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Phys. Rev. A 77, 022706 (2008) [7 pages]

Nonstatistical enhancement of the 1s2s2p 4P state in electron transfer in 0.5–1.0-MeV∕u C4,5+ + He and Ne collisions

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D. Strohschein1, D. Röhrbein2, T. Kirchner2, S. Fritzsche3,4, J. Baran1, and J. A. Tanis1
1Department of Physics, Western Michigan University, Kalamazoo, Michigan 49008, USA
2Institut für Theoretische Physik, Technische Universität Clausthal, D-38768 Clausthal-Zellerfeld, Germany
3Gesellschaft für Schwerionenforschung (GSI), D-64291 Darmstadt, Germany
4Max-Planck-Institut für Kernphysik, D-69029 Heidelberg, Germany

Received 29 November 2007; published 14 February 2008

Nonstatistical enhancements for formation of the metastable 1s2s2p 4P state compared to the similarly configured 1s2s2p 2P and 1s2s2p 2P+ states are observed following single electron transfer to C4+(1s2s 3S) and double electron transfer to C5+(1s) ions, respectively. Previously, similar enhancements were observed in the population of the 4P metastable state resulting from electron transfer in ∼1 MeV∕u F7,8++He and Ne collisions [ J. A. Tanis et al. Phys. Rev. Lett. 92 133201 (2004)]. The enhancements were attributed to a dynamical Pauli exchange mechanism involving projectile and target electrons having the same spin alignment. Recently, it was suggested that the enhancement might be due to cascade effects following electron transfer to states with n>3. To further understand the observed enhancement of the 4P state, new investigations of Auger emission spectra in collisions of 0.5–1 MeV∕u C4,5+ with He and Ne targets have been conducted. Experimental ratios of the resulting 4P intensities to the sum of the 2P and 2P+ intensities for the collision systems studied give values three to four times larger than expected based solely on spin statistics for single transfer to C4+(1s2s 3S) and double transfer to C5+(1s). Theoretical calculations suggest that about half of the observed enhancement is caused by cascade effects.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.77.022706
DOI:
10.1103/PhysRevA.77.022706
PACS:
34.70.+e, 34.50.Fa