Approximation of unbounded functions by modified Landau and Bernstein polynomials on the entire plane
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Submitted 1963-01-01 | SovietRxiv: ru-196301.95844 | Translated from Russian

Abstract Generated abstract

This note studies approximation of unbounded twice continuously differentiable functions on the whole Euclidean plane by modified Landau polynomials and two forms of modified Bernstein polynomials. Under conditions on the scaling sequence and on the exponential growth of the function, it derives asymptotic expressions for the approximation errors in terms of second partial derivatives, including Laplacian-type formulas for Landau operators and corresponding quadratic-form formulas for Bernstein operators. The results are specialized to choices such as power scaling and logarithmic scaling, yielding explicit rates for functions with prescribed exponential growth, and the author notes that the arguments extend to higher-dimensional spaces.

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MATHEMATICS

Zh. Kh. Van

APPROXIMATION OF UNBOUNDED FUNCTIONS BY MODIFIED LANDAU AND BERNSTEIN POLYNOMIALS ON THE WHOLE PLANE

(Presented by Academician A. N. Kolmogorov on February 27, 1963)

  1. In the present note asymptotic formulas are given which express the order of approximation by modified Landau and Bernstein polynomials of continuous unbounded functions defined in a multidimensional Euclidean space. For simplicity of exposition we shall consider only the case of two variables. It is not difficult to see that the results of this note can be extended to a larger number of variables.

  2. We shall denote the whole plane by \(R_2\), points of \(R_2\) by
    \(t \equiv (t_1,t_2)\), \(x \equiv (x_1,x_2)\), and \(\|x\|=\sqrt{x_1^2+x_2^2}\). Let \(T(\|x\|)\) be a monotonically increasing function: \(T(\|x\|)\uparrow\infty\) \((\|x\|\to\infty)\).

We shall consider, on the whole plane, the modified Landau and Bernstein polynomials

\[ L_n[f(\alpha_n t);\alpha_n^{-1}x] = \frac{n}{\pi}\int_E f(\alpha_n t)\prod_{i=1}^{2}\left[1-(t_i-\alpha_n^{-1}x_i)^2\right]^n\,dt, \]

\[ L_n^{(s)}[f(\alpha_n t);\alpha_n^{-1}x] = \frac{1}{n^{2s-1}\pi} \sum_{|\nu_i|\le n^s} f\left(\frac{\nu_1\alpha_n}{n^s},\frac{\nu_2\alpha_n}{n^s}\right) \prod_{i=1}^{2} \left[1-\left(\frac{\nu_i}{n^s}-\frac{x_i}{\alpha_n}\right)^2\right]^n, \]

\[ B_n^{(1)}[f(\alpha_n t);\alpha_n^{-1}x] = \]

\[ = \sum_{\nu_1=0}^{n_1}\sum_{\nu_2=0}^{n_2} f\left(\frac{2\nu_1-n_1}{n_1}\alpha_n,\frac{2\nu_2-n_2}{n_2}\alpha_n\right) \prod_{i=1}^{2} \binom{n_i}{\nu_i} \frac{(1+\alpha_n^{-1}x_i)^{\nu_i}(1-\alpha_n^{-1}x_i)^{n_i-\nu_i}}{2^{n_i}}, \]

\[ B_n^{(2)}[f(\alpha_n t);\alpha_n^{-1}x] = \sum_{0\le \nu_1+\nu_2\le n} f\left(\left(\frac{2\nu_1}{n}-\frac12\right)\alpha_n, \left(\frac{2\nu_2}{n}-\frac12\right)\alpha_n\right) p_{\nu_1,\nu_2;n}(x), \]

where \(\alpha_n\uparrow\infty\), \(s\ge 1\), \(n_1+n_2=n\), \(E\) is the square
\(-1\le x_1\le 1\), \(-1\le x_2\le 1\), and

\[ p_{\nu_1,\nu_2;n}(x) = \binom{n}{\nu_1,\nu_2} \frac{(1/2+\alpha_n^{-1}x_1)^{\nu_1}(1/2+\alpha_n^{-1}x_2)^{\nu_2} (1-\alpha_n^{-1}x_1-\alpha_n^{-1}x_2)^{n-\nu_1-\nu_2}}{2^n}, \]

\[ \binom{n}{\nu_1,\nu_2} = \frac{n!}{\nu_1!\nu_2!(n-\nu_1-\nu_2)!}. \]

Introduce the notation:
\(\Delta_n(\alpha_n)=L_n-f\), \(\Delta_n^{(s)}(\alpha_n)=L_n^{(s)}-f\),
\(\delta_n^{(1)}(\alpha_n)=B_n^{(1)}-f\), and
\(\delta_n^{(2)}(\alpha_n)=B_n^{(2)}-f\).

