Atkinson's theorem
In operator theory, the Atkinson's theorem gives a characterization of Fredholm operators.
The theorem
Let H be a Hilbert space and L(H) the bounded operators on H. The following is the classical definition of a Fredholm operator: a T ∈ L(H) is said to be a Fredholm operator if Ker(T) is finite dimensional, Ker(T*) is finite dimensional, and Ran(T) is closed.
Atkinson's theorem states:
- A T ∈ L(H) is a Fredholm operator if and only if T is invertible modulo compact perturbation, i.e. TS = I + C1 and ST = I + C2 for some bounded operator S and compact operators C1 and C2.
In other words, a operator T ∈ L(H) is Fredholm, in the classical sense, if and only if its projection in the Calkin algebra is invertible.
Sketch of proof
The outline of a proof is as follows. For the ⇒ implication, express H as the orthogonal direct sum
The restriction T : Ker(T)⊥ → Ran(T) is a bijection, therefore invertible by the open mapping theorem. Extending this inverse by 0 on Ran(T)⊥ = Ker(T*) to an operator S defined on all of H. Then I - TS is the finite rank projection onto Ker(T*) and I - ST projection onto Ker(T). This proves the only if part of the theorem.
For the converse, suppose now ST = I + C2 for some compact operator C2. If x ∈ Ker(T), then STx = x + C2x = 0. So Ker(T) is contained in an eigenspace of C2, which is finite dimensional (see spectral theory of compact operators). Therefore Ker(T) is fintie dimensional. Same argument shows Ker(T*) is also.
To prove that Ran(T) is closed, we make use of the approximation property: let F be a finite rank operator such that ||F - C2|| < r. Then for every x in Ker(F),
- ||S||·||Tx|| ≥ ||STx|| = ||x + C2x|| = ||x + Fx +C2x - Fx|| ≥ ||x|| - ||C2 - F||·||x|| ≥ (1 - r)||x||.
Thus T is bounded below on Ker(F), which implies T(Ker(F)) is closed. On the other hand, T(Ker(F)⊥) is finite dimensional, since Ker(F)⊥ = Ran(F*) is finite dimensional. Therefore Ran(T) = T(Ker(F)) + T(Ker(F)⊥) is closed and this proves the theorem.
Reference
- F.V. Atkinson, The normal solvability of linear equations in normed spaces, Mat. Sb. 28 (70), 1951, 3-14.