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L^p boundedness of singular integrals with homogeneous Dini-continuous kernels of mean zero

Proved
DbarRegularity.homogeneousSingularIntegral_lp

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

calderon-zygmundcauchy-riemannelliptic-regularityharmonic-analysissingular-integrals

Let Ω:Rd→C\Omega:\mathbb{R}^d\to\mathbb{C}Ω:Rd→C be homogeneous of degree 000, i.e. Ω(tx)=Ω(x)\Omega(tx)=\Omega(x)Ω(tx)=Ω(x) for t>0t>0t>0, and assume

  1. ∫Sd−1Ω dσ=0\displaystyle\int_{S^{d-1}}\Omega\,d\sigma=0∫Sd−1​Ωdσ=0, where σ\sigmaσ is the surface measure on the unit sphere Sd−1S^{d-1}Sd−1 (condition (24));
  2. the modulus w(δ)=sup⁡{∣Ω(x)−Ω(x′)∣:∣x∣=∣x′∣=1, ∣x−x′∣≤δ}w(\delta)=\sup\{|\Omega(x)-\Omega(x')|: |x|=|x'|=1,\ |x-x'|\le\delta\}w(δ)=sup{∣Ω(x)−Ω(x′)∣:∣x∣=∣x′∣=1, ∣x−x′∣≤δ} satisfies ∫01w(δ)δ dδ<∞\displaystyle\int_0^1\frac{w(\delta)}{\delta}\,d\delta<\infty∫01​δw(δ)​dδ<∞ (condition (25)).

Rd\mathbb{R}^dRd carries Lebesgue measure mmm, and ∥⋅∥p\|\cdot\|_p∥⋅∥p​ is the Lp(Rd)L^p(\mathbb{R}^d)Lp(Rd) norm. Let 1<p<∞1<p<\infty1<p<∞ and for f∈Lp(Rd)f\in L^p(\mathbb{R}^d)f∈Lp(Rd) and ε>0\varepsilon>0ε>0 put

Tεf(x)=∫∣y∣≥εΩ(y)∣y∣df(x−y) dy.T_\varepsilon f(x)=\int_{|y|\ge\varepsilon}\frac{\Omega(y)}{|y|^d}f(x-y)\,dy .Tε​f(x)=∫∣y∣≥ε​∣y∣dΩ(y)​f(x−y)dy.

Then

(a) there is a constant ApA_pAp​, independent of fff and ε\varepsilonε, such that ∥Tεf∥p≤Ap∥f∥p\|T_\varepsilon f\|_p\le A_p\|f\|_p∥Tε​f∥p​≤Ap​∥f∥p​;

(b) for each f∈Lpf\in L^pf∈Lp the limit Tf=lim⁡ε→0TεfTf=\lim_{\varepsilon\to0}T_\varepsilon fTf=limε→0​Tε​f exists in the LpL^pLp norm, and ∥Tf∥p≤Ap∥f∥p\|Tf\|_p\le A_p\|f\|_p∥Tf∥p​≤Ap​∥f∥p​.

Formalization Note The sphere measure is Mathlib's volume.toSphere on sphere (0 : EuclideanSpace ℝ (Fin d)) 1; condition (24) does not change if the measure is multiplied by a positive constant. The modulus w(δ)w(\delta)w(δ) is the supremum ⨆ … ‖Ω x - Ω x'‖ₑ in ℝ≥0∞, and condition (25) is ∫⁻ δ in Ioc 0 1, w δ / ENNReal.ofReal δ < ⊤. TεfT_\varepsilon fTε​f is the Bochner integral ∫ y in {y | ε ≤ ‖y‖}, …; for f∈Lpf\in L^pf∈Lp it converges absolutely at every xxx. The limit ε→0\varepsilon\to0ε→0 is taken along 𝓝[>] 0, and the limit operator is the function g. ENNReal.ofReal p is the exponent, so p<∞p<\inftyp<∞. The constant A : ℝ≥0 depends on Ω\OmegaΩ and ppp. Part (c) of Stein's theorem, an explicit formula for the Fourier transform of TfTfTf when f∈L2f\in L^2f∈L2, is not included.

