FOURIER SERIES AND MAXIMAL THEOREMS
MATHEMATICS
Submitted 1967-01-01 | SovietRxiv: ru-196701.93124 | Translated from Russian

Abstract Generated abstract

This note studies double Fourier series of periodic functions in two variables, their conjugate functions and series, and related maximal functions defined through Cesàro means and singular integral truncations. It examines a question of almost everywhere existence for the double conjugate function, giving a measure estimate for logarithmic level sets and using it to identify a gap in Stein’s previously stated nonexistence argument. The paper proves integrability results for maximal functions under \(L\log L\) and \(L(\log L)^2\) assumptions, shows the sharpness of these conditions by example, and records Fourier representation results for conjugate functions. It also extends a theorem of Marcinkiewicz by showing that diagonal Cesàro means of positive order converge almost everywhere to \(f\) for every integrable function of two variables.

Full Text

UDC 517.51

MATHEMATICS

L. V. ZHIZHIASHVILI

FOURIER SERIES AND MAXIMAL THEOREMS

(Presented by Academician I. N. Vekua on 8 VII 1966)

Consider a function of two variables \(f(x,y)\). Suppose that it is periodic with respect to each of the variables and that \(f(x,y)\in L(R)\), where \(R=[-\pi,\pi;-\pi,\pi]\). Denote by \(\bar f_i(x,y)\) \((i=1,2,3)\) the conjugate functions of two variables

\[ \bar f_1(x,y)=-\frac{1}{2\pi}\int_{-\pi}^{\pi} f(x+s,y)\operatorname{ctg}\frac{s}{2}\,ds, \]

\[ \bar f_2(x,y)=-\frac{1}{2\pi}\int_{-\pi}^{\pi} f(x,y+t)\operatorname{ctg}\frac{t}{2}\,dt, \]

\[ \bar f_3(x,y)=\frac{1}{4\pi^2}\int_{-\pi}^{\pi}\int_{-\pi}^{\pi} f(x+s,y+t)\operatorname{ctg}\frac{s}{2}\operatorname{ctg}\frac{t}{2}\,dt\,ds. \]

By \(\sigma[f]\) we shall denote the double Fourier series of the function \(f(x,y)\), and by the symbols \(\bar\sigma[f;x]\), \(\bar\sigma[f;y]\), and \(\bar\sigma[f;x,y]\) the double conjugate trigonometric series to the series \(\sigma[f]\), respectively in the variable \(x\), in the variable \(y\), and in the totality of the variables \(x\) and \(y\). Further, let \(\sigma_{mn}^{(i,\alpha,\beta)}(x,y)\) \((i=0,1,2,3)\), \(\alpha,\beta>0\), be the Cesàro \((C;\alpha,\beta)\)-means respectively of the series \(\sigma[f]\), \(\bar\sigma[f;x]\), \(\bar\sigma[f;y]\), \(\bar\sigma[f;x,y]\), and put

\[ \varphi_i(x,y)=\sup_{m,n\ge0}\left|\sigma_{mn}^{(i,\alpha,\beta)}(x,y)\right|\qquad (i=0,1,2,3), \]

\[ \varphi_4(x,y)=\sup_{0<\varepsilon,\eta\le\pi} \left|\int_{\varepsilon}^{\pi}\int_{\eta}^{\pi} \frac{f(x+s,y+t)-f(x-s,y+t)-f(x+s,y-t)+f(x-s,y-t)} {\operatorname{tg}s/2\,\operatorname{tg}t/2}\,dt\,ds\right|, \]

\[ \varphi_5(x,y)=\sup_{0<\varepsilon\le\pi} \left|\int_{\varepsilon}^{\pi} \frac{f(x+s,y)-f(x-s,y)}{\operatorname{tg}s/2}\,ds\right|, \]

\[ \varphi_6(x,y)=\sup_{0<\eta\le\pi} \left|\int_{\eta}^{\pi} \frac{f(x,y+t)-f(x,y-t)}{\operatorname{tg}t/2}\,dt\right|. \]

Further, if \(s_{ij}(x,y)\) \((i,j=0,1,\ldots)\) denote the partial sums of the series \(\sigma[f]\), then the expressions

\[ \sigma_n^\alpha(x,y)=\sum_{k=0}^{n} A_{n-k}^{\alpha-1}s_{kk}(x,y),\qquad \alpha>0, \]

will be called the \((C,\alpha)\)-means of the series \(\sigma[f]\).

In the present note we give assertions concerning questions of the existence of the function \(\bar f_3(x,y)\) and the summability of the functions \(\varphi_i(x,y)\) \((i=0,\ldots,6)\); we also study the behavior of the \((C,\alpha)\)-means of the series \(\sigma[f]\).

