- Autor(in)
- Referenz
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10 S. A. Edelstein, T. F. Gallagher, Rydberg Atoms, Adv. Atomic and Molec. Phys. 14 (1978) 365
11 S. Feneuille, P. Jacquinot, Atomic Rydberg States, Adv. Atomic and Molec. Phys. 17 (1981) 99
12 L. W. Johnson, R. D. Riess, Numerical Analysis, Addison Wesley Publ. Co., Reading/Massachusetts 1982
13 W. H. Press, B. P. Flannery, S. E. Teukolsky, W. T. Vetterling, Numerical Recipes: The Art of Scientific Computing. Cambridge University Press, Cambridge/England 1986
1 R. Landua, E. Klempt, Phys. Rev. Lett. 48 (1982) 1722;
2 G. Reifenröther, E. Klempt, Nucl. Phys. A503 (1989) 885;
3 H. J. Silverstone, Phys. Rev. A18 (1978) 1853
4 G. Reifenröther, Leichte antiprotonische Atome: Von der Bildung bis zur Vernichtung. Doctoral Dissertation, Johannes-Gutenberg-University Mainz 1989
5 R. Abrines, I. C. Percival, Proc. Phys. Soc. 88 (1966) 861;
6 J. S. Cohen, Phys. Rev. A36 (1987) 2024
7 R. Landua, Untersuchung von Kaskadenprozessen in exotischen Helium-Atomen. Doctoral Dissertation, Johannes-Gutenberg-University Mainz 1980
8 G. Reifenröther, Die Kaskade des myonischen Heliums. Diplom Thesis, Johannes-Gutenberg-University Mainz 1986
9 W. Gordon, Ann. Physik, 5. Serie Vol. 2 (1929) 1031;
G. Reifenröther, E. Klempt, R. Landua, Phys. Lett. B191 (1987) 15;
J. S. Cohen, Phys. Rev. A26 (1982) 3008
Phys. Lett. B203 (1988) 9
Phys. Lett. B245 (1990) 129
Proc. Phys. Soc. 88 (1966) 873;
R. E. Olson, A. Salop, Phys. Rev. A16 (1977) 531;
see also appendix f in L. D. Landau, E. M. Lifschitz, Quantenmechanik (Lehrbuch der Theoretischen Physik, Bd. III), 6. Aufl., Akademie-Verlag, Berlin 1979
- Seitenbereich
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0172 - 0180
- Schlagwort(e)
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<KWD>Exotic atoms and molecules
Zeeman and Stark effects
- Zusammenfsg.
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In a gaseous helium or hydrogen target slow muons or antiprotons are captured into orbits with a high principal quantum number (<I>n</I> = 15 to 50) to form (μ<sup>-</sup> α)<sup>+</sup> ions, (<I>p</I>α)<sup>+</sup> ions, or (<I>pp</I>) atoms respectively. In the subsequent deexcitation process Stark mixing of the intermediary states plays an important role. The successful Mainz Cascade Model assumed Δ<I>n</I> = 0 for the Stark transitions, although formally no such selection rule exists. This note examines the reasons why Δ<I>n</I> ≠ 0 Stark transitions play only a negligible role in the deexcitation cascade.
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- Forschungsartikel