Electron-electron interaction in projectile electron loss

H.-P. Hülskötter, B. Feinberg, W. E. Meyerhof, A. Belkacem, J. R. Alonso, L. Blumenfeld, E. A. Dillard, H. Gould, N. Guardala, G. F. Krebs, M. A. McMahan, M. E. Rhoades-Brown, B. S. Rude, J. Schweppe, D. W. Spooner, K. Street, P. Thieberger, and H. E. Wegner
Phys. Rev. A 44, 1712 – Published 1 August 1991
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Abstract

In ion-atom collisions where the projectile is ionized, target electrons act not only coherently by screening the target nucleus but they may also act incoherently by directly ejecting a projectile electron. This electron-electron interaction should be relatively most important for targets that have a low nuclear charge, since the cross section for a neutral target is roughly proportional to Zt2+Zt, where Zt2 is the contribution due to the target nucleus and Zt comes from the target electrons. In order to investigate the electron-electron interaction, we have measured and calculated cross sections for Li2+, C5+, and O7+ on H2 and He, Au52+ on H2, He, C, and N2, Au75+ on H2 and N2, U86+ on H2 and He, and U90+ on H2. The collision energies range from 0.75 to 405 MeV/nucleon. The calculations have been performed in the plane-wave Born approximation. We demonstrate that for energies where the target electrons have sufficient kinetic energy in the projectile frame to ionize the projectile, the electron-electron interaction can lead to a significant increase in the total electron-loss cross section.

  • Received 17 December 1990

DOI:https://doi.org/10.1103/PhysRevA.44.1712

©1991 American Physical Society

Authors & Affiliations

H.-P. Hülskötter

  • Department of Physics, Stanford University, Stanford, California 94305

B. Feinberg

  • Accelerator and Fusion Research Division, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

W. E. Meyerhof

  • Department of Physics, Stanford University, Stanford, California 94305

A. Belkacem

  • Department of Physics, Stanford University, Stanford, California 94305
  • Chemical Sciences Division, Building 71-259, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

J. R. Alonso

  • Accelerator and Fusion Research Division, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

L. Blumenfeld

  • Chemical Sciences Division, Building 71-259, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

E. A. Dillard

  • Department of Physics, Stanford University, Stanford, California 94305

H. Gould

  • Chemical Sciences Divison, Building 71-259, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

N. Guardala

  • Department of Physics, Stanford University, Stanford, California 94305

G. F. Krebs and M. A. McMahan

  • Accelerator and Fusion Research Division, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

M. E. Rhoades-Brown

  • Accelerator Development Department, Brookhaven National Laboratory, Upton, New York 11973

B. S. Rude

  • Accelerator and Fusion Research Divison, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

J. Schweppe

  • Chemical Sciences Division, Building 71-259, Lawrence Berkeley Laboratory, One Cyclotron Road, Berkeley, California 94720

D. W. Spooner

  • Department of Physics, Stanford University, Stanford, California 94305

K. Street

  • Berkeley High School, Berkeley, California 94703

P. Thieberger and H. E. Wegner

  • Department of Physics, Brookhaven National Laboratory, Upton, New York 11973

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Vol. 44, Iss. 3 — August 1991

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