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Angular-momentum transfer in collisional ionization

Journal Article · · Physical Review A; (United States)
 [1];  [2]
  1. Department of Physics and Center for Theoretical Studies of Physical Systems, Clark Atlanta University, Atlanta, Georgia 30314 (United States)
  2. School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332 (United States)

The double-differential cross sections for ionization in [ital e][sup [minus]]+H([ital nl]) collisions are reported as a function of the impact energy [ital E] of the projectile, final energy [ital E][sub [ital f]], and angular momentum [ital L][sub [ital f]] of the ejected electron. This process is assumed to occur via an energy-changing and angular-momentum-changing binary collision between the Rydberg electron in a prepared state ([ital nl]) and the projectile electron [ital e][sup [minus]] or H(1[ital s]). The atomic projectile can also be excited during this process. Systematic trends in the variation of the classical ionization cross sections with final angular momentum [ital L][sub [ital f]] of the ejected electron are discussed and are in accord with a previous quantal treatment, whereby the nondipole ([Delta][ital l][gt]1) transitions are much more important in the low- and intermediate-energy range of relative motion, and that the value of the final angular momentum of the ejected electron depends mainly on the initial value of the principal quantum number [ital n] of the Rydberg atom.

OSTI ID:
7295900
Journal Information:
Physical Review A; (United States), Journal Name: Physical Review A; (United States) Vol. 50:1; ISSN 1050-2947; ISSN PLRAAN
Country of Publication:
United States
Language:
English

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