察到A(1)A(')中Br-79-Br-81同位素分裂的nu(3)依赖性国家与理论预期高度吻合。我们的分散荧光光谱探测了X(1)A(')状态的振动结构,该状态的振动结构比无振动水平高出9000 cm(-1)。观察到的水平总数是先前报告的两倍以上。最早由[Chen J. Mol。光谱。 209,254(2001)],这些光谱揭示了许多自旋轨道与低位(3)A(')状态相互作用的扰动。报告了基态振动项能量的邓纳姆展开拟合的结果,并与以前的实验和理论研究进行了比较。我们的结果导致了一些修改后的作业,包括X(1)A(')C-H拉伸基本面。在全球范围内,X(1)A('),a(3)A(')和A(1)A(')的振动频率与理论预测非常一致。 (c)2006年美国物理研究所。

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