Spectral theory of matrices
The classical result for square matrices is the Jordan canonical form, which states the following: Theorem. Let ''A'' be an ''n'' × ''n'' complex matrix, i.e. ''A'' a linear operator acting on C''n''. If ''λ''1...''λk'' are the distinct eigenvalues of ''A'', then C''n'' can be decomposed into the invariant subspaces of ''A'' : The subspace ''Yi'' = ''Ker''(''λi'' − ''A'')''m'' where ''Ker''(''λi'' − ''A'')''m'' = ''Ker''(''λi'' − ''A'')''m''+1. Furthermore, the poles of the resolvent function ''ζ'' → (''ζ'' − ''A'')−1 coincide with the set of eigenvalues of ''A''.Compact operators
Statement
Proof
;Preliminary Lemmas The theorem claims several properties of the operator ''λ'' − ''C'' where ''λ'' ≠ 0. Without loss of generality, it can be assumed that ''λ'' = 1. Therefore we consider ''I'' − ''C'', ''I'' being the identity operator. The proof will require two lemmas. This fact will be used repeatedly in the argument leading to the theorem. Notice that when ''X'' is a Hilbert space, the lemma is trivial. ;Concluding the ProofInvariant subspaces
As in the matrix case, the above spectral properties lead to a decomposition of ''X'' into invariant subspaces of a compact operator ''C''. Let ''λ'' ≠ 0 be an eigenvalue of ''C''; so ''λ'' is an isolated point of ''σ''(''C''). Using the holomorphic functional calculus, define the Riesz projection ''E''(''λ'') by : where ''γ'' is a Jordan contour that encloses only ''λ'' from ''σ''(''C''). Let ''Y'' be the subspace ''Y'' = ''E''(''λ'')''X''. ''C'' restricted to ''Y'' is a compact invertible operator with spectrum , therefore ''Y'' is finite-dimensional. Let ''ν'' be such that ''Ker''(''λ'' − ''C'')''ν'' = ''Ker''(''λ'' − ''C'')''ν'' + 1. By inspecting the Jordan form, we see that (''λ'' − ''C'')''ν'' = 0 while (''λ'' − ''C'')''ν'' − 1 ≠ 0. The Laurent series of the resolvent mapping centered at ''λ'' shows that : So ''Y'' = ''Ker''(''λ'' − ''C'')''ν''. The ''E''(''λ'') satisfy ''E''(''λ'')2 = ''E''(''λ''), so that they are indeed projection operators or spectral projections. By definition they commute with ''C''. Moreover ''E''(''λ'')''E''(''μ'') = 0 if λ ≠ μ. * Let ''X''(''λ'') = ''E''(''λ'')''X'' if λ is a non-zero eigenvalue. Thus ''X''(''λ'') is a finite-dimensional invariant subspace, the generalised eigenspace of λ. * Let ''X''(0) be the intersection of the kernels of the ''E''(''λ''). Thus ''X''(0) is a closed subspace invariant under ''C'' and the restriction of ''C'' to ''X''(0) is a compact operator with spectrum .Operators with compact power
If ''B'' is an operator on a Banach space ''X'' such that ''Bn'' is compact for some ''n'', then the theorem proven above also holds for ''B''.See also
*References
* John B. Conway, A course in functional analysis, Graduate Texts in Mathematics ''96'', Springer 1990. {{Spectral theory Functional analysis Spectral theory Linear operators