Abstract

There exists two distinct off-shell ${\mathcal{N}}=2$ supergravities in three dimensions. They are also referred to as ${\mathcal{N}}=(1,1)$ and ${\mathcal{N}}=(2,0)$ supergravities, and they arise from the coupling of the Weyl multiplet to a compensating scalar or vector multiplet, respectively, followed by fixing of conformal symmetries. The ${\mathcal{N}} =(p,q)$ terminology refers to the underlying anti-de Sitter superalgebras $OSp(2,p) \oplus OSp(2,q)$ with $R$-symmetry group $SO(p) \times SO(q)$. We construct off-shell invariants of these theories up to fourth order in derivatives. As an application of these results, we determine the special combinations of the ${\mathcal{N}}=(1,1)$ invariants that admit anti-de Sitter vacuum solution about which there is a ghost-free massive spin-2 multiplet of propagating modes. We also show that the ${\mathcal{N}}=(2,0)$ invariants do not allow such possibility.

Highlights

  • Theories which admit anti-de Sitter space as a vacuum solution, their underlying supersymmetry algebra is OSp(p, q) whose bosonic part is O(2, 2) ⊕ SO(p) × SO(q) [1,2,3]

  • There exists two distinct off-shell N = 2 supergravities in three dimensions. They are referred to as N = (1, 1) and N = (2, 0) supergravities, and they arise from the coupling of the Weyl multiplet to a compensating scalar or vector multiplet, respectively, followed by fixing of conformal symmetries

  • The N = (1, 1) and N = (2, 0) supergravities arise from the coupling of Weyl multiplet to a compensating scalar or vector multiplets, respectively, followed by fixing of conformal symmetries

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Summary

Superconformal tensor calculus

We shall describe the Weyl multiplet based on the superconformal algebra OSp(4|2) in three dimensions. We will present the off-shell scalar and vector multiples which will be used in the subsequent sections as compensators. The rules for combining these multiplets to obtain new (composite) multiplets and action formula will follow. The action formula will be used together with the composite multiplet formula to obtain several off-shell supergravity invariants. We shall record for completeness the Chern-Simons invariant which does not require any compensating multiplet coupling since it is superconformal invariant by itself [8]

The Weyl and compensating multiplets
Combination of local supermultiplets
Action formulae
Conclusions
A Complex spinor conventions
B Fierz identities
Full Text
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