首页> 外文期刊>Journal of Physics, B. Atomic, Molecular and Optical Physics: An Institute of Physics Journal >Low energy differential and integral electron-impact cross sections for the 2s(2)2p(4) P-3 -> 2p(3)3s S-3(o) excitation in atomic oxygen
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Low energy differential and integral electron-impact cross sections for the 2s(2)2p(4) P-3 -> 2p(3)3s S-3(o) excitation in atomic oxygen

机译:在原子氧中2s(2)2p(4)P-3-> 2p(3)3s S-3(o)激发的低能微分和积分电子碰撞截面

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0Differential and integral cross sections (ICSs) for 2s(2)2p(4) P-3 --> 2p(3)3s S-3(o) excitation in atomic oxygen have been measured at electron-impact energies of 15, 17.5, 20, 22.5 and 27.5 eV. Differential measurements were conducted with a conventional electron energy-loss spectrometer and a microwave discharge source of atomic oxygen. Relative differential cross sections (DCSs) were determined between 15 and 30 eV impact energy. With the help of theoretical predictions of the shape of the DCS at large angles, measured results were extrapolated to 1800 scattering angle and relative ICSs were deduced. The relative excitation function was normalized to the 30 eV impact energy ICS given by Kanik et al (2001 J. Phys. B: At. MoL Opt. Phys. 34 2647). Normalization of the ICS values allowed the measured DCSs to be put on the absolute scale. Theoretical calculations of the DCSs were carried out using the R-matrix with the pseudostates approach. A total of 22 spectroscopic bound and autoionizing states, together with 19 pseudostates, were included in the close-coupling expansion. The pseudostates were chosen to simulate continuum target states. Theoretical results, along with other available experimental data, have been compared with the current experimental results. [References: 17]
机译:0 2s(2)2p(4)P-3-> 2p(3)3s的微分截面和积分截面(ICSs)在原子冲击能为15、17.5的情况下已测量出原子氧中的S-3(o)激发,20、22.5和27.5 eV。用常规的电子能量损失谱仪和原子氧的微波放电源进行差示测量。在15至30 eV的冲击能量之间确定了相对微分截面(DCS)。借助对大角度DCS形状的理论预测,将测量结果外推到1800散射角,并推导出相对ICS。相对激励函数被标准化为Kanik等人给出的30eV冲击能量ICS(2001 J. Phys。B:At。MoL Opt。Phys。34 2647)。 ICS值的归一化允许将测量的DCS置于绝对标度上。 DCS的理论计算是使用R-矩阵和伪态方法进行的。紧密耦合扩展中总共包括22个光谱的束缚态和自电离态,以及19个伪态。选择伪状态以模拟连续目标状态。理论结果以及其他可用的实验数据已与当前的实验结果进行了比较。 [参考:17]

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