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dc.identifier.urihttp://hdl.handle.net/11401/76655
dc.description.sponsorshipThis work is sponsored by the Stony Brook University Graduate School in compliance with the requirements for completion of degree.en_US
dc.formatMonograph
dc.format.mediumElectronic Resourceen_US
dc.language.isoen_US
dc.publisherThe Graduate School, Stony Brook University: Stony Brook, NY.
dc.typeDissertation
dcterms.abstractThis dissertation is divided into three main parts where we derive various properties of the T-dually extended superspaces. In the first part we reformulate the manifestly T-dual description of the massless sector of the closed bosonic string, directly from the geometry associated with the (left and right) affine Lie algebra of the coset space Poincar Ì e/Lorentz. This construction initially doubles not only the (space- time) coordinates for translations but also those for Lorentz transformations (and their “dual†). As a result, the Lorentz connection couples directly to the string (as does the vielbein), rather than being introduced indirectly through covariant derivatives as previously. This not only reproduces the old definition of T-dual torsion, but automatically gives a general, covariant definition of T-dual curvature (but still with some undetermined connections). In the second part we give the manifestly T-dual formulation of the massless sector of the classical 3D Type II superstring in off-shell 3D N = 2 superspace, including the action. It has a simple relation to the known superspace of 4D N = 1 supergravity in 4D M-theory via 5D F-theory. The pre-potential appears as part of the vielbein, without derivatives. In the last and the most involved part we find the pre-potential in the superspace with AdS5 × S5 background. The pre-potential appears as part of the vielbeins, without derivatives. In both subspaces (AdS5 and S5) we use Poincare coordinates. We pick one bulk coordinate in AdS5 and one bulk coordinate in S5 to define the space-cone gauge. Such space-cone gauge destroys the bulk Lorentz covariance. However, it still preserves boundary Lorentz covariance (and gives projective superspace) SO ( 3, 1) ⊗ SO (4) and so symmetries of boundary CFT are manifest.
dcterms.available2017-09-20T16:50:53Z
dcterms.contributorRocek, Martinen_US
dcterms.contributorSiegel, Warrenen_US
dcterms.contributorNieuwenhuizen, Peter vanen_US
dcterms.contributorDu, Xuen_US
dcterms.contributorKhuri, Marcus.en_US
dcterms.creatorPolacek, Martin
dcterms.dateAccepted2017-09-20T16:50:53Z
dcterms.dateSubmitted2017-09-20T16:50:53Z
dcterms.descriptionDepartment of Physicsen_US
dcterms.extent116 pg.en_US
dcterms.formatApplication/PDFen_US
dcterms.formatMonograph
dcterms.identifierhttp://hdl.handle.net/11401/76655
dcterms.issued2017-05-01
dcterms.languageen_US
dcterms.provenanceMade available in DSpace on 2017-09-20T16:50:53Z (GMT). No. of bitstreams: 1 Polacek_grad.sunysb_0771E_13327.pdf: 659001 bytes, checksum: ab828d1b2ee8b4861cf60b68a45c33b5 (MD5) Previous issue date: 1en
dcterms.publisherThe Graduate School, Stony Brook University: Stony Brook, NY.
dcterms.subjectPhysics
dcterms.subjectF theory, String theory, Supergravity, T-duality
dcterms.titleAspects of T-dually extended Superspaces
dcterms.typeDissertation


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