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Phase transitions of orientifold gauge theories at large N in finite volume

Asad Naqvi, Timothy Hollowood Orcid Logo

Journal of High Energy Physics, Volume: "04", Issue: 04, Pages: 087 - 087

Swansea University Author: Timothy Hollowood Orcid Logo

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DOI (Published version): 10.1088/1126-6708/2007/04/087

Abstract

In this paper we consider the phase structure of ``orientifold'' gauge theories--obtained from unitary supersymmetric gauge theories by replacing adjoint Majorana fermions by Dirac fermions in the symmetric or anti-symmetric representations--in finite volume S^3 x S^1. If the radius of the...

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Published in: Journal of High Energy Physics
ISSN: 1029-8479
Published: 2006
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URI: https://cronfa.swan.ac.uk/Record/cronfa28526
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first_indexed 2016-06-03T19:16:13Z
last_indexed 2018-02-09T05:12:45Z
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spelling 2016-06-03T14:36:14.1984510 v2 28526 2016-06-03 Phase transitions of orientifold gauge theories at large N in finite volume ea9ca59fc948276ff2ab547e91bdf0c2 0000-0002-3258-320X Timothy Hollowood Timothy Hollowood true false 2016-06-03 SPH In this paper we consider the phase structure of ``orientifold'' gauge theories--obtained from unitary supersymmetric gauge theories by replacing adjoint Majorana fermions by Dirac fermions in the symmetric or anti-symmetric representations--in finite volume S^3 x S^1. If the radius of the S^3 is small the calculations can be performed at weak coupling for any value of the S^1 radius. We demonstrate that there is a confinement/de-confining type of phase transition even when the fermions have periodic (non-thermal) boundary conditions around S^1. At small radius of S^1, the theory is in a phase where charge conjugation and large non-periodic gauge transformation are spontaneously broken. But for large radius of S^1 the phase preseves these symmetries just as in the related supersymmetric Journal Article Journal of High Energy Physics "04" 04 087 087 1029-8479 30 9 2006 2006-09-30 10.1088/1126-6708/2007/04/087 http://inspirehep.net/record/727296 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-06-03T14:36:14.1984510 2016-06-03T14:36:13.9956497 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Asad Naqvi 1 Timothy Hollowood 0000-0002-3258-320X 2
title Phase transitions of orientifold gauge theories at large N in finite volume
spellingShingle Phase transitions of orientifold gauge theories at large N in finite volume
Timothy Hollowood
title_short Phase transitions of orientifold gauge theories at large N in finite volume
title_full Phase transitions of orientifold gauge theories at large N in finite volume
title_fullStr Phase transitions of orientifold gauge theories at large N in finite volume
title_full_unstemmed Phase transitions of orientifold gauge theories at large N in finite volume
title_sort Phase transitions of orientifold gauge theories at large N in finite volume
author_id_str_mv ea9ca59fc948276ff2ab547e91bdf0c2
author_id_fullname_str_mv ea9ca59fc948276ff2ab547e91bdf0c2_***_Timothy Hollowood
author Timothy Hollowood
author2 Asad Naqvi
Timothy Hollowood
format Journal article
container_title Journal of High Energy Physics
container_volume "04"
container_issue 04
container_start_page 087
publishDate 2006
institution Swansea University
issn 1029-8479
doi_str_mv 10.1088/1126-6708/2007/04/087
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/727296
document_store_str 0
active_str 0
description In this paper we consider the phase structure of ``orientifold'' gauge theories--obtained from unitary supersymmetric gauge theories by replacing adjoint Majorana fermions by Dirac fermions in the symmetric or anti-symmetric representations--in finite volume S^3 x S^1. If the radius of the S^3 is small the calculations can be performed at weak coupling for any value of the S^1 radius. We demonstrate that there is a confinement/de-confining type of phase transition even when the fermions have periodic (non-thermal) boundary conditions around S^1. At small radius of S^1, the theory is in a phase where charge conjugation and large non-periodic gauge transformation are spontaneously broken. But for large radius of S^1 the phase preseves these symmetries just as in the related supersymmetric
published_date 2006-09-30T03:34:43Z
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score 11.013148

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