  Magnetotransport properties are investigated in the bilayer quantum Hall
state at the total filling factor $\nu=2$. We measured the activation energy
elaborately as a function of the total electron density and the density
difference between the two layers. Our experimental data demonstrate clearly
the emergence of the canted antiferromagnetic (CAF) phase between the
ferromagnetic phase and the spin-singlet phase. The stability of the CAF phase
is discussed by the comparison between experimental results and theoretical
calculations using a Hartree-Fock approximation and an exact diagonalization
study. The data reveal also an intrinsic structure of the CAF phase divided
into two regions according to the dominancy between the intralayer and
interlayer correlations.
