Abstract
Full Text
Reports of the Academy of Sciences of the USSR
1958. Volume 123, No. 2
MATHEMATICS
E. A. BREDIKHINA
FOURIER SERIES AS A DEVICE FOR APPROXIMATING ALMOST-PERIODIC FUNCTIONS
(Presented by Academician V. I. Smirnov on 30 V 1958)
1. One of the questions in the theory of harmonic approximation is that of establishing the dependence between the deviations of the partial sums of the Fourier series of a continuous (2\pi)-periodic function and the best approximations of this function by trigonometric polynomials.
In the present note we briefly set forth some results of considering an analogous question for almost-periodic functions. Namely, a dependence is established between the deviations of the partial sums of the Fourier series of an almost-periodic function, whose Fourier exponents have no finite limit points, and the best approximations of this function by entire functions of finite degree.
Let the Fourier series of the almost-periodic function (f(x)) be written in the following form:
[
f(x)\sim \sum_{k=-\infty}^{\infty} A_k e^{i\Lambda_k x}
\tag{1}
]
[
\left(\Lambda_0=0;\quad \Lambda_k<\Lambda_{k+1}\ \text{for } k=0,1,2,\ldots;\right.
]
[
\left.
\lim_{k\to\infty}\Lambda_k=\infty,\ \Lambda_k=-\Lambda_{-k};\quad |A_k|+|A_{-k}|\ne 0\ \text{for } k\ne 0
\right).
]
Denote by (L=L(f)) the sequence ({\Lambda_k}) ((k=1,2,\ldots)). Put
[
R_\lambda(f)=\sup_x \left| f(x)-\sum_{|\Lambda_k|\le \lambda} A_k e^{i\Lambda_k x}\right|;
]
[
\alpha_\lambda(f)=\sum_{|\Lambda_k|>\lambda}|A_k|,\qquad
E_\lambda(f)=\inf_{F(z)\in B_\lambda}\left{\sup_x |f(x)-F(x)|\right},
]
where (B_\lambda) is the class of entire functions of degree (\le \lambda), bounded on the real axis.
Let (l={\lambda_k}) ((k=1,2,\ldots;\ 0<\lambda_k<\lambda_{k+1})) be an increasing sequence of positive numbers. Put
[
N_l(\lambda)=\sum_{\lambda_k\le \lambda}1.
]
We shall say that the sequence (l) belongs to the class (A) if there is an (a>0) such that (\lambda_{k+1}-\lambda_k>a) ((k=1,2,\ldots)). Denote by (A_\sigma) the class of all sequences (l), each of which can be partitioned into a finite number of sequences belonging to the class (A). Thus, (l\in A_\sigma) if the representation
[
l=\bigcup_{j=1}^{r} l^{(j)},\quad \text{where } l^{(j)}\in A\ (j=1,2,\ldots,r).
]
is possible.
Let (\mathcal{L}) be the class of all lacunary sequences (l). A sequence (l) belongs to the class (\mathcal{L}) if there exists (\theta>1) such that
(\lambda_{k+1}/\lambda_k \geqslant \theta). By (\mathcal{L}\sigma) we denote the class of all sequences (l), each of which can be divided into a finite number of lacunary ones. Thus, (\mathcal{L}\sigma) is the class of sequences (l) admitting the representation
[
l=\bigcup_{j=1}^{r} l^{(j)}, \quad \text{where } l^{(j)}\in \mathcal{L}\ (j=1,2,\ldots,r).
]
The inclusions (A_\sigma \supset A), (\mathcal{L}_\sigma \supset \mathcal{L}) are obvious.
- We formulate the main theorem of the note.
Theorem 1. Let (0<\lambda<\mu); then, for any almost-periodic function (f(x)) whose Fourier exponents have no finite limit points, the inequality
[
R_\lambda(f)\leqslant \Phi(\lambda,\mu)E_\lambda(f),
\tag{2}
]
holds, where
[
\Phi(\lambda,\mu)=1+\frac{4}{\pi}+2[N_L(\mu)-N_L(\lambda)]
+\frac{2}{\pi}\ln\frac{\mu+\lambda}{\mu-\lambda}.
]
The method of proof of Theorem 1 is a generalization and development of the method set out in the author’s paper ((^7)).
In applications of Theorem 1 the parameter (\mu) is chosen so as to minimize, as far as possible, the factor (\Phi(\lambda,\mu)).
