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304.6K下HD分子拉曼Q支谱线的混合与展宽

Line Mixing and Broadening in the Raman Q Branch of HD at 304.6 K.

作者信息

Sheldon GD, Sinclair PM, Drummond JR, May AD

机构信息

Department of Physics, University of Toronto, 60 St. George Street, Toronto, Ontario, M5S 1A7, Canada

出版信息

J Mol Spectrosc. 1998 Dec;192(2):406-416. doi: 10.1006/jmsp.1998.7696.

Abstract

The Q-branch lines of pure HD were measured at densities ranging from 1 to 7 Amagat at 304.6 K. Each profile was fitted to the well-known Rosenkranz expression to extract the size of the asymmetry due to line mixing as well as to the linewidth. Line mixing and broadening coefficients were obtained by fitting the asymmetries and widths to a straight line as a function of gas density. Apart from a single existing measurement for the Q(0) line, our mixing coefficients are the first direct measurements of the asymmetry due to line mixing in HD. Our broadening coefficients are consistent with the best earlier measurements but are an order of magnitude more precise. Agreement is found with some existing semiclassical calculations of broadening. We have fitted our HD broadening coefficients to a variety of empirical energy gap laws. Our conclusions are that none of the exponential gap law (EGL), the modified exponential gap (MEG) law, and the statistical power gap (SPG) law successfully models our broadening coefficients. We present a modified version of the EGL and the MEG laws, which are successful in reproducing the experimental results. Using the fitted parameters of the new gap law, we have calculated the relaxation matrix of HD at room temperature. With this relaxation matrix, we have simulated the Q-branch spectrum at a number of densities between 49.1 and 490 Amagat and compared the results with previous high-density measurements. At all densities and frequencies, the simulated spectral intensity was found to agree with the measured strength within about 5% of the peak of the spectrum. In addition, the comparison provides evidence of a nonlinear vibrational dephasing shift in HD. Copyright 1998 Academic Press.

摘要

在304.6 K温度下,对纯HD的Q支谱线在1至7阿马格密度范围内进行了测量。将每个谱形拟合到著名的罗森克兰茨表达式,以提取由于谱线混合以及线宽导致的不对称性大小。通过将不对称性和宽度拟合为气体密度的函数的直线,获得了谱线混合和展宽系数。除了对Q(0)线的单次现有测量外,我们的混合系数是首次对HD中谱线混合引起的不对称性进行直接测量。我们的展宽系数与早期最佳测量结果一致,但精度提高了一个数量级。与一些现有的展宽半经典计算结果相符。我们已将HD展宽系数拟合到各种经验能隙定律。我们的结论是,指数能隙定律(EGL)、修正指数能隙(MEG)定律和统计功率能隙(SPG)定律均未能成功模拟我们的展宽系数。我们提出了EGL和MEG定律的修正版本,它们成功地再现了实验结果。利用新能隙定律的拟合参数,我们计算了室温下HD的弛豫矩阵。利用该弛豫矩阵,我们模拟了49.1至490阿马格之间多种密度下的Q支谱,并将结果与以前的高密度测量结果进行了比较。在所有密度和频率下,发现模拟的光谱强度与测量强度在光谱峰值的约5%范围内相符。此外,该比较提供了HD中非线性振动退相移的证据。版权所有1998年学术出版社。

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