首页> 外文期刊>The Journal of Chemical Physics >Fluorescence excitation and emission spectroscopy of the A-tilde~1A' -X-tilde~1A' system of CHBr
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Fluorescence excitation and emission spectroscopy of the A-tilde~1A' -X-tilde~1A' system of CHBr

机译:CHBr A-tilde〜1A“ <-X-tilde〜1A'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~n_0 with n = 2-8 and combination bands 2_0~n3_0~1(n=l_-8),2_0~n3_0~2(n=1-6),2_0~n3_0~3(n=1-2),1_0~12_0~n(n=5-7),1_0~12_0~n3_0~1(n=4-6),and 1_0~12_0~n3_0~2(n = 5) in the A-tilde<- X-tilde~1A' 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 ~(79)Br,CH ~(81)Br).The derived A-tilde~1A" vibrational intervals are combined with results of [Yu et al.J.Chem.Phys.115,5433 (2001)] to derive barriers to linearity for the 2~n,2~n3~1,and 2~n3~2 progressions.The A-tilde~1A" state C-H stretching frequency is determined here for the first time,and the observed v_3 dependence of the ~(79)Br-~(81)Br isotope splitting in the A-tilde~1A" state is in good agreement with theoretical expectations.Our dispersed fluorescence spectra probe the vibrational structure of the X-tilde~1A' state up to approx 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 et al.J.Mol.Spectrosc.209,254 (2001)],these spectra reveal numerous perturbations due to spin-orbit interaction with the low-lying a-tilde~3A" 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-tilde~1A' C-H stretching fundamental.Globally,the vibrational frequencies of X-tilde~1A',a-tilde~3A",and A-tilde~1A" are in excellent agreement with theoretical predictions.
机译:我们报告了CHBr在450-750 nm范围内的荧光激发和发射光谱。共有30个冷带,涉及纯弯曲能级2〜n_0(n = 2-8)和组合带2_0〜n3_0〜1(n = l_- 8),2_0〜n3_0〜2(n = 1-6),2_0〜n3_0〜3(n = 1-2),1_0〜12_0〜n(n = 5-7),1_0〜12_0〜n3_0〜1( n = 4-6),除了许多热带外,还观察到A-波浪线<-X-波浪线〜1A'系统中的1_0〜12_0〜n3_0〜2(n = 5)。在脉冲冷却条件下使用脉冲放电源对光谱进行了测量,并进行了旋转分析,得出了两种溴代异构体(CH〜(79)Br,CH〜 (81)Br)。将得出的A-tilde〜1A“振动间隔与[Yu等人,J.Chem.Phys.115,5433(2001)]的结果相结合,得出2〜n的线性障碍。 2〜n3〜1和2〜n3〜2级数。这里首次确定A-tilde〜1A“状态CH的拉伸频率,并观察到v_3的依赖性。 〜(79)Br-〜(81)Br同位素在A-tilde〜1A“态分裂与理论预期吻合良好。我们的分散荧光光谱探测了X-tilde〜1A'态的振动结构,直至大约在无振动水平以上约9000 cm〜(-1)处;观测到的水平总数是以前报告的水平的两倍以上。[Chen等人,J.Mol.Spectrosc.209,254(2001)]首次报道,这些光谱揭示了由于与低地a-tilde〜3A“状态的自旋轨道相互作用而引起的许多扰动。报道了基态振动项能量的Dunham膨胀拟合结果,并与先前的实验和理论研究进行了比较。结果导致对X-tilde〜1A'CH的拉伸基础进行了一些修改。在全球范围内,X-tilde〜1A',a-tilde〜3A“和A-tilde〜1A”的振动频率非常一致有理论上的预测。

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