  We examine the phenomenon of Landau Damping in relativistic plasmas via a
study of the relativistic Vlasov-Poisson system (rVP) on the torus for initial
data sufficiently close to a spatially uniform steady state. We find that if
the steady state is regular enough (essentially in a Gevrey class of degree in
a specified range) and that the deviation of the initial data from this steady
state is small enough in a certain norm, the evolution of the system is such
that its spatial density approaches a uniform constant value sub-exponentially
fast (i.e. like $\exp(-C|t|^{\overline{\nu}})$ for $\overline{\nu} \in (0,1)$).
We take as \emph{a priori} assumptions that solutions launched by such initial
data exist for all times (by no means guaranteed with rVP, but reasonable since
we are close to a spatially uniform state) and that the various norms in
question are continuous in time (which should be a consequence of an abstract
version of the Cauchy-Kovalevskaya Theorem). In addition, we must assume a kind
of "reverse Poincar\'e inequality" on the Fourier transform of the solution. In
spirit, this assumption amounts to the requirement that there exists
$0<\varkappa<1$ so that the mass in the annulus $\varkappa \le |v| < 1$ for the
solution launched by the initial data is uniformly small for all $t$.
