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Quark condensate in massless QCD from planar equivalence

Adi Armoni Orcid Logo, Graham Shore, Gabriele Veneziano

Nucl. Phys. B, Volume: 740, Issue: 1-2, Pages: 23 - 35

Swansea University Authors: Adi Armoni Orcid Logo, Graham Shore

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DOI (Published version): 10.1016/j.nuclphysb.2006.01.044

Abstract

A previous estimate of the quark condensate in one-flavour mass- less QCD from the known value of the gluino condensate in super Yang-Mills (SYM) theory is extended to Nf > 1 by considering the large-N limit of an SU(N) gauge theory with one flavour in the antisymmetric representation and nf...

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Published in: Nucl. Phys. B
Published: 2006
Online Access: http://arxiv.org/abs/hep-ph/0511143
URI: https://cronfa.swan.ac.uk/Record/cronfa17504
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first_indexed 2014-03-21T02:30:08Z
last_indexed 2018-02-09T04:51:11Z
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spelling 2015-11-25T22:58:14.7053332 v2 17504 2014-03-20 Quark condensate in massless QCD from planar equivalence 3f75faad0563a2d3b191191a2efee956 0000-0002-8105-0645 Adi Armoni Adi Armoni true false 28a24f55687c82d6f3ee378ead3cf234 Graham Shore Graham Shore true false 2014-03-20 SPH A previous estimate of the quark condensate in one-flavour mass- less QCD from the known value of the gluino condensate in super Yang-Mills (SYM) theory is extended to Nf &#62; 1 by considering the large-N limit of an SU(N) gauge theory with one flavour in the antisymmetric representation and nf = Nf − 1 extra flavours in the fundamental representation. We argue that, even at nf ̸= 0, suitably chosen correlators in this theory can be mapped to those of SYM as N → ∞. We give arguments why this correspondence should be particularly good for Nf = 3 and compare our prediction with available (real and Monte Carlo) data. Journal Article Nucl. Phys. B 740 1-2 23 35 17 4 2006 2006-04-17 10.1016/j.nuclphysb.2006.01.044 http://arxiv.org/abs/hep-ph/0511143 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2015-11-25T22:58:14.7053332 2014-03-20T22:00:39.0601146 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Adi Armoni 0000-0002-8105-0645 1 Graham Shore 2 Gabriele Veneziano 3
title Quark condensate in massless QCD from planar equivalence
spellingShingle Quark condensate in massless QCD from planar equivalence
Adi Armoni
Graham Shore
title_short Quark condensate in massless QCD from planar equivalence
title_full Quark condensate in massless QCD from planar equivalence
title_fullStr Quark condensate in massless QCD from planar equivalence
title_full_unstemmed Quark condensate in massless QCD from planar equivalence
title_sort Quark condensate in massless QCD from planar equivalence
author_id_str_mv 3f75faad0563a2d3b191191a2efee956
28a24f55687c82d6f3ee378ead3cf234
author_id_fullname_str_mv 3f75faad0563a2d3b191191a2efee956_***_Adi Armoni
28a24f55687c82d6f3ee378ead3cf234_***_Graham Shore
author Adi Armoni
Graham Shore
author2 Adi Armoni
Graham Shore
Gabriele Veneziano
format Journal article
container_title Nucl. Phys. B
container_volume 740
container_issue 1-2
container_start_page 23
publishDate 2006
institution Swansea University
doi_str_mv 10.1016/j.nuclphysb.2006.01.044
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://arxiv.org/abs/hep-ph/0511143
document_store_str 0
active_str 0
description A previous estimate of the quark condensate in one-flavour mass- less QCD from the known value of the gluino condensate in super Yang-Mills (SYM) theory is extended to Nf &#62; 1 by considering the large-N limit of an SU(N) gauge theory with one flavour in the antisymmetric representation and nf = Nf − 1 extra flavours in the fundamental representation. We argue that, even at nf ̸= 0, suitably chosen correlators in this theory can be mapped to those of SYM as N → ∞. We give arguments why this correspondence should be particularly good for Nf = 3 and compare our prediction with available (real and Monte Carlo) data.
published_date 2006-04-17T03:20:13Z
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score 11.037056

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