Hadamard well-posedness requires existence, uniqueness, and continuous dependence of on . A compact operator with infinite-dimensional range cannot have closed range: otherwise its inverse on the orthogonal complement of its kernel would be bounded, making the identity on an infinite-dimensional space compact. Hence the inverse on is unbounded. If uniqueness also fails, and data outside the range have no exact solution. In every case at least stability fails, so the inverse problem is ill posed.
If , the partial Neumann series satisfies
Since , the series converges in operator norm and
If and , apply this identity to :
The normal equation for a linear inverse problem is
It has a solution exactly when
When solutions exist they form
They are unique exactly when , while is always the unique solution in and the solution of minimum norm. Here is the Moore-Penrose inverse.
The operator is positive, self-adjoint, and compact. Because is infinite dimensional, the spectral theorem for compact Hermitian operators gives positive spectral values tending to zero. Even if , zero remains in the spectrum as a limit point. Hence for every ,
The strict inequality needed for the operator-norm Neumann series is impossible, so formula (3) cannot be applied directly to invert .
Let be a singular system for . The Picard criterion for is
after discarding the component in . For , the partial series acts diagonally:
For each the multiplier in the numerator tends to one and lies in . The Picard summability condition therefore supplies an dominating sequence, so the dominated convergence theorem gives
This is the series form of Landweber iteration.
For , put and define the bounded operator
Part (e) shows for every as . Since ,
Choose the a priori rule
Then while
For ,
Thus with this parameter rule is a regularization of an inverse problem.

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