Singular integral operators of convolution type

In mathematics, singular integral operators of convolution type are the singular integral operators that arise on Rⁿ and Tⁿ through convolution by distributions; equivalently they are the singular integral operators that commute with translations. The classical examples in harmonic analysis are the harmonic conjugation operator on the circle, the Hilbert transform on the circle and the real line, the Beurling transform in the complex plane and the Riesz transforms in Euclidean space. The continuity of these operators on L² is evident because the Fourier transform converts them into multiplication operators. Continuity on L^p spaces was first established by Marcel Riesz. The classical techniques include the use of Poisson integrals, interpolation theory and the Hardy–Littlewood maximal function. For more general operators, fundamental new techniques, introduced by Alberto Calderón and Antoni Zygmund in 1952, were developed by a number of authors to give general criteria for continuity on L^p spaces. This article explains the theory for the classical operators and sketches the subsequent general theory.

L² theory

Hilbert transform on the circle

The theory for L² functions is particularly simple on the circle.^[1]^[2] If f ∈ L²(T), then it has a Fourier series expansion

f(\theta )=\sum _{{n\in {\mathbf {Z}}}}a_{n}e^{{in\theta }}.

Hardy space H²(T) consists of the functions for which the negative coefficients vanish, a_n = 0 for n < 0. These are precisely the square-integrable functions that arise as boundary values of holomorphic functions in the open unit disk. Indeed, f is the boundary value of the function

F(z)=\sum _{{n\geq 0}}a_{n}z^{n},

in the sense that the functions

f_{r}(\theta )=F(re^{{i\theta }}),

defined by the restriction of F to the concentric circles |z| = r, satisfy

\|f_{r}-f\|_{2}\rightarrow 0.

The orthogonal projection P of L²(T) onto H²(T) is called the Szegő projection. It is a bounded operator on L²(T) with operator norm 1. By Cauchy's theorem

F(z)={1 \over 2\pi i}\int _{{|\zeta |=1}}{f(\zeta ) \over \zeta -z}\,d\zeta ={1 \over 2\pi }\int _{{-\pi }}^{{\pi }}{f(\theta ) \over 1-e^{{-i\theta }}z}\,d\theta .

Thus

\displaystyle {F(re^{{i\varphi }})={1 \over 2\pi }\int _{{-\pi }}^{{\pi }}{f(\varphi -\theta ) \over 1-re^{{i\theta }}}\,d\theta .}

When r = 1, the integrand on the right hand side has a singularity at θ = 0. The truncated Hilbert transform is defined by

\displaystyle {H_{\varepsilon }f(\varphi )={i \over \pi }\int _{{\varepsilon \leq |\theta |\leq \pi }}{f(\varphi -\theta ) \over 1-e^{{i\theta }}}\,d\theta ={1 \over \pi }\int _{{|\zeta -e^{{i\varphi }}|\geq \delta }}{f(\zeta ) \over \zeta -e^{{i\varphi }}}\,d\zeta ,}

where δ = |1 – e^iε|. Since it is defined as convolution with a bounded function, it is a bounded operator on L²(T). Now

\displaystyle {H_{\varepsilon }{1}={i \over \pi }\int _{\varepsilon }^{\pi }2\Re (1-e^{{i\theta }})^{{-1}}\,d\theta ={i \over \pi }\int _{\varepsilon }^{\pi }1\,d\theta =i-{i\varepsilon \over \pi }.}

If f is a polynomial in z then

\displaystyle {H_{\varepsilon }f(z)-{i(1-\varepsilon ) \over \pi }f(z)={1 \over \pi i}\int _{{|\zeta -z|\geq \delta }}{f(\zeta )-f(z) \over \zeta -z}\,d\zeta .}

By Cauchy's theorem the right hand side tends to 0 uniformly as ε, and hence δ, tends to 0. So

\displaystyle {H_{\varepsilon }f\rightarrow if}

uniformly for polynomials. On the other hand, if u(z) = z it is immediate that

\displaystyle {\overline {H_{\varepsilon }f}=-u^{{-1}}H_{\varepsilon }(u\overline {f}).}

Thus if f is a polynomial in z⁻¹ without constant term

\displaystyle {H_{\varepsilon }f\rightarrow -if}

uniformly.

Define the Hilbert transform on the circle by

\displaystyle {H=i(2P-I).}

Thus if f is a trigonometric polynomial

\displaystyle {H_{\varepsilon }f\rightarrow Hf}

uniformly.

It follows that if f is any L² function

\displaystyle {H_{\varepsilon }f\rightarrow Hf}

in the L² norm.

This is an immediate consequence of the result for trigonometric polynomials once it is established that the operators H_ε are uniformly bounded in operator norm. But on [–π,π]

\displaystyle {(1-e^{{i\theta }})^{{-1}}=[(1-e^{{i\theta }})^{{-1}}-i\theta ^{{-1}}]+i\theta ^{{-1}}.}

The first term is bounded on the whole of [–π,π], so it suffices to show that the convolution operators S_ε defined by

\displaystyle {S_{\varepsilon }f(\varphi )=\int _{{\varepsilon \leq |\theta |\leq \pi }}f(\varphi -\theta )\theta ^{{-1}}\,d\theta }

are uniformly bounded. With respect to the orthonormal basis e^inθ convolution operators are diagonal and their operator norms are given by taking the supremum of the moduli of the Fourier coefficients. Direct computation shows that these all have the form

\displaystyle {{1 \over \pi }\left|\int _{a}^{b}{\sin t \over t}\,dt\right|}

with 0 < a < b. These integrals are well-known to be uniformly bounded.

It also follows that, for a continuous function f on the circle, H_εf converges uniformly to Hf, so in particular pointwise. The pointwise limit is a Cauchy principal value, written

\displaystyle {Hf={\mathrm {P.V.}}\,{1 \over \pi }\int {f(\zeta ) \over \zeta -e^{{i\varphi }}}\,d\zeta .}

If f is just in L² then H_εf converges to Hf pointwise almost everywhere. In fact define the Poisson operators on L² functions by

T_{r}\left(\sum a_{n}e^{{in\theta }}\right)=\sum r^{{|n|}}a_{n}e^{{in\theta }},

for r < 1. Since these operators are diagonal, it is easy to see that T_rf tends to f in L² as r increases to 1. Moreover, as Lebesgue proved, T_rf also tends pointwise to f at each Lebesgue point of f. On the other hand, it is also known that T_rHf – H_{1 – r} f tends to zero at each Lebesgue point of f. Hence H_{1 – r} f tends pointwise to f on the common Lebesgue points of f and Hf and therefore almost everywhere.^[3]^[4]^[5]

Results of this kind on pointwise convergence are proved more generally below for L^p functions using the Poisson operators and the Hardy–Littlewood maximal function of f.

The Hilbert transform has a natural compatibility with orientation-preserving diffeomorphisms of the circle.^[6] Thus if H is a diffeomorphism of the circle with

H(e^{{i\theta }})=e^{{ih(\theta )}},\,\,\,h(\theta +2\pi )=h(\theta )+2\pi ,

then the operators

H_{\varepsilon }^{h}f(e^{{i\varphi }})={\frac {1}{\pi }}\int _{{|e^{{ih(\theta )}}-e^{{ih(\varphi )}}|\geq \varepsilon }}{\frac {f(e^{{i\theta }})}{e^{{i\theta }}-e^{{i\varphi }}}}e^{{i\theta }}\,d\theta ,

are uniformly bounded and tend in the strong operator topology to H. Moreover, if Vf(z) = f(H(z)), then VHV⁻¹ – H is an operator with smooth kernel, so a Hilbert–Schmidt operator.

In fact if G is the inverse of H with corresponding function g(θ), then

(VH_{\varepsilon }^{h}V^{{-1}}-H_{\varepsilon })f(e^{{i\varphi }})={1 \over \pi }\int _{{|e^{{i\theta }}-e^{{i\varphi }}|\geq \varepsilon }}\left[{g^{\prime }(\theta )e^{{ig(\theta )}} \over e^{{ig(\theta )}}-e^{{ig(\varphi )}}}-{e^{{i\theta }} \over e^{{i\theta }}-e^{{i\varphi }}}\right]\,f(e^{{i\theta }})\,d\theta .

