压力诱导35C10和16O2毫米波长旋转跃迁的N2展宽

D. Brinza, H. Pickett, E. Cohen
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引用次数: 0

摘要

C10作为一种催化物质在平流层臭氧耗竭中的重要性目前引起人们的兴趣。C10是氯原子与臭氧快速反应的产物,它在高层大气中的分布已由Logan等人模拟[1]。平流层C10的体积混合比的测量现在是用机载微波发射光谱仪进行的。167 GHz、241 GHz和278 GHz的J=9/2-7/2、J= 13/2-11/2和J= 15/2-13/2跃迁曲线对碰撞线形函数中压力展宽参数γ的取值较为敏感。Waters等人[2]通过线性插值HF (γ = 4.5 MHz/mbar, μ = 1.8D)和CO (γ = 2.4 MHz/mbar, μ = 0.11D)的值,估计C10 (μ = 1.24D)的γ = 3.8 MHz/mbar。本文概述了用v = 0 2Π3/2 35C10的J=9/2-11/2和J=13/2-15/2跃迁的N2线展宽法测定207K和370K间C10的γ。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Pressure Induced Broadening of 35C10 and 16O2 Millimeter-Wavelength Rotational Transitions By N2
The importance of C10 as a catalytic species in stratospheric ozone depletion is of current interest. A product of the fast reaction of atomic chlorine and ozone, C10 distribution in the upper atmosphere has been modeled by Logan et al. [1]. Measurement of volume mixing ratios of stratospheric C10 is now performed by means of aircraft-based microwave emission spectrometers. The profiles obtained by analysis of the J=9/2-7/2, J = 13/2-11/2 and J = 15/2-13/2 transitions at 167 GHz, 241 GHz, and 278 GHz respectively are sensitive to the value of the pressure broadening parameter γ used in the collisional line shape function. Waters et al. [2] estimated γ = 3.8 MHz/mbar for C10 (μ = 1.24D) by linear interpolation of values for HF (γ = 4.5 MHz/mbar, μ = 1.8D) and CO (γ = 2.4 MHz/mbar, μ = 0.11D). This summary describes the determination of γ for C10 between 207K and 370K by N2 line broadening of the J=9/2-11/2 and J=13/2-15/2 transitions of v = 0 2Π3/2 35C10.
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