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Strong coupling N=2 gauge theory with arbitrary gauge group

Timothy Hollowood Orcid Logo

Volume: "2", Pages: 335 - 355

Swansea University Author: Timothy Hollowood Orcid Logo

Abstract

A complete definition of the cycles, on the auxiliary Riemann surface defined by Martinec and Warner for describing pure N=2 gauge theories with arbitrary group, is provided. The strong coupling monodromies around the vanishing cycles are shown to arise from a set of dyons which becomes massless at...

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Published: 1997
Online Access: http://inspirehep.net/record/449512
URI: https://cronfa.swan.ac.uk/Record/cronfa28566
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spelling 2016-06-03T14:36:45.0866490 v2 28566 2016-06-03 Strong coupling N=2 gauge theory with arbitrary gauge group ea9ca59fc948276ff2ab547e91bdf0c2 0000-0002-3258-320X Timothy Hollowood Timothy Hollowood true false 2016-06-03 SPH A complete definition of the cycles, on the auxiliary Riemann surface defined by Martinec and Warner for describing pure N=2 gauge theories with arbitrary group, is provided. The strong coupling monodromies around the vanishing cycles are shown to arise from a set of dyons which becomes massless at the singularities. It is shown how the correct weak coupling monodromies are reproduced and how the dyons have charges which are consistent with the spectrum that can be calculated at weak coupling using conventional semi-classical methods. In particular, the magnetic charges are co-root vectors as required by the Dirac-Schwinger-Zwanziger quantization Journal Article "2" 335 355 31 10 1997 1997-10-31 http://inspirehep.net/record/449512 COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2016-06-03T14:36:45.0866490 2016-06-03T14:36:45.0866490 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Timothy Hollowood 0000-0002-3258-320X 1
title Strong coupling N=2 gauge theory with arbitrary gauge group
spellingShingle Strong coupling N=2 gauge theory with arbitrary gauge group
Timothy Hollowood
title_short Strong coupling N=2 gauge theory with arbitrary gauge group
title_full Strong coupling N=2 gauge theory with arbitrary gauge group
title_fullStr Strong coupling N=2 gauge theory with arbitrary gauge group
title_full_unstemmed Strong coupling N=2 gauge theory with arbitrary gauge group
title_sort Strong coupling N=2 gauge theory with arbitrary gauge group
author_id_str_mv ea9ca59fc948276ff2ab547e91bdf0c2
author_id_fullname_str_mv ea9ca59fc948276ff2ab547e91bdf0c2_***_Timothy Hollowood
author Timothy Hollowood
author2 Timothy Hollowood
format Journal article
container_volume "2"
container_start_page 335
publishDate 1997
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/449512
document_store_str 0
active_str 0
description A complete definition of the cycles, on the auxiliary Riemann surface defined by Martinec and Warner for describing pure N=2 gauge theories with arbitrary group, is provided. The strong coupling monodromies around the vanishing cycles are shown to arise from a set of dyons which becomes massless at the singularities. It is shown how the correct weak coupling monodromies are reproduced and how the dyons have charges which are consistent with the spectrum that can be calculated at weak coupling using conventional semi-classical methods. In particular, the magnetic charges are co-root vectors as required by the Dirac-Schwinger-Zwanziger quantization
published_date 1997-10-31T03:34:47Z
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score 11.036706

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