  We find mode-locking steps in simulated current-voltage characteristics of
driven vortex lattices with {\it random} pinning when an applied ac-current is
{\it perpendicular} to the dc-current. For low frequencies there is
mode-locking only above a non-zero threshold ac force amplitude, while for
large frequencies there is mode-locking for any small ac force. This is
consistent with the nature of {\it transverse} temporal order in the different
regimes in the absence of an applied ac-drive. For large frequencies the
magnitude of the fundamental mode-locked step depends linearly with the ac
force amplitude.
