  Ruderman-Kittel-Kasuya-Yosida (RKKY) is an essential long range magnetic
interaction between magnetic impurities or magnetic layered structures, the
magnitude of which oscillates with the distance ($\mathrm{R}$) between them. We
have investigated the RKKY interaction between two magnetic impurities in both
time-reversal and inversion symmetry broken Weyl semimetals (WSMs) where the
energy dispersion is tilted in momentum space and the momentum of the
conduction electron is locked with the pseudo-spin. Two important features are
revealed, firstly, at the small tilt limit, we show that the RKKY coupling
varies quadratically with the tilt parameter and strikingly, at large
separation distance $\mathrm{R}$, the coupling decays as $1/\mathrm{R}$
compared to the conventional of $1/\mathrm{R}^{3}$ dependence exhibited by WSMs
with non-tilted dispersion. The slower decay by two orders i.e. ($1/\mathrm{R}$
as opposed to $1/\mathrm{R}^{3}$) of the RKKY coupling is significant for
maintaining long range RKKY coupling. Secondly, the RKKY coupling exhibits an
anisotropy with respect to the angle between the tilt direction ($\mathbf{w}$)
and the separation direction $\mathbf{R}$ unlike the case of non-tilted WSMs
which exhibit isotropic RKKY coupling. Consequently, the RKKY coupling in
tilted WSMs alternately favours ferromagnetic and anti-ferromagnetic orders and
vice-versa with the change of the angle. Our results are derived analytically
and verified by numerical calculations based on realistic parameter values.
