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Measurement of Stark width of some Ar I transitions and the investigation of local thermodynamic equilibrium (LTE) in an atmospheric d.c. argon plasma jet.

机译:大气直流中某些Ar I跃迁的Stark宽度的测量和局部热力学平衡(LTE)的研究氩等离子体射流。

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The Stark widths of seven Ar I transitions are reported. Axial line shape data from an atmospheric d.c. argon plasma jet were Abel-inverted to obtain radial line shapes. The electron-density was determined by Stark width measurements of the hydrogen H{dollar}sbbeta{dollar} transition. In the electron-density region of {dollar}leq{dollar}6 {dollar}times{dollar} 10{dollar}sp{lcub}22{rcub}{dollar} m{dollar}sp{lcub}-3{rcub}{dollar} the experimental Ar I Stark widths are fitted to a linear dependence on the electron-density. Values of Stark width extrapolated to other electron-densities are compared to measurements reported in the literature on the 4s-4p array. Experimental values are up to 45% smaller than those predicted by Griem's theory of Stark broadening. The experimental values of the electron-impact parameter W are reported.; An investigation has been made of the conditions for local thermodynamic equilibrium (LTE) to exist in an atmospheric argon plasma jet. The experiment measures the emission coefficient of seven Ar I transitions and the line shape of the hydrogen H{dollar}sbbeta{dollar} transition. After transforming the side-on data into radial space the excited neutral argon atom-density and the electron-density are determined. It is found LTE does not exist below an electron-density of 6 {dollar}times{dollar} 10{dollar}sp{lcub}33{rcub}{dollar} m{dollar}sp{lcub}-3{rcub}{dollar} in our experimental conditions. The two-temperature Saha equation is shown to give non-physical results for gas temperatures in our electron-density range of 2-6 {dollar}times{dollar} 10{dollar}sp{lcub}22{rcub}{dollar} m{dollar}sp{lcub}-3{rcub}{dollar}. Diffusion effects are important under the experimental conditions studied.
机译:报告了七个Ar I跃迁的Stark宽度。来自大气直流的轴向线形数据将氩气等离子体射流进行Abel倒置以获得径向线形状。电子密度通过氢H {sbbeta {dollar}跃迁的斯塔克宽度测量来确定。在{dollar} leq {dollar} 6 {dollar} times {dollar} 10 {dollar} sp {lcub} 22 {rcub} {dollar} m {dollar} sp {lcub} -3 {rcub}的电子密度区域中{实验} Ar I Stark宽度与电子密度线性相关。将外推到其他电子密度的Stark宽度值与文献中4s-4p阵列中报道的测量值进行比较。实验值比格里姆(Griem)的斯塔克拓宽理论所预测的值小45%。报告了电子冲击参数W的实验值。已经对大气氩等离子体射流中存在局部热力学平衡(LTE)的条件进行了研究。实验测量了七个Ar I跃迁的发射系数和氢H {dollar} sbbeta {dollar}跃迁的线形。将侧面数据转换为径向空间后,即可确定激发的中性氩原子密度和电子密度。发现LTE在电子密度低于6 {dollar}×{dollar} 10 {dollar} sp {lcub} 33 {rcub} {dollar} m {dollar} sp {lcub} -3 {rcub} {在我们的实验条件下。结果表明,在我们的电子密度范围为2-6 {dollar}乘以{dollar} 10 {dollar} sp {lcub} 22 {rcub} {dollar} m的电子密度范围内,两温度的萨哈方程给出的气体温度非物理结果。 {dollar} sp {lcub} -3 {rcub} {dollar}。在研究的实验条件下,扩散作用很重要。

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