For any nonzero ,
either
1. The equation
has a nonzero solution
, or
2. The equation
has a unique solution
for any function
.
In the second case, the solution depends continuously on
. The Fredholm alternative applies when
is a compact operator,
such as an integral operator with a smooth integral
kernel.
The Fredholm alternative can be restated as follows: any nonzero which is not an eigenvalue
of a compact operator is in the resolvent,
i.e.,
,
is bounded. The basic special case is when
is finite-dimensional, in which case
any nondegenerate matrix is diagonalizable.