dc.contributor | Univ Cruzeiro Sul | |
dc.contributor | Universidade Estadual Paulista (Unesp) | |
dc.contributor | Chinese Acad Sci | |
dc.contributor | Joint Inst Nucl Res | |
dc.contributor | Argonne Natl Lab | |
dc.contributor | Peking Univ | |
dc.date.accessioned | 2013-09-30T18:57:23Z | |
dc.date.accessioned | 2014-05-20T14:11:20Z | |
dc.date.available | 2013-09-30T18:57:23Z | |
dc.date.available | 2014-05-20T14:11:20Z | |
dc.date.created | 2013-09-30T18:57:23Z | |
dc.date.created | 2014-05-20T14:11:20Z | |
dc.date.issued | 2011-02-14 | |
dc.identifier | Physical Review C. College Pk: Amer Physical Soc, v. 83, n. 2, p. 5, 2011. | |
dc.identifier | 0556-2813 | |
dc.identifier | http://hdl.handle.net/11449/24437 | |
dc.identifier | 10.1103/PhysRevC.83.025205 | |
dc.identifier | WOS:000287367900007 | |
dc.identifier | WOS000287367900007.pdf | |
dc.description.abstract | We 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.language | eng | |
dc.publisher | Amer Physical Soc | |
dc.relation | Physical Review C | |
dc.rights | Acesso restrito | |
dc.source | Web of Science | |
dc.title | Strong D* -> D pi and B* -> B pi couplings | |
dc.type | Artículos de revistas | |