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In [[mathematics]], the '''resolvent formalism''' is a technique for applying concepts from [[complex analysis]] to the study of the [[spectrum (functional analysis)|spectrum]] of [[Operator (mathematics)|operator]]s on [[Hilbert space]]s and more general spaces.
 
The '''resolvent''' captures the spectral properties of an operator in the analytic structure of the resolvent. Given an operator ''A'', the resolvent may be defined as
 
: <math> R(z;A)= (A-zI)^{-1}. </math>
 
Among other uses, the resolvent may be used to solve the inhomogeneous [[Fredholm integral equation]]s; a commonly used approach is a series solution, the [[Liouville-Neumann series]].
 
The resolvent of ''A'' can be used to directly obtain information about the spectral decomposition
of ''A''. For example, suppose <math> \lambda </math> is an isolated [[eigenvalue]] in the
[[spectrum]] of ''A''. That is, suppose there exists a simple closed curve <math> C_\lambda </math>
in the complex plane
that separates <math> \lambda </math> from the rest of the spectrum of ''A''.
Then the [[residue (complex analysis)|residue]]
 
: <math> \frac{-1}{2\pi i} \oint_{C_\lambda} (A- z I)^{-1}~ dz </math>
 
defines a [[projection operator]] onto the <math> \lambda </math> [[eigenspace]] of ''A''.  
 
The [[Hille-Yosida theorem]] relates the resolvent to an integral over the one-parameter [[group (mathematics)|group]] of transformations generated by ''A''. Thus, for example, if ''A'' is [[Hermitian operator|Hermitian]], then <math>U(t)=\exp(itA)</math> is a one-parameter group of unitary operators. The resolvent can be expressed as the integral
 
: <math>R(z;A)= \int_0^\infty e^{-zt}U(t) dt.</math>
 
==History==
The first major use of the resolvent operator was by [[Ivar Fredholm]], in a landmark 1903 paper in ''Acta Mathematica'' that helped establish modern [[operator theory]].  The name ''resolvent'' was given by [[David Hilbert]].
 
==Resolvent identity==
 
For all <math>z, w</math> in <math>\rho(A)</math>, the [[resolvent set]] of an operator <math>A</math>, we have that the '''resolvent identity''' (also called Hilbert's identity) holds:<ref>Dunford and Schwartz, Vol I, Lemma 6, p568.</ref>
:<math>R(z; A) - R(w; A) = (w-z) R(z;A) R(w;A)\,</math>
(Note that Dunford and Schwartz define the resolvent as <math>(zI-A)^{-1}</math> so that the formula above is slightly different from theirs.)
 
==Compact resolvent==
When studying an [[unbounded operator]] <math>A:H\to H</math> on a [[Hilbert space]] <math>H</math>, if there exists <math>z\in\rho(A)</math> such that <math>R(z;A)</math> is a [[compact operator]], we say that <math>A</math> has compact resolvent. The spectrum <math>\sigma(A)</math> of such <math>A</math> is a discrete subset of <math>\mathbb{C}</math>. If furthermore <math>A</math> is [[self-adjoint]], then <math>\sigma(A)\subset\mathbb{R}</math> and there exists an orthonormal basis <math>\{v_i\}_{i\in\mathbb{N}}</math> of eigenvectors of <math>A</math> with eigenvalues <math>\{\lambda_i\}_{i\in\mathbb{N}}</math> respectively. Also, <math>\{\lambda_i\}</math> has no finite accumulation point.<ref>Taylor, p515.</ref>
 
==See also==
* [[Resolvent set]]
* [[Stone's theorem]]
* [[Holomorphic functional calculus]]
* [[Spectral theory]]
* [[Compact operator]]
* [[Unbounded operator]]
 
==References==
<references/>
* [[Nelson Dunford]], [[Jacob T. Schwartz]] ''Linear Operators'', Part I General Theory ISBN 0-471-60848-3, Part II Spectral Theory, Self Adjoint Operators in Hilbert Space ISBN 0-471-60847-5, Part III Spectral Operators ISBN 0-471-60846-7
* E.I. Fredholm, "Sur une classe d'equations fonctionnelles", ''Acta Mathematica'', '''27'''  (1903)  pp.&nbsp;365–390.
* {{Citation
| last = Kato
| first = Tosio
| title = Perturbation Theory for Linear Operators
| edition = 2nd
| publisher = Spinger-Verlag
| location = New York, NY
| year = 1980
| isbn = 0-387-07558-5 }}.
*{{Citation
| last = Taylor
| first = Michael E. | authorlink = Michael E. Taylor
| title = Partial Differential Equations I
| publisher = Spinger-Verlag
| location = New York, NY
| year = 1996
| isbn = 7-5062-4252-4 }}
 
[[Category:Fredholm theory]]
[[Category:Formalism (deductive)]]

Revision as of 16:31, 22 January 2014

In mathematics, the resolvent formalism is a technique for applying concepts from complex analysis to the study of the spectrum of operators on Hilbert spaces and more general spaces.

The resolvent captures the spectral properties of an operator in the analytic structure of the resolvent. Given an operator A, the resolvent may be defined as

R(z;A)=(AzI)1.

Among other uses, the resolvent may be used to solve the inhomogeneous Fredholm integral equations; a commonly used approach is a series solution, the Liouville-Neumann series.

The resolvent of A can be used to directly obtain information about the spectral decomposition of A. For example, suppose λ is an isolated eigenvalue in the spectrum of A. That is, suppose there exists a simple closed curve Cλ in the complex plane that separates λ from the rest of the spectrum of A. Then the residue

12πiCλ(AzI)1dz

defines a projection operator onto the λ eigenspace of A.

The Hille-Yosida theorem relates the resolvent to an integral over the one-parameter group of transformations generated by A. Thus, for example, if A is Hermitian, then U(t)=exp(itA) is a one-parameter group of unitary operators. The resolvent can be expressed as the integral

R(z;A)=0eztU(t)dt.

History

The first major use of the resolvent operator was by Ivar Fredholm, in a landmark 1903 paper in Acta Mathematica that helped establish modern operator theory. The name resolvent was given by David Hilbert.

Resolvent identity

For all z,w in ρ(A), the resolvent set of an operator A, we have that the resolvent identity (also called Hilbert's identity) holds:[1]

R(z;A)R(w;A)=(wz)R(z;A)R(w;A)

(Note that Dunford and Schwartz define the resolvent as (zIA)1 so that the formula above is slightly different from theirs.)

Compact resolvent

When studying an unbounded operator A:HH on a Hilbert space H, if there exists zρ(A) such that R(z;A) is a compact operator, we say that A has compact resolvent. The spectrum σ(A) of such A is a discrete subset of . If furthermore A is self-adjoint, then σ(A) and there exists an orthonormal basis {vi}i of eigenvectors of A with eigenvalues {λi}i respectively. Also, {λi} has no finite accumulation point.[2]

See also

References

  1. Dunford and Schwartz, Vol I, Lemma 6, p568.
  2. Taylor, p515.
  • Nelson Dunford, Jacob T. Schwartz Linear Operators, Part I General Theory ISBN 0-471-60848-3, Part II Spectral Theory, Self Adjoint Operators in Hilbert Space ISBN 0-471-60847-5, Part III Spectral Operators ISBN 0-471-60846-7
  • E.I. Fredholm, "Sur une classe d'equations fonctionnelles", Acta Mathematica, 27 (1903) pp. 365–390.
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