Any bounded operator 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. When 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.
In the following, are Banach spaces, is the space of bounded operators under theoperator norm, and denotes the space of compact operators. denotes theidentity operator on,, and.
If a linear operator is compact, then it is continuous.
is a closed subspace of (in the norm topology). Equivalently,[5]
given a sequence of compact operators mapping (whereare Banach) and given that converges to with respect to theoperator norm, is then compact.
In particular, the limit of a sequence of finite rank operators is a compact operator.
Conversely, if are Hilbert spaces, then every compact operator from is the limit of finite rank operators. Notably, this "approximation property" is false for general Banach spaces and.[2][4]
where thecomposition of sets is taken element-wise. In particular, forms a two-sidedideal in.
if the range of is closed in, then the range of is finite-dimensional.
If is a Banach space and there exists aninvertible bounded compact operator then is necessarily finite-dimensional.[7]
Now suppose that is a Banach space and is a compact linear operator, and is theadjoint ortranspose ofT.
For any, is aFredholm operator of index 0. In particular, is closed. This is essential in developing the spectral properties of compact operators. One can notice the similarity between this property and the fact that, if and are subspaces of where is closed and is finite-dimensional, then is also closed.
If is any bounded linear operator then both and are compact operators.[5]
If then the range of is closed and the kernel of is finite-dimensional.[5]
A crucial property of compact operators is theFredholm alternative in the solution of linear equations. Let be a compact operator, a given function, and the unknown function to be solved for. Then the Fredholm alternative states that the equationbehaves 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 operator on an infinite-dimensional Banach space has spectrum that is either a finite subset of which includes 0, or the spectrum is acountably infinite subset of which has as its onlylimit point. Moreover, in either case the non-zero elements of the spectrum areeigenvalues of with finite multiplicities (so that has a finite-dimensionalkernel for all complex).
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.
For Hilbert spaces, another equivalent definition of compact operators is given as follows.
An operator on an infinite-dimensionalHilbert space,
,
is said to becompact if it can be written in the form
,
where and are orthonormal sets (not necessarily complete), and 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 is for some and every, then the operator has finite rank,i.e., a finite-dimensional range, and can be written as
.
An important subclass of compact operators is thetrace-class ornuclear operators, i.e., such that. While all trace-class operators are compact operators, the converse is not necessarily true. For example tends to zero for while.
Let be Banach spaces. A bounded linear operator is calledcompletely continuous if, for everyweakly convergentsequence from, the sequence is norm-convergent in (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 if is areflexive Banach space, then every completely continuous operator 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.
The scaling operator for any nonzero is compact if and only if the space is finite-dimensional. This can be proven directly, or as a corollary ofRiesz's lemma.[9]
In particular, everyHilbert–Schmidt integral operator is compact. That is, if is any domain in and the integral kernel satisfies, then the integral operator on defined by is a compact operator.
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Kutateladze, S.S. (1996).Fundamentals of Functional Analysis. Texts in Mathematical Sciences. Vol. 12 (2nd ed.). New York: Springer-Verlag. p. 292.ISBN978-0-7923-3898-7.
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