How we discovered the nonet of light scalar mesons

dc.creatorvan Beveren, Eef
dc.creatorRupp, George
dc.date2007-10-16
dc.date2007-10-30
dc.date.accessioned2026-07-07T11:53:37Z
dc.date.available2026-07-07T11:53:37Z
dc.descriptionAs has been confirmed meanwhile by lattice-QCD calculations (see e.g. hep-lat/0702023), the confinement spectrum of non-exotic quark-antiquark systems has its ground state for scalar mesons well above 1 GeV in the Resonance Spectrum Expansion (RSE). For instance, in the S-wave Kaon-pion RSE amplitude, a broad resonance was predicted slightly above 1.4 GeV [hep-ex/0106077], which is confirmed by experiment as the K*0(1430). However, a complete nonet of light scalar mesons was predicted (Zeit.Phys.C30,615 [http://www-spires.slac.stanford.edu/spires/find/hep?key=1573454]) as well, when a model strongly related to the RSE and initially developed to describe the heavy quarkonia resonance spectra (Phys.Rev.D21,772 [http://www-spires.slac.stanford.edu/spires/find/hep?key=363162]) was applied in the light-quark sector. Thus, it was found that the light scalar-meson nonet constitutes part of the ordinary meson spectrum, albeit represented by "extraordinary" [hep-ph/0701038] poles [hep-ex/0106077]. Similar resonances and bound states appear in the charmed sector [hep-ph/0305035], and are predicted in the B-meson spectrum [hep-ph/0312078, hep-ph/0406242]. A recent work [hep-ph/0703286] confirmed the presence of light scalar-meson poles in the RSE amplitude for S-wave and P-wave pion-pion and Kaon-pion contributions to three-body decay processes measured by the BES, E791 and FOCUS collaborations.
dc.descriptionContribution MENU2007 proceedings, 10 pages; Figures added
dc.identifierhttps://arxiv.org/abs/0710.3056
dc.identifierhttp://arxiv.org/abs/0710.3056
dc.identifierECONFC070910:130,2007
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/204603
dc.subjectHigh Energy Physics - Phenomenology
dc.titleHow we discovered the nonet of light scalar mesons
dc.typetext

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