Abstract

Gravitational domain wall solutions in gauged supergravity are often constructed within truncations that do not include vectors. As a consequence the gauge group is only a global symmetry of this truncation. The consistency of the truncation requires the restriction to solutions with vanishing Noether charge under this global symmetry, since otherwise vector fields are sourced. We show that this has interesting consequences for the orbit structure of the solutions under the global symmetries. We investigate this for CSO(p, q, r)-gaugings in various dimensions with scalar fields truncated to the mathrm{S}mathrm{L}left(n,mathbb{R}right)/mathrm{SO}(n) subcoset. We prove that the seed solution — which generates all other solutions using only global transformations — has a diagonal coset matrix. This means that there exists a transformation at the boundary of the geometry that diagonalises the coset matrix and that this same transformation also diagonalises the whole flow as a consequence of the vanishing charge.

Highlights

  • Isometry local and destroys the rest1 of the original global symmetry by the introduction of a scalar potential

  • The consistency of the truncation requires the restriction to solutions with vanishing Noether charge under this global symmetry, since otherwise vector fields are sourced

  • We show that this has interesting consequences for the orbit structure of the solutions under the global symmetries

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Summary

CSO-gauged SUGRA

We consider a consistent truncation of gauged supergravity theories such that only the scalars φi For example in N = 8, D = 4 maximal gauged SUGRA the scalar manifold is E7(7)/ SU(8), describing 70 real scalars. Those 70 can be split into 35 scalars and 35 pseudo-scalars. Consider the coset representative L of SL(n, R)/ SO(n) in its fundamental representation It is multiplied by the left with the SL(n, R) isometry transformations and from the right with the SO(n) isotropy group:. When r > 0 this is larger than the CSO(p, q, r)-group, as we will explain below

Supersymmetric domain wall flows
Noether charges
Normal forms
Discussion
A Noether currents
B Normal forms and vanishing Noether charges

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