As A. Zygmund showed \((^1)\), if \(f(x,y)\in L\log^+ L\), then the function \(\bar f_3(x,y)\) exists almost everywhere. In \((^2)\) he also posed the question: if \(f(x,y)\in\)

\(\in L(R)\), then does there exist almost everywhere the function \(f_3(x,y)\), where

\[ \bar f_3(x,y)=\lim_{(\varepsilon,\eta)_\lambda\to 0} \int_{\varepsilon}^{\pi}\int_{\eta}^{\pi} \frac{f(x+s,y+t)-f(x-s,y+t)-f(x+s,y-t)+f(x-s,y-t)} {\operatorname{tg}s/2+\operatorname{tg}t/2}\,dt\,ds, \tag{1} \]

where the symbol \((\varepsilon,\eta)_\lambda\to 0\) means that \(\varepsilon\to 0\), \(\eta\to 0\), and \(1/\lambda \leq \varepsilon/\eta \leq \lambda\), \(\lambda\geq 1\). E. Stein (see \((^3)\), Theorem 5) showed that, in contrast to the case of a function of one variable, the limit (1) may fail to exist on a set of positive planar measure even in the case when \(\lambda=1\).

Below we shall show that the scheme of the proof (see \((^3)\), Theorem 5) given by E. Stein contains an error. To verify this, we shall need the following

Lemma. Let \((x,y)\in [0,1/3;0,1/3]\equiv I\) and \(\varepsilon>0\). Then, if

\[ E^\varepsilon(\alpha)\equiv E(\alpha)= \left\{(x,y)\in I:\frac{1}{xy|\ln x|^\varepsilon|\ln y|^\varepsilon}\geq \alpha\right\}, \]

then for every \(\alpha\geq \alpha_0(\varepsilon)>0\) the measure

\[ \operatorname{mes}E(\alpha)\ll \begin{cases} \dfrac{A}{\alpha}(\ln \alpha)^{1-2\varepsilon}, & \text{if } 1-2\varepsilon>0,\\[6pt] \dfrac{A'}{\alpha}, & \text{if } 1-2\varepsilon<0, \end{cases} \]

where \(A\) and \(A'\) are certain positive constants.

Proof. Put

\[ E_1(\alpha)= \left\{(x,y)\in I:\frac{1}{xy|\ln x|^\varepsilon|\ln y|^\varepsilon}\geq \alpha,\ y\leq x\right\}, \]

\[ E_2(\alpha)= \left\{(x,y)\in I:\frac{1}{xy|\ln x|^\varepsilon|\ln y|^\varepsilon}\geq \alpha,\ y>x\right\}, \]

\[ E_3(\alpha)= \left\{(x,y)\in I:\frac{1}{xy|\ln x|^{2\varepsilon}}\geq \alpha\right\}, \]

\[ E_4(\alpha)= \left\{(x,y)\in I:\frac{1}{xy|\ln y|^{2\varepsilon}}\geq \alpha\right\}. \]

It is not difficult to see that \(E(\alpha)\subset E_1(\alpha)+E_2(\alpha)\subset E_3(\alpha)+E_4(\alpha)\). Consequently, the measure

\[ \operatorname{mes}E(\alpha)\leq \operatorname{mes}E_3(\alpha)+\operatorname{mes}E_4(\alpha). \tag{2} \]

But the set

\[ E_3(\alpha)= \left\{(x,y)\in I:\ y\leq \frac{1}{\alpha x|\ln x|^{2\varepsilon}}\right\}. \tag{3} \]

Let the number \(x_0\equiv x_0(\alpha,\varepsilon)\) be chosen so that \(1/\alpha x_0|\ln x_0|^{2\varepsilon}=1/3\). It is clear that

\[ 1/\alpha^2<x_0<1/\alpha,\qquad \alpha\geq \alpha_0(\varepsilon). \tag{4} \]

Thus, taking into account (3) and (4), we shall have

\[ \operatorname{mes}E_3(\alpha)\ll \frac{1}{\alpha}\int_{1/\alpha^2}^{1/3}\frac{dx}{x|\ln x|^{2\varepsilon}} +\frac{1}{\alpha} \ll \begin{cases} \dfrac{A}{2\alpha}(\ln\alpha)^{1-2\varepsilon}, & 1-2\varepsilon>0,\\[6pt] A'/2\alpha, & 1-2\varepsilon<0;\ \alpha\geq \alpha_0(\varepsilon). \end{cases} \tag{5} \]

Similarly,

\[ \operatorname{mes}E_4(\alpha)\ll \begin{cases} \dfrac{A}{2\alpha}(\ln\alpha)^{1-2\varepsilon}, & 1-2\varepsilon>0,\\[6pt] A'/2\alpha, & 1-2\varepsilon<0,\ \alpha\geq \alpha_0(\varepsilon). \end{cases} \tag{6} \]

From (2), (5), and (6) the validity of the lemma follows.

Analyzing the proof of the lemma, it is not difficult to see that if \(1-2\varepsilon=0\), i.e. \(\varepsilon=1/2\), then

\[ \operatorname{mes}E(\alpha)\ll \frac{A''}{\alpha}\ln\ln\alpha,\qquad \alpha\geq \alpha_0(\varepsilon). \]

Let us note here also that the following estimate is valid:

\[ \operatorname{mes} E(\alpha) \geqslant \frac{B}{\alpha}(\ln \alpha)^{1-2\varepsilon},\quad 1-2\varepsilon>0,\ \alpha\geqslant \alpha_0(\varepsilon), \tag{7} \]

where \(B\) is a positive constant. But the proof of relation (7) is more complicated than the proof of the lemma, and therefore we do not give it here.

