In this paper we study the properties of a gas of fermions coupling to a U(
1) gauge field at wave vectors q<<Lambda><<k(F) at dimensions larger than 1
, where Lambda<<k(F) is a high-momentum cutoff and k(F) is the Fermi wave v
ector. In particular, we shall consider the e(2)-->infinity limit, where ch
arge and current fluctuations at wave vectors q<<Lambda> are forbidden. By
generalizing a method reported in a previous paper [Phys. Rev. B 62, 7019 (
2000)], we show that the system can be described as a "marginal" Fermi Liqu
id of spin 1/2; chargeless fermions with vanishing wave functions overlap w
ith the bare fermions in the system.