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| Journal Article | PreJuSER-33607 |
; ;
2003
Springer
Wien [u.a.]
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Please use a persistent id in citations: http://hdl.handle.net/2128/10718 doi:10.1007/s00601-003-0019-x
Abstract: The Faddeev equation for the three-body bound state with two- and three-body forces is solved directly as three-dimensional integral equation. The numerical feasibility and stability of the algorithm, which does not employ partial wave decomposition is demonstrated. The three-body binding energy and the full wave function are calculated with Malfliet-Tjon-type two-body potentials and scalar two-meson exchange three-body forces. For two- and three- body forces of ranges and strengths typical of nuclear forces the single-particle momentum distribution and the two-body correlation function are similar to the ones found for realistic nuclear forces.
Keyword(s): three-body problem ; force ; bound state: binding energy ; integral equations: solution ; bound state: wave function ; potential ; momentum spectrum ; correlation function: two-particle ; numerical calculations ; tables
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