| dc.contributor.author | Hohm, Olaf | |
| dc.contributor.author | Samtleben, Henning | |
| dc.date.accessioned | 2014-09-05T18:22:30Z | |
| dc.date.available | 2014-09-05T18:22:30Z | |
| dc.date.issued | 2014-09 | |
| dc.date.submitted | 2014-07 | |
| dc.identifier.issn | 1550-7998 | |
| dc.identifier.issn | 1550-2368 | |
| dc.identifier.uri | http://hdl.handle.net/1721.1/89212 | |
| dc.description.abstract | We develop exceptional field theory for E[subscript 8(8)], defined on a (3 + 248)-dimensional generalized spacetime with extended coordinates in the adjoint representation of E[subscript 8(8)]. The fields transform under E[subscript 8(8)] generalized diffeomorphisms and are subject to covariant section constraints. The bosonic fields include an “internal” dreibein and an E[subscript 8(8)]-valued “zweihundertachtundvierzigbein” (248-bein). Crucially, the theory also features gauge vectors for the E[subscript 8(8)] E bracket governing the generalized diffeomorphism algebra and covariantly constrained gauge vectors for a separate but constrained E[subscript 8(8)] gauge symmetry. The complete bosonic theory, with a novel Chern-Simons term for the gauge vectors, is uniquely determined by gauge invariance under internal and external generalized diffeomorphisms. The theory consistently comprises components of the dual graviton encoded in the 248-bein. Upon picking particular solutions of the constraints the theory reduces to D = 11 or type IIB supergravity, for which the dual graviton becomes pure gauge. This resolves the dual graviton problem, as we discuss in detail. | en_US |
| dc.description.sponsorship | United States. Dept. of Energy (Cooperative Research Agreement DE-FG02-05ER41360) | en_US |
| dc.publisher | American Physical Society | en_US |
| dc.relation.isversionof | http://dx.doi.org/10.1103/PhysRevD.90.066002 | en_US |
| dc.rights | Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. | en_US |
| dc.source | American Physical Society | en_US |
| dc.title | Exceptional field theory. III. E[subscript 8(8)] | en_US |
| dc.type | Article | en_US |
| dc.identifier.citation | Hohm, Olaf, and Henning Samtleben. "Exceptional field theory. III. E[subscript 8(8)]." Phys. Rev. D 90, 066002 (September 2014). © 2014 American Physical Society | en_US |
| dc.contributor.department | Massachusetts Institute of Technology. Center for Theoretical Physics | en_US |
| dc.contributor.department | Massachusetts Institute of Technology. Laboratory for Nuclear Science | en_US |
| dc.contributor.mitauthor | Hohm, Olaf | en_US |
| dc.relation.journal | Physical Review D | en_US |
| dc.eprint.version | Final published version | en_US |
| dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
| eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
| dc.date.updated | 2014-09-04T22:00:24Z | |
| dc.language.rfc3066 | en | |
| dc.rights.holder | American Physical Society | |
| dspace.orderedauthors | Hohm, Olaf; Samtleben, Henning | en_US |
| mit.license | PUBLISHER_POLICY | en_US |
| mit.metadata.status | Complete | |