From Theorem 1, formulated under very general conditions, a number of theorems follow. Let us consider some of them.
- Let (f(x)) be a continuous (2\pi)-periodic function, and let (E_n^(f)) be the best approximation of this function by trigonometric polynomials of order (n). Then (see ((^1)), pp. 374–375) (E_n^(f)=E_n(f)). Putting in inequality (2) (\lambda=n), (\mu=n+1-\varepsilon), where (\varepsilon) is sufficiently small, we obtain Lebesgue’s theorem ((^2), pp. 193–194).
The following theorem is a generalization of Lebesgue’s theorem to the almost-periodic case.
Theorem 2. Let the sequence (L(f)) have the following property: there exists a function (\varphi(\lambda)), nonnegative for (\lambda>\lambda_0), such that
[
N_L\left(\lambda+\frac{\lambda}{e^{\varphi(\lambda)}}\right)-N_L(\lambda)
=O[1+\varphi(\lambda)].
]
Then (R_\lambda(f)\leqslant \Phi(\lambda)E_\lambda(f)), where (\Phi(\lambda)=O[1+\varphi(\lambda)]).
For the proof of Theorem 2 it is enough to put in inequality (2)
[
\mu=\lambda+\frac{\lambda}{e^{\varphi(\lambda)}}.
]
We note two theorems contained in Theorem 2.
Theorem 3. If (L(f)\in A_\sigma), then (R_\lambda(f)\leqslant \Phi(\lambda)E_\lambda(f)), where (\Phi(\lambda)=O(\ln\lambda)).
Proof. For (L(f)\in A_\sigma) there exists (a>0) such that
[
N_L(\lambda+a)-N_L(\lambda)=O(1).
]
Putting in Theorem 2 (\varphi(\lambda)=\ln \dfrac{\lambda}{a}), we obtain the assertion to be proved.
Theorem 4. If (L(f)\in \mathcal{L}\sigma), then (R\lambda(f)=O[E_\lambda(f)]).
Proof. It is known ((^4)) that for (L(f)\in \mathcal{L}_\sigma) we have (N_L(2\lambda)-N_L(\lambda)=O(1)); therefore the condition of Theorem 2 is fulfilled for (\varphi(\lambda)=0).
This theorem is a generalization, to almost-periodic functions, of Theorem 4 of the paper ((^4)).
- Let us consider theorems providing new criteria for the uniform and absolute convergence of Fourier series of almost-periodic functions. Here the following theorem is the starting point.
Theorem 5. The Fourier series (1) of an almost-periodic function (f(x)) converges uniformly if there exists a numerical sequence ({\mu_n}) ((n=1,2,\ldots)) satisfying the conditions:
1) (\mu_n>\Lambda_n) for (n>n_0);
2) (\displaystyle \lim_{n\to\infty} E_{\Lambda_n}(f)\,[N_L(\mu_n)-N_L(\Lambda_n)]=0;)
3) (\displaystyle \lim_{n\to\infty} E_{\Lambda_n}(f)\ln\frac{\mu_n+\Lambda_n}{\mu_n-\Lambda_n}=0.)
To prove Theorem 5 it is enough to put (\mu=\mu_n,\ \lambda=\Lambda_n) in inequality (2) and take into account that (\displaystyle \lim_{\lambda\to\infty} E_\lambda(f)=0) (\bigl((^1),) pp. 371–372\bigr).
Theorem 6. The Fourier series (1) of the almost-periodic function (f(x)) converges uniformly if
[
\lim_{n\to\infty} E_{\Lambda_n}(f)\ln\frac{\Lambda_{n+1}+\Lambda_n}{\Lambda_{n+1}-\Lambda_n}=0.
]
Theorem 6 follows from Theorem 5 for (\mu_n=\Lambda_{n+1}).
Let us note a consequence of Theorem 6, which holds by virtue of the inequality
[
E_\lambda(f)\leq 2\pi\omega_f\left(\frac{1}{\lambda}\right),\qquad
\text{where }\ \omega_f(\delta)=\sup_{|x-y|\leq\delta}|f(x)-f(y)|
]
(\bigl((^1),) pp. 371–373\bigr).
Corollary. The Fourier series (1) of the almost-periodic function (f(x)) converges uniformly if
[
\lim_{n\to\infty}\omega_f\left(\frac{1}{\Lambda_n}\right)\ln\frac{\Lambda_{n+1}+\Lambda_n}{\Lambda_{n+1}-\Lambda_n}=0.
