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Effects of autoionization in electron loss from helium-like highly charged ions in collisions with photons and fast atomic particles

机译:自电离对氦原子电子损失的影响   带电离子与光子和快速原子粒子碰撞

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摘要

We study theoretically single electron loss from helium-like highly chargedions involving excitation and decay of autoionizing states of the ion. Electronloss is caused by either photo absorption or the interaction with a fast atomicparticle (a bare nucleus, a neutral atom, an electron). The interactions withthe photon field and the fast particles are taken into account in the firstorder of perturbation theory. Two initial states of the ion are considered:$1s^2$ and $(1s2s)_{J=0}$. We analyze in detail how the shape of the emissionpattern depends on the atomic number $Z_{I}$ of the ion discussing, inparticular, the inter-relation between electron loss via photo absorption anddue to the impact of atomic particles in collisions at modest relativistic andextreme relativistic energies. According to our results, in electron loss fromthe $1s^2$ state autoionization may substantially influence the shape of theemission spectra only up to $Z_{I} \approx 35-40$. A much more prominent roleis played by autoionization in electron loss from $(1s2s)_{J=0}$ where it notonly strongly affect the shape of the emission pattern but also maysubstantially increase the total loss cross section.
机译:我们从理论上研究像氦一样的高电荷的单电子损失,其中涉及离子的自电离态的激发和衰减。电子损耗是由光吸收或与快速原子粒子(裸核,中性原子,电子)的相互作用引起的。一阶扰动理论考虑了与光子场和快速粒子的相互作用。考虑离子的两个初始状态:$ 1s ^ 2 $和$(1s2s)_ {J = 0} $。我们详细分析了发射图形的形状如何取决于离子的原子数$ Z_ {I} $,尤其讨论了在相对论中,通过光吸收引起的电子损失与碰撞中原子粒子的影响之间的相互关系。和极端的相对论能量。根据我们的结果,从$ 1s ^ 2 $状态自动电离的电子损失可能仅在直到$ Z_ {I} \大约35-40 $时才实质上影响发射光谱的形状。自电离作用在$(1s2s)_ {J = 0} $的电子损失中起着更为重要的作用,它不仅强烈影响发射图形的形状,而且还可能显着增加总损失截面。

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