Abstract

The SU(3)--invariant sector of maximal supergravity in four dimensions with an SO(8) gauging is uplifted to $D=11$ supergravity. In order to do this, the SU(3)--neutral sector of the tensor and duality hierarchies of the $D=4$ ${\cal N}=8$ supergravity is first worked out. The consistent $D=11$ embedding of the full, dynamical SU(3) sector is then expressed at the level of the $D=11$ metric and three-form gauge field in terms of these $D=4$ tensors. The redundancies introduced by this approach are eliminated at the level of the $D=11$ four-form field strength by making use of the $D=4$ duality hierarchy. Our results encompass previously known truncations of $D=11$ supergravity down to sectors of SO(8) supergravity with symmetry larger than SU(3), and include new ones. In particular, we obtain a new consistent truncation of $D=11$ supergravity to minimal $D=4$ ${\cal N}=2$ gauged supergravity.

Highlights

  • Being complicated theories with large field contents, it proves useful for applications to truncate maximal gauged supergravities to smaller subsectors that are invariant under some symmetry group

  • The goal of this paper is to provide the consistent uplift of the SU(3) sector of SO(8) gauged supergravity into D 1⁄4 11 by using the uplifting formulas of [25], putting them to the test

  • Expressing the D 1⁄4 11 embedding at the level of the four-form field strength and employing these D 1⁄4 4 dualizations, redundancy-free uplifting formulas are obtained that contain only the dynamically independent fields that feature in the conventional D 1⁄4 4 N 1⁄4 8 Lagrangian

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Summary

INTRODUCTION

Being complicated theories with large field contents, it proves useful for applications to truncate maximal gauged supergravities to smaller subsectors that are invariant under some symmetry group. A systematic approach to the consistent uplift of D 1⁄4 4 N 1⁄4 8 SO(8) supergravity to D 1⁄4 11 was proposed in [25], similar to the method employed in [29,30] to uplift D 1⁄4 4 N 1⁄4 8 ISO(7) supergravity [31] into type IIA This approach relies on the tensor hierachy [32,33] of maximal four-dimensional supergravity—the extension of its field content to include the magnetic gauge fields along with higher rank potentials in representations of E7ð7Þ. Expressing the D 1⁄4 11 embedding at the level of the four-form field strength and employing these D 1⁄4 4 dualizations, redundancy-free uplifting formulas are obtained that contain only the dynamically independent fields (that is, the metric, the scalars and the electric vectors) that feature in the conventional D 1⁄4 4 N 1⁄4 8 Lagrangian. Contact with the consistent uplift of previously known subsectors is made and a new D 1⁄4 11 embedding of D 1⁄4 4 N 1⁄4 2 pure gauged supergravity is established.

Field content and Lagrangian
ΛΣHΛð2Þ
Some further subsectors
Vacuum structure
Uplift of some further subsectors
G2-invariant sector
DISCUSSION
S7 as the join of S1 and a Sasaki-Einstein S5
S7 with its homogeneous Sasaki-Einstein structure
S7 as the sine-cone over a nearly Kähler S6
Full Text
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