No Cover Image

Journal article 854 views

Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories

Giuseppe Carlino, Kenichi Konishi, Prem Kumar Orcid Logo, Hitoshi Murayama

Nuclear Physics B, Volume: 608, Issue: 1-2, Pages: 51 - 102

Swansea University Author: Prem Kumar Orcid Logo

Full text not available from this repository: check for access using links below.

DOI (Published version): 10.1016/S0550-3213(01)00253-X

Abstract

We determine the vacuum structure and phases of N = 1 theories obtained via a mass μ for the adjoint chiral superfield in N = 2, SO(nc) SQCD. For large number of flavors these theories have two groups of vacua. The first exhibits dynamical breaking of flavor symmetry USp(2nf) → U(nf) and arises as a...

Full description

Published in: Nuclear Physics B
Published: 2001
URI: https://cronfa.swan.ac.uk/Record/cronfa16136
Tags: Add Tag
No Tags, Be the first to tag this record!
first_indexed 2013-09-26T11:46:07Z
last_indexed 2020-07-16T18:28:35Z
id cronfa16136
recordtype SURis
fullrecord <?xml version="1.0"?><rfc1807><datestamp>2020-07-16T14:40:36.2672982</datestamp><bib-version>v2</bib-version><id>16136</id><entry>2013-09-20</entry><title>Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories</title><swanseaauthors><author><sid>087fd097167d724ce1b13cb285741ef5</sid><ORCID>0000-0003-0867-4213</ORCID><firstname>Prem</firstname><surname>Kumar</surname><name>Prem Kumar</name><active>true</active><ethesisStudent>false</ethesisStudent></author></swanseaauthors><date>2013-09-20</date><deptcode>SPH</deptcode><abstract>We determine the vacuum structure and phases of N = 1 theories obtained via a mass &#x3BC; for the adjoint chiral superfield in N = 2, SO(nc) SQCD. For large number of flavors these theories have two groups of vacua. The first exhibits dynamical breaking of flavor symmetry USp(2nf) &#x2192; U(nf) and arises as a relevant deformation of a non- trivial superconformal theory. These are in the confined phase. The second group, in an IR-free phase with unbroken flavor symmetry, is produced from a Coulomb branch singularity with Seiberg&#x2019;s dual gauge symmetry. In the large-&#x3BC; regime both groups of vacua are well-described by dual quarks and mesons, and dynamical symmetry breaking in the first group occurs via meson condensation. We follow the description of these vacua from weak to strong coupling and demonstrate a nontrivial agreement between the phases and the number of vacua in the two regimes. We construct the semiclassical monopole flavor multiplets and argue that their multiplicity is consistent with the number of N = 1 vacua.</abstract><type>Journal Article</type><journal>Nuclear Physics B</journal><volume>608</volume><journalNumber>1-2</journalNumber><paginationStart>51</paginationStart><paginationEnd>102</paginationEnd><publisher/><keywords/><publishedDay>31</publishedDay><publishedMonth>8</publishedMonth><publishedYear>2001</publishedYear><publishedDate>2001-08-31</publishedDate><doi>10.1016/S0550-3213(01)00253-X</doi><url/><notes/><college>COLLEGE NANME</college><department>Physics</department><CollegeCode>COLLEGE CODE</CollegeCode><DepartmentCode>SPH</DepartmentCode><institution>Swansea University</institution><apcterm/><lastEdited>2020-07-16T14:40:36.2672982</lastEdited><Created>2013-09-20T11:08:05.4027793</Created><path><level id="1">Faculty of Science and Engineering</level><level id="2">School of Biosciences, Geography and Physics - Physics</level></path><authors><author><firstname>Giuseppe</firstname><surname>Carlino</surname><order>1</order></author><author><firstname>Kenichi</firstname><surname>Konishi</surname><order>2</order></author><author><firstname>Prem</firstname><surname>Kumar</surname><orcid>0000-0003-0867-4213</orcid><order>3</order></author><author><firstname>Hitoshi</firstname><surname>Murayama</surname><order>4</order></author></authors><documents/><OutputDurs/></rfc1807>
spelling 2020-07-16T14:40:36.2672982 v2 16136 2013-09-20 Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories 087fd097167d724ce1b13cb285741ef5 0000-0003-0867-4213 Prem Kumar Prem Kumar true false 2013-09-20 SPH We determine the vacuum structure and phases of N = 1 theories obtained via a mass μ for the adjoint chiral superfield in N = 2, SO(nc) SQCD. For large number of flavors these theories have two groups of vacua. The first exhibits dynamical breaking of flavor symmetry USp(2nf) → U(nf) and arises as a relevant deformation of a non- trivial superconformal theory. These are in the confined phase. The second group, in an IR-free phase with unbroken flavor symmetry, is produced from a Coulomb branch singularity with Seiberg’s dual gauge symmetry. In the large-μ regime both groups of vacua are well-described by dual quarks and mesons, and dynamical symmetry breaking in the first group occurs via meson condensation. We follow the description of these vacua from weak to strong coupling and demonstrate a nontrivial agreement between the phases and the number of vacua in the two regimes. We construct the semiclassical monopole flavor multiplets and argue that their multiplicity is consistent with the number of N = 1 vacua. Journal Article Nuclear Physics B 608 1-2 51 102 31 8 2001 2001-08-31 10.1016/S0550-3213(01)00253-X COLLEGE NANME Physics COLLEGE CODE SPH Swansea University 2020-07-16T14:40:36.2672982 2013-09-20T11:08:05.4027793 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Giuseppe Carlino 1 Kenichi Konishi 2 Prem Kumar 0000-0003-0867-4213 3 Hitoshi Murayama 4
title Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
spellingShingle Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
Prem Kumar
title_short Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
title_full Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
title_fullStr Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
title_full_unstemmed Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
title_sort Vacuum structure and flavor symmetry breaking in supersymmetric SO(nc) gauge theories
author_id_str_mv 087fd097167d724ce1b13cb285741ef5
author_id_fullname_str_mv 087fd097167d724ce1b13cb285741ef5_***_Prem Kumar
author Prem Kumar
author2 Giuseppe Carlino
Kenichi Konishi
Prem Kumar
Hitoshi Murayama
format Journal article
container_title Nuclear Physics B
container_volume 608
container_issue 1-2
container_start_page 51
publishDate 2001
institution Swansea University
doi_str_mv 10.1016/S0550-3213(01)00253-X
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
document_store_str 0
active_str 0
description We determine the vacuum structure and phases of N = 1 theories obtained via a mass μ for the adjoint chiral superfield in N = 2, SO(nc) SQCD. For large number of flavors these theories have two groups of vacua. The first exhibits dynamical breaking of flavor symmetry USp(2nf) → U(nf) and arises as a relevant deformation of a non- trivial superconformal theory. These are in the confined phase. The second group, in an IR-free phase with unbroken flavor symmetry, is produced from a Coulomb branch singularity with Seiberg’s dual gauge symmetry. In the large-μ regime both groups of vacua are well-described by dual quarks and mesons, and dynamical symmetry breaking in the first group occurs via meson condensation. We follow the description of these vacua from weak to strong coupling and demonstrate a nontrivial agreement between the phases and the number of vacua in the two regimes. We construct the semiclassical monopole flavor multiplets and argue that their multiplicity is consistent with the number of N = 1 vacua.
published_date 2001-08-31T03:18:26Z
_version_ 1763750452247134208
score 11.013731