  In this work, we determine states of electronic order of small-angle twisted
bilayer graphene. Ground states are determined for weak and strong couplings
which are representatives for varying distances of the twist-angle from its
magic value. In the weak-coupling regime, charge density waves emerge which
break translational and $C_{3}$-rotational symmetry. In the strong
coupling-regime, we find rotational and translational symmetry breaking Mott
insulating states for all commensurate moir\'e band fillings. Depending on the
local occupation of superlattice sites hosting up to four electrons, global
spin-(ferromagnetic) and valley symmetries are also broken which may give rise
to a reduced Landau level degeneracy as observed in experiments for
commensurate band fillings. The formation of those particular electron orders
is traced back to the important role of characteristic non-local interactions
which connect all localized states belonging to one hexagon formed by the AB-
and BA-stacked regions of the superlattice.
