We study BPS-saturated domain walls in the supersymmetric SU(2) gauge theor
y. For a theory with a very light adjoint scalar (mass m less than or simil
ar to Lambda/400) we use the perturbed N = 2 Seiberg-Witten theory to calcu
late the actual field configuration of the domain wall. The wall has a sand
wich-like five-layer structure of three distinct phases - electric confinem
ent, Coulomb and oblique confinement-separated by two separate transition r
egions. For larger scalar masses, the three-phase structure disappears and
the Seiberg-Witten theory becomes inadequate because of two major problems:
First, the higher-derivative interactions between the light fields become
relevant and second, both the magnetic monopole condensate and the dyon con
densate show up in the same region of space, a phenomenon indescribable in
terms of a local field theory. Nevertheless, we argue that the BPS-saturate
d domain wall continues to exist in this regime and give a qualitative desc
ription of the scalar and gaugino condensates, Finally, we discuss the doma
in walls in MQCD and translate the BPS conditions into coupled non-linear d
ifferential equations. (C) 1999 Elsevier Science B.V. All rights reserved.