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dc.contributor.author | Jamin, Matthias | |
dc.contributor.author | Pich Zardoya, Antonio | |
dc.date.accessioned | 2015-02-25T13:25:41Z | |
dc.date.available | 2015-02-25T13:25:41Z | |
dc.date.issued | 1997 | |
dc.identifier.citation | Jamin, Matthias Pich Zardoya, Antonio 1997 Bottom quark mass and alpha(s) from the Upsilon system Nuclear Physics B 507 1-2 334 352 | |
dc.identifier.uri | http://hdl.handle.net/10550/42301 | |
dc.description.abstract | The mass of the bottom quark and the strong coupling constant alpha(s) are determined from QCD moment sum rules for the T system. Two analyses are performed using both the pole mass M-b as well as the mass m(b) in the <(MS)over bar> scheme. In the pole-mass scheme large perturbative corrections resulting from Coulombic contributions have to be resummed. In the <(MS)over bar> scheme this can be avoided by an appropriate choice for the renormalization scale. For the bottom quark mass we obtain M-b = 4.60+/-0.02 GeV and m(b)(m(b)) = 4.13+/-0.00 GeV. Our combined result from both determinations for the strong coupling is alpha(s)(M-Z) = 0.119+/-0.008. | |
dc.language.iso | eng | |
dc.relation.ispartof | Nuclear Physics B, 1997, vol. 507, num. 1-2, p. 334-352 | |
dc.subject | Física | |
dc.title | Bottom quark mass and alpha(s) from the Upsilon system | |
dc.type | journal article | es_ES |
dc.date.updated | 2015-02-25T13:25:41Z | |
dc.identifier.doi | 10.1016/S0550-3213(97)00558-0 | |
dc.identifier.idgrec | 081671 | |
dc.rights.accessRights | open access | es_ES |