  The Seiberg--Witten equations, when dimensionally reduced to $\bf R^{2}\mit$,
naturally yield the Liouville equation, whose solutions are parametrized by an
arbitrary analytic function $g(z)$. The magnetic flux $\Phi$ is the integral of
a singular Kaehler form involving $g(z)$; for an appropriate choice of $g(z)$ ,
$N$ coaxial or separated vortex configurations with $\Phi=\frac{2\pi N}{e}$ are
obtained when the integral is regularized. The regularized connection in the
$\bf R^{1}\mit$ case coincides with the kink solution of $\varphi^{4}$ theory.
