We find all the general forms which a spacetime metric can take, when this
spacetime obeys a discrete or continuous axial symmetry, whether it is rota
ting or not. If the spacetime is not symmetrical under a reflection through
a plane orthogonal to its symmetry axis, there are two different classes:
the first class corresponds to a discrete symmetry of order two, all the ot
her symmetries, be they discrete or continuous, are linked to the same gene
ral metric form. If the spacetime does possess this reflection symmetry, we
have four classes of metrics. The three classes having discrete admit a no
nstatic metric.