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The Riesz transforms are bounded on Lp

Statement

Assume Countable Choice. Let n≥1 and 1≤j≤n. The j-th Riesz transform Rj of Riesz transforms on Euclidean space extends uniquely to a bounded operator on Lp(Rn;C) for every 1<p<∞, with norm at most Cn,p, a constant depending only on n and p: the Riesz kernel Kj(x)=cnxj/∣x∣n+1 is a standard 1-Hölder Calderón–Zygmund kernel with constant Cn=cn2n+1(3n+4), so that ∥Rjf∥p≤Cn,p(1+∣Sn−1∣2−1Cn)max⁡(p,(p−1)−1)∥f∥p(f∈Lp(Rn;C)).

Facts & Assumptions

Given: Countable Choice; the dimension n≥1 and index 1≤j≤n; the Riesz kernel Kj(x)=cnxj/∣x∣n+1 and operator Rj of Riesz transforms on Euclidean space; a compactly supported f∈L2(Rn;C); a test function φ∈Cc∞(Rn) supported off supp⁡f.

[F1]

∣Kj(x)∣≤cn∣x∣−n for x≠0; ∣Kj(x−h)−Kj(x)∣≤Cn∣h∣ ∣x∣−(n+1) with Cn=cn2n+1(3n+4) whenever ∣h∣≤∣x∣/2; and ∫Sn−1Kj(rω) dσ(ω)=0 for every r>0 (Riesz kernel size, difference and spherical-cancellation bounds).

[F2]

For every Schwartz function g the truncated integrals ∫∣y∣>εKj(y)g(x−y) dy converge as ε↓0 for every x, and the limit is a continuous representative of the L2 class Rjg (The Riesz transform is the principal value of its kernel, with the matching constant).

[F3]

Rj is the L2 Fourier multiplier with symbol mj(ξ)=−iξj/∣ξ∣ for ξ≠0 and mj(0)=0, is bounded with ∥Rjg∥2≤∥g∥2 for all g∈L2, and satisfies ⟨Rjf,g⟩=∫mjf^ g^‾ for the first-variable-linear pairing ⟨u,v⟩=∫uv‾ (Riesz transforms on Euclidean space, Riesz transforms are L2 contractions and square to minus the identity in sum, Plancherel theorem, The Hilbert-space adjoint of a bounded operator).

[F4]

A pointwise bound ∣k∣≤c∣⋅∣−n implies the annular condition with A1=c∣Sn−1∣log⁡2; a standard δ-Hölder kernel with constant A2′ is a Calderón–Zygmund kernel with Hörmander constant A2=∣Sn−1∣2−δδ−1A2′; and a Calderón–Zygmund operator with constants A1,A2 and L2 norm B extends uniquely to a bounded operator on Lp for 1<p<∞ with ∥Tg∥p≤Cn,p(A2+B)max⁡(p,(p−1)−1)∥g∥p (Calderón–Zygmund kernels and their associated operators, Standard (Hölder) Calderón–Zygmund kernels, Standard Hölder kernels satisfy the Hörmander condition, Calderón–Zygmund operators are bounded on Lp).

[F5]

Fubini interchanges absolutely integrable complex double integrals, and locally integrable functions with equal distribution pairings agree almost everywhere. (Fubini's theorem for L^1 functions on a sigma-finite product, Locally integrable functions embed in distributions)

[F6]

Under Countable Choice, for every nonnegative Borel function g, ∫Rng(x) dx=∫0∞∫Sn−1g(rω)rn−1 dσ(ω) dr, with σ a finite Borel measure. (Polar coordinates decompose Lebesgue measure into r^{n-1} dr d sigma)

Proof

technique · direct
1.1F1given

The published estimates give the size bound ∣Kj(x)∣≤cn∣x∣−n, the first-difference bound ∣Kj(x−h)−Kj(x)∣≤Cn∣h∣∣x∣−(n+1) for ∣h∣≤∣x∣/2, and the vanishing of every spherical mean. The explicit kernel is smooth on the punctured space, hence Borel measurable and locally integrable there.

1.2F3givenalgebra

Rj is L2-bounded with ∥Rjg∥2≤∥g∥2, since ∣mj∣≤1 and the L2 multiplier bound gives ∥Rj∥≤1; hence B=1 is an admissible L2 norm bound. Moreover Rj is skew-adjoint: for f,g∈L2, ⟨Rjf,g⟩=∫mjf^ g^‾=∫f^ (−mj)g^‾=⟨f,−Rjg⟩, because mj‾=−mj for the purely imaginary symbol; that is, Rj∗=−Rj.

2.1F1F4F6step 1.1algebra

By [F6], the size bound gives ∫R≤∣x∣≤2R∣Kj(x)∣ dx≤cn∣Sn−1∣∫R2Rdr/r=cn∣Sn−1∣log⁡2. For every h≠0, directly integrating the difference bound gives ∫∣x∣≥2∣h∣∣Kj(x−h)−Kj(x)∣ dx≤Cn∣h∣∣Sn−1∣∫2∣h∣∞r−2dr=∣Sn−1∣Cn/2. Thus Kj is a base Calderón–Zygmund kernel with A1=cn∣Sn−1∣log⁡2 and A2=∣Sn−1∣Cn/2; its first-difference estimate now establishes standard 1-Hölder status with A2′=Cn.

2.2F2F3step 1.2algebraF5

Off-support representation: let f∈L2 be compactly supported, let φ∈Cc∞ be supported off supp⁡f, and put d:=dist⁡(supp⁡f,supp⁡φ)>0. Using the adjoint identity of [F3], skew-adjointness from step 1.2 and the Schwartz principal-value formula [F2], and writing Kj for the real-valued kernel, ⟨Rjf,φ⟩=⟨f,Rj∗φ⟩=−∫f(y)Rjφ(y)‾ dy=−∬Kj(y−x)f(y)φ(x)‾ dx dy=∬Kj(x−y)f(y)φ(x)‾ dx dy, where Rjφ(y)‾=lim⁡ε↓0∫∣y−x∣>εKj(y−x)φ(x)‾ dx is an absolutely convergent integral on the two supports (there ∣x−y∣≥d>0, so the limit may be taken inside the y-integration), Fubini applies over the bounded supports, and the last step uses the oddness Kj(−z)=−Kj(z). Since this holds for every test function supported off supp⁡f, the L2 class Rjf agrees almost everywhere off supp⁡f with the locally integrable function x↦∫Kj(x−y)f(y) dy; this is the off-support representation (3) required of a Calderón–Zygmund operator.

3.1F4step 2.1step 1.2step 2.2∎

By steps 2.1, 1.2 and 2.2 the operator Rj is a standard-kernel Calderón–Zygmund operator with annular constant cn∣Sn−1∣log⁡2, Hörmander constant ∣Sn−1∣2−1Cn and L2 norm B=1; the strict-range theorem [F4] therefore gives its unique extension to a bounded operator on Lp(Rn;C), 1<p<∞, with ∥Rjf∥p≤Cn,p(1+∣Sn−1∣2−1Cn)max⁡(p,(p−1)−1)∥f∥p. This is the assertion.

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