Domain of the position operator on , eq. (3)
DefinitionHeathcoteUnbounded_PositionDomainfunctional-analysismathematical-physics
The position operator on acts by . Its domain, equation (3) of the source, is
i.e. exactly those square-integrable for which is again square-integrable.
Formalization Note is a subset of Mathlib's Lp ℂ 2 volume on ℝ; the integral is a Lebesgue integral in of , 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
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.