It is shown that the Anderson-Mott metal-insulator transition of paramagnet
ic interacting disordered electrons in an external magnetic field is in the
same universality class as the transition from a ferromagnetic metal to a
ferromagnetic insulator discussed recently. As a consequence, large correct
ions to scaling exist in the magnetic-field universality class, which have
been neglected in previous theoretical descriptions. The nature and consequ
ences of these corrections to scaling are discussed.