The assertion that

\[ \operatorname{mes} E(\alpha)\geqslant B'/\alpha,\quad 1-2\varepsilon<0,\quad \alpha\geqslant \alpha_0(\varepsilon),\quad B'>0, \]

is, generally speaking, false. Thus, according to the lemma and (7), we shall have

\[ \operatorname{mes} E(\alpha)\sim (\ln \alpha)^{1-2\varepsilon}/\alpha,\quad 1-2\varepsilon>0\quad (\alpha\to\infty). \]

Now, analyzing the proof of E. Stein (see \({}^{3}\), Theorem 5, pp. 159–160), one can conclude that the function \(f_\delta(x,y)\) belongs to the class \(L(\log L)^{1-\varepsilon}\) (\(\varepsilon>0\), arbitrarily small) only when \(\delta>1-\varepsilon>1/2\); that is, \(1-2\delta<0\), and, according to the lemma,

\[ \operatorname{mes} E^\delta(\alpha)\leqslant A'/\alpha,\quad \alpha\geqslant \alpha_0(\delta), \]

which contradicts assertion (13.6) of E. Stein (see \({}^{3}\), p. 160). Consequently, E. Stein (see \({}^{3}\), p. 154) obtains no contradiction, and thereby he has not proved that if \(f(x,y)\in L(\log L)^\alpha\) for some \(\alpha\in[0,1)\), then, generally speaking, the double conjugate series \(\bar\sigma[f;x,y]\) is not summable almost everywhere by the Poisson method. Consequently, Stein’s conclusion on the nonexistence of \(\bar f_3(x,y)\), made in the conclusion and referring to Theorem 5, is insufficiently convincing.

We now give results connected with questions of summability of the functions \(\varphi_i(x,y)\) \((i=0,\ldots,6)\).

Theorem 1. If \(f(x,y)\in L\log L\), then

\[ \varphi_i(x,y)\in L^q(R)\quad \text{for all }q\in(0,1)\quad (i=0,\ldots,4). \tag{8} \]

If, however, \(f(x,y)\in L(\log L)^2\), then

\[ \varphi_i(x,y)\in L(R)\quad (i=0,\ldots,4). \tag{9} \]

Let us note that for functions \(f(x,y)\in L(\log L)^\alpha\) for all \(\alpha\in[0,1)\), assertion (8) is, generally speaking, false; and for the validity of assertion (9) the condition \(f(x,y)\in L(\log L)^2\) is also essential, since the following theorem is true.

Theorem 2. There exists a nonnegative \(2\pi\)-periodic function \(f_0(x,y)\in L(\log L)^{2-\varepsilon}\) for all \(\varepsilon\in(0,2]\), however \(\varphi_i(x,y)\notin L(R)\) \((i=0,\ldots,4)\).

For the summability of the functions \(\varphi_i(x,y)\) \((i=5,6)\), the condition \(f(x,y)\in L\log L\) is sufficient, which follows from a known theorem of A. Zygmund \({}^{4}\).

Theorem 3. Let \(f(x,y)\in L(R)\). If \(\bar f_i(x,y)\) \((i=1,2)\) are summable, then the series \(\bar\sigma[f;x]\) and \(\bar\sigma[f;y]\) are Fourier series respectively of the functions \(\bar f_1(x,y)\) and \(\bar f_2(x,y)\); but if \(f(x,y)\in L\log L\) and \(\bar f_3(x,y)\in L(R)\), then the series \(\bar\sigma[f;x,y]\) is also the Fourier series of the function \(\bar f_3(x,y)\).

J. Marcinkiewicz \({}^{5}\) proved that if \(f(x,y)\in L\log L\), then almost everywhere \(\sigma_n^1(x,y)\to f(x,y)\) as \(n\to\infty\). In fact, the following is true.

Theorem 4. If \(f(x,y)\in L(R)\), then for every \(\alpha>0\), almost everywhere

\[ \lim_{n\to\infty}\sigma_n^\alpha(x,y)=f(x,y). \]

The author expresses deep gratitude to Prof. P. L. Ulyanov for valuable advice.

Received
8 VII 1966

REFERENCES

\({}^{1}\) A. Zygmund, Fund. Math., 36, 207 (1949).
\({}^{2}\) A. Zygmund, Rend. Mat. e applic., 17, fasc. 2—4, 468 (1957).
\({}^{3}\) E. M. Stein, Ann. Math., 74, No. 1, 140 (1961).
\({}^{4}\) A. Zygmund, Fund. Math., 13, 284 (1929).
\({}^{5}\) J. Marcinkiewicz, Ann. Scuola norm. super Pisa, 8, 149 (1939).

Submission history

FOURIER SERIES AND MAXIMAL THEOREMS