  Continuous-time random walks combining diffusive scattering and ballistic
propagation on lattices model a class of L\'evy walks. The assumption that
transitions in the scattering phase occur with exponentially-distributed
waiting times leads to a description of the process in terms of multiple
states, whose distributions evolve according to a set of delay differential
equations, amenable to analytic treatment. We obtain an exact expression of the
mean squared displacement associated with such processes and discuss the
emergence of asymptotic scaling laws in regimes of diffusive and superdiffusive
(subballistic) transport, emphasizing, in the latter case, the effect of
initial conditions on the transport coefficients. Of particular interest is the
case of rare ballistic propagation, in which case a regime of superdiffusion
may lurk underneath one of normal diffusion.
