The bottom $\bar{\rm MS}$ quark mass from sum rules at next-to-next-to-leading order

dc.creatorBeneke, M.
dc.creatorSigner, A.
dc.date1999-06-24
dc.date1999-11-28
dc.date.accessioned2026-07-07T10:33:53Z
dc.date.available2026-07-07T10:33:53Z
dc.descriptionWe determine the bottom $\bar{\rm MS}$ quark mass $\bar{m}_b$ and the quark mass in the potential subtraction scheme from moments of the $b\bar{b}$ production cross section and from the mass of the Upsilon 1S state at next-to-next-to-leading order in a reorganized perturbative expansion that sums Coulomb exchange to all orders. We find $\bar{m}_b(\bar{m}_b)=(4.25\pm 0.08) $GeV and $m_{b,\rm PS}(2 {GeV})=(4.59\pm 0.08) $GeV for the potential-subtracted mass at the scale 2 GeV, adopting a conservative error estimate.
dc.description14 pages, LaTeX, 2 figures; v2: journal version
dc.identifierhttps://arxiv.org/abs/hep-ph/9906475
dc.identifierhttp://arxiv.org/abs/hep-ph/9906475
dc.identifierPhys.Lett.B471:233-243,1999
dc.identifierdoi:10.1016/S0370-2693(99)01348-9
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/179284
dc.subjectHigh Energy Physics - Phenomenology
dc.titleThe bottom $\bar{\rm MS}$ quark mass from sum rules at next-to-next-to-leading order
dc.typetext

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