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   <dc:title>f_(600), ρ(800), ρ(770) and K*(892), quark mass dependence from unitarized SU(3) Chiral Perturbation Theory</dc:title>
   <dc:creator>Nebreda Manjón, Jenifer</dc:creator>
   <dc:creator>Peláez Sagredo, José Ramón</dc:creator>
   <dc:subject>51-73</dc:subject>
   <dc:subject>Física-Modelos matemáticos</dc:subject>
   <dc:subject>Física matemática</dc:subject>
   <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>
   <dc:description>We 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>
   <dc:description>Unión Europea. FP7</dc:description>
   <dc:description>Ministerio de Educación y Ciencia</dc:description>
   <dc:description>U.Complutense/Banco Santander</dc:description>
   <dc:description>FIS2006-03438</dc:description>
   <dc:description>Depto. de Física Teórica</dc:description>
   <dc:description>Fac. de Ciencias Físicas</dc:description>
   <dc:description>TRUE</dc:description>
   <dc:description>pub</dc:description>
   <dc:date>2023-06-20T04:02:56Z</dc:date>
   <dc:date>2023-06-20T04:02:56Z</dc:date>
   <dc:date>2010-08</dc:date>
   <dc:type>journal article</dc:type>
   <dc:identifier>https://hdl.handle.net/20.500.14352/44848</dc:identifier>
   <dc:identifier>0094-243X</dc:identifier>
   <dc:identifier>10.1063/1.3483380</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>HadronPhysics2 (227431)</dc:relation>
   <dc:relation>FPA2007-29115-E</dc:relation>
   <dc:relation>FPA2008-00592</dc:relation>
   <dc:relation>FIS2006-03438</dc:relation>
   <dc:relation>PR34/07-15875-BSCH</dc:relation>
   <dc:relation>UCM-BSCH GR58/08 910309</dc:relation>
   <dc:rights>open access</dc:rights>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>American Institute of Physics</dc:publisher>
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