Abstract

Half-maximal, mathcal{N} = 4, sectors of D = 4 mathcal{N} = 8 supergravity with a dyonic ISO(7) gauging are investigated. We focus on a half-maximal sector including three vector multiplets, that arises as a certain SO(3)R-invariant sector of the full theory. We discuss the embedding of this sector into the largest half-maximal sector of the mathcal{N} = 8 supergravity retaining six vector multiplets. We also provide its canonical mathcal{N} = 4 formulation and show that, from this perspective, our model leads in its own right to a new explicit gauging of mathcal{N} = 4 supergravity. Finally, expressions for the restricted duality hierarchy are given and the vacuum structure is investigated. Five new non-supersymmetric AdS vacua are found numerically. The previously known mathcal{N} = 2 and mathcal{N} = 3 AdS vacua are also contained in our mathcal{N} = 4 model. Unlike when embedded in previously considered sectors with fewer fields, these vacua exhibit their full mathcal{N} = 2 and mathcal{N} = 3 supersymmetry within our mathcal{N} = 4 model.

Highlights

  • Attain AdS extrema [13, 14, 20, 21]

  • We focus on a half-maximal sector including three vector multiplets, that arises as a certain SO(3)R-invariant sector of the full theory

  • We discuss the embedding of this sector into the largest half-maximal sector of the N = 8 supergravity retaining six vector multiplets

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Summary

Field content

In order to determine the field content of the SO(3)R-invariant sector of the dyonic ISO(7)gauged maximal supergravity, one needs to know how the SO(3)R subgroup is embedded into ISO(7). More details about the group-theoretical embedding of the vector fields into maximal supergravity are presented in appendix A. More details about the group-theoretical embedding of the (pseudo-) scalars into maximal supergravity are presented in appendix A. The group-theoretical decomposition of the 1 + 27 three-form potentials dual to electric components of the embedding tensor in the ISO(7) maximal theory is given by (1, 1, 1). Yielding a total of seven three-forms in the SO(3)R-invariant sector C0 ≡ (1, 1) ⊂ 1 , Cij ≡ (5, 1) + (1, 1) ⊂ 27

Lagrangian and equations of motion
New non-supersymmetric vacua
Discussion
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