Super-Yang-Mills and M5-branes
We uplift 5-dimensional super-Yang-Mills theory to a 6-dimensional gauge theory with the help of a space-like constant vector η M , whose norm determines the YM coupling constant. After the localization of η M the 6D gauge theory acquires Lorentzian invariance as well as scale invariance. We discuss...
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container_title | The journal of high energy physics |
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creator | Singh, Harvendra |
description | We uplift 5-dimensional super-Yang-Mills theory to a 6-dimensional gauge theory with the help of a space-like constant vector
η
M
, whose norm determines the YM coupling constant. After the localization of
η
M
the 6D gauge theory acquires Lorentzian invariance as well as scale invariance. We discuss KK states, instantons and the flux quantization. The theory admits extended solutions like 1/2 BPS ‘strings’ and monopoles. |
doi_str_mv | 10.1007/JHEP08(2011)136 |
format | Article |
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η
M
, whose norm determines the YM coupling constant. After the localization of
η
M
the 6D gauge theory acquires Lorentzian invariance as well as scale invariance. We discuss KK states, instantons and the flux quantization. The theory admits extended solutions like 1/2 BPS ‘strings’ and monopoles.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP08(2011)136</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>Branes ; Classical and Quantum Gravitation ; Elementary Particles ; Flux quantization ; Gauge theory ; High energy physics ; Instantons ; Invariance ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Relativity Theory ; Scale invariance ; String Theory ; Uplift ; Yang-Mills theory</subject><ispartof>The journal of high energy physics, 2011-08, Vol.2011 (8), Article 136</ispartof><rights>SISSA, Trieste, Italy 2011</rights><rights>SISSA, Trieste, Italy 2011.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c310t-20459114ee86e01692b87aa809ba7aa0e2ebbdcb2213d4d20178dda55418018b3</citedby><cites>FETCH-LOGICAL-c310t-20459114ee86e01692b87aa809ba7aa0e2ebbdcb2213d4d20178dda55418018b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP08(2011)136$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/JHEP08(2011)136$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41120,41488,42189,42557,51319,51576</link.rule.ids><linktorsrc>$$Uhttps://doi.org/10.1007/JHEP08(2011)136$$EView_record_in_Springer_Nature$$FView_record_in_$$GSpringer_Nature</linktorsrc></links><search><creatorcontrib>Singh, Harvendra</creatorcontrib><title>Super-Yang-Mills and M5-branes</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>We uplift 5-dimensional super-Yang-Mills theory to a 6-dimensional gauge theory with the help of a space-like constant vector
η
M
, whose norm determines the YM coupling constant. After the localization of
η
M
the 6D gauge theory acquires Lorentzian invariance as well as scale invariance. We discuss KK states, instantons and the flux quantization. The theory admits extended solutions like 1/2 BPS ‘strings’ and monopoles.</description><subject>Branes</subject><subject>Classical and Quantum Gravitation</subject><subject>Elementary Particles</subject><subject>Flux quantization</subject><subject>Gauge theory</subject><subject>High energy physics</subject><subject>Instantons</subject><subject>Invariance</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Relativity Theory</subject><subject>Scale invariance</subject><subject>String Theory</subject><subject>Uplift</subject><subject>Yang-Mills theory</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kDFPwzAUhC0EEqUws6FKLDCYvmfHiT2iqtBWrUACBibLjt2qVUiC3Qz8e1wFCRamu-Hu3tNHyCXCHQIU48Vs-gzyhgHiLfL8iAwQmKIyK9TxH39KzmLcAaBABQNy9dK1PtB3U2_oaltVcWRqN1oJaoOpfTwnJ2tTRX_xo0Py9jB9nczo8ulxPrlf0pIj7CmDTCjEzHuZe8BcMSsLYyQoa5KCZ95aV1rGkLvMpR8L6ZwRIkMJKC0fkut-tw3NZ-fjXu-aLtTppGZcSSYU5zKlxn2qDE2Mwa91G7YfJnxpBH2AoHsI-gBBJwipAX0jpmS98eF397_KN3EQWxo</recordid><startdate>20110801</startdate><enddate>20110801</enddate><creator>Singh, Harvendra</creator><general>Springer-Verlag</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</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></search><sort><creationdate>20110801</creationdate><title>Super-Yang-Mills and M5-branes</title><author>Singh, Harvendra</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c310t-20459114ee86e01692b87aa809ba7aa0e2ebbdcb2213d4d20178dda55418018b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Branes</topic><topic>Classical and Quantum Gravitation</topic><topic>Elementary Particles</topic><topic>Flux quantization</topic><topic>Gauge theory</topic><topic>High energy physics</topic><topic>Instantons</topic><topic>Invariance</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Relativity Theory</topic><topic>Scale invariance</topic><topic>String Theory</topic><topic>Uplift</topic><topic>Yang-Mills theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Singh, Harvendra</creatorcontrib><collection>CrossRef</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_linktorsrc</fulltext></delivery><addata><au>Singh, Harvendra</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Super-Yang-Mills and M5-branes</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2011-08-01</date><risdate>2011</risdate><volume>2011</volume><issue>8</issue><artnum>136</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>We uplift 5-dimensional super-Yang-Mills theory to a 6-dimensional gauge theory with the help of a space-like constant vector
η
M
, whose norm determines the YM coupling constant. After the localization of
η
M
the 6D gauge theory acquires Lorentzian invariance as well as scale invariance. We discuss KK states, instantons and the flux quantization. The theory admits extended solutions like 1/2 BPS ‘strings’ and monopoles.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/JHEP08(2011)136</doi><oa>free_for_read</oa></addata></record> |
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subjects | Branes Classical and Quantum Gravitation Elementary Particles Flux quantization Gauge theory High energy physics Instantons Invariance Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Relativity Theory Scale invariance String Theory Uplift Yang-Mills theory |
title | Super-Yang-Mills and M5-branes |
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