In mathematics, the resolvent formalism is a technique for applying concepts from complex analysis to the study of the spectrum of operators on Banach spaces and more general spaces. Formal justification for the manipulations can be found in the framework of holomorphic functional calculus.
The resolvent captures the spectral properties of an operator in the analytic structure of the functional. Given an operator A, the resolvent may be defined as
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 in the complex plane that separates λ from the rest of the spectrum of A. Then the residue
The Hille–Yosida theorem relates the resolvent through a Laplace transform to an integral over the one-parameter group of transformations generated by A. Thus, for example, if A is a Hermitian, then U(t) = exp(itA) is a one-parameter group of unitary operators. The resolvent of iA can be expressed as the Laplace transform
The first major use of the resolvent operator as a series in A (cf. Liouville–Neumann series) 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.
(Note that Dunford and Schwartz, cited, define the resolvent as (zI −A)−1, instead, so that the formula above differs in sign from theirs.)
The second resolvent identity is a generalization of the first resolvent identity, above, useful for comparing the resolvents of two distinct operators. Given operators A and B, both defined on the same linear space, and z in ρ(A)∩ρ(B) the following identity holds,
When studying an unbounded operator A: H → H on a Hilbert space H, if there exists such that is a compact operator, we say that A has compact resolvent. The spectrum of such A is a discrete subset of . If furthermore A is self-adjoint, then and there exists an orthonormal basis of eigenvectors of A with eigenvalues respectively. Also, has no finite accumulation point.
- Taylor, section 9 of Appendix A.
- Dunford and Schwartz, Vol I, Lemma 6, p. 568.
- Hille and Phillips, Theorem 4.8.2, p. 126
- Taylor, p. 515.
- Dunford, Nelson; Schwartz, Jacob T. (1988), Linear Operators, Part I General Theory, Hoboken, NJ: Wiley-Interscience, ISBN 0-471-60848-3
- Fredholm, Erik I. (1903), "Sur une classe d'equations fonctionnelles" (PDF), Acta Mathematica, 27: 365–390, doi:10.1007/bf02421317
- Hille, Einar; Phillips, Ralph S. (1957), Functional Analysis and Semi-groups, Providence: American Mathematical Society, ISBN 978-0-8218-1031-6.
- Kato, Tosio (1980), Perturbation Theory for Linear Operators (2nd ed.), New York, NY: Springer-Verlag, ISBN 0-387-07558-5.
- Taylor, Michael E. (1996), Partial Differential Equations I, New York, NY: Springer-Verlag, ISBN 7-5062-4252-4