  Ho\v{r}ava-Lifshitz gravity is shown to exhibit a peculiar behavior, when
scattering amplitudes are considered. At low energies it seems to classicalize
i.e. the effective size of the interaction grows as a function of the
$s$-parameter, with BHs forming part of the spectrum; but when the probing
energy is increased such that higher order operators become important, this
behavior changes and the classicalon recedes to a new configuration where
ordinary quantum regimes take over. Eventually, the theory behaves as a usual
field theory that allows probing arbitrarily small distances. In particular,
the classical potential created by a point-like source is finite everywhere
exhibiting a Vainshtein alike screening behavior. The transition from one
behavior to the other is carefully described in a particular case.
