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Solution to Faddeev equations with two-body experimental amplitudes as input and application to J(P)=1/2(+), S=0 baryon resonances

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Solution to Faddeev equations with two-body experimental amplitudes as input and application to J(P)=1/2(+), S=0 baryon resonances

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dc.contributor.author Martínez Torres, Alberto
dc.contributor.author Khemchandani, K. P.
dc.contributor.author Oset Báguena, Eulogio
dc.date.accessioned 2015-09-07T10:48:24Z
dc.date.available 2015-09-07T10:48:24Z
dc.date.issued 2009
dc.identifier.citation Martínez Torres, Alberto Khemchandani, K. P. Oset Báguena, Eulogio 2009 Solution to Faddeev equations with two-body experimental amplitudes as input and application to J(P)=1/2(+), S=0 baryon resonances Physical Review C 79 6 065207
dc.identifier.uri http://hdl.handle.net/10550/46879
dc.description.abstract We solve the Faddeev equations for the two meson-one baryon system ππN and coupled channels using the experimental two-body t-matrices for the πN interaction as input and unitary chiral dynamics to describe the interaction between the rest of coupled channels. In addition to the N∗(1710) obtained before with the ππN channel, we obtain, for Jπ=1/2+ and total isospin of the three-body system I=1/2, a resonance peak whose mass is around 2080 MeV and width of 54 MeV, while for I=3/2 we find a peak around 2126 MeV and 42 MeV of width. These two resonances can be identified with the N∗(2100) and the Δ(1910), respectively. We obtain another peak in the isospin 1/2 configuration, around 1920 MeV which can be interpreted as a resonance in the Na0(980) and Nf0(980) systems.
dc.language.iso eng
dc.relation.ispartof Physical Review C, 2009, vol. 79, num. 6, p. 065207
dc.subject Física
dc.title Solution to Faddeev equations with two-body experimental amplitudes as input and application to J(P)=1/2(+), S=0 baryon resonances
dc.type journal article es_ES
dc.date.updated 2015-09-07T10:48:25Z
dc.identifier.doi 10.1103/PhysRevC.79.065207
dc.identifier.idgrec 056200
dc.rights.accessRights open access es_ES

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