  We examine the transport of magnetic energy in a simplified model of a
magnetic metamaterial, consisting of a one-dimensional array of split-ring
resonators, in the presence of correlated disorder in the resonant frequencies.
The computation of the average participation ratio (PR) reveals that on
average, the modes for the correlated disorder system are less localized than
in the uncorrelated case. The numerical computation of the mean square
displacement of an initially localized magnetic excitation for the correlated
case shows a substantial departure from the uncorrelated (Anderson-like) case.
A long-time asymptotic fit $\langle n^2\rangle \sim t^\alpha$ reveals that, for
the uncorrelated system $\alpha\sim 0$, while for the correlated case
$\alpha>0$, spanning a whole range of behavior ranging from localization to
super-diffusive behavior. The transmission coefficient of a plane wave across a
single magnetic dimer reveals the existence of well-defined regions in disorder
strength-magnetic coupling space, where unit transmission for some
wavevector(s) is possible. This implies, according to the random dimer model
(RDM) of Dunlap et al., a degree of mobility. A comparison between the
mobilities of the correlated SRR system and the RDM shows that the RDM model
has better mobility at low disorder while our correlated SRR model displays
better mobility at medium and large disorder.
