dc.contributorUniv Cruzeiro Sul
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.contributorChinese Acad Sci
dc.contributorJoint Inst Nucl Res
dc.contributorArgonne Natl Lab
dc.contributorPeking Univ
dc.date.accessioned2013-09-30T18:57:23Z
dc.date.accessioned2014-05-20T14:11:20Z
dc.date.available2013-09-30T18:57:23Z
dc.date.available2014-05-20T14:11:20Z
dc.date.created2013-09-30T18:57:23Z
dc.date.created2014-05-20T14:11:20Z
dc.date.issued2011-02-14
dc.identifierPhysical Review C. College Pk: Amer Physical Soc, v. 83, n. 2, p. 5, 2011.
dc.identifier0556-2813
dc.identifierhttp://hdl.handle.net/11449/24437
dc.identifier10.1103/PhysRevC.83.025205
dc.identifierWOS:000287367900007
dc.identifierWOS000287367900007.pdf
dc.description.abstractWe compute g(D*D pi) and g(B*B pi) using a framework in which all elements are constrained by Dyson-Schwinger equation studies of QCD and therefore incorporates a consistent, direct, and simultaneous description of light and heavy quarks and the states they may constitute. We link these couplings with the heavy-light-meson leptonic decay constants and thereby obtain g(D*D pi) = 15.9(-1.0)(+2.1) and g(B*B pi) = 30.0(-1.4)(+3.2). From the latter, we infer (g) over cap (B) = 0.37(-0.02)(+0.04). A comparison between g(D*D pi) and g(B*B pi) indicates that when the c quark is a system's heaviest constituent, Lambda(QCD)/m(c)-corrections are not under good control.
dc.languageeng
dc.publisherAmer Physical Soc
dc.relationPhysical Review C
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.titleStrong D* -> D pi and B* -> B pi couplings
dc.typeArtículos de revistas


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