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

We 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 Co...

Descripción completa

Detalles Bibliográficos
Autores principales: Beneke, M., Signer, A.
Lenguaje:eng
Publicado: 1999
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(99)01348-9
http://cds.cern.ch/record/391636
_version_ 1780893747993640960
author Beneke, M.
Signer, A.
author_facet Beneke, M.
Signer, A.
author_sort Beneke, M.
collection CERN
description We 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.
id cern-391636
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
record_format invenio
spelling cern-3916362023-03-12T06:04:48Zdoi:10.1016/S0370-2693(99)01348-9http://cds.cern.ch/record/391636engBeneke, M.Signer, A.The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading orderParticle Physics - PhenomenologyWe 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.We determine the bottom MS quark mass m b and the quark mass in the potential subtraction scheme from moments of the b 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 m b ( m b )=(4.25±0.08) GeV and m b, PS (2 GeV )=(4.59±0.08) GeV for the potential-subtracted mass at the scale 2 GeV, adopting a conservative error estimate.We 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.hep-ph/9906475CERN-TH-99-163DTP-99-60CERN-TH-99-163DTP-99-60oai:cds.cern.ch:3916361999-06-25
spellingShingle Particle Physics - Phenomenology
Beneke, M.
Signer, A.
The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title_full The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title_fullStr The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title_full_unstemmed The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title_short The bottom $\overline{MS}$ quark mass from sum rules at next-to-next-to-leading order
title_sort bottom $\overline{ms}$ quark mass from sum rules at next-to-next-to-leading order
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(99)01348-9
http://cds.cern.ch/record/391636
work_keys_str_mv AT benekem thebottomoverlinemsquarkmassfromsumrulesatnexttonexttoleadingorder
AT signera thebottomoverlinemsquarkmassfromsumrulesatnexttonexttoleadingorder
AT benekem bottomoverlinemsquarkmassfromsumrulesatnexttonexttoleadingorder
AT signera bottomoverlinemsquarkmassfromsumrulesatnexttonexttoleadingorder

Ejemplares similares