“Massless” vector field in de Sitter universe

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  • T. Garidi
    Université Paris Diderot Paris 7 1 APC, CNRS UMR 7164, , F-75205 Paris Cedex 13, France
  • J.-P. Gazeau
    Université Paris Diderot Paris 7 1 APC, CNRS UMR 7164, , F-75205 Paris Cedex 13, France
  • S. Rouhani
    Islamic Azad University 2 Plasma Physics Research Center, , P.O. Box 14835-157, Tehran, Iran
  • M. V. Takook
    Razi University 3 Department of Physics, , P. O. Box 67155, Kermanshah, Iran

Abstract

<jats:p>We proceed to the quantization of the massless vector field in the de Sitter (dS) space. This work is the natural continuation of a previous article devoted to the quantization of the dS massive vector field [J. P. Gazeau and M. V. Takook, J. Math. Phys. 41, 5920 (2000); T. Garidi et al., ibid. 43, 6379 (2002).] The term “massless” is used by reference to conformal invariance and propagation on the dS lightcone whereas “massive” refers to those dS fields which unambiguously contract to Minkowskian massive fields at zero curvature. Due to the combined occurrences of gauge invariance and indefinite metric, the covariant quantization of the massless vector field requires an indecomposable representation of the de Sitter group. We work with the gauge fixing corresponding to the simplest Gupta–Bleuler structure. The field operator is defined with the help of coordinate-independent de Sitter waves (the modes). The latter are simple to manipulate and most adapted to group theoretical approaches. The physical states characterized by the divergencelessness condition are, for instance, easy to identify. The whole construction is based on analyticity requirements in the complexified pseudo-Riemannian manifold for the modes and the two-point function.</jats:p>

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