  We study the phase transition in the abelian lattice gauge theory using the
Wilson-Polyakov line as the order parameter. The Wilson-Polyakov line remains
very small at strong coupling and becomes non-zero at weak coupling, signalling
a confinement to deconfinement phase transition. The decondensation of monopole
loops is responsible for this phase transition. A finite size scaling analysis
of the susceptibility of the Wilson line gives a ratio for $\gamma/\nu$ which
is quite close to the corresponding value in the 3-d planar model. A scaling
behaviour for the monopole loop distribution function is also established at
the point of the second order phase transition. A measurement of the plaquette
susceptibility at the transition point shows that it does not scale with the
four dimensional volume as is expected of a first order bulk transition.
