Conference Paper/Proceeding/Abstract 916 views
The Running of the bare coupling in SU(N) gauge theories
Volume: "LAT2007", Start page: 280
Swansea University Author: Chris Allton
Abstract
For N>4 there is a first order bulk transition that cleanly separates the strong and weak coupling regimes of SU(N) lattice gauge theories with the plaquette action. We find that in this case the calculated string tension can be readily fitted throughout the weak coupling region by a standard 3-l...
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2007
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http://inspirehep.net/record/763258 |
URI: | https://cronfa.swan.ac.uk/Record/cronfa28424 |
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<?xml version="1.0"?><rfc1807><datestamp>2016-08-08T12:46:37.6047714</datestamp><bib-version>v2</bib-version><id>28424</id><entry>2016-06-02</entry><title>The Running of the bare coupling in SU(N) gauge theories</title><swanseaauthors><author><sid>de706a260fa1e1e47430693e135f41c7</sid><ORCID>0000-0003-0795-124X</ORCID><firstname>Chris</firstname><surname>Allton</surname><name>Chris Allton</name><active>true</active><ethesisStudent>false</ethesisStudent></author></swanseaauthors><date>2016-06-02</date><deptcode>SPH</deptcode><abstract>For N>4 there is a first order bulk transition that cleanly separates the strong and weak coupling regimes of SU(N) lattice gauge theories with the plaquette action. We find that in this case the calculated string tension can be readily fitted throughout the weak coupling region by a standard 3-loop perturbative expression modified by lattice spacing corrections of the expected form. While our fits demand the presence of the latter, they are not constraining enough to tell us which of the various bare coupling schemes is a `good' one, in the sense that terms in the beta-function beyond 3-loops are indeed negligible (in the relevant range of scales). To resolve this ambiguity we work in SU(3), using the Schrodinger Functional coupling scheme as a benchmark, and find that the Parisi mean-field improved coupling scheme matches it very well. Using the latter scheme, we have fitted the values of the string tension that have been calculated for SU(3) to SU(8), to obtain Lambda_MSbar/sqrt(sigma) = 0.503(2)(40) + 0.33(3)(3)/N**2, where the first error is statistical and the second is our estimate of the systematic error from all sources.</abstract><type>Conference Paper/Proceeding/Abstract</type><journal/><volume>"LAT2007"</volume><paginationStart>280</paginationStart><publisher/><keywords/><publishedDay>31</publishedDay><publishedMonth>12</publishedMonth><publishedYear>2007</publishedYear><publishedDate>2007-12-31</publishedDate><doi/><url>http://inspirehep.net/record/763258</url><notes/><college>COLLEGE NANME</college><department>Physics</department><CollegeCode>COLLEGE CODE</CollegeCode><DepartmentCode>SPH</DepartmentCode><institution>Swansea University</institution><apcterm/><lastEdited>2016-08-08T12:46:37.6047714</lastEdited><Created>2016-06-02T15:05:42.8787157</Created><path><level id="1">Faculty of Science and Engineering</level><level id="2">School of Biosciences, Geography and Physics - Physics</level></path><authors><author><firstname>Michael</firstname><surname>Teper</surname><order>1</order></author><author><firstname>Aurora</firstname><surname>Trivini</surname><order>2</order></author><author><firstname>Chris</firstname><surname>Allton</surname><orcid>0000-0003-0795-124X</orcid><order>3</order></author></authors><documents/><OutputDurs/></rfc1807> |
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2016-08-08T12:46:37.6047714 v2 28424 2016-06-02 The Running of the bare coupling in SU(N) gauge theories de706a260fa1e1e47430693e135f41c7 0000-0003-0795-124X Chris Allton Chris Allton true false 2016-06-02 SPH For N>4 there is a first order bulk transition that cleanly separates the strong and weak coupling regimes of SU(N) lattice gauge theories with the plaquette action. We find that in this case the calculated string tension can be readily fitted throughout the weak coupling region by a standard 3-loop perturbative expression modified by lattice spacing corrections of the expected form. While our fits demand the presence of the latter, they are not constraining enough to tell us which of the various bare coupling schemes is a `good' one, in the sense that terms in the beta-function beyond 3-loops are indeed negligible (in the relevant range of scales). To resolve this ambiguity we work in SU(3), using the Schrodinger Functional coupling scheme as a benchmark, and find that the Parisi mean-field improved coupling scheme matches it very well. Using the latter scheme, we have fitted the values of the string tension that have been calculated for SU(3) to SU(8), to obtain Lambda_MSbar/sqrt(sigma) = 0.503(2)(40) + 0.33(3)(3)/N**2, where the first error is statistical and the second is our estimate of the systematic error from all sources. Conference Paper/Proceeding/Abstract "LAT2007" 280 31 12 2007 2007-12-31 http://inspirehep.net/record/763258 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-08-08T12:46:37.6047714 2016-06-02T15:05:42.8787157 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Michael Teper 1 Aurora Trivini 2 Chris Allton 0000-0003-0795-124X 3 |
title |
The Running of the bare coupling in SU(N) gauge theories |
spellingShingle |
The Running of the bare coupling in SU(N) gauge theories Chris Allton |
title_short |
The Running of the bare coupling in SU(N) gauge theories |
title_full |
The Running of the bare coupling in SU(N) gauge theories |
title_fullStr |
The Running of the bare coupling in SU(N) gauge theories |
title_full_unstemmed |
The Running of the bare coupling in SU(N) gauge theories |
title_sort |
The Running of the bare coupling in SU(N) gauge theories |
author_id_str_mv |
de706a260fa1e1e47430693e135f41c7 |
author_id_fullname_str_mv |
de706a260fa1e1e47430693e135f41c7_***_Chris Allton |
author |
Chris Allton |
author2 |
Michael Teper Aurora Trivini Chris Allton |
format |
Conference Paper/Proceeding/Abstract |
container_volume |
"LAT2007" |
container_start_page |
280 |
publishDate |
2007 |
institution |
Swansea University |
college_str |
Faculty of Science and Engineering |
hierarchytype |
|
hierarchy_top_id |
facultyofscienceandengineering |
hierarchy_top_title |
Faculty of Science and Engineering |
hierarchy_parent_id |
facultyofscienceandengineering |
hierarchy_parent_title |
Faculty of Science and Engineering |
department_str |
School of Biosciences, Geography and Physics - Physics{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Biosciences, Geography and Physics - Physics |
url |
http://inspirehep.net/record/763258 |
document_store_str |
0 |
active_str |
0 |
description |
For N>4 there is a first order bulk transition that cleanly separates the strong and weak coupling regimes of SU(N) lattice gauge theories with the plaquette action. We find that in this case the calculated string tension can be readily fitted throughout the weak coupling region by a standard 3-loop perturbative expression modified by lattice spacing corrections of the expected form. While our fits demand the presence of the latter, they are not constraining enough to tell us which of the various bare coupling schemes is a `good' one, in the sense that terms in the beta-function beyond 3-loops are indeed negligible (in the relevant range of scales). To resolve this ambiguity we work in SU(3), using the Schrodinger Functional coupling scheme as a benchmark, and find that the Parisi mean-field improved coupling scheme matches it very well. Using the latter scheme, we have fitted the values of the string tension that have been calculated for SU(3) to SU(8), to obtain Lambda_MSbar/sqrt(sigma) = 0.503(2)(40) + 0.33(3)(3)/N**2, where the first error is statistical and the second is our estimate of the systematic error from all sources. |
published_date |
2007-12-31T03:34:33Z |
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1763751466150920192 |
score |
11.03559 |