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.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.rights.uri |
info:eu-repo/semantics/openAccess |
|
dc.source |
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.subject |
Física |
|
dc.title |
Bottom quark mass and alpha(s) from the Upsilon system |
|
dc.type |
info:eu-repo/semantics/article |
|
dc.date.updated |
2015-02-25T13:25:41Z |
|
dc.identifier.doi |
http://dx.doi.org/10.1016/S0550-3213(97)00558-0 |
|
dc.identifier.idgrec |
081671 |
|