首页> 外文期刊>The Journal of Chemical Physics >Rovibronic bands of the (A)over-tilde B-2(2) -(X)over-tilde B-2(1) transition of C6H5O and C6D5O detected with cavity ringdown absorption near 1.2 mu m
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Rovibronic bands of the (A)over-tilde B-2(2) -(X)over-tilde B-2(1) transition of C6H5O and C6D5O detected with cavity ringdown absorption near 1.2 mu m

机译:检测到C6H5O和C6D5O的(A)波浪形B-2(2)<-(X)波浪形B-2(1)的电子振动带,腔衰荡吸收在1.2微米附近

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We recorded several rovibronic bands of C6H5O and C6D5O in their (A) over tilde B-2(2)<-(X) over tilde B-2(1) transitions in the range 1.14-1.31 mu m with the cavity ringdown technique. While the electronic transition is forbidden, several vibronic bands are observed. By comparison of rovibronic contours of observed and simulated bands to determine their types of transition, and by consideration of vibrational wavenumbers of the upper state based on quantum-chemical calculations, we were able to provide vibronic assignments of observed bands and derive several experimental vibrational wavenumbers (given as nu in unit of cm(-1) in this paper) for the (A) over tilde B-2(2) state, namely, nu(12)=947, nu(13)=793, nu(14)=417, nu(15)=964, nu(16)=866, nu(17)=723, nu(18)=680, and nu(19)=499 for C6H5O, and nu(12)=772, nu(13)=626, nu(14)=365, nu(15)=812, nu(17)=599, nu(18)=532, and nu(19)=436 for C6D5O. Transitions involving vibrationally excited levels of nu(20) were also observed; nu(20) of the (A) over tilde state is greater by 50 cm(-1) than the (X) over tilde state of C6H5O. A weak origin at 7681 cm(-1) for the (A) over tilde <-(X) over tilde transition of C6H5O (7661 cm(-1) for C6D5O) with a c-type contour was observed. Observed isotopic ratios of vibrational wavenumbers for the (A) over tilde state of C6H5O to those of C6D5O are in good agreement with the predictions from quantum-chemical calculations at the B3LYP/aug-cc-pVTZ level. (C) 2008 American Institute of Physics. [DOI: 10.1063/1.2992077]
机译:我们用腔衰荡技术记录了C6H5O和C6D5O在(A)上在波浪线B-2(2)<-(X)上在波浪线B-2(1)过渡上的几个电子振动带,范围为1.14-1.31μm。禁止电子跃迁时,观察到几个振动带。通过比较观察带和模拟带的电子振动轮廓,以确定它们的过渡类型,并通过基于量子化学计算的上层态振动波数,我们能够提供观察带的电子振动分配,并得出几个实验振动波数(在波浪线B-2(2)上的(A)状态下(以nu为单位,以cm(-1)为单位给出nu),即nu(12)= 947,nu(13)= 793,nu(14 )= 417,nu(15)= 964,nu(16)= 866,nu(17)= 723,nu(18)= 680和nu(19)= 499(对于C6H5O),以及nu(12)= 772,对于C6D5O,nu(13)= 626,nu(14)= 365,nu(15)= 812,nu(17)= 599,nu(18)= 532,nu(19)= 436。还观察到涉及振动激发水平的nu(20)的跃迁; (A)在波浪线状态下的nu(20)比C6H5O在波浪线状态下的(X)大50 cm(-1)。观察到在C6H5O的波浪线过渡处(A)的波浪线<-(X)处(7681 cm(-1)对于C型轮廓)的弱起源在7681 cm(-1)。观察到的(A)C6H5O的波峰状态的振动波数与C6D5O的振动波数的同位素比与在B3LYP / aug-cc-pVTZ水平进行的量子化学计算预测相符。 (C)2008美国物理研究所。 [DOI:10.1063 / 1.2992077]

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