Since the kernel on the right hand side is smooth on T × T, it follows that the operators on the right hand side are uniformly bounded and hence so too are the operators H_ε^h. To see that they tend strongly to H, it suffices to check this on trigonometric polynomials. In that case

H_{\varepsilon }^{h}f(\zeta )={1 \over \pi i}\int _{{|H(z)-H(\zeta )|\geq \varepsilon }}{\frac {f(z)}{z-\zeta }}dz={1 \over \pi i}\int _{{|H(z)-H(\zeta )|\geq \varepsilon }}{f(z)-f(\zeta ) \over z-\zeta }\,dz+{\frac {f(\zeta )}{\pi i}}\int _{{|H(z)-H(\zeta )|\geq \varepsilon }}{dz \over z-\zeta }.

In the first integral the integrand is a trigonometric polynomial in z and ζ and so the integral is a trigonometric polynomial in ζ. It tends in L² to the trigonometric polynomial

{1 \over \pi i}\int {f(z)-f(\zeta ) \over z-\zeta }\,dz.

The integral in the second term can be calculated by the principle of the argument. It tends in L² to the constant function 1, so that

\lim _{{\varepsilon \to 0}}H_{\varepsilon }^{h}f(\zeta )=f(\zeta )+{1 \over \pi i}\int {f(z)-f(\zeta ) \over z-\zeta }\,dz,

where the limit is in L². On the other hand, the right hand side is imdependent of the diffeomorphism. Since for the identity diffeomorphism, the left hand side equals Hf, it too equals Hf (this can also be checked directly if f is a trigonometric polynomial). Finally, letting ε → 0,

(VHV^{{-1}}-H)f(e^{{i\varphi }})={\frac {1}{\pi }}\int \left[{g^{\prime }(\theta )e^{{ig(\theta )}} \over e^{{ig(\theta )}}-e^{{ig(\varphi )}}}-{e^{{i\theta }} \over e^{{i\theta }}-e^{{i\varphi }}}\right]\,f(e^{{i\theta }})\,d\theta .

The direct method of evaluating Fourier coefficients to prove the uniform boundedness of the operator H^ε does not generalize directly to L^p spaces with 1 < p < ∞. Instead a direct comparison of H^εf with the Poisson integral of the Hilbert transform is used classically to prove this. If f has Fourier series

f(e^{{i\theta }})=\sum _{{n\in {\mathbf {Z}}}}a_{n}e^{{in\theta }},

its Poisson integral is defined by

\displaystyle {P_{r}f(e^{{i\theta }})=\sum _{{n\in {\mathbf {Z}}}}a_{n}r^{{|n|}}e^{{in\theta }}={1 \over 2\pi }\int _{0}^{{2\pi }}{(1-r^{2})f(e^{{i\theta }}) \over 1-2r\cos \theta +r^{2}}\,d\theta =K_{r}\star f(e^{{i\theta }}),}

where the Poisson kernel K_r is given by

\displaystyle {K_{r}(e^{{i\theta }})=\sum _{{n\in {\mathbf {Z}}}}r^{{|n|}}e^{{in\theta }}={1-r^{2} \over 1-2r\cos \theta +r^{2}}.}

In f is in L^p(T) then the operators P_r satisfy

\displaystyle {\|P_{r}f-f\|_{p}\rightarrow 0.}

In fact the K_r are positive so

\displaystyle {\|K_{r}\|_{1}={1 \over 2\pi }\int _{0}^{{2\pi }}K_{r}(e^{{i\theta }})\,d\theta =1.}

Thus the operators P_r have operator norm bounded by 1 on L^p. The convergence statement above follows by continuity from the result for trigonometric polynomials, where it is an immediate consequence of the formula for the Fourier coefficients of K_r.

The uniform boundedness of the operator norm of H_ε follows because HP_r − H_1−r is given as convolution by the function ψ_r, where^[7]

{\begin{aligned}\psi _{r}(e^{{i\theta }})&=1+{\frac {1-r}{1+r}}\cot \left({\tfrac {\theta }{2}}\right)K_{r}(e^{{i\theta }})\\&\leq 1+{\frac {1-r}{1+r}}\cot \left({\tfrac {1-r}{2}}\right)K_{r}(e^{{i\theta }})\end{aligned}}

for 1 − r ≤ |θ| ≤ π, and, for |θ| < 1 − r,

\displaystyle {\psi _{r}(e^{{i\theta }})=1+{2r\sin \theta \over 1-2r\cos \theta +r^{2}}.}

These estimates show that the L¹ norms ∫ |ψ_r| are uniformly bounded. Since H is a bounded operator, it follows that the operators H_ε are uniformly bounded in operator norm on L²(T). The same argument can be used on L^p(T) once it is known that the Hilbert transform H is bounded in operator norm on L^p(T).

Hilbert transform on the real line

As in the case of the circle, the theory for L² functions is particularly easy to develop. In fact, as observed by Rosenblum and Devinatz, the two Hilbert transforms can be related using the Cayley transform.^[8]

The Hilbert transform H_R on L²(R) is defined by

\widehat {H_{{{\mathbf {R}}}}f}=\left(i\chi _{{[0,\infty )}}-i\chi _{{(-\infty ,0]}}\right)\widehat {f},

where the Fourier transform is given by

\displaystyle {\widehat {f}(t)={1 \over {\sqrt {2\pi }}}\int _{{-\infty }}^{\infty }f(x)e^{{-itx}}\,dx.}

Define the Hardy space H²(R) to be the closed subspace of L²(R) consisting of functions for which the Fourier transform vanishes on the negative part of the real axis. Its orthogonal complement is given by functions for which the Fourier transform vanishes on the positive part of the real axis. It is the complex conjugate of H²(R). If P_R is the orthogonal projection onto H²(R), then

\displaystyle {H_{{{\mathbf {R}}}}=i(2P_{{{\mathbf {R}}}}-I).}

The Cayley transform

\displaystyle {C(x)={x-i \over x+i}}

carries the extended real line onto the circle, sending the point at ∞ to 1, and the upper halfplane onto the unit disk.

Define the unitary operator from L²(T) onto L²(R) by

\displaystyle {Uf(x)=\pi ^{{-1/2}}(x+i)^{{-1}}f(C(x)).}

This operator carries the Hardy space of the circle H²(T) onto H²(R). In fact for |w| < 1, the linear span of the functions

f_{w}(z)={\frac {1}{1-wz}}

is dense in H²(T). Moreover,

Uf_{w}(x)={\frac {1}{{\sqrt {\pi }}}}{\frac {1}{(1-w)(x-\overline {z})}}

where

\displaystyle {z=C^{{-1}}(\overline {w}).}

On the other hand, for z ∈ H, the linear span of the functions

\displaystyle {g_{z}(t)=e^{{itz}}\chi _{{[0,\infty )}}(t)}

is dense in L²((0,∞)). By the Fourier inversion formula, they are the Fourier transforms of

\displaystyle {h_{z}(x)=\widehat {g_{z}}(-x)={i \over {\sqrt {2\pi }}}(x+z)^{{-1}},}

so the linear span of these functions is dense in H²(R). Since U carries the f_w's onto multiples of the h_z's, it follows that U carries H²(T) onto H²(R). Thus

\displaystyle {UH_{{{\mathbf {T}}}}U^{*}=H_{{{\mathbf {R}}}}.}

In Nikolski (1986), part of the L² theory on the real line and the upper halfplane is developed by transferring the results from the circle and the unit disk. The natural replacements for concentric circles in the disk are lines parallel to the real axis in H. Under the Cayley transform these correspond to circles in the disk that are tangent to the unit circle at the point one. The behaviour of functions in H²(T) on these circles is part of the theory of Carleson measures. The theory of singular integrals, however, can be developed more easily by working directly on R.