Theorem 1. Let \(\alpha_n\uparrow\infty\), \(\beta_n\downarrow 0\) \((n\to\infty)\), and

\[ 1^\circ.\quad \alpha_n\beta_n\to 0,\qquad n\beta_n^4\to 0\quad (n\to\infty). \]

\[ 2^\circ.\quad \left(\frac{n}{\alpha_n}\right)^2 \exp\{T(\sqrt{2}\alpha_n)-2n\beta_n^2\}\to 0 \quad (n\to\infty). \]

Then for every function \(f(x)\in C^{2}(R_{2})\), \(f(x)=O(e^{T(\|x\|)})\) \((\|x\|\to\infty)\), the asymptotic equality

\[ \Delta_n(\alpha_n)\sim \frac{\alpha_n^2}{4n}\left(\frac{\partial^2 f}{\partial x_1^2}+\frac{\partial^2 f}{\partial x_2^2}\right)\qquad (n\to\infty) \tag{1} \]

holds.

Theorem 2. Let \(s\ge 3/2\). Under the same assumptions as in Theorem 1, we have

\[ \Delta_n^{(s)}(\alpha_n)\sim \frac{\alpha_n^2}{4n}\left(\frac{\partial^2 f}{\partial x_1^2}+\frac{\partial^2 f}{\partial x_2^2}\right)\qquad (n\to\infty). \tag{2} \]

In particular, if we take \(\alpha_n=n^\theta\left(0<\theta<\frac{1}{m+2}\right)\), \(T(\|x\|)=\|x\|^m\), and choose \(\beta_n=n^{-\theta-\delta}\), where \(\delta\) satisfies the conditions

\[ \max(0,\,1/4-\theta)<\delta<1/2[1-(m+2)\theta], \]

then from Theorem 1 we obtain the following result.

Theorem 3. For every function \(f(x)\in C^{2}(R_{2})\), \(f(x)=O(e^{\|x\|^m})\) \((\|x\|\to\infty)\), the asymptotic equality

\[ \Delta_n(n^\theta)\sim \frac{1}{4}\left(\frac{\partial^2 f}{\partial x_1^2}+\frac{\partial^2 f}{\partial x_2^2}\right)\left(\frac{1}{n}\right)^{1-2\theta}\qquad (n\to\infty). \tag{3} \]

If we take \(\alpha_n=\log\log n\), then for a broader class of unbounded functions we obtain (choosing \(\beta_n=\dfrac{1}{n^{1/4}\sqrt{\log n}}\)) the following theorem.

Theorem 4. For every function \(f\in C^{2}(R_{2})\), \(f(x)=O(e^{\|x\|})\) \((\|x\|\to\infty)\), we have

\[ \Delta_n(\log\log n)\sim \frac{(\log\log n)^2}{4n}\left(\frac{\partial^2 f}{\partial x_1^2}+\frac{\partial^2 f}{\partial x_2^2}\right)\qquad (n\to\infty). \tag{4} \]

If \(s\ge 3/2\), then for the polynomials \(L_n^{(s)}\) asymptotic formulas analogous to formulas (3) and (4) are valid. We shall not give them here.

Theorem 5. Let \(\alpha_n\uparrow\infty\), \(\beta_n\downarrow 0\) \((n\to\infty)\), and as \(n\to\infty\):

\(1^\circ.\ \alpha_n\beta_n\to 0.\)

\(2^\circ.\ n\exp\{T(\sqrt{2}\alpha_n)-1/3\,n\beta_n^2\}\to 0.\)

Then for every \(f(x)\in C^{2}(R_{2})\), \(f(x)=O(e^{T(\|x\|)})\) \((\|x\|\to\infty)\), as \(n\to\infty\) the asymptotic equality

\[ \delta_n^{(2)}(\alpha_n)\sim \frac{\alpha_n^2}{2n}\left\{\left[\frac{1}{4}-\left(\frac{x_1}{\alpha_n}\right)^2\right]\frac{\partial^2 f}{\partial x_1^2} -2\left(\frac{1}{2}+\frac{x_1}{\alpha_n}\right)\left(\frac{1}{2}+\frac{x_2}{\alpha_n}\right)\frac{\partial^2 f}{\partial x_1\partial x_2} +\left[\frac{1}{4}-\left(\frac{x_2}{\alpha_n}\right)^2\right]\frac{\partial^2 f}{\partial x_2^2}\right\}. \tag{5} \]

