Flaud JM, Arcas P, Burger H, Polanz O, Halonen L
CNRS, Universite de Paris-Sud, Bat. 210, Orsay Cedex, 91405, France
J Mol Spectrosc. 1997 Jun;183(2):310-35. doi: 10.1006/jmsp.1997.7278.
High resolution Fourier transform spectra of a natural and a 130 Te monoisotopic sample of H2 Te have been recorded at a resolution of 0.0022 cm-1 in the 11.6 μm spectral region, as well as a spectrum of a natural sample of H2 Te at a resolution of 0.0051 cm-1 in the 2.4 μm region. In the 11.6 μm region the main absorbing band is the nu2 band, the analysis of which was rather easy. On the other hand, in the 2.4 μm region three bands are absorbing, namely 2nu1 , nu1 + nu3 , and 2nu3 , the last being much weaker than the others. The analysis in this spectral domain was much more difficult because of resonances. Indeed it proved not possible to reproduce the observed lines without taking into account the Darling-Dennison interaction between the levels of the (200) and (002) states and the Coriolis interactions between the levels of (200) and (101) and between those of (101) and (002). Considering these interactions allowed us to calculate very satisfactorily all the experimental levels, and precise sets of vibrational energies and rotational and coupling constants were obtained for the seven most abundant H2 Te isotopic species, namely H2 130 Te, H2 128 Te, H2 126 Te, H2 125 Te, H2 124 Te, H2 123 Te, and H2 122 Te. For the most abundant species, H2 130 Te, the band centers in cm-1 are nu0 (nu2 ) = 860.6563, nu0 (2nu1 ) = 4062.8842, nu0 (nu1 + nu3 ) = 4063.3697, and nu0 (2nu3 ) = 4137.0454. These results, combined with those obtained for other vibrational states, have been used to derive the equilibrium rotational constants and their corrections. Finally, by neglecting the electronic corrections, the equilibrium structure of H2 130 Te was obtained as follows: r e (Te-H) = 1.65145(10) A, alphae (HTeH) = 90.2635(90)degrees.
在11.6μm光谱区域,以0.0022cm-1的分辨率记录了天然H2Te样品和130Te单同位素样品的高分辨率傅里叶变换光谱,同时在2.4μm区域以0.0051cm-1的分辨率记录了天然H2Te样品的光谱。在11.6μm区域,主要吸收带是ν2带,对其分析相对容易。另一方面,在2.4μm区域有三个吸收带,即2ν1、ν1+ν3和2ν3,最后一个比其他两个弱得多。由于共振,该光谱域的分析要困难得多。事实上,不考虑(200)和(002)态能级之间的达林-丹尼森相互作用以及(200)和(101)态能级之间以及(101)和(002)态能级之间的科里奥利相互作用,就不可能重现观测到的谱线。考虑这些相互作用使我们能够非常令人满意地计算出所有实验能级,并获得了七种最丰富的H2Te同位素物种,即H2130Te、H2128Te、H2126Te、H2125Te、H2124Te、H2123Te和H2122Te的精确振动能量、转动常数和耦合常数集。对于最丰富的物种H2130Te,以cm-1为单位的带中心分别为ν0(ν2)=860.6563、ν0(2ν1)=4062.8842、ν0(ν1+ν3)=4063.3697和ν0(2ν3)=4137.0454。这些结果与其他振动状态获得的结果相结合,已用于推导平衡转动常数及其修正值。最后,忽略电子修正,得到H2130Te的平衡结构如下:re(Te-H)=1.65145(10) Å,αe(HTeH)=90.2635(90)度。