3d N = 8 Lorentzian Bagger-Lambert-Gustavsson theory as a scaling limit of 3d superconformal N = 6 Aharony-Bergman-Jafferis-Maldacena theory
We elaborate on the suggestion made in arXiv:0806.3498 that the 3d N=8 superconformal SU(N) Chern-Simons-matter theory of 'Lorentzian' Bagger-Lambert-Gustavson type (L-BLG) can be obtained by a scaling limit (involving sending the level k to infinity and redefining the fields) from the N=6...
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Veröffentlicht in: | Physical review. D, Particles and fields Particles and fields, 2009-02, Vol.79 (4), Article 046002 |
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description | We elaborate on the suggestion made in arXiv:0806.3498 that the 3d N=8 superconformal SU(N) Chern-Simons-matter theory of 'Lorentzian' Bagger-Lambert-Gustavson type (L-BLG) can be obtained by a scaling limit (involving sending the level k to infinity and redefining the fields) from the N=6 superconformal U(N)xU(N) Chern-Simons-matter theory of Aharony, Bergman, Jafferis, and Maldacena (ABJM). We show that to implement such limit in a consistent way one is to extend the ABJM theory by an Abelian 'ghost' multiplet. The corresponding limit at the 3-algebra level also requires extending the nonantisymmetric Bagger-Lambert 3-algebra underlying the ABJM theory by a negative-norm generator. We draw analogy with similar scaling limits discussed previously for bosonic Chern-Simons theory and comment on some implications of this relation between the ABJM and L-BLG theories. |
doi_str_mv | 10.1103/PhysRevD.79.046002 |
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A.</creator><creatorcontrib>Antonyan, E. ; Tseytlin, A. A.</creatorcontrib><description>We elaborate on the suggestion made in arXiv:0806.3498 that the 3d N=8 superconformal SU(N) Chern-Simons-matter theory of 'Lorentzian' Bagger-Lambert-Gustavson type (L-BLG) can be obtained by a scaling limit (involving sending the level k to infinity and redefining the fields) from the N=6 superconformal U(N)xU(N) Chern-Simons-matter theory of Aharony, Bergman, Jafferis, and Maldacena (ABJM). We show that to implement such limit in a consistent way one is to extend the ABJM theory by an Abelian 'ghost' multiplet. The corresponding limit at the 3-algebra level also requires extending the nonantisymmetric Bagger-Lambert 3-algebra underlying the ABJM theory by a negative-norm generator. 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We draw analogy with similar scaling limits discussed previously for bosonic Chern-Simons theory and comment on some implications of this relation between the ABJM and L-BLG theories.</description><subject>LORENTZ INVARIANCE</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>QUANTUM FIELD THEORY</subject><subject>SCALING</subject><subject>SIMULATION</subject><subject>SU GROUPS</subject><subject>U GROUPS</subject><issn>1550-7998</issn><issn>0556-2821</issn><issn>1550-2368</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNo1kMtOwzAURCMEEqXwA6wssXZx7CROFixaHgVUHkKwjm5u7DYosSvbrRS-gY8m0LKaWYyORieKzmM2iWMmLl9XvX9T25uJLCYsyRjjB9EoTlNGucjyw32XRZEfRyfefzImeCblKPoWNXkmVyQnC-uUCV8NGDKD5VI5uoCuUi7Q-cYH2HpvDQkrZV1PwBMgHqFtzJK0TdcEYjUZUH6zVg6t0dZ10P6RMzJdgbOmpzPllh0Y-ghaK9d4-gRtDagM7Lmn0ZGG1quzfY6jj7vb9-t7uniZP1xPFxS5TAPFqhI5yoLHvAKGPK01ZInkCpJE1hUgE7nmWNSQcZkArxkq1FWBIDGuZS3G0cWOa31oSo9NULgaXhuFoRyoWSZEPqz4boXOeu-ULteu6cD1ZczKX-vlv_VSFuXOuvgBV-F45w</recordid><startdate>20090201</startdate><enddate>20090201</enddate><creator>Antonyan, E.</creator><creator>Tseytlin, A. 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A.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physical review. D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Antonyan, E.</au><au>Tseytlin, A. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>3d N = 8 Lorentzian Bagger-Lambert-Gustavsson theory as a scaling limit of 3d superconformal N = 6 Aharony-Bergman-Jafferis-Maldacena theory</atitle><jtitle>Physical review. D, Particles and fields</jtitle><date>2009-02-01</date><risdate>2009</risdate><volume>79</volume><issue>4</issue><artnum>046002</artnum><issn>1550-7998</issn><issn>0556-2821</issn><eissn>1550-2368</eissn><eissn>1089-4918</eissn><abstract>We elaborate on the suggestion made in arXiv:0806.3498 that the 3d N=8 superconformal SU(N) Chern-Simons-matter theory of 'Lorentzian' Bagger-Lambert-Gustavson type (L-BLG) can be obtained by a scaling limit (involving sending the level k to infinity and redefining the fields) from the N=6 superconformal U(N)xU(N) Chern-Simons-matter theory of Aharony, Bergman, Jafferis, and Maldacena (ABJM). We show that to implement such limit in a consistent way one is to extend the ABJM theory by an Abelian 'ghost' multiplet. The corresponding limit at the 3-algebra level also requires extending the nonantisymmetric Bagger-Lambert 3-algebra underlying the ABJM theory by a negative-norm generator. We draw analogy with similar scaling limits discussed previously for bosonic Chern-Simons theory and comment on some implications of this relation between the ABJM and L-BLG theories.</abstract><cop>United States</cop><doi>10.1103/PhysRevD.79.046002</doi></addata></record> |
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subjects | LORENTZ INVARIANCE PHYSICS OF ELEMENTARY PARTICLES AND FIELDS QUANTUM FIELD THEORY SCALING SIMULATION SU GROUPS U GROUPS |
title | 3d N = 8 Lorentzian Bagger-Lambert-Gustavsson theory as a scaling limit of 3d superconformal N = 6 Aharony-Bergman-Jafferis-Maldacena theory |
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