In a bilayer electronic system the layer index may be viewed as the z compo
nent of an isospin-1/2. An XY isospin-ordered ferromagnetic phase was obser
ved in quantum Hall systems and is predicted to exist at zero magnetic fiel
d at low density. This phase is a superfluid for opposite currents in the t
wo layers. At B = 0 the system is gapless but superfluidity is not destroye
d by weak disorder. In the quantum Hall case, weak disorder generates a ran
dom gauge field which probably does not destroy superfluidity. Experimental
signatures include Coulomb drag and collective mode measurements.