Theorem 6. Let \(\alpha_n\uparrow\infty\), \(\beta_n\downarrow 0\) \((n\to\infty)\), and as \(n_i\to\infty\) \((i=1,2)\):

\(1^\circ.\ \alpha_n\beta_n\to 0.\)

\(2^\circ.\ n\exp\{T(\sqrt{2}\alpha_n)-1/n_i\beta_n^2\}\to 0.\)

Then for every function \(f(x)\in C^{2}(R_{2})\), \(f(x)=O(e^{T(\|x\|)})\) \((\|x\|\to\infty)\), as \(n\to\infty\) the asymptotic formula

\[ \delta_n^{(1)}(\alpha_n)\sim \frac{\alpha_n^2}{2n_1}(1-\alpha_n^{-2}x_1^2)\frac{\partial^2 f}{\partial x_1^2} + \frac{\alpha_n^2}{2n_2}(1-\alpha_n^{-2}x_2^2)\frac{\partial^2 f}{\partial x_2^2} + \frac{\varepsilon_1\alpha_n^2}{n_1} + \frac{\varepsilon_2\alpha_n^2}{n_2}, \tag{6} \]

where \(\varepsilon_1\to 0\) as \(n_1\to\infty\) and \(\varepsilon_2\to 0\) as \(n_2\to\infty\).

From Theorem 5 there follow, in particular, the following results.

Theorem 7. For any function \(f(x)\in C^2(R_2)\), \(f(x)=O\!\left(e^{\|x\|^m}\right)\) as \(\|x\|\to\infty\), as \(n\to\infty\) we have

\[ \delta_n^{(2)}(n^\theta)\sim \frac12\left\{ \left[\frac14-\left(\frac{x_1}{n^\theta}\right)^2\right]\frac{\partial^2 f}{\partial x_1^2} -2\left(\frac12+\frac{x_1}{n^\theta}\right) \left(\frac12+\frac{x_2}{n^\theta}\right) \frac{\partial^2 f}{\partial x_1\partial x_2} +\left[\frac14-\left(\frac{x_2}{n^\theta}\right)^2\right]\frac{\partial^2 f}{\partial x_2^2} \right\} \left(\frac1n\right)^{1-2\theta}. \tag{7} \]

Theorem 8. For any function \(f(x)\in C^2(R_2)\), \(f(x)=O\!\left(e^{\|x\|^{\|x\|}}\right)\) as \(\|x\|\to\infty\), as \(n\to\infty\) we have

\[ \delta_n^{(2)}(\log\log n)\sim \frac{(\log\log n)^2}{2n} \left\{ \left[\frac14-\left(\frac{x_1}{\log\log n}\right)^2\right]\frac{\partial^2 f}{\partial x_1^2} -2\left(\frac12+\frac{x_1}{\log\log n}\right) \left(\frac12+\frac{x_2}{\log\log n}\right) \frac{\partial^2 f}{\partial x_1\partial x_2} +\left[\frac14-\left(\frac{x_2}{\log\log n}\right)^2\right]\frac{\partial^2 f}{\partial x_2^2} \right\}. \tag{8} \]

For the proof of Theorems 7 and 8, in Theorem 5 we put, respectively,

\[ \beta_n=n^{-\theta-\delta},\qquad \max(0,\;{}^{1}/_{4}-\theta)<\delta<{}^{1}/_{2}\,[1-(m+2)\theta] \quad\text{and}\quad R=\frac{1}{n^{1/4}\sqrt{\log n}}. \]

From Theorem 6 one can obtain analogous results for Bernstein polynomials of the first type.

Tirin University
Changchun, China

Received
28 XII 1962

CITED LITERATURE

\(^{1}\) D. D. Stancu, Com. Acad. R. P. R., 9, No. 8, 773 (1959).
\(^{2}\) J. Albrycht, J. Radecki, Zesz. Nauk. Uniw. Poznanin., No. 25, 3 (1960).
\(^{3}\) G. G. Lorentz, Bernstein Polynomials, Toronto, 1953.

Submission history

Approximation of unbounded functions by modified Landau and Bernstein polynomials on the entire plane