  We study the chiral magnetic effect (CME) in tilted multi-Weyl Semimetals
(WSM) employing a two-band lattice model. We focus on the type-II phase of
mWSMs, introduced by incorporating a Lorentz symmetry violating tilt term. We
add to the understanding of the CME (and anomalous Hall effect) in the type-II
phase of mWSMs and near the Lifshitz transition by varying tilt. Like the
elementary WSM, our results also indicate that the Berry curvature drives the
CME for higher monopole charges. We find a peak in the CME at the transition
point and discuss its significance using the density of states. Along the way
we also examine both observables as a function of the energy separation of the
Weyl points.
