We analyze the structure of models with unbroken and spontaneously bro
ken U(1)(a) x U(1)(b) gauge symmetry. We show that the quantum correct
ions to the 2N gauge charges, with N = number of fermions + number of
scalars, can be absorbed in the redefinition of three independent gaug
e couplings (g(a), g(b), and g(ab)). We establish the (one-loop) condi
tions on the matter content for g(ab) = 0 (a value usually assumed in
the literature) and we show that in the minimal extensions of the Stan
dard Model with an extra U(1) symmetry the choice g(ab) = 0 is not sta
ble under radiative corrections induced by the standard Higgs fields.
Moreover, g(ab) = 0 to all orders seems to require an exact symmetry.
The spontaneous breaking of the gauge symmetry induces further mixing
between the two gauge bosons and introduces a fourth independent physi
cal parameter. A consequence of our analysis is that the usual tree-le
vel description with only three physical parameters (i.e., two gauge c
ouplings and one gauge boson mixing angle) is not in general a justifi
ed zero order limit of the treatment including radiative corrections.