  We find all the exact eigenstates and eigenvalues of a spin-1/2 model on
square lattice: $H=16g \sum_i S^y_i S^x_{i+x} S^y_{i+x+y} S^x_{i+y}$. We show
that the ground states for $g<0$ and $g>0$ have different quantum orders
described by Z2A and Z2B projective symmetry groups. The phase transition at
$g=0$ represents a new kind of phase transitions that changes quantum orders
but not symmetry. Both the Z2A and Z2B states are described by $Z_2$ lattice
gauge theories at low energies. They have robust topologically degenerate
ground states and gapless edge excitations.
