MATHEMATICS
M. F. TIMAN
Submitted 1962-01-01 | RussiaRxiv: ru-196201.33316 | Translated from Russian

Abstract

Full Text

MATHEMATICS

M. F. TIMAN

SOME LINEAR PROCESSES OF SUMMATION OF FOURIER SERIES AND BEST APPROXIMATION

(Presented by Academician V. I. Smirnov, March 15, 1962)

  1. Consider the space (L_p) ((1 \leq p \leq \infty)) of all measurable periodic functions of period (2\pi), for which, when (1 \leq p < \infty),

[
|f(x)|_{L_p}
=
\left{\int_0^{2\pi} |f(x)|^p\,dx\right}^{1/p}
<\infty,
]

and, when (p=\infty),

[
|f(x)|{L\infty}
=
\operatorname{vrai\,sup}_{0\leq x\leq 2\pi}|f(x)|<\infty.
]

Let ({\lambda_k^{(n)}}) ((k=0,1,2,\ldots,n;\ n=1,2,\ldots;\ \lambda_0^{(n)}=1;\ \lambda_{n+1}^{(n)}=0)) be an arbitrary triangular matrix of numbers, and

[
U_n(f;x;\lambda)
=
\frac{a_0}{2}
+
\sum_{k=1}^{n}\lambda_k^{(n)}
\bigl(a_k\cos kx+b_k\sin kx\bigr),
]

where (a_k, b_k) are the Fourier coefficients of the function (f(x)). Denote

[
R_n(f;\lambda){L_p}
=
|f(x)-U_n(f;x;\lambda)|
.
]

Theorem 1. If (f(x)\in L_p) ((1\leq p\leq \infty)), then for any matrix ({\lambda_k^{(n)}}) the inequality

[
R_n(f;\lambda){L_p}
\leq
C\left{
\sum
}^{n
\left|\lambda_k^{(n)}-2\lambda_{k+1}^{(n)}+\lambda_{k+2}^{(n)}\right|
(n-k+1)E_k(f){L_p}
\times
\right.
]
[
\left.
{}\times
\sum
}^{n}\frac{1}{\nu+1
+
\left|1-\lambda_1^{(n)}\right|
\sum_{\nu=0}^{n}E_\nu(f)_{L_p}
\right},
\tag{1}
]

where

[
E_n(f){L_p}
=
\inf

\left|
f(x)-
\sum_{k=0}^{n}(\alpha_k\cos kx+\beta_k\sin kx)
\right|_{L_p}
\qquad (1\leq p\leq \infty),
]

and (C) is an absolute constant. Moreover, in the case (1<p<\infty),

[
R_n(f;\lambda){L_p}
\leq
C_p
\sum
}^{n
\left|\lambda_k^{(n)}-\lambda_{k+1}^{(n)}\right|
E_k(f)_{L_p}.
\tag{2}
]

Inequality (1) for (p=\infty) and (p=1) may be regarded as a generalization of Lebesgue’s inequality

[
|f(x)-S_n(f;x)|{L_p}
\leq
C E_n(f)
\ln n
\qquad
(p=1,\ p=\infty;\ n>1),
]

which corresponds to the case (\lambda_k^{(n)}=1) ((k=0,1,\ldots,n)), while inequality (2) is a generalization of the well-known inequality

[
|f(x)-S_n(f;x)|{L_p}
\leq
C_p E_n(f)

\qquad
(1<p<\infty),
]

where (S_n(f;x)) is the partial sum of the Fourier series of the function (f(x)).

  1. Inequality (1) contains various estimates for particular methods of summation of Fourier series. We shall consider some of them here.

Normal Zygmund means. Let

[
\lambda_k^{(n)}=1-\left(\frac{k}{n+1}\right)^r
\quad (k=0,1,2,\ldots,n;\ r\geqslant 1).
\tag{3}
]

Theorem 2. For the matrix (3), for any (r\geqslant 1), the inequality

[
R_n(f;\lambda){L_p}\leqslant \frac{C}{n^r}
\sum
}^{n}\nu^{r-1}E_{\nu-1}(f)_{L_p
\quad (1\leqslant p\leqslant \infty),
\tag{4}
]

holds, where (C) is an absolute constant(^*).

In particular, for (r=1), for Fejér sums the inequality

[
R_n(f;\lambda){L_p}\leqslant \frac{C}{n}
\sum
}^{n}E_k(f)_{L_p
\quad (1\leqslant p\leqslant \infty).
\tag{5}
]

holds.

The last estimate can be obtained directly from the integral representation for Fejér sums(^ {**}). Indeed, by monotonicity of

[
\omega_2(f;t){L_p}=\sup,}|f(x+h)-2f(x)+f(x-h)|_{L_p
]

[
\left|f(x)-\frac{1}{n}\sum_{\nu=0}^{n-1}S_\nu(f;x)\right|{L_p}
\leqslant
C_1\left{\omega_2\left(f;\frac{1}{n}\right)

+\frac{1}{n}\int_{\pi/n}^{\pi}\frac{\omega_2(f;t)_{L_p}}{t^2}\,dt\right}
\leqslant
]

[
\leqslant
C_2\frac{1}{n}\int_{\pi/n}^{\pi}\frac{\omega_2(f;t){L_p}}{t^2}\,dt
=
\frac{C_2}{n}\sum
}^{n-1
\int_{\pi/(\nu+1)}^{\pi/\nu}
\frac{\omega_2(f;t)_{L_p}}{t^2}\,dt.
]

It remains to take into account that (see (3), p. 344)

[
\omega_2\left(f;\frac{1}{n}\right){L_p}
\leqslant
\frac{M}{n^2}\sum
}^{n}kE_{k-1}(f)_{L_p
\quad (1\leqslant p\leqslant \infty).
]

Bernstein–Rogozinskii sums and Jackson–Vallée-Poussin sums. Let

[
\lambda_k^{(n)}=\cos \frac{k\pi}{2n+1}
\quad (k=0,1,\ldots,n);
\tag{6}
]

[
\lambda_k^{(2n)}=
\begin{cases}
1-\dfrac{3}{2}\left(\dfrac{k}{n}\right)^2+\dfrac{3}{4}\left(\dfrac{k}{n}\right)^3,
& (0\leqslant k\leqslant n),\[6pt]
\dfrac{1}{4}\left(2-\dfrac{k}{n}\right)^3,
& (n\leqslant k\leqslant 2n),\[6pt]
0,
& (k>2n).
\end{cases}
\tag{7}
]

Theorem 3. For the matrices (6) and (7) the inequality

[
R_n(f;\lambda){L_p}\leqslant
\frac{C}{n^2}\sum
}^{n}\nu E_{\nu-1}(f)_{L_p
\quad (1\leqslant p\leqslant \infty),
\tag{8}
]

holds, where (C) is an absolute constant.

(\ ^*) Theorem 2 was reported by the author on 12 X 1961 at the seminar of the Department of Higher Mathematics of the Dnepropetrovsk Agricultural Institute. We note that the means appearing on the right-hand side of inequality (4) play an important role in inverse theorems of constructive function theory (see (3), Chs. 6 and 7) and, as far as we know, were first introduced in paper (1) (see (1), Theorem 4).

(\ ^{**}) Estimate (5) was obtained by another method by S. B. Stechkin (5).

  1. There exist examples showing that, in the general case, for (p=\infty) and (p=1) the estimates given in Theorems 2 and 3 cannot be improved in order.

At the same time, using the methods applied by the author earlier in papers ((^{2,4})), one can show that in a number of cases these estimates are crude even in order, if (1

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MATHEMATICS