H²(R) consists exactly of L² functions f that arise of boundary values of holomorphic functions on H in the following sense:^[9] f is in H² provided that there is a holomorphic function F(z) on H such that the functions f_y(x) = f(x + iy) for y > 0 are in L² and f_y tends to f in L² as y → 0. In this case F is necessarily unique and given by Cauchy's integral formula:

\displaystyle {F(z)={1 \over 2\pi i}\int _{{-\infty }}^{\infty }{f(s) \over s-z}\,ds.}

In fact, identifying H² with L²(0,∞) via the Fourier transform, for y > 0 multiplication by e^−yt on L²(0,∞) induces a contraction semigroup V_y on H². Hence for f in L²

\displaystyle {{1 \over 2\pi i}\int _{{-\infty }}^{\infty }{f(s) \over s-z}\,ds={1 \over {\sqrt {2\pi }}}\int _{{-\infty }}^{\infty }f(s)\widehat {g_{z}}(s)\,ds={1 \over {\sqrt {2\pi }}}\int _{{-\infty }}^{\infty }\widehat {f}(s)g_{z}(s)\,ds=V_{y}Pf(x).}

If f is in H², F(z) is holomorphic for Im z > 0, since the family of L² functions g_z depends holomorphically on z. Moreover, f_y = V_yf tends to f in H² since this is true for the Fourier transforms. Conversely if such an F exists, by Cauchy's integral theorem and the above identity applied to f_y

\displaystyle {f_{{y+t}}=V_{t}Pf_{y}}

for t > 0. Letting t tend to 0, it follows that Pf_y = f_y, so that f_y lies in H². But then so too does the limit f. Since

\displaystyle {V_{t}f_{y}=f_{{y+t}}=V_{y}f_{t},}

uniqueness of F follows from

\displaystyle {f_{t}=\lim _{{y\rightarrow 0}}f_{{y+t}}=\lim _{{y\rightarrow 0}}V_{t}f_{y}=V_{t}f.}

For f in L², the truncated Hilbert transforms are defined by

{\begin{aligned}H_{{\varepsilon ,R}}f(x)&={1 \over \pi }\int _{{\varepsilon \leq |y-x|\leq R}}{f(y) \over x-y}\,dy={1 \over \pi }\int _{{\varepsilon \leq |y|\leq R}}{f(x-y) \over y}\,dy\\H_{{\varepsilon }}f(x)&={1 \over \pi }\int _{{|y-x|\geq \varepsilon }}{f(y) \over x-y}\,dy={1 \over \pi }\int _{{|y|\geq \varepsilon }}{f(x-y) \over y}\,dy.\end{aligned}}

The operators H_ε,R are convolutions by bounded functions of compact support, so their operator norms are given by the uniform norm of their Fourier transforms. As before the absolute values have the form

\displaystyle {{1 \over {\sqrt {2\pi }}}\left|\int _{a}^{b}{2\sin t \over t}\,dt\right|.}

with 0 < a < b, so the operators H_ε,R are uniformly bounded in operator norm. Since H_ε,Rf tends to H_εf in L² for f with compact support, and hence for arbitrary f, the operators H_ε are also uniformly bounded in operator norm.

To prove that H_ε f tends to Hf as ε tends to zero, it suffices to check this on a dense set of functions. On the other hand,

\displaystyle {\overline {H_{\varepsilon }f}=-H_{\varepsilon }(\overline {f}),}

so it suffices to prove that H_εf tends to if for a dense set of functions in H²(R), for example the Fourier transforms of smooth functions g with compact support in (0,∞). But the Fourier transform f extends to an entire function F on C, which is bounded on Im(z) ≥ 0. The same is true of the derivatives of g. Up to a scalar these correspond to multiplying F(z) by powers of z. Thus F satisfies a Payley-Wiener estimate for Im(z) ≥ 0:^[10]

\displaystyle {|F^{{(m)}}(z)|\leq K_{{N,m}}(1+|z|)^{{-N}}}

for any m, N ≥ 0. In particular, the integral defining H_εf(x) can be computed by taking a standard semicircle contour centered on x. It consists of a large semicircle with radius R and a small circle radius ε with the two portions of the real axis between them. By Cauchy's theorem, the integral round the contour is zero. The integral round the large contour tends to zero by the Paley-Wiener estimate. The integral on the real axis is the limit sought. It is therefore given as minus the limit on the small semicircular contour. But this is the limit of

\displaystyle {{1 \over \pi }\int _{{\Gamma }}{F(z) \over z-x}\,dz.}

Where Γ is the small semicircular contour, oriented anticlockwise. By the usual techniques of contour integration, this limit equals if(x).^[11] In this case, it is easy to check that the convergence is dominated in L² since

H_{\varepsilon }f(x)={\frac {1}{\pi }}\int _{{|y-x|\geq \varepsilon }}{\frac {f(y)-f(x)}{y-x}}\,dy={\frac {1}{\pi }}\int _{{|y-x|\geq \varepsilon }}\int _{0}^{1}f^{\prime }(x+t(y-x))\,dt\,dy

so that convergence is dominated by

G(x)={\frac {1}{2\pi }}\int _{0}^{1}\int _{{-\infty }}^{\infty }|f^{\prime }(x+ty)|\,dy

which is in L² by the Paley-Wiener estimate.

It follows that for f on L²(R)

\displaystyle {H_{\varepsilon }f\rightarrow Hf.}

This can also be deduced directly because, after passing to Fourier transforms, H_ε and H become multiplication operators by uniformly bounded functions. The multipliers for H_ε tend pointwise almost everywhere to the multiplier for H, so the statement above follows from the dominated convergence theorem applied to the Fourier transforms.

As for the Hilbert transform on the circle, H_εf tends to Hf pointwise almost everywhere if f is an L² function. In fact, define the Poisson operators on L² functions by

T_{y}f(x)=\int _{{-\infty }}^{\infty }P_{y}(x-t)f(t)\,dt,

where the Poisson kernel is given by

P_{y}(x)={\frac {y}{\pi (x^{2}+y^{2})}}.

for y > 0. Its Fourier transform is

\displaystyle {\widehat {P_{y}}(t)=e^{{-y|t|}},}

from which it is easy to see that T_yf tends to f in L² as y increases to 0. Moreover, as Lebesgue proved, T_yf also tends pointwise to f at each Lebesgue point of f. On the other hand, it is also known that T_yHf – H_yf tends to zero at each Lebesgue point of f. Hence H_εf tends pointwise to f on the common Lebesgue points of f and Hf and therefore almost everywhere.^[12]^[13] The absolute values of the functions T_yf − f and T_yHf – H_yf can be bounded pointwise by multiples of the maximal function of f.^[14]

As for the Hilbert transform on the circle, the uniform boundedness of the operator norms of H_ε follows from that of the T_ε if H is known to be bounded, since HT_ε − H_ε is the convolution operator by the function

g_{\varepsilon }(x)={\begin{cases}{\frac {x}{\pi (x^{2}+\varepsilon ^{2})}}&|x|\leq \varepsilon \\{\frac {x}{\pi (x^{2}+\varepsilon ^{2})}}-{\frac {1}{\pi x}}&|x|>\varepsilon \end{cases}}

The L¹ norms of these functions are uniformly bounded.

Riesz transforms in the complex plane

The complex Riesz transforms R and R* in the complex plane are the unitary operators on L²(C) defined as multiplication by z/|z| and its conjugate on the Fourier transform of an L² function f:

\displaystyle {\widehat {Rf}(z)={\overline {z} \over |z|}\widehat {f}(z),\,\,\,\widehat {R^{*}f}(z)={z \over |z|}\widehat {f}(z).}

Idenitifying C with R², R and R* are given by

\displaystyle {R=-iR_{1}+R_{2},\,\,\,R^{*}=-iR_{1}-R_{2},}

where R₁ and R₂ are the Riesz transforms on R² defined below.

