  We get an anomalous Hall metallic state in the Honeycomb lattice with nearest
neighbors only arising as a spontaneously broken symmetry state from a local
nearest neighbor Coulomb interaction V . The key ingredient is to enlarge the
unit cell to host six atoms that permits Kekul\'e distortions and supports
self-consistent currents creating non trivial magnetic configurations with
total zero flux. We find within a variational mean field approach a metallic
phase with broken time reversal symmetry (T) very close in parameter space to a
Pomeranchuk instability. Within the T broken region the predominant
configuration is an anomalous Hall phase with non zero Hall conductivity, a
realization of a topological Fermi liquid. A T broken phase with zero Hall
conductivity is stable in a small region of the parameter space for lower
values of V .
