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Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models

Kazutoshi Ohta, Timothy Hollowood Orcid Logo

Journal of High Energy Physics, Volume: "02", Issue: 02, Pages: 042 - 042

Swansea University Author: Timothy Hollowood Orcid Logo

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DOI (Published version): 10.1088/1126-6708/2005/02/042

Abstract

We consider the vacuum structure of the finite N=2 theory with N_f=2N fundamental hypermultiplets broken to N=1 by a superpotential for the adjoint chiral multiplet. We do this in two ways: firstly, by compactification to three dimensions, in which case the effective superpotential is the Hamiltonia...

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Published in: Journal of High Energy Physics
ISSN: 1029-8479
Published: 2004
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URI: https://cronfa.swan.ac.uk/Record/cronfa28533
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first_indexed 2016-06-03T19:16:15Z
last_indexed 2018-02-09T05:12:46Z
id cronfa28533
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spelling 2016-06-03T14:36:18.8940811 v2 28533 2016-06-03 Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models ea9ca59fc948276ff2ab547e91bdf0c2 0000-0002-3258-320X Timothy Hollowood Timothy Hollowood true false 2016-06-03 SPH We consider the vacuum structure of the finite N=2 theory with N_f=2N fundamental hypermultiplets broken to N=1 by a superpotential for the adjoint chiral multiplet. We do this in two ways: firstly, by compactification to three dimensions, in which case the effective superpotential is the Hamiltonian of an integrable spin chain. In the second approach, we consider the Dijkgraaf-Vafa holomorphic matrix model. We prove that the two approaches agree as long as the couplings of the two theories are related in a particular way involving an infinite series of instanton terms. The case of gauge group SU(2) with N_f=4 is considered in greater Journal Article Journal of High Energy Physics "02" 02 042 042 1029-8479 31 5 2004 2004-05-31 10.1088/1126-6708/2005/02/042 http://inspirehep.net/record/649929 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-06-03T14:36:18.8940811 2016-06-03T14:36:18.7068799 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Kazutoshi Ohta 1 Timothy Hollowood 0000-0002-3258-320X 2
title Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
spellingShingle Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
Timothy Hollowood
title_short Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
title_full Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
title_fullStr Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
title_full_unstemmed Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
title_sort Vacua of N = 1 Supersymmetric QCD from Spin Chains and Matrix Models
author_id_str_mv ea9ca59fc948276ff2ab547e91bdf0c2
author_id_fullname_str_mv ea9ca59fc948276ff2ab547e91bdf0c2_***_Timothy Hollowood
author Timothy Hollowood
author2 Kazutoshi Ohta
Timothy Hollowood
format Journal article
container_title Journal of High Energy Physics
container_volume "02"
container_issue 02
container_start_page 042
publishDate 2004
institution Swansea University
issn 1029-8479
doi_str_mv 10.1088/1126-6708/2005/02/042
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/649929
document_store_str 0
active_str 0
description We consider the vacuum structure of the finite N=2 theory with N_f=2N fundamental hypermultiplets broken to N=1 by a superpotential for the adjoint chiral multiplet. We do this in two ways: firstly, by compactification to three dimensions, in which case the effective superpotential is the Hamiltonian of an integrable spin chain. In the second approach, we consider the Dijkgraaf-Vafa holomorphic matrix model. We prove that the two approaches agree as long as the couplings of the two theories are related in a particular way involving an infinite series of instanton terms. The case of gauge group SU(2) with N_f=4 is considered in greater
published_date 2004-05-31T03:34:44Z
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score 11.013148

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