]
Theorem 6, which is a generalization of Bohr’s criterion (\bigl((^3),) pp. 81–83\bigr), makes it possible to use more fully the properties of the modulus of continuity of an almost-periodic function when investigating its Fourier series for uniform convergence.
It is easy to see that the condition of Theorem 6 ensuring uniform convergence, when the sequence (L(f)) of frequencies contains gaps whose lengths decrease arbitrarily rapidly, can be fulfilled only at the expense of a correspondingly rapid decrease of the best approximation of the almost-periodic function.
From the theorems given below it follows that this undesirable circumstance is caused not by the essence of the matter, but by the choice of the sequence ({\mu_n}) in Theorem 6.
Theorem 7. The Fourier series (1) of the almost-periodic function (f(x)) converges uniformly if there exists a function (\varphi(\lambda)\geq 0) for (\lambda>\lambda_0), satisfying the conditions:
1) (\displaystyle N_L\left(\Lambda_n+\frac{\Lambda_n}{e^{\varphi(\Lambda_n)}}\right)-N_L(\Lambda_n)=O[1+\varphi(\Lambda_n)];)
2) (\displaystyle \lim_{n\to\infty}\varphi(\Lambda_n)E_{\Lambda_n}(f)=0.)
Theorem 7 follows from Theorem 5 for
[
\mu_n=\Lambda_n+\frac{\Lambda_n}{e^{\varphi(\Lambda_n)}}.
]
Theorem 8. Suppose that the sequence (L(f)) has the following property: there are numbers (a>0,\ m\geq 0) such that
[
N_L\left(\Lambda_n+\frac{a}{\Lambda_n^m}\right)-N_L(\Lambda_n)=O(\ln\Lambda_n).
]
Then the Fourier series (1) of the almost-periodic function (f(x)) converges uniformly if (\displaystyle \lim_{\delta\to 0}\omega_f(\delta)\ln\delta=0.)
Theorem 8 follows from Theorem 7 for (\displaystyle \varphi(\lambda)=\ln\frac{\lambda^{m+1}}{a}).
Corollary. If (L(f)\in A_{\sigma}) and (\lim_{\delta\to 0}\omega_f(\delta)\ln\delta=0), then the Fourier series (1) of the almost-periodic function (f(x)) converges uniformly.
Theorem 8 is a generalization to the almost-periodic case of the Dini–Lipschitz criterion ((^{5,2})).
Theorem 9. If (L(f)\in Л_{\sigma}), then the Fourier series (1) of the almost-periodic function (f(x)) converges absolutely; moreover, if (A_0=0), then
[
\sum_{k=-\infty}^{\infty}|A_k|\leq C_L\sup_x |f(x)|,
]
where (C_L) is a constant depending only on the sequence (L(f)).
The proof of Theorem 9 is analogous to the proof of Theorem 1 of the author’s note ((^{6})). In the proof of Theorem 9, Theorem 1 of the paper ((^{4})) and the uniform convergence of the series (1), following from Theorem 7 for (\varphi(\lambda)=0), are used in an essential way.
- In conclusion we formulate a theorem generalizing the results of the author’s paper ((^{7})) concerning best approximations of almost-periodic functions representable by lacunary series.
Theorem 10. If (L(f)\in Л_{\sigma}), then the order equalities
[
E_{\lambda}(f)\sim R_{\lambda}(f)\sim \alpha_{\lambda}(f).
]
hold.
The proof of Theorem 10 is based on the application of Theorems 4 and 9 of the present note.
Kuibyshev Aviation
Institute
Received
28 V 1958
CITED LITERATURE
(^{1}) S. N. Bernstein, Collected Works, 2, 1954.
(^{2}) I. P. Natanson, Constructive Theory of Functions, Moscow–Leningrad, 1949.
(^{3}) B. M. Levitan, Almost-Periodic Functions, Moscow, 1953.
(^{4}) S. B. Stechkin, Izv. AN SSSR, Ser. Matem., 20, No. 3 (1956).
(^{5}) A. Zygmund, Trigonometric Series, Moscow–Leningrad, 1939.
(^{6}) E. A. Bredikhina, DAN, 111, No. 6 (1956).
(^{7}) E. A. Bredikhina, DAN, 117, No. 1 (1957).