1989Physical Review LettersRequires access

Electron-electron interactions in transfer and excitation in F8+ → H2 collisions

Michael Schulz, J. P. Giese, J.K. Swenson, Sheldon Datz, Peter F. Dittner, H. F. Krause, Harald Schone, C. R. Vane, Malika Benhenni, S. M. Shafroth

Open publisher page 32 citations

Abstract

We have measured projectile Auger electrons emitted after collisions of H-like F with ${\mathrm{H}}_{2}$. The cross sections for emission of KLL, KLM, KLN, and KLO Auger electrons show maxima as a function of the projectile energy. One maximum in the KLL emission cross section is due to resonant transfer and excitation. A second maximum in the cross section for KLL emission as well as the maxima in the emission cross section for the higher-n Auger electrons are attributed to a new transfer and excitation process. This involves excitation of a projectile electron by one target electron accompanied by the capture of a second target electron.

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What this paper is about

We have measured projectile Auger electrons emitted after collisions of H-like F with ${\mathrm{H}}_{2}$. The cross sections for emission of KLL, KLM, KLN, and KLO Auger electrons show maxima as a function of the projectile energy. One maximum in the KLL emission cross section is due to resonant transfer and excitation. A second maximum in the cross section for KLL emission as well as the maxima in the emission cross section for the higher-n Auger electrons are attributed to a new transfer and excitation process. This involves excitation of a projectile electron by one target electron accompanied by the capture of a second target electron.

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Available abstract

We have measured projectile Auger electrons emitted after collisions of H-like F with ${\mathrm{H}}_{2}$. The cross sections for emission of KLL, KLM, KLN, and KLO Auger electrons show maxima as a function of the projectile energy. One maximum in the KLL emission cross section is due to resonant transfer and excitation. A second maximum in the cross section for KLL emission as well as the maxima in the emission cross section for the higher-n Auger electrons are attributed to a new transfer and excitation process. This involves excitation of a projectile electron by one target electron accompanied by the capture of a second target electron.

Key concepts: Atomic physics, Projectile, Excitation, Electron capture, Physics, Electron, Auger, Cross section (physics)

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