  The temperature dependence of quantum Hall conductivities is studied in the
context of the AdS/CMT paradigm using a model with a bulk theory consisting of
(3+1)-dimensional Einstein-Maxwell action coupled to a dilaton and an axion,
with a negative cosmological constant. We consider a solution which has a
Lifshitz like geometry with a dyonic black-brane in the bulk. There is an
$Sl(2,R)$ action in the bulk corresponding to electromagnetic duality, which
maps between classical solutions, and is broken to $Sl(2,Z)$ by Dirac
quantisation of dyons. This bulk $Sl(2,Z)$ action translates to an action of
the modular group on the 2-dimensional transverse conductivities. The
temperature dependence of the infra-red conductivities is then linked to
modular forms via gradient flow and the resulting flow diagrams show remarkable
agreement with existing experimental data on the temperature flow of both
integral and fractional quantum Hall conductivities.