Preamble
import Definitions.Def_DbarRegularity_Setting
import Mathlib.Analysis.Calculus.ContDiff.Basic
import Mathlib.MeasureTheory.Constructions.HaarToSphere
Formal statement
namespace DbarRegularity

open MeasureTheory Metric Filter Topology
open scoped ENNReal NNReal ContDiff

/-- Stein, *Singular Integrals*, Chapter II, § 4.2, Theorem 3 (a), (b) (p. 39): let `Ω` on `ℝ^d` be
homogeneous of degree `0`, with mean zero on the unit sphere `S^{d-1}` (condition (24)) and with
modulus of continuity `w(δ) = sup {|Ω(x) - Ω(x')| : |x| = |x'| = 1, |x - x'| ≤ δ}` satisfying
`∫₀¹ w(δ) / δ dδ < ∞` (condition (25)). For `1 < p < ∞`, `f ∈ L^p` and
`T_ε f (x) = ∫_{|y| ≥ ε} Ω(y) / |y|^d · f(x - y) dy`:
(a) `‖T_ε f‖_p ≤ A_p ‖f‖_p` with `A_p` independent of `f` and `ε`;
(b) `T f = lim_{ε → 0} T_ε f` exists in `L^p` and `‖T f‖_p ≤ A_p ‖f‖_p`. -/
theorem homogeneousSingularIntegral_lp {d : ℕ} (Ω : EuclideanSpace ℝ (Fin d) → ℂ)
    (hhom : ∀ x, ∀ t : ℝ, 0 < t → Ω (t • x) = Ω x)
    (hmean : ∫ x : sphere (0 : EuclideanSpace ℝ (Fin d)) 1, Ω x ∂(volume.toSphere) = 0)
    (hdini : ∫⁻ δ in Set.Ioc (0 : ℝ) 1,
      (⨆ (x : EuclideanSpace ℝ (Fin d)) (x' : EuclideanSpace ℝ (Fin d)) (_ : ‖x‖ = 1)
        (_ : ‖x'‖ = 1) (_ : ‖x - x'‖ ≤ δ), ‖Ω x - Ω x'‖ₑ) / ENNReal.ofReal δ < ⊤)
    (p : ℝ) (hp : 1 < p) :
    ∃ A : ℝ≥0,
      (∀ ε : ℝ, 0 < ε → ∀ f : EuclideanSpace ℝ (Fin d) → ℂ, MemLp f (ENNReal.ofReal p) volume →
        eLpNorm (fun x => ∫ y in {y | ε ≤ ‖y‖}, Ω y / ((‖y‖ ^ d : ℝ) : ℂ) * f (x - y))
            (ENNReal.ofReal p) volume
          ≤ A * eLpNorm f (ENNReal.ofReal p) volume) ∧
      ∀ f : EuclideanSpace ℝ (Fin d) → ℂ, MemLp f (ENNReal.ofReal p) volume →
        ∃ g : EuclideanSpace ℝ (Fin d) → ℂ, MemLp g (ENNReal.ofReal p) volume ∧
          Tendsto (fun ε : ℝ => eLpNorm
              ((fun x => ∫ y in {y | ε ≤ ‖y‖}, Ω y / ((‖y‖ ^ d : ℝ) : ℂ) * f (x - y)) - g)
              (ENNReal.ofReal p) volume)
            (𝓝[>] 0) (𝓝 0) ∧
          eLpNorm g (ENNReal.ofReal p) volume ≤ A * eLpNorm f (ENNReal.ofReal p) volume := by sorry

end DbarRegularity
Source
E. M. Stein, Singular Integrals and Differentiability Properties of Functions, Princeton Mathematical Series 30, Princeton University Press (1970), ISBN 0-691-08079-8, Chapter II, § 4.2, Theorem 3 (a), (b), p. 39 (conditions (24), (25) on the same page)
Read-back

What the Lean code literally says, in plain math · claude-opus-5-5

Read-back: DbarRegularity.homogeneousSingularIntegral_lp

Setting. d∈Nd\in\mathbb Nd∈N, Rd\mathbb R^dRd = EuclideanSpace ℝ (Fin d) with Lebesgue measure. A function Ω:Rd→C\Omega:\mathbb R^d\to\mathbb CΩ:Rd→C and a real ppp.

