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Supersymmetrizing Massive Gravity

High Energy Physics - Theory 2013-08-09 v3

Abstract

When four scalar fields with global Lorentz symmetry are coupled to gravity and take a vacuum expectation value breaking diffeomorphism invariance spontaneously, the graviton becomes massive. This model is supersymmetrized by considering four N=1 chiral superfields with global Lorentz symmetry. When the scalar components of the chiral multiplets z^A acquire a vacuum expectation value, both diffeomorphism invariance and local supersymmetry are broken spontaneously. The global Lorentz index A becomes identified with the space-time Lorentz index making the scalar fields z^A vectors and the chiral spinors psi^A spin-3/2 Rarita-Schwinger fields. The global supersymmetry is promoted to a local one using the rules of tensor calculus of coupling the N=1 supergravity Lagrangian to the four chiral multiplets. We show that the spectrum of the model in the broken phase consists of a massive spin-2 field, two massive spin-3/2 fields with different mass and a massive vector.

Keywords

Cite

@article{arxiv.1303.3580,
  title  = {Supersymmetrizing Massive Gravity},
  author = {Ola Malaeb},
  journal= {arXiv preprint arXiv:1303.3580},
  year   = {2013}
}

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R2 v1 2026-06-21T23:42:17.753Z