合成硝酸光谱与实验室和大气测量在11.3微米区域的比较

C. Young, W. Evans
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引用次数: 0

摘要

用逐线积分法生成了硝酸在11.3微米光谱区的理论吸收光谱。只考虑了v5和2v9波段。利用Dana常数计算了v5波段的旋转线位置和强度;对于2v9波段,旋转常数是基于Chevillard和Giraudet2给出的结果,并结合McGraw等人的振动常数进行从头计算。在300K和1atm下,采用洛伦兹线形,自加宽半宽度为0.75 cm-1。假定半-半宽度为常数,在此阶段忽略随转动量子数的变化。图1显示了计算光谱与Goldman等人的实验光谱的对比。计算结果与实验结果之间的差异可能是由于以下原因;(a)忽略了大量较弱的线,为了计算的目的,有必要消除一些较弱的线;(b)忽略可能的热带,下面将会指出,在885 cm−1和910 cm−1附近可能存在热带;(c)线的翅膀是超洛伦兹的可能性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Comparison of Synthetic Nitric Acid Spectra with Laboratory and Atmospheric Measurements in the 11.3 Micron Region
Theoretical absorption spectra for nitric acid in the 11.3 micron spectral region were generated by line by line integration. Only the v5 and 2v9 bands were considered. The rotational line positions and intensities were calculated using Dana's constants for the v5 band; for the 2v9 band the rotational constants were based on the results given by Chevillard and Giraudet2 in conjunction with an ab initio calculation using the vibrational constants of McGraw et al3. A Lorentzian line shape was used with a self broadened semi-­half width of 0.75 cm-1 at 300K and 1 atm. The semi-half width was assumed constant and at this stage of the work the varia­tion with rotational quantum number was ignored. Fig. 1 shows a comparison between a calculated spectra and an experimental spectrum of Goldman et al4. The differences between the calcu­lations and the experimental results could be due to the following; (a) neglect of a large number of the weaker lines, it was necessary to eliminate a number of weaker lines for computational purposes; (b) neglect of possible hot bands, as will be noted below there could be hot bands in the vicinity of 885 cm−1 and 910 cm−1; (c) the possibility that the wings of the lines are super Lorentzian.
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