Hypotheses.

  • (hom) Ω(tx)=Ω(x)\Omega(tx)=\Omega(x)Ω(tx)=Ω(x) for all x∈Rdx\in\mathbb R^dx∈Rd, t>0t>0t>0 (homogeneous of degree 0; Ω(0)\Omega(0)Ω(0) unconstrained).
  • (mean) ∫Sd−1Ω dσ=0\displaystyle\int_{S^{d-1}}\Omega\,d\sigma = 0∫Sd−1​Ωdσ=0, where σ\sigmaσ = volume.toSphere (Mathlib's surface measure on the unit sphere induced from Lebesgue measure, σ(A)=d⋅∣{rx:x∈A, 0<r<1}∣\sigma(A)=d\cdot|\{rx: x\in A,\ 0<r<1\}|σ(A)=d⋅∣{rx:x∈A, 0<r<1}∣); Bochner integral.
  • (Dini) ∫(0,1]−w(δ)δ dδ<∞\displaystyle\int^{-}_{(0,1]} \frac{w(\delta)}{\delta}\,d\delta<\infty∫(0,1]−​δw(δ)​dδ<∞ (lower Lebesgue integral in [0,∞][0,\infty][0,∞]), where w(δ)=sup⁡{∣Ω(x)−Ω(x′)∣:∣x∣=∣x′∣=1, ∣x−x′∣≤δ}∈[0,∞]w(\delta)=\sup\{|\Omega(x)-\Omega(x')| : |x|=|x'|=1,\ |x-x'|\le\delta\}\in[0,\infty]w(δ)=sup{∣Ω(x)−Ω(x′)∣:∣x∣=∣x′∣=1, ∣x−x′∣≤δ}∈[0,∞].
  • 1<p1<p1<p (real, so p<∞p<\inftyp<∞).

Definitions used. eLpNorm · (ofReal p) volume = ∥⋅∥Lp(Rd)∈[0,∞]\|\cdot\|_{L^p(\mathbb R^d)}\in[0,\infty]∥⋅∥Lp(Rd)​∈[0,∞]; MemLp f p = a.e.-strongly measurable with finite LpL^pLp norm. For ε>0\varepsilon>0ε>0: Tεf(x)=∫∣y∣≥εΩ(y)∣y∣df(x−y) dyT_\varepsilon f(x)=\displaystyle\int_{|y|\ge\varepsilon}\frac{\Omega(y)}{|y|^d}f(x-y)\,dyTε​f(x)=∫∣y∣≥ε​∣y∣dΩ(y)​f(x−y)dy (Bochner; ∣y∣d|y|^d∣y∣d is a natural-number power of a real, cast to C\mathbb CC).

Conclusion. There is A∈[0,∞)A\in[0,\infty)A∈[0,∞) (depending on d,Ω,pd,\Omega,pd,Ω,p only) such that

(a) ∀ε>0 ∀f∈Lp(Rd;C): ∥Tεf∥p≤A∥f∥p\forall\varepsilon>0\ \forall f\in L^p(\mathbb R^d;\mathbb C):\ \|T_\varepsilon f\|_p\le A\|f\|_p∀ε>0 ∀f∈Lp(Rd;C): ∥Tε​f∥p​≤A∥f∥p​;

(b) ∀f∈Lp ∃g∈Lp: ∥Tεf−g∥p→0\forall f\in L^p\ \exists g\in L^p:\ \|T_\varepsilon f-g\|_p\to0∀f∈Lp ∃g∈Lp: ∥Tε​f−g∥p​→0 as ε→0+\varepsilon\to0^+ε→0+, and ∥g∥p≤A∥f∥p\|g\|_p\le A\|f\|_p∥g∥p​≤A∥f∥p​.

Quantifier order: ∃A ∀ε ∀f\exists A\ \forall\varepsilon\ \forall f∃A ∀ε ∀f in (a); ∃A\exists A∃A (∀f ∃g\forall f\ \exists g∀f ∃g) in (b), same AAA.

