  Schwinger boson mean field theory is a powerful approach to study frustrated
magnetic systems which allows to distinguish long range magnetic orders from
quantum spin liquid phases, where quantum fluctuations remain strong up to zero
temperature. In this work, we use this framework to study the Heisenberg model
on the Kagome lattice with up to third nearest neighbour interaction and
Dzyaloshinskii-Moriya (DM) antisymmetric exchange. This model has been argued
to be relevant for the description of transition metal dichalcogenide bilayers
in certain parameter regimes, where spin liquids could be realized. By means of
the projective symmetry group classification of possible ans\"atze, we study
the effect of the DM interaction at first nearest neighbor and then compute the
$J_2$-$J_3$ phase diagram at different DM angles. We find a new phase
displaying chiral spin liquid characteristics up to spin $S=0.5$, indicating an
exceptional stability of the state.
