  We investigate the orbital Hall conductivity in bilayer graphene (G/G), by
modifying one of the layer as Haldane type with the next nearest neighbour
(NNN) hopping strength and flux. The Haldane flux in one of the layer breaks
the time reversal symmetry in both the layers and induces the gap opening at
the Dirac points $K$ and $K'$ points. It is observed that the low energy
isolated bands show large orbital magnetization and induce the Hall potential
for opposite magnetic polarization under the external fields, thereby
contribute to the orbital Hall conductivity (OHC). The self-rotation of the
isolated electrons in their respective orbits leads to strong orbital angular
momentum, which is more fundamental in non-magnetic materials. The observed OHC
is similar to the anomalous Hall conductivity (AHC). Moreover, the orbital
magnetization with opposite sign among the occupied states adds up to the
higher OHC in the gap, whereas the AHC get vanishes. We further show the
results of bilayer graphene with both the layers as Haldane type ($\rm \tilde
G/ \tilde G$), and found that the OHC behaves similar to AHC which indicate
that, the OHC is strongly depends on the band dispersion. Similarly, we show
that in the heterobilayers with one of the layer is Haldane type generates the
orbital magnetization and induces the OHC. It is concluded that, the isolated
bands in Graphene bilayers with external stimuli are of orbital nature and show
orbital ferromagnetism in the valleys in BZ.