On L²(C), the operator R and its integer powers are unitary. They can also be expressed as singular integral operators:^[15]

\displaystyle {R^{k}f(w)=\lim _{{\varepsilon \rightarrow 0}}\int _{{|z-w|\geq \varepsilon }}M_{k}(w-z)f(z)\,dx\,dy,}

where

\displaystyle {M_{k}(z)={k \over 2\pi i^{k}}{z^{k} \over |z|^{{k+2}}}\,\,\,\,(k\geq 1),\,\,\,\,M_{{-k}}(z)=\overline {M_{k}(z)}.}

Defining the truncated higher Riesz transforms as

\displaystyle {R_{\varepsilon }^{{(k)}}f(w)=\int _{{|z-w|\geq \varepsilon }}M_{k}(w-z)f(z)\,dx\,dy,}

these operators can be shown to be uniformly bounded in operator norm. For odd powers this can be deduced by the method of rotation of Calderón and Zygmund, described below.^[16] If the operators are known to be bounded in operator norm it can also be deduced using the Poisson operators.^[17]

The Poisson operators T_s on R² are defined for s > 0 by

\displaystyle {T_{s}f(x)={1 \over 2\pi }\int _{{{\mathbf {R}}^{2}}}{sf(x) \over (|x-t|^{2}+s^{2})^{{3/2}}}\,dt.}

They are given by convolution with the functions

\displaystyle {P_{s}(x)={s \over 2\pi (|x|^{2}+s^{2})^{{3/2}}}.}

P_s is the Fourier transform of the function e^{− s|x|}, so under the Fourier transform they correspond to multiplication by these functions and form a contraction semigroup on L²(R²). Since P_y is positive and integrable with integral 1, the operators T_s also define a contraction semigroup on each L^p space with 1 < p < ∞.

The higher Riesz transforms of the Poisson kernel can be computed:

\displaystyle {R^{k}P_{s}(z)={k \over 2\pi i^{k}}{z^{k} \over (|z|^{2}+s^{2})^{{k/2+1}}}}

for k ≥ 1 and the complex conjugate for − k. Indeed, the right hand side is a harmonic function F(x,y,s) of three variable and for such functions^[18]

\displaystyle {T_{{s_{1}}}F(x,y,s_{2})=F(x,y,s_{1}+s_{2}).}

As before the operators

\displaystyle {T_{\varepsilon }R^{k}-R_{\varepsilon }^{{(k)}}}

are given by convolution with integrable functions and have uniformly bounded operator norms. Since the Riesz transforms are unitary on L²(C), the uniform boundedness of the truncated Riesz transforms implies that they converge in the strong operator topology to the corresponding Riesz transforms.

The uniform boundedness of the difference between the transform and the truncated transform can also be seen for odd k using the Calderón-Zygmund method of rotation.^[19]^[20] The group T acts by rotation on functions on C via

\displaystyle {U_{\theta }f(z)=f(e^{{i\theta }}z).}

This defines a unitary representation on L²(C) and the unitary operators R_θ commute with the Fourier transform. If A is a bounded operator on L²(R) then it defines a bounded operator A⁽¹⁾ on L²(C) simply by making A act on the first coordinate. With the identification L²(R²) = L²(R) ⊗ L²(R), A⁽¹⁾ = A ⊗ I. If φ is a continuous function on the circle then a new operator can be defined by

\displaystyle {B={1 \over 2\pi }\int _{0}^{{2\pi }}\varphi (\theta )U_{\theta }A^{{(1)}}U_{\theta }^{*}\,d\theta .}

This definition is understood in the sense that

\displaystyle {(Bf,g)={1 \over 2\pi }\int _{0}^{{2\pi }}\varphi (\theta )(U_{\theta }A^{{(1)}}U_{\theta }^{*}f,g)\,d\theta }

for any f, g in L²(C). It follows that

\displaystyle {\|B\|\leq {1 \over 2\pi }\int _{0}^{{2\pi }}|\varphi (\theta )|\cdot \|A\|\,d\theta .}

Taking A to be the Hilbert transform H on L²(R) or its truncation H_ε, it follows that

{\begin{aligned}R&={1 \over 2\pi }\int _{0}^{{2\pi }}e^{{-i\theta }}U_{\theta }H^{{(1)}}U_{\theta }^{*}\,d\theta ,\\R_{\varepsilon }&={1 \over 2\pi }\int _{0}^{{2\pi }}e^{{-i\theta }}U_{\theta }H_{\varepsilon }^{{(1)}}U_{\theta }^{*}\,d\theta .\end{aligned}}

Taking adjoints gives a similar formuls for R* and its truncation. This gives a second way to verify estimate the norms of R, R* and their truncations. It has the advantage of being applicable also for L^p spaces.

The Poisson operators can also be used to show that the truncated higher Riesz transforms of a function tend to the higher Riesz transform at the common Lebesgue points of the function and its transform. Indeed, (R^kT_ε − R^(k)_ε)f → 0 at each Lebesgue point of f; while (R^k − R^kT_ε)f → 0 at each Lebesgue point of R^kf.^[21]

Beurling transform in the complex plane

Since

{\overline {z} \over z}=\left({\overline {z} \over |z|}\right)^{2},

the Beurling transform T on L² is the unitary operator equal to R². This relation has been used classically in Vekua (1962) and Ahlfors (1966) to establish the continuity properties of T on L^p spaces. The results on the Riesz transform and its powers show that T is the limit in the strong operator topology of the truncated operators

T_{\varepsilon }f(w)=-{\frac {1}{\pi }}\iint _{{|z-w|\geq \varepsilon }}{\frac {f(z)}{(w-z)^{2}}}dxdy.

Accordingly, Tf can be written as a Cauchy principal value integral:

Tf(w)=-{\frac {1}{\pi }}P.V.\iint {\frac {f(z)}{(w-z)^{2}}}dxdy=-{\frac {1}{\pi }}\lim _{{\varepsilon \to 0}}\iint _{{|z-w|\geq \varepsilon }}{\frac {f(z)}{(w-z)^{2}}}dxdy.

From the description of T and T* on Fourier transforms, it follows that if f is smooth of compact support

{\begin{aligned}T(\partial _{{\overline {z}}}f)&=\partial _{z}Tf,\\T^{*}(\partial _{z}f)=\partial _{{\overline {z}}}T^{*}f.\end{aligned}}

Like the Hilbert transform in one dimension, the Beurling transform has a compatibility with conformal changes of coordinate. Let Ω be a bounded region in C with smooth boundary ∂Ω and let φ be a univalent holomorphic map of the unit disk D onto Ω extending to a smooth diffeomorphism of the circle onto ∂Ω. If χ_Ω is the characteristic function of Ω, the operator can χ_ΩTχ_Ω defines an operaror T(Ω) on L²(Ω). Through the conformal map φ, it induces an operator, also denoted T(Ω), on L²(D) which can be compared with T(D). The same is true of the truncations T_ε(Ω) and T_ε(D).

Let U_ε be the disk |z − w| < ε and V^ε the region |φ(z) − φ(w)| < ε. On L²(D)

{\begin{aligned}T_{\varepsilon }(\Omega )f(w)&=-{\frac {1}{\pi }}\iint _{{D\backslash V_{\varepsilon }}}\left[{\varphi ^{\prime }(w)\varphi ^{\prime }(z) \over (\varphi (z)-\varphi (w))^{2}}f(z)\right]dxdy,\\T_{\varepsilon }(D)f(w)&=-{1 \over \pi }\iint _{{D\backslash U_{\varepsilon }}}{f(z) \over (z-w)^{2}}dxdy,\end{aligned}}

and the operator norms of these truncated operators are uniformly bounded. On the other hand, if

T_{\varepsilon }^{\prime }(D)f(w)=-{1 \over \pi }\iint _{{D\backslash V_{\varepsilon }}}{\frac {f(z)}{(z-w)^{2}}}dxdy,

then the difference between this operator and T_ε(Ω) is a truncated operator with smooth kernel K(w,z):

K(w,z)=-{1 \over \pi }\left[{\varphi ^{\prime }(w)\varphi ^{\prime }(z) \over (\varphi (z)-\varphi (w))^{2}}-{1 \over (z-w)^{2}}\right].