Degenerate cases.

  • d=0d=0d=0: the space is one point, the sphere is empty, (mean) and (Dini) hold trivially, {∣y∣≥ε}=∅\{|y|\ge\varepsilon\}=\emptyset{∣y∣≥ε}=∅ so Tεf=0T_\varepsilon f=0Tε​f=0; conclusion holds with g=0g=0g=0. Harmless.
  • d=1d=1d=1: sphere ={±1}=\{\pm1\}={±1}, w≡0w\equiv0w≡0 on (0,1](0,1](0,1], (mean) says (a positive multiple of) Ω(1)+Ω(−1)=0\Omega(1)+\Omega(-1)=0Ω(1)+Ω(−1)=0: the Hilbert-transform case, which is true.

Soundness checks.

  1. Lean defaults.
    • Bochner integral in (mean): www is monotone in δ\deltaδ, so the Dini condition forces w(δ)→0w(\delta)\to0w(δ)→0 (otherwise ∫c/δ=∞\int c/\delta=\infty∫c/δ=∞), hence Ω∣Sd−1\Omega|_{S^{d-1}}Ω∣Sd−1​ is uniformly continuous and bounded. It is therefore integrable for the finite measure σ\sigmaσ, so (mean) is a genuine mean-zero condition, not something that holds automatically by the "non-integrable gives 0" default.
    • iSup over an empty set: for δ>0\delta>0δ>0 and d≥1d\ge1d≥1 the pair x=x′x=x'x=x′ is admissible, so the sup is over a nonempty set. When d=0d=0d=0 it is 000, which is harmless.
    • Division in ℝ≥0∞: δ∈(0,1]\delta\in(0,1]δ∈(0,1], so ofReal δ lies in (0,1](0,1](0,1], with no division by 0 or ⊤\top⊤. If w=⊤w=\topw=⊤ the hypothesis fails, which is correct.
    • Tεf(x)T_\varepsilon f(x)Tε​f(x): Ω\OmegaΩ is bounded and ∣y∣−d1∣y∣≥ε∈Lp′|y|^{-d}\mathbf 1_{|y|\ge\varepsilon}\in L^{p'}∣y∣−d1∣y∣≥ε​∈Lp′ (since dp′>ddp'>ddp′>d), so by Hölder the integrand is integrable for every xxx. The Bochner value is the true value and not a default 0. Ω\OmegaΩ is continuous off 000, hence measurable.
    • The cast ((∥y∥d:R):C)((\|y\|^d:\mathbb R):\mathbb C)((∥y∥d:R):C) is the real ∣y∣d|y|^d∣y∣d with N\mathbb NN-exponent, as intended. It is nonzero on ∣y∣≥ε>0|y|\ge\varepsilon>0∣y∣≥ε>0.
    • No toReal, no rpow at exponent 0, no ContDiff, no ℕ subtraction. A:R≥0A:\mathbb R_{\ge0}A:R≥0​, so it cannot be ⊤\top⊤. The exponent ofReal p lies in (1,∞)(1,\infty)(1,∞).
  2. Quantifiers: AAA is chosen after d,Ω,pd,\Omega,pd,Ω,p and before ε\varepsilonε and fff; ggg is chosen after fff. This is exactly the uniform-in-ε\varepsilonε LpL^pLp bound for truncated homogeneous Calderón–Zygmund kernels with Dini-continuous mean-zero angular part, together with LpL^pLp convergence of the truncations. It is a standard true theorem, and the hypotheses are satisfiable non-trivially (e.g. Riesz kernels Ω(x)=xj/∣x∣\Omega(x)=x_j/|x|Ω(x)=xj​/∣x∣).

Remarks. Ω\OmegaΩ carries no measurability hypothesis, but measurability follows from the hypotheses as shown above. Part (b) uses the same constant AAA as (a), which is consistent because the LpL^pLp limit inherits the bound.

Verdict: no mis-formalization observed

Human review
  • Endorsed by Shuze Chen · Oct 13, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Oct 13, 2026

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

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