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Compact operator

From Wikipedia, the free encyclopedia
Type of continuous linear operator

Infunctional analysis, a branch ofmathematics, acompact operator is alinear operatorT:XY{\displaystyle T:X\to Y}, whereX,Y{\displaystyle X,Y} arenormed vector spaces, with the property thatT{\displaystyle T} mapsbounded subsets ofX{\displaystyle X} torelatively compact subsets ofY{\displaystyle Y} (subsets with compactclosure inY{\displaystyle Y}). Such an operator is necessarily abounded operator, and so continuous.[1] Some authors require thatX,Y{\displaystyle X,Y} areBanach, but the definition can be extended to more general spaces.

Any bounded operatorT{\displaystyle T} that has finiterank is a compact operator; indeed, the class of compact operators is a natural generalization of the class offinite-rank operators in an infinite-dimensional setting. WhenY{\displaystyle Y} is aHilbert space, it is true that any compact operator is a limit (inoperator norm) of finite-rank operators,[1] so that the class of compact operators can be defined alternatively as the closure of the set of finite-rank operators in thenorm topology. Whether this was true in general for Banach spaces (theapproximation property) was an unsolved question for many years; in 1973Per Enflo gave a counter-example, building on work byAlexander Grothendieck andStefan Banach.[2]

The origin of the theory of compact operators is in the theory ofintegral equations, where integral operators supply concrete examples of such operators. A typicalFredholm integral equation gives rise to a compact operatorK onfunction spaces; the compactness property is shown byequicontinuity. The method of approximation by finite-rank operators is basic in the numerical solution of such equations. The abstract idea ofFredholm operator is derived from this connection.

Definitions

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TVS case

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LetX,Y{\displaystyle X,Y} betopological vector spaces andT:XY{\displaystyle T:X\to Y} a linear operator.

The following statements are equivalent, and different authors may pick any one of these as the principal definition for "T{\displaystyle T} is a compact operator":[3]

Normed case

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If in additionX,Y{\displaystyle X,Y} are normed spaces, these statements are also equivalent to:[4]

Banach case

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If in additionY{\displaystyle Y} is Banach, these statements are also equivalent to:

Properties

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In the following,X,Y,Z,W{\displaystyle X,Y,Z,W} are Banach spaces,B(X,Y){\displaystyle B(X,Y)} is the space of bounded operatorsXY{\displaystyle X\to Y} under theoperator norm, andK(X,Y){\displaystyle K(X,Y)} denotes the space of compact operatorsXY{\displaystyle X\to Y}.IdX{\displaystyle \operatorname {Id} _{X}} denotes theidentity operator onX{\displaystyle X},B(X)=B(X,X){\displaystyle B(X)=B(X,X)}, andK(X)=K(X,X){\displaystyle K(X)=K(X,X)}.

Now suppose thatX{\displaystyle X} is a Banach space andT:XX{\displaystyle T\colon X\to X} is a compact linear operator, andT:XX{\displaystyle T^{*}\colon X^{*}\to X^{*}} is theadjoint ortranspose ofT.

Origins in integral equation theory

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A crucial property of compact operators is theFredholm alternative in the solution of linear equations. LetK{\displaystyle K} be a compact operator,f{\displaystyle f} a given function, andu{\displaystyle u} the unknown function to be solved for. Then the Fredholm alternative states that the equation(λK+I)u=f{\displaystyle (\lambda K+I)u=f}behaves much like as in finite dimensions.

Thespectral theory of compact operators then follows, and it is due toFrigyes Riesz (1918). It shows that a compact operatorK{\displaystyle K} on an infinite-dimensional Banach space has spectrum that is either a finite subset ofC{\displaystyle \mathbb {C} } which includes 0, or the spectrum is acountably infinite subset ofC{\displaystyle \mathbb {C} } which has0{\displaystyle 0} as its onlylimit point. Moreover, in either case the non-zero elements of the spectrum areeigenvalues ofK{\displaystyle K} with finite multiplicities (so thatKλI{\displaystyle K-\lambda I} has a finite-dimensionalkernel for all complexλ0{\displaystyle \lambda \neq 0}).

An important example of a compact operator iscompact embedding ofSobolev spaces, which, along with theGårding inequality and theLax–Milgram theorem, can be used to convert anelliptic boundary value problem into a Fredholm integral equation.[8] Existence of the solution and spectral properties then follow from the theory of compact operators; in particular, an elliptic boundary value problem on a bounded domain has infinitely many isolated eigenvalues. One consequence is that a solid body can vibrate only at isolated frequencies, given by the eigenvalues, and arbitrarily high vibration frequencies always exist.

