Based on the construction of generalized Halperin wave functions, we predic
t the possible existence of a large class of broken spin symmetry states in
bilayer quantum Hall structures, generalizing the recently suggested cante
d antiferromgnetic phase to many fractional fillings. We develop the approp
riate Chem-Simons theory, and establish explicitly that the low-lying neutr
al excitation is a Goldstone mode and that the charged excitations are bime
rons with continuously tunable (through the canted antiferromagnetic order
parameter) electric charge on the individual merons.