  It has been noticed that confinement effects can be described by the addition
of a $ \sqrt {- F_{\mu \nu}^a F^{a\mu \nu}} $ term in the Lagrangian density.
We now study the combined effect of such "confinement term" and that of a mass
term. The surprising result is that the interplay between these two terms gives
rise to a Coulomb interaction. Our picture has a certain correspondence with
the quasiconfinement picture described by Giles, Jaffe and de Rujula for QCD
with symmetry breaking.
