In five or more dimensions, U(1) lattice gauge theory shows a strong first-
order phase transition and metastable states in the region of the transitio
n. Monte Carlo calculations carried out in dimensions up to seven illustrat
e this behavior. These metastable states are well reproduced by gauge-fixed
mean-field theory for the "superheated state" (beta < beta(c)) and by Pade
approximants to the strong-coupling expansion for the "supercooled state"
(beta > beta(c)) In analogy to a Van der Waal's system, a cubic equation of
state is employed to connect the two metastable states in both the Monte C
arlo and analytic calculations. A Maxwell construct is developed allowing f
or the identification of the transition point and a complete, analytic desc
ription of the phase diagram in five and higher dimensions.