自旋极化电子与Xe原子的弹性碰撞

ELASTIC SCATTERING OF SPIN ELECTRON BY Xe ATOM

在电子与无自旋原子的弹性过程中,可认为电子是在一个向心的有效势V(r)中作相对论运动。由Slater定域近似下的相对论自洽场方法(SCF)求得该有效势。在求得有效势的基础上,采用相对论分波法,计算了极化电子与无自旋原子弹性碰撞的散射振幅,进而计算了微分截面和散射电子自旋极化参量。通过与有关的完全实验比较,明确了本文所采用理论方法的适用范围,即在E≥100eV的能量范围内,本文所用理论方法可较好地描述极化电子与无自旋原子的弹性碰撞过程。

In the processes of electron elastic scartering from spinless atoms, the incident electrons are treated as moving relativistically in an effective central potential V(r). The potential is calculated by relativistic self-consistent-field method with Slater local exchange approximations (i.e. Dirac-Slater SCF). Elastic scattering amplitudes are calculated by relativistic partial-wave expansion method. Then we calculated the differential cross section for electron elastic scattering from Xe atom and the spin polarization parameters. Detail comparisons of the theoretical and complete experimental results show the validity of the theoretical method adopted.