Resolvents & Operator Spectrum

The spectrum records where an operator minus a scalar multiple of the identity cannot be stably inverted. This chapter develops resolvent identities, spectral types, Neumann bounds, the spectral-radius formula, and the special geometry of self-adjoint and normal operators.

An eigenvalue detects failure of injectivity, but infinite-dimensional inversion can fail even with no eigenvector: the range may be non-dense, not closed, or dense but not all of the space. The spectrum collects every scalar where bounded invertibility fails.

Resolvent and spectrum #

Let T∈B(X)T\in\mathcal B(X) on a complex Banach space. The resolvent set is

ρ(T)={λ∈C:T−λI is bijective with bounded inverse}.\rho(T)=\{\lambda\in\mathbb C:T-\lambda I \text{ is bijective with bounded inverse}\}.

The spectrum is σ(T)=C∖ρ(T)\sigma(T)=\mathbb C\setminus\rho(T), and R(λ,T)=(T−λI)−1R(\lambda,T)=(T-\lambda I)^{-1} is the resolvent. The bounded-inverse condition is redundant once bijectivity and the Banach hypotheses are known, but keeping it in the definition makes the stability meaning explicit.

For ∣λ∣>∥T∥|\lambda|>\|T\|,

T−λI=−λ(I−Tλ)T-\lambda I=-\lambda\left(I-\frac{T}{\lambda}\right)

is invertible by the Neumann series. Therefore

σ(T)⊆{λ:∣λ∣≤∥T∥}.\sigma(T)\subseteq\{\lambda:|\lambda|\le\|T\|\}.

The spectrum of a bounded operator on a nonzero complex Banach space is nonempty and compact.

Why the resolvent is analytic #

The first resolvent identity is

R(λ,T)−R(μ,T)=(λ−μ)R(λ,T)R(μ,T).R(\lambda,T)-R(\mu,T) =(\lambda-\mu)R(\lambda,T)R(\mu,T).

Near λ0∈ρ(T)\lambda_0\in\rho(T),

R(λ,T)=R(λ0,T)∑n=0∞[(λ−λ0)R(λ0,T)]nR(\lambda,T) =R(\lambda_0,T) \sum_{n=0}^{\infty} \left[(\lambda-\lambda_0)R(\lambda_0,T)\right]^n

with the sign adjusted to the chosen T−λIT-\lambda I convention; direct factorization confirms it. This norm-convergent power series makes ρ(T)\rho(T) open and the resolvent analytic. It also shows that

∥R(λ,T)∥≥1dist(λ,σ(T)).\|R(\lambda,T)\|\ge \frac{1}{\mathop{\mathrm{dist}}(\lambda,\sigma(T))}.

For normal Hilbert-space operators equality holds; for nonnormal operators the resolvent can be much larger, producing pseudospectral sensitivity far from the spectrum.

Spectral failure modes #

A common disjoint classification for T−λIT-\lambda I is:

  • point spectrum: not injective; λ\lambda is an eigenvalue;
  • continuous spectrum: injective with dense range, but not surjective;
  • residual spectrum: injective with non-dense range.

Terminology varies slightly between texts, so the injective/range statement is more reliable than the label. Approximate eigenvectors ∥xn∥=1\|x_n\|=1 with ∥(T−λI)xn∥→0\|(T-\lambda I)x_n\|\to0 explain how stable inversion can fail without an actual eigenvector.

Spectral radius #

The spectral radius

r(T)=sup⁡{∣λ∣:λ∈σ(T)}r(T)=\sup\{|\lambda|:\lambda\in\sigma(T)\}

satisfies the Gelfand formula

r(T)=lim⁡n→∞∥Tn∥1/n=inf⁡n≥1∥Tn∥1/n.r(T)=\lim_{n\to\infty}\|T^n\|^{1/n} =\inf_{n\ge1}\|T^n\|^{1/n}.

Always r(T)≤∥T∥r(T)\le\|T\|, and strict inequality is possible. Thus r(T)<1r(T)<1 does not imply ∥T∥<1\|T\|<1, although it does imply that sufficiently large powers decay geometrically after choosing a rate above r(T)r(T).

Examples #

  • For scalar multiplication T=αIT=\alpha I, the spectrum is {α}\{\alpha\}.
  • For multiplication MgM_g on a standard LpL^p space, the spectrum is the essential range of gg.
  • The Volterra operator on C[0,1]C[0,1] has spectrum {0}\{0\} but is not the zero operator: it is quasinilpotent rather than nilpotent.
  • A compact operator has a particularly discrete nonzero spectrum; only zero can be an accumulation point.

Self-adjoint and normal structure #

For bounded self-adjoint TT on a Hilbert space,

σ(T)⊂R,r(T)=∥T∥,\sigma(T)\subset\mathbb R, \qquad r(T)=\|T\|,

and the spectral extremes control the quadratic form. For normal TT, ∥T∥=r(T)\|T\|=r(T) and the resolvent norm equals reciprocal distance to the spectrum. In general the spectrum is contained in the closure of the numerical range

W(T)={⟨Tx,x⟩:∥x∥=1};W(T)=\{\langle Tx,x\rangle:\|x\|=1\};

the closure cannot be omitted for an arbitrary bounded operator.

Spectral checklist #

  • Work over a complex Banach space, or explicitly complexify a real problem.
  • Fix whether the resolvent uses T−λIT-\lambda I or λI−T\lambda I-T before using identities.
  • Distinguish eigenvalues from the full spectrum.
  • Inspect the range and inverse norm, not only the kernel.
  • For nonnormal operators, use resolvent or pseudospectral information when perturbation sensitivity matters.

Sources

  1. bookIntroduction to Functional Analysis: Lecture Notes for 18.102pdfnotes

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