So the operators T′_ε(D) must also have uniformly bounded operator norms. To see that their difference tends to 0 in the strong operator topology, it is enough to check this for f smooth of compact support in D. By Green's theorem^[22]

\left(T_{\varepsilon }(D)-T_{\varepsilon }^{\prime }(D)\right)f(w)={\frac {1}{\pi }}\iint _{{U_{\varepsilon }}}{\partial _{z}f(z) \over z-w}dxdy-{1 \over \pi }\iint _{{V_{\varepsilon }}}{\partial _{z}f(z) \over z-w}dxdy+{1 \over 2\pi i}\int _{{\partial U_{\varepsilon }}}{\frac {f(z)}{z-w}}d\overline {z}-{\frac {1}{2\pi i}}\int _{{\partial V_{\varepsilon }}}{f(z) \over z-w}\,d\overline {z}.

All four terms on the right hand side tend to 0. Hence the difference T(Ω) − T(D) is the Hilbert–Schmidt operator with kernel K.

For pointwise convergence there is simple argument due to Mateu & Verdera (2006) showing that the truncated integrals converge to Tf precisely at its Lebesgue points, that is almost everywhere.^[23] In fact T has the following symmetry property for f, g ∈ L²(C)

\iint (Tf)g=-{1 \over \pi }\lim \int _{{|z-w|\geq \varepsilon }}{\frac {f(w)g(z)}{(w-z)^{2}}}=\iint f(Tg).

On the other hand, if χ is the characteristic function of the disk D(z,ε) with centre z and radius ε, then

T\chi (w)=-\varepsilon ^{2}{\frac {1-\chi (w)}{(w-z)^{2}}}.

Hence

T_{\varepsilon }(f)(z)={1 \over \pi \varepsilon ^{2}}\iint f(T\chi )={1 \over \pi \varepsilon ^{2}}\iint (Tf)\chi ={\mathbf {Av}}_{{D(z,\varepsilon )}}\,Tf.

By the Lebesgue differentiation theorem, the right hand side converges to Tf at the Lebesgue points of Tf.

Riesz transforms in higher dimensions

For f in the Schwartz space of Rⁿ, the jth Riesz transform is defined by

R_{j}f(x)=c_{n}\lim _{{\varepsilon \to 0}}\int _{{|y|\geq \varepsilon }}f(x-y){y_{j} \over |y|^{{n+1}}}dy={\frac {c_{n}}{n-1}}\int \partial _{j}f(x-y){1 \over |y|^{{n-1}}}dy,

where

c_{n}=\Gamma \left({\tfrac {n+1}{2}}\right)\pi ^{{-{\frac {n+1}{2}}}}.

Under the Fourier transform:

\widehat {R_{j}f}(t)={it_{j} \over |t|}\widehat {f}(t).

Thus R_j corresponds to the operator ∂_jΔ^−1/2, where Δ = −∂₁² − ... −∂_n² denotes the Laplacian on Rⁿ. By definition R_j is a bounded and skew-adjoint operator for the L² norm and

R_{1}^{2}+\cdots +R_{n}^{2}=-I.

The corresponding truncated operators

R_{{j,\varepsilon }}f(x)=c_{n}\int _{{|y|\geq \varepsilon }}f(x-y){y_{j} \over |y|^{{n+1}}}dy

are uniformly bounded in the operator norm. This can either be proved directly or can be established by the Calderón−Zygmund method of rotations for the group SO(n).^[24] This expresses the operators R_j and their truncations in terms of the Hilbert transforms in one dimension and its truncations. In fact if G = SO(n) with normalised Haar measure and H⁽¹⁾ is the Hilbert transform in the first coordinate, then

{\begin{aligned}R_{j}&=\int _{G}\varphi (g)gH^{{(1)}}g^{{-1}}\,dg,\\R_{{j,\varepsilon }}&=\int _{G}\varphi (g)gH_{\varepsilon }^{{(1)}}g^{{-1}}\,dg,\\R_{{j,\varepsilon ,R}}&=\int _{G}\varphi (g)gH_{{\varepsilon ,R}}^{{(1)}}g^{{-1}}\,dg.\end{aligned}}

where φ(g) is the (1,j) matrix coefficient of g.

In particular for f ∈ L², R_j,εf → R_jf in L². Moreover, R_j,εf tends to R_j almost everywhere. This can be proved exactly as for the Hilbert transform by using the Poisson operators defined on L²(Rⁿ) when Rⁿ is regarded as the boundary of a halfspace in Rⁿ⁺¹. Alternatively it can be proved directly from the result for the Hilbert transform on R using the expression of R_j as an integral over G.^[25]^[26]

The Poisson operators T_y on Rⁿ are defined for y > 0 by^[27]

T_{y}f(x)=c_{n}\int _{{{\mathbf {R}}^{n}}}{\frac {yf(x)}{\left(|x-t|^{2}+y^{2}\right)^{{{\frac {n+1}{2}}}}}}dt.

They are given by convolution with the functions

P_{y}(x)=c_{n}{\frac {y}{\left(|x|^{2}+y^{2}\right)^{{{\frac {n+1}{2}}}}}}.

P_y is the Fourier transform of the function e^−y|x|, so under the Fourier transform they correspond to multiplication by these functions and form a contraction semigroup on L²(Rⁿ). Since P_y is positive and integrable with integral 1, the operators T_y also define a contraction semigroup on each L^p space with 1 < p < ∞.

The Riesz transforms of the Poisson kernel can be computed

R_{j}P_{\varepsilon }(x)=c_{n}{\frac {x_{j}}{\left(|x|^{2}+\varepsilon ^{2}\right)^{{{\frac {n+1}{2}}}}}}.

The operator R_jT_ε is given by convolution with this function. It can be checked directly that the operators R_jT_ε − R_j,ε are given by convolution with functions uniformly bounded in L¹ norm. The operator norm of the difference is therefore uniformly bounded. We have (R_jT_ε − R_j,ε)f → 0 at each Lebesgue point of f; while (R_j − R_jT_ε)f → 0 at each Lebesgue point of R_jf. So R_j,εf → R_jf on the common Lebesgue points of f and R_jf.

L^p theory

Elementary proofs of M. Riesz theorem

The theorem of Marcel Riesz asserts that singular integral operators that are continuous for the $L 2$ norm are also continuous in the $L p$ norm for $1 < p < \infty$ and that the operator norms vary continuously with $p$ .

Bochner's proof for Hilbert transform on the circle ^[28]

Once it is established that the operator norms of the Hilbert transform on $L p (T)$ are bounded for even integers, it follows from the Riesz–Thorin interpolation theorem and duality that they are bounded for all $p$ with $1 < p < \infty$ and that the norms vary continuously with $p$ . Moreover, the arguments with the Poisson integral can be applied to show that the truncated Hilbert transforms $H ε$ are uniformly bounded in operator norm and converge in the strong operator topology to $H$ .

It is enough to prove the bound for real trigonometric polynomials without constant term:

f\left(e^{{i\theta }}\right)=\sum _{{m=1}}^{N}a_{m}e^{{im\theta }}+a_{{-m}}e^{{-im\theta }},\qquad a_{{-m}}=\overline {a_{m}}.

Since f + iHf is a polynomial in $e iθ$ without constant term

{\frac {1}{2\pi }}\int _{0}^{{2\pi }}(f+iHf)^{{2n}}\,d\theta =0.

Hence, taking the real part and using Hölder's inequality:

\|Hf\|_{{2n}}^{{2n}}\leq \sum _{{k=0}}^{{n-1}}{2n \choose 2k}\left|\left((Hf)^{{2k}},f^{{2n-2k}}\right)\right|\leq \sum _{{k=0}}^{{n-1}}{2n \choose 2k}\|Hf\|_{{2n}}^{{2k}}\cdot \|f\|_{{2n}}^{{2n-2k}}.

So the M. Riesz theorem follows by induction for $p$ an even integer and hence for all $p$ with $1 < p < \infty$ .

Cotlar's proof for Hilbert transform on the line ^[29]

Once it is established that the operator norms of the Hilbert transform on $L p (R)$ are bounded when $p$ is a power of 2, it follows from the Riesz–Thorin interpolation theorem and duality that they are bounded for all $p$ with $1 < p < \infty$ and that the norms vary continuously with $p$ . Moreover, the arguments with the Poisson integral can be applied to show that the truncated Hilbert transforms $H ε$ are uniformly bounded in operator norm and converge in the strong operator topology to $H$ .

