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Comparison of theoretical and absolute experimental fully differential cross sections for ion-atom impact ionization

机译:离子-原子碰撞电离的理论和绝对实验全微分截面的比较

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摘要

We report fully differential cross section (FDCS) calculations and absolute measurements for ion-atom impact ionization. Using the COLTRIMS (cold target recoil ion momentum spectroscopy) method we have obtained absolute FDCS both in the scattering plane as well as out of the scattering plane for 100 MeV amu(- 1) C6+ ionization of helium FDCS results are presented for different projectile scattering angles and ejected electron energies. The measurements are compared with a theoretical calculation employing an asymptotically exact three body final state wavefunction that contains all active two particle subsystem interactions to infinite order in perturbation theory. For the active electron a Hartree-Fock (HF) bound state wavefunction is used for the initial state and numerical continuum state eigenfunctions of a HF potential for the ion are used for the final state In the scattering plane these theoretical results are in very good agreement with experiment for small and intermediate momentum transfer. However some significant discrepancies are found for large momentum transfer and outside the scattering plane. These discrepancies disappear upon comparison with successively less differential cross sections.
机译:我们报告了离子原子碰撞电离的全微分截面(FDCS)计算和绝对测量。使用COLTRIMS(冷目标反冲离子动量谱)方法,我们获得了100 MeV amu(-1)氦氦气C6 +电离的散射平面内和散射平面外的绝对FDCS FDCS结果针对不同的弹丸散射角度和射出的电子能量。将测量结果与采用渐近精确的三体最终状态波函数的理论计算进行比较,该函数包含微扰理论中所有活跃的两个粒子子系统之间的无限次相互作用。对于活性电子,将Hartree-Fock(HF)束缚态波函数用于初始状态,并将离子的HF势的数值连续态本征函数用于最终状态。在散射平面中,这些理论结果非常吻合进行中小动量传递的实验。但是,对于大的动量传递和散射平面之外,发现了一些显着差异。通过与相继较小的横截面比较,这些差异消失了。

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