Keller F, Perrin A, Flaud J, Johns JWC, Lu Z, Looi EC
Laboratoire de Photophysique Moléculaire, CNRS UniversitéParis Sud, Bat 210, Campus d'Orsay, Orsay, Cedex, F-91405, France
J Mol Spectrosc. 1998 Oct;191(2):306-310. doi: 10.1006/jmsp.1998.7630.
The analysis of the nu6, nu7, nu8, and nu9 bands of H15N16O3 located at 646.9641, 578.4719, 743.6166, and 458.2917 cm-1, respectively, has been carried out in the 400-800 cm-1 region using high-resolution Fourier transform spectra recorded at Ottawa. Using the ground state energy levels calculated from the v = 0 rotational constants of H15N16O3 [A. P. Cox, M. C. Ellis, C. J. Attfield, and A. C. Ferris, J. Mol. Struct. 320, 91-106 (1994)], it was possible to assign the A-type nu6 and nu7 bands and the C-type nu8 and nu9 bands of H15N16O3 up to high J and Ka rotational quantum numbers. The v6 = 1, v7 = 1, v8 = 1, and v9 = 1 experimental energy levels were then introduced in a least-squares fit calculation and precise upper state Hamiltonian constants (band centers and rotational constants) were determined allowing one to reproduce the infrared data to within the experimental uncertainty. Copyright 1998 Academic Press.
利用在渥太华记录的高分辨率傅里叶变换光谱,对位于646.9641、578.4719、743.6166和458.2917 cm⁻¹处的H¹⁵N¹⁶O₃的ν₆、ν₇、ν₈和ν₉带在400 - 800 cm⁻¹区域进行了分析。根据H¹⁵N¹⁶O₃的v = 0转动常数计算出基态能级[A. P. 考克斯、M. C. 埃利斯、C. J. 阿特菲尔德和A. C. 费里斯,《分子结构杂志》320, 91 - 106 (1994)],从而有可能将H¹⁵N¹⁶O₃的A类ν₆和ν₇带以及C类ν₈和ν₉带指定到高J和Ka转动量子数。然后将v₆ = 1、v₇ = 1、v₈ = 1和v₉ = 1的实验能级引入最小二乘法拟合计算中,并确定了精确的上态哈密顿常数(带中心和转动常数),使得能够在实验不确定度范围内重现红外数据。版权所有1998年学术出版社。