E(11) and the Embedding Tensor
By Eric Bergshoeff, Teake Nutma, I. D. Baetselier. 2007
133 citations recorded by the source corpus.
We show how, using different decompositions of E11, one can calculate the representations under the duality group of the so-called ``de-form'' potentials. Evidence is presented that these potentials are in one-to-one correspondence to the embedding tensors that classify the gaugings of all maximal gauged supergravities. We supply the computer program underlying our calculations.
Subfields: Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/427a27201ef79d66847db4c99a1e07b3f034a7d7
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Citations in the corpus
- Spheres, Generalised Parallelisability and Consistent Truncations (2014, unknown): “ations generated by the generalised Lie derivative, so that [43, 59] Aµ= AA µ Eˆ A, δAµ= ∂µΛ− LAµΛ = ∂µΛ C− X AB CAA µΛ B Eˆ C. (4.4) In general [59, 60], this will extend to a whole tensor hierarchy [61]. – 25 – Recallthatconsistency ofaconventional Scherk–Schwarz truncationis essentially trivial (”
- Duality invariant actions and generalised geometry (2011, background): “In the decomposition of E11 into Ed one finds the expected fields of D dimensional supergravity as well as a hierarchy of form fields [21, 28], which play an important role in gauged supergravities, as well as an infinite number of higher level fields.”