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Gasaneo, G; Colavecchia, F D
Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996-1501 (United States); Theoretical Division, Group T-12, MS B268, Los Alamos National Laboratory, Los Alamos, NM 87544 (United States)2003
Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996-1501 (United States); Theoretical Division, Group T-12, MS B268, Los Alamos National Laboratory, Los Alamos, NM 87544 (United States)2003
AbstractAbstract
[en] In this paper we investigate different representations of an arbitrary function in terms of two-body Coulomb eigenfunctions. We discuss the standard energy basis in spherical and parabolic coordinates with the purpose of remarking explicitly that two additional parameters appear both in the Schroedinger equation and in the wavefunctions: the charge and the angular momentum. We introduce the charge and generalized angular momentum Sturmian function representations, which result when the charge or the angular momentum is used as the eigenvalue in the Coulomb Schroedinger equation, respectively. We present the connection between the generalized angular momentum representation and the Kontorovich-Lebedev transform. Finally, we extend the angular momentum representation to six dimensions, which is suitable for further applications in the three-body Coulomb problem
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Source
S0305-4470(03)62313-9; Available online at http://stacks.iop.org/0305-4470/36/8443/a33107.pdf or at the Web site for the Journal of Physics. A, Mathematical and General (ISSN 1361-6447) http://www.iop.org/; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
Journal
Journal of Physics. A, Mathematical and General; ISSN 0305-4470;
; CODEN JPHAC5; v. 36(31); p. 8443-8462

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