It is shown that U(1) chiral gauge theories with anomaly free multiplets of
Weyl fermions can be put on the lattice without breaking the gauge invaria
nce or violating any other fundamental principle. The Ginsparg-Wilson relat
ion plays a key role in this construction, which is nonperturbative and inc
ludes all topological sectors of the theory in finite volume. In particular
, the cancellation of the gauge anomaly and the absence of global topologic
al obstructions can be established on the basis of this relation and the la
ttice symmetries alone. (C) 1999 Elsevier Science B.V. All rights reserved.