  Topological states require the presence of extended bulk states, as usually
found in the picture of energy bands and topological states bridging the bulk
gaps. But in driven systems this can be circumvented, and one can get
topological states coexisting with fully localized bulk states, as in the case
of the anomalous Floquet-Anderson insulator. Here, we show the fingerprints of
this peculiar topological phase in the transport properties and their
dependence on the disorder strength, geometrical configuration (two-terminal
and multiterminal setups) and details of the driving protocol.
