2015
DOI: 10.1088/0264-9381/32/20/205008
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On the integrability of Einstein–Maxwell–(A)dS gravity in the presence of Killing vectors

Abstract: We study some symmetry and integrability properties of four-dimensional Einstein-Maxwell gravity with nonvanishing cosmological constant in the presence of Killing vectors. First of all, we consider stationary spacetimes, which lead, after a timelike Kaluza-Klein reduction followed by a dualization of the two vector fields, to a three-dimensional nonlinear sigma model coupled to gravity, whose target space is a noncompact version of CP 2 with SU(2, 1) isometry group. It is shown that the potential for the scal… Show more

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Cited by 14 publications
(24 citation statements)
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References 73 publications
(152 reference statements)
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“…One might ask whether this PSL(2, R) is related to the Ehlers transformations for the (electro)vacuum solutions to Einstein's equations. The latter symmetry is, however, broken in the presence of a cosmological constant [44]. Thus, the remarkable symmetry (3.29) is not related to Ehlers transformations and is intrinsic to supersymmetric solutions.…”
Section: Non-null Classmentioning
confidence: 98%
“…One might ask whether this PSL(2, R) is related to the Ehlers transformations for the (electro)vacuum solutions to Einstein's equations. The latter symmetry is, however, broken in the presence of a cosmological constant [44]. Thus, the remarkable symmetry (3.29) is not related to Ehlers transformations and is intrinsic to supersymmetric solutions.…”
Section: Non-null Classmentioning
confidence: 98%
“…Q I = 0 this leads to the Ercolani-Sinha solution [35], which is given in terms of elliptic functions. (6.4) can be written as 8) and thus its symmetries are determined by the transformations that leave the tensor C I JK invariant, T −1 CT T = C. Unfortunately this implies T = 1. The discrete symmetry group of (6.8), which is easily shown to be (Z 2 ) 6 × Z 3 , is not very useful for generating new solutions from known ones.…”
Section: Solutions With Running Scalarsmentioning
confidence: 99%
“…For the simple example quoted above, the addition of a cosmological constant breaks three of the eight SU(2, 1) symmetries, corresponding to the generalized Ehlers and the two Harrison transformations. This leaves a semidirect product of a one-dimensional Heisenberg group and a translation group R 2 as residual symmetry [8], that cannot be used to generate new solutions.…”
Section: Introductionmentioning
confidence: 99%
“…This was recently extended to include a non-zero cosmological constant by Leigh et al [6], where they traced the symmetries broken by the presence of the cosmological constant and recast the equations of motion as a one-dimensional system which was solved using the Hamilton-Jacobi method. A further generalisation of this method to include electromagnetic fields was done by Klemm et al [7]. In higher dimensional vacuum gravity, D-dimensional static spacetimes with (D − 2)…”
Section: Introductionmentioning
confidence: 99%