It is enough to prove the bound when f is a Schwartz function. In that case the following identity of Cotlar holds:

(Hf)^{2}=f^{2}+2H(fH(f)).

In fact, write f = f₊ + f₋ according to the $\pm i$ eigenspaces of H. Since f ± iHf extend to holomorphic functions in the upper and lower half plane, so too do their squares. Hence

f^{2}-(Hf)^{2}=\left(f_{+}+f_{-}\right)^{2}+\left(f_{+}-f_{-}\right)^{2}=2\left(f_{+}^{2}+f_{-}^{2}\right)=-2iH\left(f_{+}^{2}-f_{-}^{2}\right)=-2H(f(Hf)).

(Cotlar's identity can also be verified directly by taking Fourier transforms.)

Hence, assuming the M. Riesz theorem for $p = 2 n$ ,

\|Hf\|_{{2^{{n+1}}}}^{2}=\left\|(Hf)^{2}\right\|_{{2^{n}}}\leq \left\|f^{2}\right\|_{{2^{n}}}+2\|H(fH(f))\|_{{2^{n}}}\leq \|f\|_{{2^{{n+1}}}}^{2}+2\|H\|_{{2^{n}}}\|f\|_{{2^{{n+1}}}}\|Hf\|_{{2^{{n+1}}}}.

Since

R^{2}>1+2\|H\|_{{2^{n}}}R

for $R$ sufficiently large, the M. Riesz theorem must also hold for $p = 2 n +1$ .

Exactly the same method works for the Hilbert transform on the circle.^[30] The same identity of Cotlar is easily verified on trigonometric polynomials f by writing them as the sum of the terms with non-negative and negative exponents, i.e. the $\pm i$ eigenfunctions of $H$ . The $L p$ bounds can therefore be established when $p$ is a power of 2 and follow in general by interpolation and duality.

Calderón–Zygmund method of rotation

The method of rotation for Riesz transforms and their truncations applies equally well on $L p$ spaces for $1 < p < \infty$ . Thus these operators can be expressed in terms of the Hilbert transform on $R$ and its truncations. The integration of the functions $Φ$ from the group $T$ or $SO(n)$ into the space of operators on $L p$ is taken in the weak sense:

\left(\int _{G}\Phi (x)\,dx\,f,g\right)=\int _{G}(\Phi (x)f,g)\,dx

where f lies in $L p$ and $g$ lies in the dual space $L q$ with $1 / p + 1 / q .$ It follows that Riesz transforms are bounded on $L p$ and that the differences with their truncations are also uniformly bounded. The continuity of the $L p$ norms of a fixed Riesz transform is a consequence of the Riesz–Thorin interpolation theorem.

Pointwise convergence

The proofs of pointwise convergence for Hilbert and Riesz transforms rely on the Lebesgue differentiation theorem, which can be proved using the Hardy-Littlewood maximal function.^[31] The techniques for the simplest and best known case, namely the Hilbert transform on the circle, are a prototype for all the other transforms. This case is explained in detail here.

Let f be in L^p(T) for p > 1. The Lebesgue differentiation theorem states that

\displaystyle {A(\varepsilon )={1 \over 2\varepsilon }\int _{{x-\varepsilon }}^{{x+\varepsilon }}|f(t)-f(x)|\,dt\to 0}

for almost all x in T.^[32]^[33]^[34] The points at which this holds are called the Lebesgue points of f. Using this theorem it follows that if f is an integrable function on the circle, the Poisson integral T_rf tends pointwise to f at each Lebesgue point of f. In fact, for x fixed, A(ε) is a continuous function on [0,π]. Continuity at 0 follows because x is a Lebesgue point and elsewhere because, if h is an integrable function, the integral of |h| on intervals of decreasing length tends to 0 by Hölder's inequality.

Letting r = 1 − ε, the difference can be estimated by two integrals:

2\pi |T_{{r}}f(x)-f(x)|=\int _{{0}}^{{2\pi }}|(f(x-y)-f(x))P_{r}(y)|\,dy\leq \int _{{|y|\leq \varepsilon }}+\int _{{|y|\geq \varepsilon }}.

The Poisson kernel has two important properties for ε small

{\begin{aligned}\sup _{{y\in [-\varepsilon ,\varepsilon ]}}|P_{{1-\varepsilon }}(y)|&\leq \varepsilon ^{{-1}}.\\\sup _{{y\notin (-\varepsilon ,\varepsilon )}}|P_{{1-\varepsilon }}(y)|&\to 0.\end{aligned}}

The first integral is bounded by A(ε) by the first inequality so tends to zero as ε goes to 0; the second integral tends to 0 by the second inequality.

The same reasoning can be used to show that T_{1 − ε}Hf – H_εf tends to zero at each Lebesgue point of f.^[35] In fact the operator T_{1 − ε}Hf has kernel Q_r + i, where the conjugate Poisson kernel Q_r is defined by

\displaystyle {Q_{r}(\theta )={2r\sin \theta \over 1-2r\cos \theta +r^{2}}.}

Hence

\displaystyle {2\pi |T_{{1-\varepsilon }}Hf(x)-H_{\varepsilon }f(x)|\leq \int _{{|y|\leq \varepsilon }}|f(x-y)-f(x)|\cdot |Q_{r}(y)|\,dy+\int _{{|y|\geq \varepsilon }}|f(x-y)-f(x)|\cdot |Q_{1}(y)-Q_{r}(y)|\,dy.}

The conjugate Poisson kernel has two important properties for ε small

{\begin{aligned}\sup _{{y\in [-\varepsilon ,\varepsilon ]}}|Q_{{1-\varepsilon }}(y)|&\leq \varepsilon ^{{-1}}.\\\sup _{{y\notin (-\varepsilon ,\varepsilon )}}|Q_{1}(y)-Q_{{1-\varepsilon }}(y)|&\to 0.\end{aligned}}

Exactly the same reasoning as before shows that the two integrals tend to 0 as ε → 0.

Combining these two limit formulas it follows that H_εf tends pointwise to Hf on the common Lebesgue points of f and Hf and therefore almost everywhere.^[36]^[37]^[38]

Maximal functions

Much of the L^p theory has been developed using maximal functions and maximal transforms. This approach has the advantage that it also extends to L¹ spaces in an appropriate "weak" sense and gives refined estimates in L^p spaces for p > 1. These finer estimates form an important part of the techniques involved in Lennart Carleson's solution in 1966 of Lusin's conjecture that the Fourier series of L² functions converge almost everywhere.^[39] In the more rudimentary forms of this approach, the L² theory is given less precedence: instead there is more emphasis on the L¹ theory, in particular its measure-theoretic and probabilistic aspects; results for other L^p spaces are deduced by a form of interpolation between L¹ and L^∞ spaces. The approach is described in numerous textbooks, including the classics Zygmund (1977) and Katznelson (2004). Katznelson's account is followed here for the particular case of the Hilbert transform of functions in L¹(T), the case not covered by the development above.^[40]

If f is an L¹ function on the circle its maximal function is defined by^[41]

\displaystyle {f^{*}(t)=\sup _{{0<h\leq \pi }}{1 \over 2h}\int _{{t-h}}^{{t+h}}|f(s)|\,ds.}

f* is finite almost everywhere and is of weak L¹ type. In fact for λ > 0 if

\displaystyle {E_{f}(\lambda )=\{x:\,|f(x)|>\lambda \},\,\,f_{\lambda }=\chi _{{E(\lambda )}}f,}

then^[42]

m(E_{{f^{*}}}(\lambda ))\leq {8 \over \lambda }\int _{{E_{f}(\lambda )}}|f|\leq {8\|f\|_{1} \over \lambda },

where m denotes Lebesgue measure.

The Hardy−Littlewood inequality above leads to a proof that almost every point x of T is a Lebesgue point of an integrable function f, so that

\displaystyle {\lim _{{h\to 0}}{\frac {\int _{{x-h}}^{{x+h}}|f(t)-f(x)|\,dt}{2h}}\to 0.}

In fact let

\omega (f)(x)=\limsup _{{h\to 0}}{\frac {\int _{{x-h}}^{{x+h}}|f(t)-f(x)|\,dt}{2h}}\leq f^{*}(x)+|f(x)|.

