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No bounded operators satisfy the canonical commutation relation with a nonzero commutator
Statement refuted
Let be a complex Hilbert space and let . Then there exist bounded linear operators with
Facts & Assumptions
Given: A nonzero complex Hilbert space ; ; a hypothetical pair of bounded linear operators with .
Operator-norm estimates. For bounded operators on , : for every , , and taking the supremum gives the claim (The operator norm as the least bound and as the unit-sphere or unit-ball supremum). Consequently for every integer . Since , .
Norm identities. The operator norm is a norm on , so it is homogeneous and satisfies the triangle and reverse-triangle inequalities (The operator norm as the least bound and as the unit-sphere or unit-ball supremum, The operator norm is a norm on the space of bounded linear operators).
Counterexample
Given: The data of the refuted statement and [F1]-[F2].
[The hypothetical operators are nonzero] Suppose satisfy . Since , and by [F1]. Because , the commutator is nonzero; hence neither nor is zero.
[Commutators with powers] For every integer , [step 1.1, algebra] The case is the assumed relation. If it holds for , then , proving it by induction. No power can be zero: if one were zero, this identity would force , and iteration would give , contradicting [F1].
[Factorial lower bound] By step 2.1 and [F1]-[F2], for every , [step 1.1, step 2.1, F1, F2, algebra] Put . Iterating the resulting inequalities from gives for every .
[Contradiction] By [F1], . Let and choose an integer . For , , so [step 3.1, F1, algebra] which tends to because . This contradicts the simultaneous lower and upper bounds on . Thus no bounded pair satisfies the commutator relation, and the displayed existential claim is refuted.
Remarks
- Unboundedness is not a technicality. The refutation shows that a canonical commutation relation with cannot hold as an identity of bounded operators; at least one of the two operators must be unbounded (or the relation must be stated on a core, as for the model's componentwise operators, or replaced by the unitary Weyl form). This is why the model defines position and momentum on dense domains rather than on all of the Hilbert space.
- What is not refuted. A core relation such as the canonical commutation relations on the Schwartz classes, and the associated one-parameter unitary groups, are unaffected: the operators there are unbounded. This item makes no statement about the Weyl form, about semiboundedness, or about any physical system.
Depends on
Dependency tree · 2 levels
Sources
- G. Teschl, Mathematical Methods in Quantum Mechanics, 1st edition 2009, Section 2.1, printed pages 55-58 (PDF pages 67-70): the closed graph theorem forces observables such as position and momentum to be unbounded, with only dense domains
- J. Binney and D. Skinner, The Physics of Quantum Mechanics, Box 2.2 and Sections 2.3.1-2.3.2, printed pages 25-27 (PDF pages 33-35): the integration-by-parts Hermiticity argument for the momentum operator (wavefunctions vanishing at spatial infinity) and the canonical commutator [x,p]=i hbar