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Support of the spectral measure, the spectrum and the values of the scalar law
Statement
Assume the Axiom of Choice and the Axiom of Countable Choice (The Axiom of Choice, The Axiom of Countable Choice ()). Let be a nonzero complex Hilbert space (Hilbert space) and let be a self-adjoint operator on with spectral projection-valued measure on the Borel -algebra of and spectrum (Spectral theorem for unbounded self-adjoint operators (PVM form), Resolvent and spectrum of an unbounded operator). Then:
(a) , equivalently for every Borel set ; and for every nonempty relatively open subset . Thus the support of is exactly .
(b) For every density operator on , the scalar law of Density operators and scalar spectral probability clause (b) satisfies for every Borel set : no mass lies outside the spectrum.
(c) More generally, if is a Borel set with , then for every density operator , and if then .
Facts & Assumptions
Given: The Axiom of Choice and the Axiom of Countable Choice (The Axiom of Choice, The Axiom of Countable Choice ()); a nonzero complex Hilbert space ; a self-adjoint operator with spectral PVM and spectrum ; density operators on .
Spectrum from the calculus. The spectrum of is the essential range of the Borel function with respect to , and for the operator is with domain ; consequently, for real , if and only if for every (Unbounded Borel functional calculus: domains, products, spectral mapping, Spectral theorem for unbounded self-adjoint operators (PVM form)).
Projection-valued measure. takes values in orthogonal projections, , , , and for pairwise disjoint Borel with union the series converges in norm to for every (Projection valued measure).
Monotonicity and vanishing. If then and is an orthogonal projection with range orthogonal to the range of ; hence for every . Consequently, if then for every Borel (Projection valued measure, Scalar and complex measures from a pvm).
Scalar law. For a density operator and a PVM the assignment is a probability measure with in every expansion , , , orthonormal; in particular implies and implies (Density operators and scalar spectral probability clauses (a) and (b)).
Countable dense subset. The set is countable and dense in ( is countably infinite, Both and are dense in , and every nonempty open subset of is uncountable).
Proof
[The spectrum is the essential range of the identity] By [F1] applied to , is the essential range of the identity with respect to . For real this says: if and only if for every ; and for non-real , taking gives , where , so by [F2] and no non-real point lies in the essential range.
[The open null set equals the complement of the spectrum] Let be the set of pairs of rationals , countable by [F5], and put , a countable union of Borel sets. To see , suppose ; then with for some rationals , and choosing with gives by [F3], contradicting by step 1.1. Conversely, if , step 1.1 supplies with , and by density of the rationals [F5] there are rationals with ; then by [F3], so . Hence .
[The complement of the spectrum is null] The representation of step 2.1 writes as a countable union of Borel null sets. Enumerate these sets as , repeating if there are only finitely many, and put and for . The are pairwise disjoint, have union , and satisfy by monotonicity [F3]. Strong countable additivity [F2] therefore gives for every , so . By additivity [F2], this is equivalent to for every Borel .
[Nonempty relatively open subsets of the spectrum are not null] Let be nonempty and relatively open, so for some open . Choose and with . By step 1.1, because ; by step 3.1 applied to the Borel set , , and by the choice of . Were , monotonicity [F3] would give , a contradiction; hence . This proves clause (a) together with step 3.1.
[Clause (b)] By step 3.1 and additivity of , for every Borel ; applying the scalar law [F4] to both sides gives , and with this reads by [F4].
[Clause (c)] If then by [F4] for every density operator; if then by [F4]. Both statements are instances of the scalar law, and clause (b) is the case and respectively.
Depends on
The Axiom of Choice
The Axiom of Countable Choice ()
Hilbert space
Projection valued measure
Resolvent and spectrum of an unbounded operator
Density operators and scalar spectral probability
Both and are dense in , and every nonempty open subset of is uncountable
Scalar and complex measures from a pvm
is countably infinite
Spectral theorem for unbounded self-adjoint operators (PVM form)
Unbounded Borel functional calculus: domains, products, spectral mapping
Dependency tree · 2 levels
Sources
- G. Teschl, Mathematical Methods in Quantum Mechanics, 1st edition 2009, Section 3.1, Theorem 3.8 and Corollary 3.9, printed page 97 (support of the spectral measure and the spectrum of a self-adjoint operator)
- D. Tong, Quantum Mechanics (author-hosted lecture set), Section 5.1.1, printed page 68 (the outcome of a measurement of an observable lies in its spectrum)
- B. Zwiebach, MIT 8.05 Quantum Physics II (Fall 2013), Chapter 3 'Linear Algebra: Vector Spaces and Operators', Sections 6-7, printed pages 20-28 (adjoint operators and Hermitian operators)