Exceptional field theory. III. E[subscript 8(8)]

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 sect...

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Bibliographic Details
Main Authors: Hohm, Olaf, Samtleben, Henning
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics
Format: Article
Language:English
Published: American Physical Society 2014
Online Access:http://hdl.handle.net/1721.1/89212
Description
Summary: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.