Spectral theory of compact operators

Spectral theory of compact operators

In functional analysis, compact operators are linear operators that map bounded sets to precompact ones. Compact operators acting on a Hilbert space "H" is the closure of finite rank operators in the uniform operator topology. In general, operators on infinite dimensional spaces feature properties that do not appear in the finite dimensional case, i.e. for matrices. The family of compact operators are notable in that they share as much similarity with matrices as one can expect from a general operator. In particular, the spectral properties of compact operators resemble those of square matrices.

This article first summarize the corresponding results from the matrix case before discussing the spectral properties of compact operators. The reader will see that most statements transfer verbatim from the matricial case.

The spectral theory of compact operators was first developed by F. Riesz.

Spectral theory of matrices

The classification 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"

:mathbb{C}^n = oplus _{i = 1} ^k Y_i.

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

Let "X" be a Banach space, "C" be a compact operator acting on "X", and "σ"("C") be the spectrum of "C". The spectral properties of "C" are:

Theorem

i) Every nonzero "λ" ∈ "σ"("C") is an eigenvalue of "C".

ii) For all nonzero "λ" ∈ "σ"("C"), there exist "m" such that "Ker"("λi" - "A")"m" = "Ker"("λi" - "A")"m"+1.

iii) The eigenvalues can only accumulate at 0. If the dimension of "X" is not finite, then "σ"("C") must contain 0.

iv) "σ"("C") is countable.

v) Every nonzero "λ" ∈ "σ"("C") is a pole of the resolvent function "ζ" → ("ζ" - "C")-1.

Proof

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. The first is called Riesz's lemma:

Lemma 1 Let "X" be a Banach space and "Y" ⊂ "X", "Y" ≠ "X", be a closed subspace. For all "ε" > 0, there exists "x" ∈ "X" such that ||"x"|| = 1 and

:1 - epsilon le d(x, Y) le 1

where "d"("x", "Y") is the distance from "x" to "Y".

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.

Another useful fact is:

Lemma 2 If "C" is compact, then "Ran"("I" - "C") is closed.

Proof: Let ("I" - "C")"xn" → "y" in norm. If {"xn"} is bounded, then there exist a weakly convergent subsequence "xn k". Compactness of "C" implies "C xn k" is norm convergent. So "xn k" = ("I" - "C")"xn k" + "C xn k" is norm convergent, to some "x". This gives ("I" - "C")"xn k" → ("I" - "C")"x" = "y". The same argument goes through if the distances "d"("xn", "Ker"("I" - "C")) is bounded.

But "d"("xn", "Ker"("I" - "C")) must be bounded. Suppose this is not the case. Pass now to the quotient map of ("I" - "C"), still denoted by ("I" - "C"), on "X"/"Ker"("I" - "C"). The quotient norm on "X"/"Ker"("I" - "C") is still denoted by ||·||, and {"xn"} are now viewed as representatives of their equivalence classes in the quotient space. Take a subsequence {"xn k"} such that ||"xn k"|| > k and define a sequence of unit vectors by "zn k" = "xn k"/||"xn k"||. Again we would have ("I" - "C")"zn k" → ("I" - "C")"z" for some "z". Since ||("I" - "C")"zn k"|| = ||("I" - "C")"xn k"||/ ||"xn k"|| → 0, we have ("I" - "C")"z" = 0 i.e. "z" ∈ "Ker"("I" - "C"). Since we passed to the quotient map, "z" = 0. This is impossible because "z" is the norm limit of a sequence of unit vectors. Thus the lemma is proven.

We are now ready to prove the theorem.

i) Without loss of generality, assume "λ" = 1. "λ" ∈ "σ"("C") not being an eigenvalue means ("I" - "C") is injective but not surjective. By Lemma 2, "Y"1 = "Ran"("I" - "C") is a closed proper subspace of "X". Since ("I" - "C") is injective, "Y"2 = ("I" - "C")"Y"1 is again a closed proper subspace of "Y"1. Define "Y"n = "Ran"("I" - "C")"n". Consider the decreasing sequence of subspaces

:Y_1 supset cdots supset Y_n cdots supset Y_m cdots

where all inclusions are proper. By lemma 1, we can choose unit vectors "yn" &isin; "Yn" such that "d"("yn", "Y""n"+1) > &frac12;. Compactness of "C" means {"C yn"} must contain a norm convergent subsequence. But for "n" < "m"

:| C y_n - C y_m | = | (C-I) y_n + y_n - (C-I) y_m - y_m |

and notice that

:(C-I) y_n - (C-I) y_m - y_m in Y_{n+1},

which implies ||"Cyn - Cym"|| > &frac12;. This is a contradiction, and so "λ" must be an eigenvalue.

ii) The sequence { "Yn" = "Ker"("λi" - "A")"n"} is an increasing sequence of closed subspaces. The theorem claims it stops. Suppose it does not stop, i.e. the inclusion "Ker"("λi" - "A")"n" &sub; "Ker"("λi" - "A")"n"+1 is proper for all "n". By lemma 1, there exists a sequence {"yn"}"n" &ge; 2 of unit vectors such that "yn" &isin; "Y""n" and "d"("yn", "Y""n" - 1) > &frac12;. As before, compactness of "C" means {"C yn"} must contain a norm convergent subsequence. But for "n" < "m"

:| C y_n - C y_m | = | (C-I) y_n + y_n - (C-I) y_m - y_m |

and notice that

:(C-I) y_n + y_n - (C-I) y_m in Y_{m-1},

which implies ||"Cyn - Cym"|| > &frac12;. This is a contradiction, and so the sequence { "Yn" = "Ker"("λi" - "A")"n"} must terminate at some finite "m".

iii) Suppose eigenvalues of "C" do not accumulate at 0. We can therefore assume that there exist a sequence of distinct eigenvalues {"λn"}, with corresponding eigenvectors {"xn"}, such that |"λn"| > "ε" for all "n". Define "Yn" = "span"{"x"1..."xn"}. The sequence {"Yn"} is a strictly increasing sequence. Choose unit vectors such that "yn" &isin; "Y""n" and "d"("yn", "Y""n" - 1) = 1. Then for "n" < "m"

:| C y_n - C y_m | = | (C- lambda_n) y_n + lambda_n y_n - (C- lambda_m) y_m - lambda_m y_m |.