If g is continuous, then the ω(g) =0, so that ω(f − g) = ω(f). On the other hand, f can be approximated arbitrarily closely in L¹ by continuous g. Then, using Chebychev's inequality,

m\{x:\,\omega (f)(x)>\lambda \}=m\{x:\,\omega (f-g)(x)>\lambda \}\leq m\{x:\,(f-g)^{*}(x)>\lambda \}+m\{x:\,|f(x)-g(x)|>\lambda \}\leq C\lambda ^{{-1}}\|f-g\|_{1}.

The right hand side can be made arbitrarily small, so that ω(f) = 0 almost everywhere.

The Poisson integrals of an L¹ function f satisfy^[43]

\displaystyle {|T_{r}f|\leq f^{*}.}

It follows that T_r f tends to f pointwise almost everywhere. In fact let

\displaystyle {\Omega (f)=\limsup _{{r\rightarrow 1}}|T_{r}f-f|.}

If g is continuous, then the difference tends to zero everywhere, so Ω(f − g) = Ω(f). On the other hand, f can be approximated arbitrarily closely in L¹ by continuous g. Then, using Chebychev's inequality,

m\{x:\,\Omega (f)(x)>\lambda \}=m\{x:\,\Omega (f-g)(x)>\lambda \}\leq m\{x:\,(f-g)^{*}(x)>\lambda \}+m\{x:\,|f(x)-g(x)|>\lambda \}\leq C\lambda ^{{-1}}\|f-g\|_{1}.

The right hand side can be made arbitrarily small, so that Ω(f) = 0 almost everywhere. A more refined argument shows that convergence occurs at each Lebesgue point of f.

If f is integrable the conjugate Poisson integrals are defined and given by convolution by the kernel Q_r. This defines Hf inside |z| < 1. To show that Hf has a radial limit for almost all angles,^[44] consider

\displaystyle {F(z)=\exp(-f(z)-iHf(z)),}

where f(z) denotes the extension of f by Poisson integral. F is holomorphic in the unit disk with |F(z)| ≤ 1. The restriction of F to a countable family of concentric circles gives a sequence of functions in L^∞(T) which has a weak g limit in L^∞(T) with Poisson integral F. By the L² results, g is the radial limit for almost all angles of F. It follows that Hf(z) has a radial limit almost everywhere. This is taken as the definition of Hf on T, so that T_rH f tends pointwise to H almost everywhere. The function Hf is of weak L¹ type.^[45]

The inequality used above to prove pointwise convergence for L^p function with 1 < p < ∞ make sense for L¹ functions by invoking the maximal function. The inequality becomes

\displaystyle {|H_{\varepsilon }f-T_{{1-\varepsilon }}Hf|\leq 4f^{*}.}

Let

\displaystyle {\omega (f)=\limsup _{{\varepsilon \rightarrow 0}}|H_{\varepsilon }f-T_{{1-\varepsilon }}Hf|.}

If g is smooth, then the difference tends to zero everywhere, so ω(f − g) = ω(f). On the other hand, f can be approximated arbitrarily closely in L¹ by smooth g. Then

m\{x:\,\omega (f)(x)>\lambda \}=m\{x:\,\omega (f-g)(x)>\lambda \}\leq m\{x:\,4(f-g)^{*}(x)>\lambda \}\leq C\lambda ^{{-1}}\|f-g\|_{1}.

The right hand side can be made arbitrarily small, so that ω(f) = 0 almost everywhere. Thus the difference for f tends to zero almost everywhere. A more refined argument can be given^[46] to show that, as in case of L^p, the difference tends to zero at all Lebesgue points of f. In combination with the result for the conjugate Poisson integral, it follows that, if f is in L¹(T), then H_εf converges to Hf almost everywhere, a theorem originally proved by Privalov in 1919.

General theory

Calderón & Zygmund (1952) introduced general techniques for studying singular integral operators of convolution type. In Fourier transform the operators are given by multiplication operators. These will yield bounded operators on L² if the corresponding multiplier function is bounded. To prove boundedness on L^p spaces, Calderón and Zygmund introduced a method of decomposing L¹ functions, generalising the rising sun lemma of F. Riesz. This method showed that the operator defined a continuous operator from L¹ to the space of functions of weak L¹. The Marcinkiewicz interpolation theorem and duality then implies that the singular integral operator is bounded on all L^p for 1 < p < ∞. A simple version of this theory is described below for operators on R. As de Leeuw (1965) showed, results on R can be deduced from corresponding results for T by restricting the multiplier to the integers, or equivalently periodizing the kernel of the operator. Corresponding results for the circle were originally established by Marcinkiewicz in 1939. These results generalize to Rⁿ and Tⁿ. They provide an alternative method for showing that the Riesz transforms, the higher Riesz transforms and in particular the Beurling transform define bounded operators on L^p spaces.^[47]

Calderón-Zygmund decomposition

Let f be a non-negative integrable or continuous function on [a,b]. Let I = (a,b). For any open subinterval J of [a,b], let f_J denote the average of |f| over J. Let α be a positive constant greater than f_I. Divide I into two equal intervals (omitting the midpoint). One of these intervals must satisfy f_J < α since their sum is 2f_I so less than 2α. Otherwise the interval will satisfy α ≤ f_J < 2α. Discard such intervals and repeat the halving process with the remaining interval, discarding intervals using the same criterion. This can be continued indefinitely. The discarded intervals are disjoint and their union is an open set Ω. For points x in the complement, they lie in a nested set of intervals with lengths decreasing to 0 and on each of which the average of f is bounded by α. If f is continuous these averages tend to |f(x)|. If f is only integrable this is only true almost everywhere, for it is true at the Lebesgue points of f by the Lebesgue differentiation theorem. Thus f satisfies |f(x)| ≤ α almost everywhere on Ω^c, the complement of Ω. Let J_n be the set of discarded intervals and define the "good" function g by

\displaystyle {g(x)=\chi _{{J_{n}}}(f)\,\,\,(x\in J_{n}),\,\,\,\,\,g(x)=f(x)\,\,\,(x\in \Omega ^{c}).}

By construction |g(x)| ≤ 2α almost everywhere and

\displaystyle {\|g\|_{1}\leq \|f\|_{1}.}

Combining these two inequalities gives

\displaystyle {\|g\|_{p}^{p}\leq (2\alpha )^{{p-1}}\|f\|_{1}.}

Define the "bad" function b by b = f − g. Thus b is 0 off Ω and equal to f minus its average on J_n. So the average of b on J_n is zero and

\displaystyle {\|b\|_{1}\leq 2\|f\|_{1}.}

Moreover, since |b| ≥ α on Ω

\displaystyle {m(\Omega )\leq \alpha ^{{-1}}\|f\|_{1}.}

The decomposition

\displaystyle {f(x)=g(x)+b(x)}

is called the Calderón–Zygmund decomposition.^[48]

Multiplier theorem

Let K(x) be a kernel defined on R\{0} such that

W(f)=\lim _{{\varepsilon \to 0}}\int _{{|x|\geq \varepsilon }}K(x)f(x)\,dx

exists as a tempered distribution for f a Schwartz function. Suppose that the Fourier transform of T is bounded, so that convolution by W defines a bounded operator T on L²(R). Then if K satisfies Hörmander's condition

A=\sup _{{y\neq 0}}\int _{{|x|\geq 2|y|}}|K(x-y)-K(x)|\,dx<\infty ,

then T defines a bounded operator on L^p for 1 < p < ∞ and a continuous operator from L¹ into functions of weak type L¹.^[49]

In fact by the Marcinkiewicz interpolation argument and duality, it suffices to check that if f is smooth of compact support then

m\{x:\,|Tf(x)|\geq 2\lambda \}\leq (2A+4\|T\|)\cdot \lambda ^{{-1}}\|f\|_{1}.

