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Fine tuning and six-dimensional gauged N =(1, 0) supergravity vacua

dc.contributor.authorGüven, R.en_US
dc.contributor.authorLiu, James T.en_US
dc.contributor.authorPope, Christopher N.en_US
dc.contributor.authorSezgin, E.en_US
dc.date.accessioned2006-12-19T19:23:54Z
dc.date.available2006-12-19T19:23:54Z
dc.date.issued2004-02-21en_US
dc.identifier.citationGüven, R; Liu, James T; Pope, C N; Sezgin, E (2004). "Fine tuning and six-dimensional gauged N =(1, 0) supergravity vacua." Classical and Quantum Gravity. 21(4): 1001-1014. <http://hdl.handle.net/2027.42/49215>en_US
dc.identifier.issn0264-9381en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/49215
dc.description.abstractWe find a new family of supersymmetric vacuum solutions in the six-dimensional chiral gauged N = (1, 0) supergravity theory. They are generically of the form AdS3 × S3, where the 3-sphere is squashed homogeneously along its Hopf fibres. The squashing is freely adjustable, corresponding to changing the 3-form charge, and the solution is supersymmetric for all squashings. In a limit where the length of the Hopf fibres goes to zero, one recovers, after a compensating rescaling of the fibre coordinate, a solution that is locally the same as the well-known (Minkowski)4 × S2 vacuum of this theory. It can now be viewed as a fine tuning of the new more general family. The traditional ‘cosmological constant problem’ is replaced in this theory by the problem of why the four-dimensional (Minkowski)4 × S2 vacuum should be selected over other members of the equally supersymmetric AdS3 × S3 family. We also obtain a family of dyonic string solutions in the gauged N = (1, 0) theory, whose near-horizon limits approach the AdS3 times squashed S3 solutions.en_US
dc.format.extent3118 bytes
dc.format.extent167885 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.publisherIOP Publishing Ltden_US
dc.titleFine tuning and six-dimensional gauged N =(1, 0) supergravity vacuaen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumMichigan Center for Theoretical Physics, University of Michigan, Ann Arbor, MI 48109-1120, USAen_US
dc.contributor.affiliationotherDepartment of Mathematics, Boğaziçi University, Bebek, Istanbul 34342, Turkeyen_US
dc.contributor.affiliationotherGeorge P and Cynthia W Mitchell Institute for Fundamental Physics, Texas A&M University, College Station, TX 77843-4242, USAen_US
dc.contributor.affiliationotherGeorge P and Cynthia W Mitchell Institute for Fundamental Physics, Texas A&M University, College Station, TX 77843-4242, USAen_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/49215/2/cqg4_4_019.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1088/0264-9381/21/4/019en_US
dc.identifier.sourceClassical and Quantum Gravity.en_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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