But :(C- lambda_n) y_n + lambda_n y_n - (C- lambda_m) y_m in Y_{m-1},

therefore ||"Cyn - Cym"|| > "ε", a contradiction.

iv) This is an immediate consequence of iii). The set of eigenvalues {"λ"} is the union

:cup_n { |lambda| > frac{1}{n} } = cup_n S_n .

Because "σ"("C") is a bounded set and the eigenvalues can only accumulate at 0, each "Sn" is finite, which gives the desired result.

v) As in the matrix case, this is a direct application of the holomorphic functional calculus.

Invariant 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" &ne; 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

:, E(lambda) = {1over 2pi i}int _{gamma} (xi - C)^{-1} d xi

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 {"λ"}, therefore "Y" is finite dimensional. Let "&nu;" be such that "Ker"("λ" - "C")"&nu;" = "Ker"("λ" - "C")"&nu;" + 1. By inspecting the Jordan form, we see that ("λ" - "C")"&nu;" = 0 while ("λ" - "C")"&nu;" - 1 &ne; 0. The Laurent series of the resolvent mapping centered at "λ" shows that

:, E(lambda) (lambda - C)^{ u} = (lambda - C)^{ u}E(lambda) = 0.

So "Y" = "Ker"("λ" - "C")"&nu;".

The E(lambda) satisfy E(lambda)^2=E(lambda), so that they are indeed projection operators or spectral projections. By definition they commute with "C".Moreover E(lambda)E(mu)=0 if lambda and mu are distinct.

* Let X(lambda)=E(lambda)X if lambda is a non-zero eigenvalue. Thus X(lambda) is a finite-dimensional invariant subspace, the generalised eigenspace of lambda.

* Let X(0) be the intersection of the kernels of the E(lambda). Thus X(0) is a closed subspace invariant under "C" and the restriction of "C" to X(0) is a compact operator with spectrum {0}.

Operator with compact power

Let "B" be an operator on "X" such that "Bn" is compact for some "n". The theorem proven above holds for "B".

References

* John B. Conway, A course in functional analysis, Graduate Texts in Mathematics "96", Springer 1990. ISBN 0-387-97245-5


Wikimedia Foundation. 2010.

Игры ⚽ Поможем сделать НИР

Look at other dictionaries:

  • Spectral theory of ordinary differential equations — In mathematics, the spectral theory of ordinary differential equations is concerned with the determination of the spectrum and eigenfunction expansion associated with a linear ordinary differential equation. In his dissertation Hermann Weyl… …   Wikipedia

  • Spectral theory — In mathematics, spectral theory is an inclusive term for theories extending the eigenvector and eigenvalue theory of a single square matrix. The name was introduced by David Hilbert in his original formulation of Hilbert space theory, which was… …   Wikipedia

  • Compact operator on Hilbert space — In functional analysis, compact operators on Hilbert spaces are a direct extension of matrices: in the Hilbert spaces, they are precisely the closure of finite rank operators in the uniform operator topology. As such, results from matrix theory… …   Wikipedia

  • Compact operator — In functional analysis, a branch of mathematics, a compact operator is a linear operator L from a Banach space X to another Banach space Y, such that the image under L of any bounded subset of X is a relatively compact subset of Y. Such an… …   Wikipedia

  • Spectral theorem — In mathematics, particularly linear algebra and functional analysis, the spectral theorem is any of a number of results about linear operators or about matrices. In broad terms the spectral theorem provides conditions under which an operator or a …   Wikipedia

  • Fredholm theory — In mathematics, Fredholm theory is a theory of integral equations. In the narrowest sense, Fredholm theory concerns itself with the solution of the Fredholm integral equation. In a broader sense, the abstract structure of Fredholm s theory is… …   Wikipedia

  • Sturm-Liouville theory — In mathematics and its applications, a classical Sturm Liouville equation, named after Jacques Charles François Sturm (1803 1855) and Joseph Liouville (1809 1882), is a real second order linear differential equation of the formwhere y is a… …   Wikipedia

  • Operator theory — In mathematics, operator theory is the branch of functional analysis that focuses on bounded linear operators, but which includes closed operators and nonlinear operators. Operator theory also includes the study of algebras of operators. Contents …   Wikipedia

  • Mercer's theorem — In mathematics, specifically functional analysis, Mercer s theorem is a representation of a symmetric positive definite function on a square as a sum of a convergent sequence of product functions. This theorem, presented in (Mercer 1909), is one… …   Wikipedia

  • List of mathematics articles (S) — NOTOC S S duality S matrix S plane S transform S unit S.O.S. Mathematics SA subgroup Saccheri quadrilateral Sacks spiral Sacred geometry Saddle node bifurcation Saddle point Saddle surface Sadleirian Professor of Pure Mathematics Safe prime Safe… …   Wikipedia

Share the article and excerpts

Direct link
Do a right-click on the link above
and select “Copy Link”