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f_(600), ρ(800), ρ(770) and K*(892), quark mass dependence from unitarized SU(3) Chiral Perturbation Theory

dc.contributor.authorNebreda Manjón, Jenifer
dc.contributor.authorPeláez Sagredo, José Ramón
dc.date.accessioned2023-06-20T04:02:56Z
dc.date.available2023-06-20T04:02:56Z
dc.date.issued2010-08
dc.description©American Institute of Physics. International Conference on Hadron Spectroscopy (13. 2009.Tallahassee, Filadelfia). Work partially supported by Spanish Ministerio de Educación y Ciencia contracts: FPA2007-29115-E, FPA2008-00592 and FIS2006-03438, U.Complutense/Banco Santander grant PR34/07-15875-BSCH and UCM-BSCH GR58/08 910309 as well as the European Community-Research Infrastructure Integrating Activity “Study of Strongly Interacting Matter” (HadronPhysics2, Grant Agreement n. 227431) under the Seventh Framework Programme of the EU.
dc.description.abstractWe study the strange and non-strange quark mass dependence of the parameters of the f_0(600), κ(800), ρ(770) and K*(892) resonances generated from elastic meson-meson scattering using unitarized one-loop Chiral Perturbation Theory. We fit simultaneously all experimental scattering data up to 0.8-1 GeV together ith lattice results on decay constants and scattering lengths up to a pion mass of 440 MeV. Then, the strange and non-strange quark masses are varied from the chiral limit up to values of interest for lattice studies. In these amplitudes, the mass and width of the ρ(770) and K* (892) present a similar and smooth quark mass dependence. In contrast, both scalars present a similar non-analyticity at high quark masses. Nevertheless the f_0(600) dependence on both quark masses is stronger than for the к(800) and the vectors. We also confirm the lattice assumption of quark mass independence of the vector two-meson coupling that, in contrast, is violated for scalars
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipUnión Europea. FP7
dc.description.sponsorshipMinisterio de Educación y Ciencia
dc.description.sponsorshipU.Complutense/Banco Santander
dc.description.sponsorshipFIS2006-03438
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/35133
dc.identifier.doi10.1063/1.3483380
dc.identifier.issn0094-243X
dc.identifier.officialurlhttp://dx.doi.org/10.1063/1.3483380
dc.identifier.relatedurlhttp://scitation.aip.org
dc.identifier.urihttps://hdl.handle.net/20.500.14352/44848
dc.issue.number5
dc.journal.titleAIP conference proceedings
dc.language.isoeng
dc.publisherAmerican Institute of Physics
dc.relation.projectIDHadronPhysics2 (227431)
dc.relation.projectIDFPA2007-29115-E
dc.relation.projectIDFPA2008-00592
dc.relation.projectIDFIS2006-03438
dc.relation.projectIDPR34/07-15875-BSCH
dc.relation.projectIDUCM-BSCH GR58/08 910309
dc.rights.accessRightsopen access
dc.subject.cdu51-73
dc.subject.ucmFísica-Modelos matemáticos
dc.subject.ucmFísica matemática
dc.titlef_(600), ρ(800), ρ(770) and K*(892), quark mass dependence from unitarized SU(3) Chiral Perturbation Theory
dc.typejournal article
dc.volume.number1257
dcterms.references1. C. Hanhart, J. R. Peláez and G. Rios, Phys. Rev. Lett. 100, 152001 (2008). 2. J. Nebreda and J. R. Peláez in preparation. 3. A. Dobado and J. R. Peláez, Phys. Rev. D 47 (1993) 4883; Phys. Rev. D 56 (1997) 3057. 4. A. Gómez Nicola and J. R. Peláez, Phys. Rev. D 65, 054009 (2002). 5. S. R. Beane et al. [NPLQCD Collaboration], Phys. Rev. D 77, 094507 (2008) and Phys. Rev. D 77, 014505 (2008); S. R. Beane et al. Phys. Rev. D 74, 114503 (2006); Ph. Boucaud et al. [ETM collaboration], Comput. Phys. Commun. 179, 695 (2008). 6. G. Amoros, J. Bijnens and P. Talavera, Nucl. Phys. B 602, 87 (2001). 7. J. R. Peláez, Mod. Phys. Lett. A 19, 2879 (2004). 8. S. Aoki et al. [CP-PACS Collaboration], Phys. Rev. D 76, 094506 (2007).
dspace.entity.typePublication
relation.isAuthorOfPublication70900239-cb8b-49f3-931f-9dc6a8b7d8d5
relation.isAuthorOfPublication.latestForDiscovery70900239-cb8b-49f3-931f-9dc6a8b7d8d5

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