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Covariance-refined preparation uncertainty without operator products
Statement
Assume the Axiom of Countable Choice (The Axiom of Countable Choice ()). Let be a complex Hilbert space with inner product linear in the first argument (Real and complex inner product spaces, with the inner product linear in the first argument, Hilbert space), let be symmetric densely defined operators on (Symmetric, self-adjoint and essentially self-adjoint operators, Adjoint of a densely defined operator), and let satisfy . Put and define the covariance of the pair in the preparation by . Then:
(a) ; ; and is symmetric in its two arguments: ;
(b) covariance-refined bound: so in particular ;
(c) equality holds in (b)'s first inequality if and only if and are linearly dependent (in the convention that or counts as dependence);
(d) if in addition — that is and — then the pairing is defined and in particular it is purely imaginary, and consequently
Clauses (a)-(c) use no product or and no assumption on the domains of such products. The quantities are preparation quantities of the vector ; no measurement model, apparatus error or energy-time interpretation is asserted.
Facts & Assumptions
Given: symmetric densely defined on a complex Hilbert space , a unit vector , the numbers , vectors and .
for symmetric, , ; and , so the mean of a symmetric operator in any vector of its domain is real (Symmetric, self-adjoint and essentially self-adjoint operators, Adjoint of a densely defined operator).
Cauchy–Schwarz in a complex inner product space: , with equality if and only if are linearly dependent; and (Cauchy–Schwarz: , with equality exactly for linearly dependent vectors).
The weak-form Robertson lemma of Weak-form Robertson uncertainty on a common domain states in clause (b) exactly the inequality for the present data; it is recorded here for comparison, and is derived below from [F2] without operator products.
If then , hence .
Proof
[Means, centered vectors and covariance] By [F1], and are real, so and are well-defined vectors of (the sums lie in because and are scalars). By [F4], , which is real by definition. This is (a).
[The refined bound] Apply [F2] to : , and [F2] again gives . Squaring the first inequality and substituting the second gives , which is (b) and reproduces [F3] without any operator product.
[Equality case] Equality holds in exactly when equality holds in , since the second step is an identity with added, i.e. it is always an equality. By [F2] that holds exactly for linearly dependent . This is (c).
[Commutator pairing] Assume . Then and , so both (symmetry of applied to and ) and (symmetry of ) are defined. Writing , the computation with real gives by [F4]. Hence , which is purely imaginary. Substituting into (b) gives and, taking square roots, . This is (d).
Depends on
Weak-form Robertson uncertainty on a common domain
Cauchy–Schwarz: , with equality exactly for linearly dependent vectors
Symmetric, self-adjoint and essentially self-adjoint operators
Adjoint of a densely defined operator
Real and complex inner product spaces, with the inner product linear in the first argument
Hilbert space
The Axiom of Countable Choice ()
Dependency tree · 2 levels
Sources
- G. Teschl, Mathematical Methods in Quantum Mechanics, 1st edition 2009, Section 2.1 pp. 55-57 and Section 3.1 pp. 88-92 (symmetric operators, variances and the Robertson inequality)
- MIT 8.05 Quantum Physics II (Fall 2013), Chapter 5 'Uncertainty Principle and Compatible Observables', pp. 1-8 (variance, covariance and Cauchy-Schwarz refined uncertainty)