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Conformally invariant wave equation for a symmetric second rank tensor (“spin-2”) in a d-dimensional curved background

J. Ben Achour1,*, E. Huguet1,†, and J. Renaud2,‡

  • 1Université Paris Diderot-Paris 7, APC-Astroparticule et Cosmologie (UMR-CNRS 7164), Batiment Condorcet, 10 rue Alice Domon et Léonie Duquet, F-75205 Paris Cedex 13, France
  • 2Université Paris-Est, APC-Astroparticule et Cosmologie (UMR-CNRS 7164), Batiment Condorcet, 10 rue Alice Domon et Léonie Duquet, F-75205 Paris Cedex 13, France

  • *benachou@apc.univ-paris7.fr
  • huguet@apc.univ-paris7.fr
  • jacques.renaud@u-pem.fr

Phys. Rev. D 89, 064041 – Published 18 March, 2014

DOI: https://doi.org/10.1103/PhysRevD.89.064041

Abstract

We build the general conformally invariant linear wave operator for a free, symmetric, second-rank tensor field in a d-dimensional (d2) metric manifold, and explicitly show the special case of maximally symmetric spaces. Under the assumptions made, this conformally invariant wave operator is unique. The corresponding conformally invariant wave equation can be obtained from a Lagrangian which is explicitly given. We discuss how our result compares to previous works; in particular, we hope to clarify the situation between conflicting results.

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