English

Deformations of Fuchsian AdS representations are Quasi-Fuchsian

Representation Theory 2013-05-30 v2 General Relativity and Quantum Cosmology Differential Geometry

Abstract

Let Γ\Gamma be a finitely generated group, and let \opRep(Γ,\SO(2,n))\op{Rep}(\Gamma, \SO(2,n)) be the moduli space of representations of Γ\Gamma into \SO(2,n)\SO(2,n) (n2n \geq 2). An element ρ:Γ\SO(2,n)\rho: \Gamma \to \SO(2,n) of \opRep(Γ,\SO(2,n))\op{Rep}(\Gamma, \SO(2,n)) is \textit{quasi-Fuchsian} if it is faithful, discrete, preserves an acausal subset in the conformal boundary \Einn\Ein_n of the anti-de Sitter space; and if the associated globally hyperbolic anti-de Sitter space is spatially compact - a particular case is the case of \textit{Fuchsian representations}, i.e. composition of a faithfull, discrete and cocompact representation ρf:Γ\SO(1,n)\rho_f: \Gamma \to \SO(1,n) and the inclusion \SO(1,n)\SO(2,n)\SO(1,n) \subset \SO(2,n). In \cite{merigot} we proved that quasi-Fuchsian representations are precisely representations which are Anosov as defined in \cite{labourie}. In the present paper, we prove that quasi-Fuchsian representations form a connected component of \opRep(Γ,\SO(2,n))\op{Rep}(\Gamma, \SO(2,n)). This is an almost direct corollary of the following result: let Γ\Gamma be the fundamental group of a globally hyperbolic spacetime locally modeled on \AdSn\AdS_n, and let ρ:Γ\SO0(2,n)\rho: \Gamma \to \SO_0(2,n) be the holonomy representation. Then, if Γ\Gamma is Gromov hyperbolic, the ρ(Γ)\rho(\Gamma)-invariant achronal limit set in \Einn\Ein_n is acausal.

Keywords

Cite

@article{arxiv.1301.4309,
  title  = {Deformations of Fuchsian AdS representations are Quasi-Fuchsian},
  author = {Thierry Barbot},
  journal= {arXiv preprint arXiv:1301.4309},
  year   = {2013}
}