The pointwise convolution integral is a.e. strongly measurable
ProvedDbarRegularity.aestronglyMeasurable_integral_mul_subconvolutionharmonic-analysismeasure-theory
Let and let be almost-everywhere strongly measurable. Then the function
is almost-everywhere strongly measurable on .
No integrability is assumed: at points where is not integrable the Bochner integral is by convention, and the statement still holds. This is the basic measurability fact for convolution operators defined pointwise by the integral.
Formalization Note. is EuclideanSpace ℝ (Fin d) with Lebesgue measure volume; the integral is the Bochner integral ∫ y, K (x - y) * f y, which Lean sets to when the integrand is not integrable.
Preamble
import Mathlib.MeasureTheory.Integral.Prod import Mathlib.MeasureTheory.Group.Prod import Mathlib.MeasureTheory.Measure.Haar.InnerProductSpace import Mathlib.Analysis.InnerProductSpace.PiL2
Formal statement
namespace DbarRegularity
open MeasureTheory
open scoped ENNReal
/-- The convolution-type integral `x ↦ ∫ K(x - y) f(y) dy` of a.e.-strongly measurable functions
is a.e.-strongly measurable. -/
theorem aestronglyMeasurable_integral_mul_sub {d : ℕ} (K f : EuclideanSpace ℝ (Fin d) → ℂ)
(hK : AEStronglyMeasurable K volume) (hf : AEStronglyMeasurable f volume) :
AEStronglyMeasurable (fun x => ∫ y, K (x - y) * f y) volume := by sorry
end DbarRegularity
Source
E. M. Stein, Singular Integrals and Differentiability Properties of Functions, Princeton University Press (1970), Chapter II, § 2.2, p. 29