首页> 外文期刊>Molecular physics >Special issue: 22nd colloquium on high-resolution molecular spectroscopy HRMS Dijon 2011 (Part 2) Experimental and theoretical studies of room-temperature sub-millimetre CH_3 ~(35)Cl line shapes broadened by H_2
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Special issue: 22nd colloquium on high-resolution molecular spectroscopy HRMS Dijon 2011 (Part 2) Experimental and theoretical studies of room-temperature sub-millimetre CH_3 ~(35)Cl line shapes broadened by H_2

机译:特刊:第22届高分辨率分子光谱学术讨论会HRMS第戎2011(第2部分)室温亚毫米CH_3〜(35)Cl线形被H_2加宽的实验和理论研究

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Hydrogen-broadening coefficients of methyl chloride rotational lines J=6→7, 10→11, 17→18, 22→23 and 31→32 at 296K are measured as functions of the quantum number K using a sensitive frequency-modulation technique. As expected for this light perturber, the observed line shapes are well described by Voigt profile model. A clear dependence of the collisional broadening on K is observed for most transitions. From a detailed study of the K-components of the transition J=6→7 situated at 186GHz no variation of the broadening of the hyperfine components related to 35Cl quadrupole is stated. Given the absence of refined ab initio computed potential energy surfaces and the impracticality of quantum-mechanical calculations for the considered molecular system, theoretical values of these broadening coefficients are estimated by a semi-classical approach with exact trajectories and a model interaction potential including both long-range and short-range (atom-atom) interactions of the active molecule rigorously treated as a symmetric top. It is shown that the short-range forces yield important contributions to the collisional line width for all values of the rotational quantum numbers J and K. Various models are also tested for the isotropic part of the interaction potential which governs the relative translational motion. It is demonstrated that for the very light perturbing molecule H2 the calculated line widths, practically independent from the rotational quantum number J (for K≤J), are particularly sensitive to the position and slope of the repulsive wall. Modifications required in the semi-classical formalism for a correct application of the cumulant expansion are also tested and it is stated that no difference is observed for the CH_3Cl-H_2 system characterised by quite weak interactions.
机译:使用灵敏的频率调制技术,测量了在296K时氯甲烷旋转线J = 6→7、10→11、17→18、22→23和31→32的氢扩散系数,作为量子数K的函数。如对此光干扰器所预期的那样,Voigt轮廓模型很好地描述了观察到的线形。在大多数过渡过程中,观察到碰撞加宽对K的明显依赖性。通过对位于186 GHz的跃迁J = 6→7的K分量进行的详细研究,未发现与35Cl四极杆有关的超精细分量的展宽变化。考虑到缺乏精确的从头算起的势能面并且考虑分子系统的量子力学计算不切实际,这些扩展系数的理论值是通过半经典方法估算的,它们具有精确的轨迹和模型相互作用势,包括长活性分子的短程和短程(原子-原子)相互作用被严格视为对称顶部。结果表明,对于旋转量子数J和K的所有值,短程力对碰撞线宽度产生了重要贡献。还针对相互作用势的各向同性部分(支配相对平移运动)测试了各种模型。结果表明,对于非常轻的扰动分子H2,计算出的线宽实际上与旋转量子数J(对于K≤J)无关,它对斥壁的位置和斜率特别敏感。还测试了半古典形式主义中正确应用累积量扩展所需的修改,并且指出,对于以相互作用非常弱为特征的CH_3Cl-H_2系统,未观察到差异。

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