“…It is well known that the transmission probability through a potential is always equal for particles moving in opposite directions i.e., the tunneling characteristics are invariant with respect to the replacement x→Ϫx in the equation of motion. 4 According to this invariance, U eff (x,k y ,ϩ1)ϭU eff (Ϫx,k y ,Ϫ1) in Eq. ͑2͒ will lead to the independence of the transmission probability on the spin direction.…”