  We discuss topological electronic states described by the Dirac Hamiltonian
plus an additional one in three-dimension. When the additional Hamiltonian is
an element of an Abelian group, electronic states become topologically
nontrivial even in the absence of fundamental symmetries such as the
time-reversal and the particle-hole symmety. The symmetry-breaking topological
states are charercterized by the Chern number defined in the two-dimensional
partial Brillouin zone. The topological insulators under Zeeman field are an
example of the symmetry-breaking topological matters. We show the transision
from the topological insulating phase to the topological semimetal one under
the strong Zeeman field.
