Journal article 926 views
QCD sum rules on the lattice
Nuclear Physics B - Proceedings Supplements, Volume: 63, Issue: 1-3, Pages: 263 - 265
Swansea University Author:
Chris Allton
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DOI (Published version): 10.1016/S0920-5632(97)00740-8
Abstract
We study the work of Leinweber by applying the Continuum Model of QCD Sum Rules (QCDSR) to the analysis of (quenched) lattice correlation functions. We expand upon his work in several areas and find that, while the QCDSR Continuum Model very adequately fits lattice data, it does so only for non-phys...
Published in: | Nuclear Physics B - Proceedings Supplements |
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ISSN: | 09205632 |
Published: |
1998
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URI: | https://cronfa.swan.ac.uk/Record/cronfa28449 |
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2016-08-08T12:22:56.2639767 v2 28449 2016-06-02 QCD sum rules on the lattice de706a260fa1e1e47430693e135f41c7 0000-0003-0795-124X Chris Allton Chris Allton true false 2016-06-02 SPH We study the work of Leinweber by applying the Continuum Model of QCD Sum Rules (QCDSR) to the analysis of (quenched) lattice correlation functions. We expand upon his work in several areas and find that, while the QCDSR Continuum Model very adequately fits lattice data, it does so only for non-physical values of its parameters. The non-relativistic model is found to predict essentially the same form for the correlation functions as the QCDSR Continuum Model but without the latter's restrictions. By fitting lattice data to a general form which includes the non-relativistic quark model as a special case, we confirm it as the model of choice. Journal Article Nuclear Physics B - Proceedings Supplements 63 1-3 263 265 09205632 31 12 1998 1998-12-31 10.1016/S0920-5632(97)00740-8 http://inspirehep.net/record/448452 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-08-08T12:22:56.2639767 2016-06-02T15:06:07.7140749 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Stefano Capitani 1 Chris Allton 0000-0003-0795-124X 2 |
title |
QCD sum rules on the lattice |
spellingShingle |
QCD sum rules on the lattice Chris Allton |
title_short |
QCD sum rules on the lattice |
title_full |
QCD sum rules on the lattice |
title_fullStr |
QCD sum rules on the lattice |
title_full_unstemmed |
QCD sum rules on the lattice |
title_sort |
QCD sum rules on the lattice |
author_id_str_mv |
de706a260fa1e1e47430693e135f41c7 |
author_id_fullname_str_mv |
de706a260fa1e1e47430693e135f41c7_***_Chris Allton |
author |
Chris Allton |
author2 |
Stefano Capitani Chris Allton |
format |
Journal article |
container_title |
Nuclear Physics B - Proceedings Supplements |
container_volume |
63 |
container_issue |
1-3 |
container_start_page |
263 |
publishDate |
1998 |
institution |
Swansea University |
issn |
09205632 |
doi_str_mv |
10.1016/S0920-5632(97)00740-8 |
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/448452 |
document_store_str |
0 |
active_str |
0 |
description |
We study the work of Leinweber by applying the Continuum Model of QCD Sum Rules (QCDSR) to the analysis of (quenched) lattice correlation functions. We expand upon his work in several areas and find that, while the QCDSR Continuum Model very adequately fits lattice data, it does so only for non-physical values of its parameters. The non-relativistic model is found to predict essentially the same form for the correlation functions as the QCDSR Continuum Model but without the latter's restrictions. By fitting lattice data to a general form which includes the non-relativistic quark model as a special case, we confirm it as the model of choice. |
published_date |
1998-12-31T03:34:36Z |
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1763751468716785664 |
score |
11.021648 |