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Position-momentum uncertainty on the maximal domains of the line
Statement
Assume the Axiom of Choice and the Axiom of Countable Choice (The Axiom of Choice, The Axiom of Countable Choice ()). Fix and let and be the position and momentum operators of Position and momentum operators on Euclidean L2 on ; by Self-adjointness, Fourier representation and translation identities of position and momentum both are self-adjoint, and . Let have , and put Then:
(a) , and with and (absolutely convergent complex integrals, the weak derivative) one has
(b) ; consequently and
(c) equality holds if and only if are linearly dependent and ;
(d) no assumption on the products or is used: the assertion holds on the full maximal domain of the pair, and the means , the centered vectors and the variances are finite on it.
The statement concerns a preparation vector only; it asserts no apparatus error, jointly measured distribution or physical interpretation.
Facts & Assumptions
Given: a unit vector with , its weak derivative , the numbers , the vectors and the variances.
has a unique continuous locally absolutely continuous representative with ; moreover for all and as (One-dimensional functions have unique absolutely continuous representatives, Endpoint trace bound and decay of H1 functions clause (c)).
There is with , on , outside ; for , satisfies on , outside , and (Explicit compactly supported smooth cutoffs).
Complex conjugation preserves and : this follows from the weak-derivative definition applied to the conjugate test functions, since for real-valued and hence for all test functions by linearity.
Smooth-factor Leibniz rule: if is smooth and is bounded for and , then with (Weak Leibniz rule with a smooth factor).
Weak product rule for bounded Sobolev factors: if , then with (Weak product rule for bounded Sobolev functions).
If has compact support, then : the absolutely continuous representative of (for ) vanishes outside a compact set, so its limiting difference and the difference formula give zero (One-dimensional functions have unique absolutely continuous representatives, applied with ).
Cauchy–Schwarz and its consequence: and (Cauchy–Schwarz: , with equality exactly for linearly dependent vectors).
Dominated convergence: if pointwise and with , then (Dominated convergence).
Covariance-refined uncertainty of Covariance-refined preparation uncertainty without operator products: for symmetric densely defined operators and a unit vector , with centered vectors , and , one has , with ; equality in holds exactly when and are linearly dependent (clauses (b) and (c) there, the equality clause being that of the Cauchy–Schwarz step).
Proof
[Integrability of the two pairings] Since , Cauchy–Schwarz gives and ; so are well-defined complex numbers.
[Smooth cutoffs and products in W^{1,2}] For put and . By [F2], and are bounded (by and ), so [F4] gives with ; also is bounded and compactly supported. By [F3] and [F1], with . Hence [F5] applies to and : , compactly supported, with using .
[The integrated identity] By [F6] applied to the compactly supported (hence ) class , .
[Limits as ] As : (i) pointwise with , so by [F8]; (ii) is bounded by and supported in , so by absolute continuity of the integral; (iii) pointwise with by step 1.1, so by [F8]. Passing to the limit in step 2.1 gives , that is .
[The second identity] Applying the same construction with replaced by (so , compactly supported, with ) and using [F6], ; as the first term tends to as in step 3.1(ii) and the second to by dominated convergence (). Hence .
[The means] is real because is self-adjoint and ; is real because is self-adjoint and . Moreover , and gives , real as required. This is (a).
[The pairing] Expand . Here and (both means real), so the last three terms sum to . And , using step 3.1. Hence , with imaginary part .
[The uncertainty bound] By [F9] (or [F7] applied to and ), . This is (b).
[Equality and scope] By the equality clause of [F9], equality in holds exactly when are linearly dependent; given step 6.1, the further condition is exactly by the identity of [F9]. This is (c). No product or was used anywhere: the means, the centered vectors and the pairings were formed from and only, so (d) holds.
Depends on
Position and momentum operators on Euclidean L2
Self-adjointness, Fourier representation and translation identities of position and momentum
Covariance-refined preparation uncertainty without operator products
One-dimensional functions have unique absolutely continuous representatives
Endpoint trace bound and decay of H1 functions
Weak product rule for bounded Sobolev functions
Weak Leibniz rule with a smooth factor
Explicit compactly supported smooth cutoffs
Cauchy–Schwarz: , with equality exactly for linearly dependent vectors
Dominated convergence
with the integral pairing is a Hilbert space
The space as the quotient by null functions
Hilbert space
The Axiom of Countable Choice ()
The Axiom of 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 (position and momentum as self-adjoint operators and their preparation uncertainty)
- MIT 8.05 Quantum Physics II (Fall 2013), Chapter 5 'Uncertainty Principle and Compatible Observables', pp. 1-8 (the Heisenberg uncertainty relation and equality states)