D. Filipović, B. Marinković, V. Pejčev, L. Vŭsković
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引用次数: 19
摘要
给出了氩的最低三个电子态的绝对归一化微分电子碰撞激发截面(dscs):最低共振4s[3/2]1 (Paschen记法中的1s4)态和两个相邻的亚稳态4s[3/2]2和4s'[½]0 (Paschen记法中的155和1s3)态。直接,即没有级联贡献,实验得到了在20、40、50和80 eV下4s[3/2]1态和在20和40 eV冲击能下4s[3/2]2和4s'[1 /2] 0态的激发截面。测量的散射角在5°~ 150°之间,角分辨率优于2°。确定了r = DCS(4s[3/2]2)/DCS(4s'[1 /2] 0)和r' = DCS(4s[3/2]1)/DCS(4s'[1 /2]1)的比值,并对已有的实验和理论结果进行了比较。相对于45 '[1 / 2]1状态的DCS,建立了绝对DCS量表(Filipovic et al . 2000 J. Phys;B:。利用能量损失光谱中的峰值强度比。将dcs外推到0°和180°,并对产量积分、动量传递和粘度截面进行数值积分。
Electron-impact excitation of argon: II. The lowest resonance 4s[3/2]1 and metastable 4s[3/2]2 and 4s'[½]0 states
Absolute normalized differential electron-impact excitation cross sections (DCSs) are presented for the lowest three electronic states of argon: the lowest resonance 4s[3/2]1 (1s4 in Paschen's notation) state and two neighbouring metastable 4s[3/2]2 and 4s'[½]0 (1s5 and 1s3 in Paschen's notation) states. Direct, i.e. free of a cascade contribution, excitation cross sections were obtained experimentally for the 4s[3/2]1 state at 20, 40, 50 and 80 eV and for the 4s[3/2]2 and 4s'[½]0 states at 20 and 40 eV impact energies. The measurements were performed at scattering angles between 5° and 150° with an angular resolution of better than 2°. The ratios: r = DCS(4s[3/2]2)/DCS(4s'[½]0) and r' = DCS(4s[3/2]1)/DCS(4s'[½]1) were determined and compared with other available experimental and theoretical results. The absolute DCS scale was established with respect to DCSs of the 4s'[½]1 state (Filipovic et al 2000 J. Phys. B: At. Mol. Opt. Phys. 33 677) using the peak intensity ratios in the energy-loss spectra. The DCSs were extrapolated to 0° and 180° and numerically integrated to yield integral, momentum transfer and viscosity cross sections.