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Continuous functional calculus under resolvent convergence
Statement
Assume the Axiom of Choice. Let be self-adjoint operators on a complex Hilbert space and suppose in the strong resolvent sense. Then for every bounded continuous and every . If in the norm resolvent sense, then for every bounded continuous with . In both cases the conclusion does not depend on the nonreal parameter used in the definition of convergence.
Facts & Assumptions
On nonzero complex , AC supplies the spectral PVM of each self-adjoint , representing as the integral of the identity on its squared-integrability domain. The unbounded calculus has the exact product domain , and sums and products agree with their pointwise counterparts on their domains (Spectral theorem for unbounded self-adjoint operators (PVM form), Unbounded Borel functional calculus: domains, products, spectral mapping).
The bounded PVM calculus is linear, unital, multiplicative and conjugation preserving, satisfies and , and . Its Countable Choice assumptions are supplied by AC (Bounded borel pvm integral, Pvm integral is a star homomorphism, Scalar and complex measures from a pvm, The Axiom of Choice).
exists for nonreal with . Convergence is initially assumed at one fixed nonreal parameter only (Resolvent of a self-adjoint operator: nonreal resolvents and the estimate, Resolvent and spectrum of an unbounded operator, Norm and strong resolvent convergence).
For fixed nonreal , the linear span of , , , is uniformly dense in (The resolvent star algebra is dense in C_0(R)). Only its function-algebra density assertion is used; parameter independence is proved below.
Scalar dominated convergence holds with an integrable majorant (Dominated convergence). Operator norm bounds give and, by applying this twice, (A bounded linear operator between normed spaces, The operator norm as the least bound and as the unit-sphere or unit-ball supremum).
Proof
Given: AC, the self-adjoint operators and convergence at a fixed nonreal in the indicated mode.
If , all operators, resolvents and bounded functions of them are the unique full-domain operator, so all assertions hold. Suppose . For nonreal put . Both and are bounded on the real line. The product-domain rule in [A1] shows that maps into and on , while on . Thus with the convention of [A3]. The bounded calculus agrees with its unbounded truncation definition because the truncations are eventually the same bounded function.
Put . The scalar identity and [A2] give these identities for each single operator . Define and , which is independent of . Expanding the product using the preceding identities yields : its two terms are and , whose mixed terms cancel. The left factor has norm at most . Consequently in the strong case, since is fixed, and in the norm case. This proves parameter independence without taking a strong limit on a varying vector.
In particular convergence holds at and , and , , with the analogous formulas for . Both sequences are uniformly bounded. If and strongly and , then . In the norm case the same inequality with operator norms proves convergence of products when the factors are uniformly bounded. Iteration and finite linear combinations, using [A2], therefore prove convergence for every polynomial in with zero constant term.
Given and , choose one such polynomial with by [A4]. The bounded calculus gives . For fixed the last term tends to zero by step 3.1; since is arbitrary, strong convergence follows for each (including directly). The operator-norm inequality is , proving the norm version as well.
In the norm case, if has a common finite limit at both ends, then . Unital linearity gives , so step 4.1 proves the assertion.
For the strong case let be any bounded continuous function and set . For integers define . These are continuous, compactly supported, between zero and one, equal to one on , and converge pointwise to one. Thus by dominated convergence with majorant , integrable against the finite measure of mass . For fixed , both and belong to , so their calculi converge strongly by step 4.1.
Bounded multiplicativity and linearity give the exact four-term decomposition . Applying it to , its norm is at most . If the claim is immediate. Otherwise choose so that the first term is less than half a prescribed positive error, using step 5.2, and then so that the other two together are less than its other half. This proves strong convergence for bounded continuous .
Step 2.1 proves independence of every nonreal parameter, step 5.1 the norm conclusion and step 6.1 the strong conclusion. AC supplies the spectral and countable-choice calculus hypotheses; the cutoffs are explicit. The zero Hilbert space and zero function have been treated in steps 1.1 and 6.1; no limit at either infinity is required in the strong case.
Source notes
Teschl, Theorem 6.31 and its proof, pp.179-180, gives the polynomial approximation and four-term cutoff route, with Corollary 6.32 giving parameter independence. Here the latter is proved first using a resolvent-difference factorization with a fixed right factor. The library convention is , so . No general continuity of adjoints for strongly convergent bounded operators is assumed.
Depends on
- Norm and strong resolvent convergence
- The resolvent star algebra is dense in C_0(R)
- Unbounded Borel functional calculus: domains, products, spectral mapping
- Spectral theorem for unbounded self-adjoint operators (PVM form)
- Dominated convergence
- A bounded linear operator between normed spaces
- The operator norm as the least bound and as the unit-sphere or unit-ball supremum
- The Axiom of Choice
- Bounded borel pvm integral
- Pvm integral is a star homomorphism
- Scalar and complex measures from a pvm
- Resolvent of a self-adjoint operator: nonreal resolvents and the estimate
- Resolvent and spectrum of an unbounded operator
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Sources
- Gerald Teschl, Mathematical Methods in Quantum Mechanics, second edition (standard reference, not scraped)