ABSTRACT
Z
u
(x^; d)g(d) ds(d); x^ 2 ; (7.1.2)
is known as the far eld operator and
true
denotes the far eld pattern
of the fundamental solution (1.2.40). The far eld operator F has smooth
kernel, is thus compact in L
( ) and in general equation (7.1.1) does not
have a solution. We temporarily assume that we are able to solve (7.1.1)
and in a second step show how to modify the approach to treat the general
case.