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Weak type (1,1) bound for the Hardy–Littlewood maximal function with constant 5^d

Proved
DbarRegularity.maximalFunction_weakType_one

by Mazecto · Oct 11, 2026 · Mathlib 0df444a (Lean v4.33.1)

harmonic-analysismaximal-functionmeasure-theorysingular-integrals

Let MfMfMf be the Hardy–Littlewood maximal function of f:Rd→Cf:\mathbb{R}^d\to\mathbb{C}f:Rd→C,

Mf(x)=sup⁡r>01∣B(x,r)∣∫B(x,r)∣f(y)∣ dy∈[0,∞],Mf(x)=\sup_{r>0}\frac{1}{|B(x,r)|}\int_{B(x,r)}|f(y)|\,dy\in[0,\infty],Mf(x)=r>0sup​∣B(x,r)∣1​∫B(x,r)​∣f(y)∣dy∈[0,∞],

where B(x,r)B(x,r)B(x,r) is the open ball and ∣⋅∣|\cdot|∣⋅∣ is Lebesgue measure mmm. Then for every fff and every α>0\alpha>0α>0,

m{x:Mf(x)>α}≤5dα∫Rd∣f(y)∣ dy.m\{x: Mf(x)>\alpha\}\le\frac{5^d}{\alpha}\int_{\mathbb{R}^d}|f(y)|\,dy.m{x:Mf(x)>α}≤α5d​∫Rd​∣f(y)∣dy.

This is the weak type (1,1)(1,1)(1,1) inequality of the Hardy–Littlewood maximal theorem, with an explicit constant depending only on the dimension.

Formalization Note. maximalFunction f (from Definitions.Def_DbarRegularity_Setting) takes values in ℝ≥0∞, and α\alphaα is in ℝ≥0. No measurability or integrability is assumed on fff: the left side is the outer Lebesgue measure of the superlevel set, and the right side is the lower Lebesgue integral ∫⁻ x, ‖f x‖ₑ, which is +∞+\infty+∞ when f∉L1f\notin L^1f∈/L1 (the bound is then trivial). The case d=0d=0d=0 is included.

Preamble
import Definitions.Def_DbarRegularity_Setting
Formal statement
namespace DbarRegularity

open MeasureTheory
open scoped ENNReal NNReal

/-- Weak type `(1,1)` bound for the Hardy–Littlewood maximal function on `ℝ^d` with the explicit
constant `5^d`: `|{M f > α}| ≤ (5^d / α) ∫ |f|` for every `f` and every `α > 0`. -/
theorem maximalFunction_weakType_one (d : ℕ) (f : EuclideanSpace ℝ (Fin d) → ℂ) (α : ℝ≥0)
    (hα : 0 < α) :
    volume {x | (α : ℝ≥0∞) < maximalFunction f x} ≤
      (5 : ℝ≥0∞) ^ d / α * ∫⁻ x, ‖f x‖ₑ := by sorry

end DbarRegularity
Source
E. M. Stein, Singular Integrals and Differentiability Properties of Functions, Princeton Mathematical Series 30, Princeton University Press (1970), Chapter I, § 1.3, Theorem 1 (b), p. 5, with the constant A = 5^d noted there

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