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Simultaneous K -Plus- L -Shell Ionization in Light-Ion-Atom Collisions

T. K. Li, R. L. Watson, J. S. Hansen

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Abstract

The probability of simultaneous $K$-plus-$L$-shell ionization in collisions between Ca, Ti, and Fe target atoms and projectiles of 1.5 - 12.5-MeV/amu deuterons and $\ensuremath{\alpha}$ particles has been investigated. The results show that the fraction of $K\ensuremath{\beta}$ x rays emitted in the presence of an $L$-shell vacancy (a) decreases with increasing projectile velocity above a projectile-to-$L$-shell-electron velocity ratio of 1; (b) decreases with increasing target atomic number; and (c) increases with projectile charge (approximately as ${z}_{1}^{2}$). The projectile velocity dependence is in fairly good agreement with a simple classical model based upon the assumption that multiple-vacancy production results from simultaneous Coulomb collisions with $K$-and $L$-shell electrons during the ion's passage through the atom.

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The probability of simultaneous $K$-plus-$L$-shell ionization in collisions between Ca, Ti, and Fe target atoms and projectiles of 1.5 - 12.5-MeV/amu deuterons and $\ensuremath{\alpha}$ particles has been investigated. The results show that the fraction of $K\ensuremath{\beta}$ x rays emitted in the presence of an $L$-shell vacancy (a) decreases with increasing projectile velocity above a projectile-to-$L$-shell-electron velocity ratio of 1; (b) decreases with increasing target atomic number; and (c) increases with projectile charge (approximately as ${z}_{1}^{2}$). The projectile velocity dependence is in fairly good agreement with a simple classical model based upon the assumption that multiple-vacancy production results from simultaneous Coulomb collisions with $K$-and $L$-shell electrons during the ion's passage through the atom.

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Available abstract

The probability of simultaneous $K$-plus-$L$-shell ionization in collisions between Ca, Ti, and Fe target atoms and projectiles of 1.5 - 12.5-MeV/amu deuterons and $\ensuremath{\alpha}$ particles has been investigated. The results show that the fraction of $K\ensuremath{\beta}$ x rays emitted in the presence of an $L$-shell vacancy (a) decreases with increasing projectile velocity above a projectile-to-$L$-shell-electron velocity ratio of 1; (b) decreases with increasing target atomic number; and (c) increases with projectile charge (approximately as ${z}_{1}^{2}$). The projectile velocity dependence is in fairly good agreement with a simple classical model based upon the assumption that multiple-vacancy production results from simultaneous Coulomb collisions with $K$-and $L$-shell electrons during the ion's passage through the atom.

Key concepts: Projectile, Electron capture, Physics, Ionization, Atomic physics, Ion, Electron, Charge (physics)

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