Take a Calderón−Zygmund decomposition of f as above

f(x)=g(x)+b(x)

with intervals J_n and with α = λμ, where μ > 0. Then

m\{x:\,|Tf(x)|\geq 2\lambda \}\leq m\{x:\,|Tg(x)|\geq \lambda \}+m\{x:\,|Tb(x)|\geq \lambda \}.

The term for g can be estimated using Chebychev's inequality:

m\{x:\,|Tg(x)|\geq 2\lambda \}\leq \lambda ^{{-2}}\|Tg\|_{2}^{2}\leq \lambda ^{{-2}}\|T\|^{2}\|g\|_{2}^{2}\leq 2\lambda ^{{-1}}\mu \|T\|^{2}\|f\|_{1}.

If J* is defined to be the interval with the same centre as J but twice the length, the term for b can be broken up into two parts:

m\{x:\,|Tb(x)|\geq \lambda \}\leq m\{x:\,x\notin \cup J_{n}^{*},\,\,\,|Tb(x)|\geq \lambda \}+m(\cup J_{n}^{*}).

The second term is easy to estimate:

m(\cup J_{n}^{*})\leq \sum m(J_{n}^{*})=2\sum m(J_{n})\leq 2\lambda ^{{-1}}\mu ^{{-1}}\|f\|_{1}.

To estimate the first term note that

b=\sum b_{n},\qquad b_{n}=(f-{\mathbf {Av}}_{{J_{n}}}(f))\chi _{{J_{n}}}.

Thus by Chebychev's inequality:

m\{x:\,x\notin \cup J_{m}^{*},\,\,\,|Tb(x)|\geq \lambda \}\leq \lambda ^{{-1}}\int _{{(\cup J_{m}^{*})^{c}}}|Tb(x)|\,dx\leq \lambda ^{{-1}}\sum _{n}\int _{{(J_{n}^{*})^{c}}}|Tb_{n}(x)|\,dx.

By construction the integral of b_n over J_n is zero. Thus, if y_n is the midpoint of J_n, then by Hörmander's condition:

\int _{{(J_{n}^{*})^{c}}}|Tb_{n}(x)|\,dx=\int _{{(J_{n}^{*})^{c}}}\left|\int _{{J_{n}}}(K(x-y)-K(x-y_{n}))b_{n}(y)\,dy\right|\,dx\leq \int _{{J_{n}}}|b_{n}(y)|\int _{{(J_{n}^{*})^{c}}}|K(x-y)-K(x-y_{n})|\,dxdy\leq A\|b_{n}\|_{1}.

Hence

m\left\{x:\,x\notin \cup J_{m}^{*},|Tb(x)|\geq \lambda \right\}\leq \lambda ^{{-1}}A\|b\|_{1}\leq 2A\lambda ^{{-1}}\|f\|_{1}.

Combining the three estimates gives

m\{x:\,|Tf(x)|\geq \lambda \}\leq \left(2\mu \|T\|^{2}+2\mu ^{{-1}}+2A\right)\lambda ^{{-1}}\|f\|_{1}.

The constant is minimized by taking

\mu =\|T\|^{{-1}}.

The Markinciewicz interpolation argument extends the bounds to any L^p with 1 < p < 2 as follows.^[50] Given a > 0, write

f=f_{a}+f^{a},

where f_a = f if |f| < a and 0 otherwise and f^a = f if |f| ≥ a and 0 otherwise. Then by Chebychev's inequality and the weak type L¹ inequality above

m\{x:\,|Tf(x)|>a\}\leq m\left\{x:\,|Tf_{a}(x)|>{\tfrac {a}{2}}\right\}+m\left\{x:\,|Tf^{a}(x)|>{\tfrac {a}{2}}\right\}\leq 4a^{{-2}}\|T\|^{2}\|f_{a}\|_{2}^{2}+Ca^{{-1}}\|f^{a}\|_{1}.

Hence

{\begin{aligned}\|Tf\|_{p}^{p}&=p\int _{0}^{\infty }a^{{p-1}}m\{x:\,|Tf(x)|>a\}\,da\\&\leq p\int _{0}^{\infty }a^{{p-1}}\left(4a^{{-2}}\|T\|^{2}\|f_{a}\|_{2}^{2}+Ca^{{-1}}\|f^{a}\|_{1}\right)da\\&=4\|T\|^{2}\iint _{{|f(x)|<a}}|f(x)|^{2}a^{{p-3}}\,dx\,da+2C\iint _{{|f(x)|\geq a}}|f(x)|a^{{p-2}}\,dx\,da\\&\leq \left(4\|T\|^{2}(2-p)^{{-1}}+C(p-1)^{{-1}}\right)\int |f|^{p}\\&=C_{p}\|f\|_{p}^{p}.\end{aligned}}

By duality

\|Tf\|_{q}\leq C_{p}\|f\|_{q}.

Continuity of the norms can be shown by a more refined argument^[51] or follows from the Riesz–Thorin interpolation theorem.

Notes

↑ Torchinsky 2004, pp. 65–66
↑ Bell 1992, pp. 14–15
↑ Krantz 1999
↑ Torchinsky 1986
↑ Stein & Rami 2005, pp. 112–114
↑
See:
↑ Garnett 2007, p. 102
↑
See:
↑ Stein & Shakarchi 2005, pp. 213–221
↑ Hörmander 1990
↑ Titchmarsh, 1939 & 102–105
↑
See:
- Krantz 1999
- Torchinsky 1986
- Duoandikoetxea 2001, pp. 49–51
↑ Stein & Shakarchi 2005, pp. 112–114
↑ Stein & Weiss 1971
↑ Astala, Ivaniecz & Martin 2009, pp. 101–102
↑ Grafakos 2005
↑ Stein & Weiss 1971
↑ Stein & Weiss 1971, p. 51
↑ Grafakos 2008
↑ Stein & Weiss 1971, pp. 222–223
↑ Stein & Weiss 1971
↑ Astala, Iwaniecz & Martin 2009, pp. 93–95
↑ Astala, Iwaniecz & Martin 2009, pp. 97–98
↑ Grafokos 2008, pp. 272–274
↑ Grafakos 2008
↑ Stein & Weiss 1971, pp. 222–223, 236–237
↑ Stein & Weiss 1971
↑ Grafakos 2005, p. 215−216
↑ Grafakos 2005, p. 255−257
↑ Gohberg & Krupnik 1992, pp. 19–20
↑
See:
- Stein & Weiss 1971, pp. 12–13
- Torchinsky 2004
↑ Torchinsky 2005, pp. 41–42
↑ Katznelson 2004, pp. 10–21
↑ Stein, Shakarchi & 112-114
↑ Garnett 2007, pp. 102–103
↑ Krantz 1999
↑ Torchinsky 1986
↑ Stein & Shakarchi 2005, pp. 112–114
↑ Arias de Reyna 2002
↑
See also:
↑ Krantz 1999, p. 71
↑ Katznelson 2004, pp. 74–75
↑ Katznelson 2004, p. 76
↑ Katznelson 2004, p. 64
↑ Katznelson 2004, p. 66
↑ Katznelson 2004, pp. 78–79
↑
See:
- Hörmander 1990
- Torchinsky 2005
- Grafakos 2008
- Stein 1970
- Stein & Weiss 1971, pp. 257–267
↑ Torchinsky 2005, pp. 74–76,84–85
↑ Grafakos 2008, pp. 290–293
↑ Hörmander 1990, p. 245
↑ Torchinsky 2005, pp. 87–91

References

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Singular integral operators of convolution type

L2 theory

Hilbert transform on the circle

Hilbert transform on the real line

Riesz transforms in the complex plane

Beurling transform in the complex plane

Riesz transforms in higher dimensions

Lp theory

Elementary proofs of M. Riesz theorem

Bochner's proof for Hilbert transform on the circle [28]

Cotlar's proof for Hilbert transform on the line [29]

Calderón–Zygmund method of rotation

Pointwise convergence

Maximal functions

General theory

Calderón-Zygmund decomposition

Multiplier theorem

Notes

References

L² theory

L^p theory

Bochner's proof for Hilbert transform on the circle ^[28]

Cotlar's proof for Hilbert transform on the line ^[29]