3d N = 3 generalized Giveon-Kutasov duality
A bstract We generalize the Giveon-Kutasov duality for the 3d N = 3 U( N ) k,k + nN Chern-Simons matter gauge theory with F fundamental hypermultiplets by introducing SU( N ) and U(1) Chern-Simons levels differently. We study the supersymmetric partition functions and the superconformal indices of t...
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container_title | The journal of high energy physics |
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creator | Kubo, Naotaka Nii, Keita |
description | A
bstract
We generalize the Giveon-Kutasov duality for the 3d
N
= 3 U(
N
)
k,k
+
nN
Chern-Simons matter gauge theory with
F
fundamental hypermultiplets by introducing SU(
N
) and U(1) Chern-Simons levels differently. We study the supersymmetric partition functions and the superconformal indices of the duality, which supports the validity of the duality proposal. From the duality, we can map out the low-energy phases: for example, confinement appears for
F
+
k
−
N
= −
n
= 1 or
N
= 2
F
=
k
= −
n
= 2. For
F
+
k
−
N <
0, supersymmetry is spontaneously broken, which is in accord with the fact that the partition function vanishes. In some cases, the theory shows supersymmetry enhancement to 3d
N
= 4. For
k
= 0, we comment on the magnetic description dual to the so-called “ugly” theory, where the usual decoupled sector is still interacting with others for
n
≠ 0. We argue that the SU(
N
)
0
“ugly-good” duality (which corresponds to the
n →
∞ limit in our setup) is closely related to the S-duality of the 4d
N
= 2 SU(
N
) superconformal gauge theory with 2
N
fundamental hypermultiplets. By reducing the number of flavors via real masses, we suggest possible ways to flow to the “bad” theories. |
doi_str_mv | 10.1007/JHEP04(2022)158 |
format | Article |
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bstract
We generalize the Giveon-Kutasov duality for the 3d
N
= 3 U(
N
)
k,k
+
nN
Chern-Simons matter gauge theory with
F
fundamental hypermultiplets by introducing SU(
N
) and U(1) Chern-Simons levels differently. We study the supersymmetric partition functions and the superconformal indices of the duality, which supports the validity of the duality proposal. From the duality, we can map out the low-energy phases: for example, confinement appears for
F
+
k
−
N
= −
n
= 1 or
N
= 2
F
=
k
= −
n
= 2. For
F
+
k
−
N <
0, supersymmetry is spontaneously broken, which is in accord with the fact that the partition function vanishes. In some cases, the theory shows supersymmetry enhancement to 3d
N
= 4. For
k
= 0, we comment on the magnetic description dual to the so-called “ugly” theory, where the usual decoupled sector is still interacting with others for
n
≠ 0. We argue that the SU(
N
)
0
“ugly-good” duality (which corresponds to the
n →
∞ limit in our setup) is closely related to the S-duality of the 4d
N
= 2 SU(
N
) superconformal gauge theory with 2
N
fundamental hypermultiplets. By reducing the number of flavors via real masses, we suggest possible ways to flow to the “bad” theories.</description><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP04(2022)158</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Classical and Quantum Gravitation ; Elementary Particles ; Gauge theory ; High energy physics ; Partitions (mathematics) ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Regular Article - Theoretical Physics ; Relativity Theory ; String Theory ; Supersymmetry ; Symmetry</subject><ispartof>The journal of high energy physics, 2022-04, Vol.2022 (4), p.158</ispartof><rights>The Author(s) 2022</rights><rights>The Author(s) 2022. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-2169-5812</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP04(2022)158$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://doi.org/10.1007/JHEP04(2022)158$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,864,27923,27924,41119,42188,51575</link.rule.ids></links><search><creatorcontrib>Kubo, Naotaka</creatorcontrib><creatorcontrib>Nii, Keita</creatorcontrib><title>3d N = 3 generalized Giveon-Kutasov duality</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A
bstract
We generalize the Giveon-Kutasov duality for the 3d
N
= 3 U(
N
)
k,k
+
nN
Chern-Simons matter gauge theory with
F
fundamental hypermultiplets by introducing SU(
N
) and U(1) Chern-Simons levels differently. We study the supersymmetric partition functions and the superconformal indices of the duality, which supports the validity of the duality proposal. From the duality, we can map out the low-energy phases: for example, confinement appears for
F
+
k
−
N
= −
n
= 1 or
N
= 2
F
=
k
= −
n
= 2. For
F
+
k
−
N <
0, supersymmetry is spontaneously broken, which is in accord with the fact that the partition function vanishes. In some cases, the theory shows supersymmetry enhancement to 3d