The compact operators from a Banach space to itself form a two-sidedideal in thealgebra of all bounded operators on the space. Indeed, the compact operators on an infinite-dimensional separable Hilbert space form a maximal ideal, so thequotient algebra, known as theCalkin algebra, issimple. More generally, the compact operators form anoperator ideal.

Compact operator on Hilbert spaces

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Main article:Compact operator on Hilbert space

For Hilbert spaces, another equivalent definition of compact operators is given as follows.

An operatorT{\displaystyle T} on an infinite-dimensionalHilbert space(H,,){\displaystyle ({\mathcal {H}},\langle \cdot ,\cdot \rangle )},

T:HH{\displaystyle T\colon {\mathcal {H}}\to {\mathcal {H}}},

is said to becompact if it can be written in the form

T=n=1λnfn,gn{\displaystyle T=\sum _{n=1}^{\infty }\lambda _{n}\langle f_{n},\cdot \rangle g_{n}},

where{f1,f2,}{\displaystyle \{f_{1},f_{2},\ldots \}} and{g1,g2,}{\displaystyle \{g_{1},g_{2},\ldots \}} are orthonormal sets (not necessarily complete), andλ1,λ2,{\displaystyle \lambda _{1},\lambda _{2},\ldots } is a sequence of positive numbers with limit zero, called thesingular values of the operator, and the series on the right hand side converges in the operator norm. The singular values canaccumulate only at zero. If the sequence becomes stationary at zero, that isλN+k=0{\displaystyle \lambda _{N+k}=0} for someNN{\displaystyle N\in \mathbb {N} } and everyk=1,2,{\displaystyle k=1,2,\dots }, then the operator has finite rank,i.e., a finite-dimensional range, and can be written as

T=n=1Nλnfn,gn{\displaystyle T=\sum _{n=1}^{N}\lambda _{n}\langle f_{n},\cdot \rangle g_{n}}.

An important subclass of compact operators is thetrace-class ornuclear operators, i.e., such thatTr(|T|)<{\displaystyle \operatorname {Tr} (|T|)<\infty }. While all trace-class operators are compact operators, the converse is not necessarily true. For exampleλn=1n{\textstyle \lambda _{n}={\frac {1}{n}}} tends to zero forn{\displaystyle n\to \infty } whilen=1|λn|={\textstyle \sum _{n=1}^{\infty }|\lambda _{n}|=\infty }.

Completely continuous operators

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LetX,Y{\displaystyle X,Y} be Banach spaces. A bounded linear operatorT:XY{\displaystyle T:X\to Y} is calledcompletely continuous if, for everyweakly convergentsequence(xn){\displaystyle (x_{n})} fromX{\displaystyle X}, the sequence(Txn){\displaystyle (Tx_{n})} is norm-convergent inY{\displaystyle Y} (Conway 1985, §VI.3).

Compact operators on a Banach space are always completely continuous, but theconverse is false, because there exists a completely continuous operator that is not compact. However, the converse is true ifX{\displaystyle X} is areflexive Banach space, then every completely continuous operatorT:XY{\displaystyle T:X\to Y} is compact.

Somewhat confusingly, compact operators are sometimes referred to as "completely continuous" in older literature, even though they are not necessarily completely continuous by the definition of that phrase in modern terminology.

Examples

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See also

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Notes

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  1. ^abConway 1985, Section 2.4
  2. ^abEnflo 1973
  3. ^Schaefer & Wolff 1999, p. 98.
  4. ^abBrézis, H. (2011).Functional analysis, Sobolev spaces and partial differential equations. H.. Brézis. New York: Springer.ISBN 978-0-387-70914-7.OCLC 695395895.
  5. ^abcdefghiRudin 1991, pp. 103–115.
  6. ^N.L. Carothers,A Short Course on Banach Space Theory, (2005) London Mathematical Society Student Texts64, Cambridge University Press.
  7. ^abcConway 1990, pp. 173–177.
  8. ^William McLean, Strongly Elliptic Systems and Boundary Integral Equations, Cambridge University Press, 2000
  9. ^Kreyszig 1978, Theorems 2.5-3, 2.5-5.

References

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