Double field theory and $ \mathcal{N} = {4} $ gauged supergravity

By David Geissbühler. 2011

134 citations recorded by the source corpus.

Subfields: Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/0e7f1b50818e81f3a4535e90b0cf70960114b170

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Citations in the corpus

Duality invariant M-theory: gauged supergravities and Scherk-Schwarz reductions (2012, methodology): “However, in [11, 12, 13] it is shown that for backgrounds satisfying an appropriate Scherk–Schwarz ansatz the strong constraint is sufficient but not necessary for the reduced theory to be consistent; the constraint can be consistently weakened on the internal space.”
Duality orbits of non‐geometric fluxes (2012, methodology): “Recently it has been pointed out how to obtain gaugings of N = D = 4 supergravity by means of twisted double torus reductions of DFT [7,8], even though at that stage, the so-called weak and strong constraints imposed for consistency of DFT represented a further restriction that prevented one from de”
The spacetime of double field theory: Review, remarks, and outlook (2013, background): “There have been a series of papers discussing the construction of gauged supergravity in lower dimensions by means of a generalized Scherk-Schwarz compactification of DFT [21–23].”
Duality Symmetric String and M-Theory (2013, background): “C − f A BC ξˇB 1 ξˇC 2 . (4.109) The conditions for this theory to be consistent, i.e. closure of the gauge algebra, Jacobiator generatingatrivial transformationandinvariance oftheaction,werestudiedin[175,178,193]. The conclusion is that although strong and weak constraints on the twist matrix are s”
Non‐geometric fluxes in supergravity and double field theory (2012, background): “gravity or strongly constrained DFT, whereas some gauged supergravity solutions in dimension D ě 7 have been shown to correspond to DFT solutions where the strong constraint is relaxed [23] (see also [18,19,24]). We believe, nevertheless, that the new action and ﬁeld variables considered in this pap”
β-supergravity: a ten-dimensional theory with non-geometric fluxes, and its geometric framework (2013, background): “ation of our potential matching the one derived from a superpotential of gauged supergravity; let us though give a further argument in favor of our scalar potential being the correct one. The work of [27, 65, 66, 32] starts with a generic generalized vielbein in DFT. Upon few assumptions, among whic”
Gauged double field theory (2012, methodology): “sults with those of [7], we see that both actions diﬀer by exactly the same term. This term can have a higher dimensional origin in the following manifestly G-invariant additional piece in the action [9] △SDFT = − 1 6 Z dNXddYe−2dF abcF abc = Z dNXddYe−2d△R , (3.38) where the indices are contracted ”
Exotic Branes in String Theory (2012, result): “However, more recently, it was shown [129–132] (see also [9,133,134]) that one can generalize DFT in a way such that its non-geometric Scherk–Schwarz compactification reproduces the constraint equations in the low dimensional theory expected for non-geometric compactifications.”
Exploring double field theory (2013, methodology): “For the Neveu-Schwarz sector, it was shown in [42–44] that closure of the algebra of generalized diffeomorphisms and gauge invariance of the action of DFT give rise to a set of constraints that are not in one to one correspondence with the strong constraint.”
Extended geometry and gauged maximal supergravity (2013, methodology): “In this paper, we extend the DFT constructions of [16, 17, 18, 19, 20], following the definitions introduced in [10], for the case d = 6, when the symmetry group is 1 E7.”
On the Riemann tensor in double field theory (2011, background): “(See [5–42] for previous work and further developments.”