  We derive the effective field theory from the microscopic Hamiltonian of
interacting two-dimensional (pseudo) Dirac electrons by performing a statistic
gauge transformation. The quantized Hall conductance are expected to be
$\sigma_{xy}=\frac{e^2}{h}(2k-1)$ with $k$ is arbitrary integer. There are also
topological excitations which have fractional charge and obey fractional
statistics.
