operator theory
Resolvent and Spectrum of an Operator
You should know: bounded operators, banach algebras
Overview
The spectrum of a bounded linear operator T on a Banach space generalises the set of eigenvalues from linear algebra. The spectrum sigma(T) consists of all scalars lambda for which T - lambda I is not invertible. The resolvent set rho(T) is its complement, and on rho(T) the resolvent operator R(lambda, T) = (T - lambda I)^{-1} is a bounded operator-valued analytic function. Spectral theory underpins the spectral theorem for self-adjoint operators, perturbation theory, and the study of differential equations.
Intuition
For a finite matrix, the spectrum is exactly the set of eigenvalues. In infinite dimensions, there are more ways to fail invertibility: the operator could fail to be injective (eigenvalue), or injective but not have dense range (residual spectrum), or have dense but non-closed range (continuous spectrum). The resolvent R(lambda, T) = (T - lambda I)^{-1} encodes all spectral information: it is analytic outside sigma(T) and has singularities on sigma(T). Spectral theory is the study of these singularities.
Formal Definition
Let T in B(X) where X is a complex Banach space. The resolvent set rho(T) = {lambda in C : T - lambda I is bijective with bounded inverse}. The spectrum sigma(T) = C \ rho(T). The resolvent operator is R(lambda, T) = (T - lambda I)^{-1} in B(X) for lambda in rho(T). The spectrum decomposes: the point spectrum sigma_p(T) consists of eigenvalues (T - lambda I not injective), the continuous spectrum sigma_c(T) where T - lambda I is injective with dense but not closed range, and the residual spectrum sigma_r(T) where T - lambda I is injective with non-dense range.
Notation
| Notation | Meaning |
|---|---|
| Spectrum of operator T | |
| Resolvent set of T | |
| Resolvent operator at lambda | |
| Spectral radius of T | |
| Point spectrum (eigenvalues) |
Theorems
Worked Examples
- 1
Point spectrum: If Rx = lambda x then (0,x_1,x_2,...) = (lambda x_1, lambda x_2,...). The first component gives 0 = lambda x_1. If lambda != 0 then x_1 = 0, then x_2 = 0, etc., forcing x = 0. If lambda = 0, Rx = 0 requires x = 0. So sigma_p(R) = {}.
- 2
For |lambda| > 1: ||(R - lambda I)|| >= |lambda| - ||R|| = |lambda| - 1 > 0 and (R - lambda I) is invertible by a Neumann argument (or directly: (R - lambda I)^{-1} exists and is bounded). So |lambda| > 1 implies lambda in rho(R).
- 3
For |lambda| < 1: The adjoint R* is the left shift: R*(x_1,x_2,...) = (x_2,x_3,...). We check R*e_1 = 0 where e_1 = (1,0,0,...), so 0 is an eigenvalue of R*, meaning 0 in sigma_p(R*). For any lambda with |lambda| < 1, one shows lambda is an eigenvalue of R*, hence lambda in sigma_r(R) subset sigma(R).
- 4
For |lambda| = 1: A limiting argument shows lambda in sigma(R). Combining, sigma(R) = {lambda : |lambda| <= 1}.
✓ Answer
The spectrum of the right shift on l^2 is the closed unit disk, with empty point spectrum. The spectral radius is 1 = ||R||.
Practice Problems
Show that the spectrum sigma(T) of T in B(X) is a closed subset of C.
For T in B(X), which is always true about sigma(T)?
Quiz
Summary
- The spectrum sigma(T) = C \ rho(T) generalises eigenvalues to infinite-dimensional spaces.
- sigma(T) is always a non-empty compact subset of the disk |lambda| <= ||T||.
- The resolvent R(lambda,T) = (T - lambda I)^{-1} is analytic in lambda on rho(T).
- The resolvent identity: R(lambda,T) - R(mu,T) = (mu - lambda)R(lambda,T)R(mu,T).
- The spectrum decomposes into point, continuous, and residual parts.
References
- BookRudin, W. — Functional Analysis (2nd ed.), Chapter 10
- BookKato, T. — Perturbation Theory for Linear Operators, Chapter III
- Websiteen.wikipedia.org
Mathematics