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Quark masses from lattice QCD at the next-to-leading order / G. Martinelli, V. Lubicz, M. Crisafulli, E. Franco, Marco Ciuchini, Chris Allton

Nuclear Physics B, Volume: 431, Issue: 3, Pages: 667 - 685

Swansea University Author: Chris Allton

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Abstract

Using the results of several quenched lattice simulations, we predict the value of the strange and charm quark masses in the continuum at the next-to-leading order, $m~{\overline{MS}}_s(\mu=2\,\, \rm{GeV})= (127 \pm 18)\,\, \rm{MeV}$ and $m~{\overline{MS}}_{ch}(\mu=2 \,\,\rm{GeV})=(1.47 \pm 0.28)\,\...

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Published in: Nuclear Physics B
ISSN: 05503213
Published: 1994
Online Access: Check full text

URI: https://cronfa.swan.ac.uk/Record/cronfa28447
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spelling 2016-08-08T12:24:13.6881245 v2 28447 2016-06-02 Quark masses from lattice QCD at the next-to-leading order de706a260fa1e1e47430693e135f41c7 0000-0003-0795-124X Chris Allton Chris Allton true false 2016-06-02 SPH Using the results of several quenched lattice simulations, we predict the value of the strange and charm quark masses in the continuum at the next-to-leading order, $m~{\overline{MS}}_s(\mu=2\,\, \rm{GeV})= (127 \pm 18)\,\, \rm{MeV}$ and $m~{\overline{MS}}_{ch}(\mu=2 \,\,\rm{GeV})=(1.47 \pm 0.28)\,\, \rm{GeV}$. The errors quoted above have been estimated by taking into account the original statistical error of the lattice results and the uncertainties coming from the matching of the lattice to the continuum theory. A detailed presentation of the relevant formulae at the next-to-leading order and a discussion of the main sources of errors is also presented. Journal Article Nuclear Physics B 431 3 667 685 05503213 31 12 1994 1994-12-31 10.1016/0550-3213(94)90218-6 http://inspirehep.net/record/373987 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-08-08T12:24:13.6881245 2016-06-02T15:06:04.6252551 College of Science Physics G. Martinelli 1 V. Lubicz 2 M. Crisafulli 3 E. Franco 4 Marco Ciuchini 5 Chris Allton 0000-0003-0795-124X 6
title Quark masses from lattice QCD at the next-to-leading order
spellingShingle Quark masses from lattice QCD at the next-to-leading order
Chris, Allton
title_short Quark masses from lattice QCD at the next-to-leading order
title_full Quark masses from lattice QCD at the next-to-leading order
title_fullStr Quark masses from lattice QCD at the next-to-leading order
title_full_unstemmed Quark masses from lattice QCD at the next-to-leading order
title_sort Quark masses from lattice QCD at the next-to-leading order
author_id_str_mv de706a260fa1e1e47430693e135f41c7
author_id_fullname_str_mv de706a260fa1e1e47430693e135f41c7_***_Chris, Allton
author Chris, Allton
author2 G. Martinelli
V. Lubicz
M. Crisafulli
E. Franco
Marco Ciuchini
Chris Allton
format Journal article
container_title Nuclear Physics B
container_volume 431
container_issue 3
container_start_page 667
publishDate 1994
institution Swansea University
issn 05503213
doi_str_mv 10.1016/0550-3213(94)90218-6
college_str College of Science
hierarchytype
hierarchy_top_id collegeofscience
hierarchy_top_title College of Science
hierarchy_parent_id collegeofscience
hierarchy_parent_title College of Science
department_str Physics{{{_:::_}}}College of Science{{{_:::_}}}Physics
url http://inspirehep.net/record/373987
document_store_str 0
active_str 0
description Using the results of several quenched lattice simulations, we predict the value of the strange and charm quark masses in the continuum at the next-to-leading order, $m~{\overline{MS}}_s(\mu=2\,\, \rm{GeV})= (127 \pm 18)\,\, \rm{MeV}$ and $m~{\overline{MS}}_{ch}(\mu=2 \,\,\rm{GeV})=(1.47 \pm 0.28)\,\, \rm{GeV}$. The errors quoted above have been estimated by taking into account the original statistical error of the lattice results and the uncertainties coming from the matching of the lattice to the continuum theory. A detailed presentation of the relevant formulae at the next-to-leading order and a discussion of the main sources of errors is also presented.
published_date 1994-12-31T03:43:29Z
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