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dc.contributor.authorGarrido, Eduardo-
dc.contributor.authorFedorov, D.V.-
dc.contributor.authorJensen, A.S.-
dc.contributor.authorFynbo, H.O.U.-
dc.date.accessioned2009-08-14T11:00:48Z-
dc.date.available2009-08-14T11:00:48Z-
dc.date.issued2005-02-07-
dc.identifier.citationNuclear Physics A 748 (1-2): (2005) 27–38en_US
dc.identifier.issn0375-9474-
dc.identifier.urihttp://hdl.handle.net/10261/15983-
dc.description12 pages, 1 figure.--PACS nrs.: 21.45.+v; 31.15.Ja; 25.70.Ef.--Available online on Nov 10, 2004.--ArXiv pre-print available at: http://arxiv.org/abs/nucl-th/0411078v1en_US
dc.description.abstractSequential three-body decay proceeds via spatially confined quasi-stationary two-body configurations. Direct three-body decay populates the three-body continuum without intermediate steps. The relative importance of these decay modes is discussed in a schematic model employing only Coulomb or centrifugal barrier potentials. Decisive dimensionless charge, mass and energy ratios are derived. Sequential decay is usually favored for charged particles. Small charge and small mass of high energy is preferably emitted first. Without Coulomb potential the sequential decay is favored except when both resonance energy and intermediate two-body energy are large.en_US
dc.format.extent129407 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoengen_US
dc.publisherElsevieren_US
dc.rightsclosedAccessen_US
dc.subject[PACS] Few-body systemsen_US
dc.subject[PACS] Hyperspherical methodsen_US
dc.subject[PACS] Resonancesen_US
dc.titleAnatomy of three-body decay I: schematic modelsen_US
dc.typeartículoen_US
dc.identifier.doi10.1016/j.nuclphysa.2004.10.014-
dc.description.peerreviewedPeer revieweden_US
dc.relation.publisherversionhttp://dx.doi.org/10.1016/j.nuclphysa.2004.10.014en_US
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