The coplanar (e, 3e) relative cross sections for double ionization of argon have been measured at an electron impact energy of E0 = 561.4 eV and under equal energy sharing among the two ¡¥ejected¡¦ electrons, Eb = Ec = 9 eV. The scattering angle is fixed to ƒáa = 1.5, corresponding to a momentum transfer K = 0.4 au to the target. The experimental results have been compared with calculations in the first Born approximation, which include only firstorder processes in the target¡Vprojectile interaction. The comparison shows severe deviations between the experimental and theoretical results. These deviations are much larger than the ones previously observed in helium under comparable kinematics. To fill this gap between theory and experiment, a decisive improvement in the theory is needed. This can be achieved by improving the first-order calculations and by including higher-order processes such as the two-step mechanism, or even new mechanisms, for instance the simultaneous ejection of the pair of target electrons.

Deviations between experimental and theoretical results in Ar (e,3e) double ionization

L Avaldi
2003

Abstract

The coplanar (e, 3e) relative cross sections for double ionization of argon have been measured at an electron impact energy of E0 = 561.4 eV and under equal energy sharing among the two ¡¥ejected¡¦ electrons, Eb = Ec = 9 eV. The scattering angle is fixed to ƒáa = 1.5, corresponding to a momentum transfer K = 0.4 au to the target. The experimental results have been compared with calculations in the first Born approximation, which include only firstorder processes in the target¡Vprojectile interaction. The comparison shows severe deviations between the experimental and theoretical results. These deviations are much larger than the ones previously observed in helium under comparable kinematics. To fill this gap between theory and experiment, a decisive improvement in the theory is needed. This can be achieved by improving the first-order calculations and by including higher-order processes such as the two-step mechanism, or even new mechanisms, for instance the simultaneous ejection of the pair of target electrons.
2003
Istituto di Nanotecnologia - NANOTEC
Istituto di Struttura della Materia - ISM - Sede Roma Tor Vergata
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/38315
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