首页> 外文期刊>Modern Physics Letters, B. Condensed Matter Physics, Statistical Physics, Applied Physics >INELASTIC COLLISIONS OF POSITRONS WITH BERYLLIUM AND MAGNESIUM IONS
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INELASTIC COLLISIONS OF POSITRONS WITH BERYLLIUM AND MAGNESIUM IONS

机译:正电子与铍和镁离子的弹性碰撞

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The collision of positrons with beryllium and magnesium positive ions is treated for the first time as a three-channel problem with the assumption that the elastic, ground-positronium and excited-positronium formation channels are open. A one-valence-electron model for the targets, based on the Clementi–Roetti Slater basis functions, as well as an improved coupled-static approach allowing for the polarization of the excited positronium, are used for calculating the partial cross-sections of eight partial waves (corresponding to 0≤l≤7, where l is the total angular momentum of the scattering problem considered). The calculations are carried out, in each case, at 19 values of the incident energy lying above the excited positronium formation threshold (i.e. above 16.42 eV in e+–Be+ scattering and above 13.02 eV in e+–Mg+ scattering). The total elastic cross-sections of e+–Mg+ scattering show a peak around the ionization threshold of Mg+ (at 14.723 eV) but for e+–Be+ scattering, display a peak at 90 eV (remember that the ionization threshold of Be+ is 18.2 eV). Although the resulting total collisional positronium formation cross-sections are smaller than the elastic ones, their relatively large values should draw the attention of experimental and theoretical physicists to the field of positron–ion collisions.
机译:正电子与铍和镁正离子的碰撞首次被视为三通道问题,其前提是假设弹性,接地-正电子和正电子-正电子形成通道是开放的。基于Clementi-Roetti Slater基函数的目标单价电子模型以及允许激发的正电子极化的改进的耦合静电方法,可用于计算八个电子的部分截面分波(对应于0≤l≤7,其中l是所考虑的散射问题的总角动量)。在每种情况下,都在高于激发的正电子形成阈值(即e + –Be +散射中高于16.42 eV,e + –Mg +散射中高于13.02 eV)的19个入射能量值下进行计算。 e + –Mg +散射的总弹性横截面在Mg +的电离阈值附近(在14.723 eV处)显示一个峰,但对于e + –Be +散射,在90 eV处显示一个峰(请记住Be +的电离阈值为18.2 eV) 。尽管所产生的总碰撞正电子形成截面小于弹性截面,但其相对较大的值应引起实验和理论物理学家对正离子碰撞领域的关注。

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