Ionization Dynamics and Exchange Effects in Pure Three-Body Coulomb Scattering
Chapter
Abstract
The measurement of two electrons in coincidence following ionization by electron impact has been performed in a variety of collision geometries [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12]. The different cases yield information on different dynamical aspects of the ionization process. Theoretically, upon analysis of ionization mechanisms certain patterns are deduced for the distributions of the vector momenta of reaction fragments. The major obstacle in a theoretical description of such scattering reactions is the inherent non-separability of many-body Coulomb interacting systems. Thus, these systems have to be represented by approximate Hamiltonians and different approximations may well lead to different interpretations of the scattering dynamics. Here we investigate pure three-body Coulombic systems above the complete break-up threshold. A cluster model is adopted in which the three-body system is approximated by three, spatially decoupled, two-body (Kepler) subsystems. This results in the well known 3C-approximation [13, 14]. Coupling between these, in the configuration space, non-interacting two-body (Rutherford) scattering systems can be introduced via position-dependent Sommerfeld parameters [15]. Analyses of the results yielded by these techniques show that dominant structures in the (theoretical) spectra of the outgoing particles can be assigned to the following underlying mechanisms:
-
Single and double-binary collisions
-
Coulomb density-of-state factors
-
interplay between collisional ionization mechanisms and exchange effects
-
Wannier ionization mode
-
Quantum interference between contributing scattering amplitudes and three-body effects.
Keywords
Incident Energy Scattering Amplitude Incident Direction Ionization Dynamics Outgoing Electron
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
Preview
Unable to display preview. Download preview PDF.
References
- [1]H. Ehrhardt, M. Schulz, T. Tekaat and K. Willmann, Phys. Rev. Lett. 22: 89 (1969).ADSCrossRefGoogle Scholar
- [2]U. Amaldi, A. Egioli, R. Marconero and G. Pizella, RevSci.Instrum. 40: 1001 (1969).ADSCrossRefGoogle Scholar
- [3]B. Lohmann, I.E. McCarthy, A.T. Stelbovic and E. Weigold, Phys. Rev. A 30 758 (1984).Google Scholar
- [4]H. Ehrhardt, G. Knoth, P. Schlemmer and K. Jung, Phys. Lett. 11A: 92 (1985).Google Scholar
- [5]A. Pochat, R.J. Tweed, J. Peresse, C.J. Joachain, B. Piraux and F.W.Jr. Byron, J. Phys. B: At Mol. Phys. 16: L775 (1983).ADSCrossRefGoogle Scholar
- [6]M. Brauner, J.S. Briggs, H. Klar, J.T. Broad, T. Rösel, K. Jung and H. Ehrhardt, J. Phys. B: At. Mol. Phys. 24: 657 (1991).ADSCrossRefGoogle Scholar
- [7]L. Frost, P. Freienstein and W. Wagner, J. Phys. B: At. Mol. Phys. 23: L715 (1990).ADSCrossRefGoogle Scholar
- [8]I.E. McCarthy and E. Weigold, Rep. Prog. Phys. 54: 781 (1991).ADSCrossRefGoogle Scholar
- [9]A.J. Murray and F.H. Read, Phys. Rev. Lett. 69: 2912 (1992).ADSCrossRefGoogle Scholar
- [10]A.J. Murray and F.H. Read Phys. Rev. A 47: 3724 (1993).Google Scholar
- [11]A.J. Murray and F.H. Read J. Phys. B: At. Mol. Phys. 26: L359 (1993).Google Scholar
- [12]J. Berakdar, J. Röder, J.S. Briggs and H. Ehrhardt, J. Phys. B: At. Mol. Phys. in press (1996).Google Scholar
- [13]G. Garibotti and J.E. Miraglia Phys.Rev.A 21: 572 (1980)Google Scholar
- [14] M. Brauner, J.S. Briggs and H. Klar, J Phys. B 22: 2265 (1989).J. Berakdar, Phys. Rev. A. 53: 2314 (1996).Google Scholar
- [16]J. Berakdar and J.S. Briggs, Phys. Rev. Lett. 72: 3799 (1994)ADSCrossRefGoogle Scholar
- J. Berakdar and J.S. Briggs, J. Phys. B 27: 4271 (1994)ADSCrossRefGoogle Scholar
- J. Berakdar and J.S. Briggs, ibid 29: 2289 (1996).Google Scholar
- [17]J. Berakdar Phys. Rev. A (1997) in press.Google Scholar
- [18]J. Berakdar and H. Klar, J. Phys. B 26: 4219 (1993).ADSCrossRefGoogle Scholar
- [19]C.J. Joachain, Comments At. Mol. Phys. 17: 261 (1986).Google Scholar
- [20]J. Röder, private communication (1996).Google Scholar
- [21]G. Wannier, Phys. Rev. 90: 817 (1953).ADSMATHCrossRefGoogle Scholar
- [22]T. Rösel, J. Röder, L. Frost, K. Jung, H. Ehrhardt, S. Jones and D.H. Madison Phys. Rev. A 46: 2539 (1992).Google Scholar
- [23]F.W. Byron Jr., C.J. Joachain, Phys. Rep. 179: 211 (1989).ADSCrossRefGoogle Scholar
Copyright information
© Springer Science+Business Media New York 1997