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首页> 外文期刊>Journal of Physics, B. Atomic, Molecular and Optical Physics: An Institute of Physics Journal >Polarization of Lyman-α and Balmer-α emission in proton-hydrogen collisions: A study using first-order Born-Faddeev-type equations
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Polarization of Lyman-α and Balmer-α emission in proton-hydrogen collisions: A study using first-order Born-Faddeev-type equations

机译:质子-氢碰撞中Lyman-α和Balmer-α发射的极化:使用一阶Born-Faddeev型方程的研究

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摘要

A three-body Born-Faddeev model is devised to calculate the total cross sections of Balmer-α and Lyman-α emissions, for the excitation of hydrogen atoms by proton impact in the energy range of 100keV-7 MeV. In addition, the polarization alignment factor A _(20)is calculated and compared against available experimental data to further test the theory. Specifically, here we use the Faddeev-Watson-Lovelace formalism to study the excitation of atomic hydrogen from its ground state to the excited states of n = 2 and 3 and magnetic sublevels l = 0, 1 and 2, wherever applicable. The first-order electronic, A ~((1)) _e, and the first-order nuclear, A ~((1)) _n, amplitudes are considered in order to calculate the excitation transition matrix (T _(PT)), while a near-the-shell condition is assumed throughout. In addition, our results were used to calculate the first-order form factors. The present results are compared, where possible, with those of other theoretical and experimental works that are currently available in the literature.
机译:设计了一个三体Born-Faddeev模型来计算Balmer-α和Lyman-α发射的总横截面,以通过质子碰撞在100keV-7 MeV的能量范围内激发氢原子。另外,计算了偏振取向因子A _(20)并将其与可用的实验数据进行比较以进一步验证该理论。具体来说,这里我们使用Faddeev-Watson-Lovelace形式主义来研究原子氢从其基态到n = 2和3以及磁子能级l = 0、1和2的激发态的激发。考虑一阶电子振幅A〜((1))_e和一阶核振幅A〜((1))_n,以计算激发跃迁矩阵(T _(PT)),而整个过程都假设是近乎空壳的情况。此外,我们的结果用于计算一阶形状因数。在可能的情况下,将本结果与文献中当前可用的其他理论和实验结果进行比较。

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