Laboratoire Interuniversitaire des Systèmes Atmosphériques, UMR CNRS 7583, Université Paris Est Créteil, Université Paris Diderot, Institut Pierre-Simon Laplace, 94010 Créteil Cedex, France.
J Chem Phys. 2013 Jan 21;138(3):034302. doi: 10.1063/1.4774094.
Complementary tests of the partially correlated speed-dependent Keilson-Storer (pCSDKS) model for the shape of isolated transition of pure water vapor [N. H. Ngo et al., J. Chem. Phys. 136, 154310 (2012)] are made using new measurements. The latter have been recorded using a high sensitivity cavity ring down spectrometer, for seven self-broadened H(2)O lines in the 1.6 μm region at room temperature and for pressures from 0.5 to 15 Torr. Furthermore, the H(2) (18)O spectra of [M. D. De Vizia et al., Phys. Rev. A 83, 052506 (2011)] in the 1.38 μm region, measured at 273.15 K and for pressures from 0.3 to 3.75 Torr have also been used for comparison with the model. Recall that the pCSDKS model takes into account the collision-induced velocity changes, the speed dependences of the broadening and shifting coefficients as well as the partial correlation between velocity and rotational-state changes. All parameters of the model have been fixed at values previously determined, except for a scaling factor applied to the input speed-dependent line broadening. Comparisons between predictions and experiments have been made by looking at the results obtained when fitting the calculated and measured spectra by Voigt profiles. The good agreement obtained for all considered lines, at different temperature and pressure conditions, confirms the consistency and the robustness of the model. Limiting cases of the model have been then derived, showing the influence of different contributions to the line shape.
使用新的测量结果对部分相关速度依赖的 Keilson-Storer(pCSDKS)模型对纯水蒸气的孤立跃迁形状的补充测试进行了[N. H. Ngo 等人,J. Chem. Phys. 136, 154310 (2012)]。后者是使用高灵敏度的腔衰荡光谱仪在室温下和 0.5 到 15 托的压力下记录的,针对七个自展宽 H(2)O 线在 1.6μm 区域。此外,[M. D. De Vizia 等人,Phys. Rev. A 83, 052506 (2011)]在 1.38μm 区域中的 H(2)(18)O 光谱,在 273.15K 和 0.3 到 3.75 托的压力下测量,也被用于与模型进行比较。回想一下,pCSDKS 模型考虑了碰撞引起的速度变化、展宽和移动系数的速度依赖性以及速度和旋转态变化之间的部分相关性。除了应用于输入速度相关线展宽的缩放因子之外,模型的所有参数都固定在先前确定的值。通过观察通过 Voigt 轮廓拟合计算和测量光谱获得的结果来进行预测和实验之间的比较。在不同温度和压力条件下,所有考虑的线都得到了很好的一致性,证实了模型的一致性和稳健性。然后导出了模型的极限情况,显示了对线形状的不同贡献的影响。