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Domain D(Q)D(Q)D(Q) of the position operator on L2(R)L^2(\mathbb R)L2(R), eq. (3)

Definition
HeathcoteUnbounded_PositionDomain

by Lucas · Oct 13, 2026 · Mathlib 0df444a (Lean v4.33.1)

functional-analysismathematical-physics

The position operator QQQ on L2(R)L^2(\mathbb R)L2(R) acts by (Qψ)(x)=x ψ(x)(Q\psi)(x)=x\,\psi(x)(Qψ)(x)=xψ(x). Its domain, equation (3) of the source, is

D(Q)={ψ∈L2(R) : ∫Rx2 ∣ψ(x)∣2 dx<∞},D(Q)=\Big\{\psi\in L^2(\mathbb R)\ :\ \int_{\mathbb R} x^2\,|\psi(x)|^2\,dx<\infty\Big\},D(Q)={ψ∈L2(R) : ∫R​x2∣ψ(x)∣2dx<∞},

i.e. exactly those square-integrable ψ\psiψ for which xψ(x)x\psi(x)xψ(x) is again square-integrable.

Formalization Note D(Q)D(Q)D(Q) is a subset of Mathlib's Lp ℂ 2 volume on ℝ; the integral is a Lebesgue integral in [0,∞][0,\infty][0,∞] of ∣x∣2∣ψ(x)∣2|x|^2|\psi(x)|^2∣x∣2∣ψ(x)∣2, which does not depend on the chosen representative.

Definition code
import Mathlib

open MeasureTheory

namespace HeathcoteUnbounded

/-- Domain of the position operator `(Qψ)(x) = x ψ(x)` on `L²(ℝ)`, eq. (3):
`D(Q) = {ψ ∈ L²(ℝ) : ∫ x² |ψ(x)|² dx < ∞}`. -/
def positionDomain : Set (Lp ℂ 2 (volume : Measure ℝ)) :=
  {f | ∫⁻ x : ℝ, ‖x‖ₑ ^ 2 * ‖(f : ℝ → ℂ) x‖ₑ ^ 2 < ⊤}

end HeathcoteUnbounded
Source
A. Heathcote, "Unbounded Operators and the Incompleteness of Quantum Mechanics", Philosophy of Science 57 (1990), 523–534, p. 4, eq. (3)
Human review
  • Endorsed by Shuze Chen · Oct 13, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 13, 2026

    Confirmed by the mission captain (proposal self-audit).

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