Abstract

The action integral contains more information than the equations of motion. Since it is an integral, changes of the integration variables occasionally also expose symmetries more easily than working directly with the equations of motion. We have previously shown that there are signs of an extended exceptional symmetry for mathcal{N}=8 supergravity in four dimensions. The symmetry is such that the fields used in the Lagrangian are not representations of the symmetry. Instead one has to add representations to obtain a representation of the extended symmetry group. In this paper we discuss an extended symmetry in four-dimensional gravity which is the “Ehlers Symmetry” in three dimensions. It cannot be spanned by the helicity states of four-dimensional gravity but it can be realised once we treat the helicity states just as field variables of the functional integral, which can be changed like variables in any integral. We also explain how this symmetry is inherent in formulations of mathcal{N}=8 supergravity in four dimensions through a truncation in the field space to pure gravity. The establishment of these “hidden” symmetries should play an important role in the perturbative behaviour of the quantum theories. Since the method used n this paper is purely algebraic we will not provide any information on the geometric role of these symmetries.

Highlights

  • This symmetry first appeared in the work of Cremmer and Julia [3], who found an unexpected symmetry at the level of the equations of motion in N = 8 supergravity

  • It cannot be spanned by the helicity states of four-dimensional gravity but it can be realised once we treat the helicity states just as field variables of the functional integral, which can be changed like variables in any integral

  • We showed that the corresponding E8(8) symmetry, thought to be special to maximal supergravity in d = 3, could be lifted to a symmetry of the d = 4 theory and in principle to the d = 11 theory [6]

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Summary

Maximal supergravity in three dimensions

For the action for the d = 3 theory (up to an overall constant) This theory does not show an E8(8) symmetry since the SO(16) R-symmetry which is the maximal subgroup of E8(8) and linearly realized does not admit vertices of odd order (κ, κ3 etc.). Having established that the d = 3 pure gravity theory possesses this symmetry, the natural step is to ask whether we can oxidize back to four dimensions, exactly as we did with supergravity [6]. This can be done as explained below

A lift back to four dimensions
Conclusions
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