N
= 4. For
k
= 0, we comment on the magnetic description dual to the so-called “ugly” theory, where the usual decoupled sector is still interacting with others for
n
≠ 0. We argue that the SU(
N
)
0
“ugly-good” duality (which corresponds to the
n →
∞ limit in our setup) is closely related to the S-duality of the 4d
N
= 2 SU(
N
) superconformal gauge theory with 2
N
fundamental hypermultiplets. By reducing the number of flavors via real masses, we suggest possible ways to flow to the “bad” theories.</description><subject>Classical and Quantum Gravitation</subject><subject>Elementary Particles</subject><subject>Gauge theory</subject><subject>High energy physics</subject><subject>Partitions (mathematics)</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Regular Article - Theoretical Physics</subject><subject>Relativity Theory</subject><subject>String Theory</subject><subject>Supersymmetry</subject><subject>Symmetry</subject><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNpFkE1Lw0AURQdBsFbXbgfcKBJ9bzIfmYULKbVVi7rQ9TDtvCkpJYmZpKC_3pQKri5cDvfCYewC4RYBzN3zfPoO8kqAENeoiiM2QhA2K6SxJ-w0pQ0AKrQwYjd54K_8nud8TRW1flv-UOCzckd1lb30nU_1jod-6LvvM3Yc_TbR-V-O2efj9GMyzxZvs6fJwyJrhJBdJnRBYANpQoyI3ksdFSkDRdQ6LqVd2ogFGmUjRFph8KuB8EZgrkKUJh-zy8Nu09ZfPaXObeq-rYZLJ7RSVhil5EDBgUpNW1Zrav8pBLfX4A4a3F6DGzTkv7uFT7U</recordid><startdate>20220426</startdate><enddate>20220426</enddate><creator>Kubo, Naotaka</creator><creator>Nii, Keita</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><orcidid>https://orcid.org/0000-0002-2169-5812</orcidid></search><sort><creationdate>20220426</creationdate><title>3d N = 3 generalized Giveon-Kutasov duality</title><author>Kubo, Naotaka ; Nii, Keita</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p224t-268e09de6e11f11aa46f5e5708f66fb49b9f181759f0fec1dac46fa72135df473</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Classical and Quantum Gravitation</topic><topic>Elementary Particles</topic><topic>Gauge theory</topic><topic>High energy physics</topic><topic>Partitions (mathematics)</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Regular Article - Theoretical Physics</topic><topic>Relativity Theory</topic><topic>String Theory</topic><topic>Supersymmetry</topic><topic>Symmetry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kubo, Naotaka</creatorcontrib><creatorcontrib>Nii, Keita</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kubo, Naotaka</au><au>Nii, Keita</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>3d N = 3 generalized Giveon-Kutasov duality</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2022-04-26</date><risdate>2022</risdate><volume>2022</volume><issue>4</issue><spage>158</spage><pages>158-</pages><eissn>1029-8479</eissn><abstract>A
bstract
We generalize the Giveon-Kutasov duality for the 3d
N
= 3 U(
N
)
k,k
+
nN
Chern-Simons matter gauge theory with
F
fundamental hypermultiplets by introducing SU(
N
) and U(1) Chern-Simons levels differently. We study the supersymmetric partition functions and the superconformal indices of the duality, which supports the validity of the duality proposal. From the duality, we can map out the low-energy phases: for example, confinement appears for
F
+
k
−
N
= −
n
= 1 or
N
= 2
F
=
k
= −
n
= 2. For
F
+
k
−
N <
0, supersymmetry is spontaneously broken, which is in accord with the fact that the partition function vanishes. In some cases, the theory shows supersymmetry enhancement to 3d
N
= 4. For
k
= 0, we comment on the magnetic description dual to the so-called “ugly” theory, where the usual decoupled sector is still interacting with others for
n
≠ 0. We argue that the SU(
N
)
0
“ugly-good” duality (which corresponds to the
n →
∞ limit in our setup) is closely related to the S-duality of the 4d
N
= 2 SU(
N
) superconformal gauge theory with 2
N
fundamental hypermultiplets. By reducing the number of flavors via real masses, we suggest possible ways to flow to the “bad” theories.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/JHEP04(2022)158</doi><orcidid>https://orcid.org/0000-0002-2169-5812</orcidid><oa>free_for_read</oa></addata></record> |
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source | DOAJ Directory of Open Access Journals; Springer Nature OA Free Journals; EZB-FREE-00999 freely available EZB journals; Alma/SFX Local Collection |
subjects | Classical and Quantum Gravitation Elementary Particles Gauge theory High energy physics Partitions (mathematics) Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Regular Article - Theoretical Physics Relativity Theory String Theory Supersymmetry Symmetry |
title | 3d N = 3 generalized Giveon-Kutasov duality |
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