UDC 517.512.7
MATHEMATICS
Submitted 1966-01-01 | RussiaRxiv: ru-196601.09256 | Translated from Russian

Abstract

Full Text

UDC 517.512.7

MATHEMATICS

S. Z. RAFALSON

ON AN ASYMPTOTIC FORMULA IN THE THEORY OF ORTHOGONAL POLYNOMIALS

(Presented by Academician S. N. Bernstein on 8 II 1966)

1. It is known that the derivatives of the orthogonal Jacobi polynomials are again orthogonal Jacobi polynomials, but with different indices. Namely, the equality holds

[
dJ_n^{(\alpha,\beta)}(x)/dx
=
\sqrt{n(n+\alpha+\beta+1)}\,J_{n-1}^{(\alpha+1,\beta+1)}(x),
\qquad n \geqslant 1
\tag{1}
]

(here (J_m^{(\alpha,\beta)}(x)) is the normalized Jacobi polynomial of degree (m) with indices (\alpha) and (\beta)).

It is of interest to determine how equality (1) changes if, instead of the weight ((1-x)^\alpha(1+x)^\beta), one considers the more general weight (q(x)(1-x)^\alpha(1+x)^\beta), where the function (q(x)) satisfies certain conditions. We shall show that in this case equality (1) is replaced by an asymptotic equality.

Theorem 1. Let ({\omega_n(x)}_0^\infty) be a system of polynomials orthonormal with weight
(p(x)=(1-x)^\alpha(1+x)^\beta q(x)), where (\alpha,\beta \geqslant -1/2), and let the function (q(x)) satisfy the following conditions: 1) (q(x)\geqslant m>0), (x\in[-1,1]); 2) (q(x)\in \operatorname{Lip} 1). Let ({\varphi_n(x)}_0^\infty) be a system of polynomials orthonormal with weight ((1-x^2)p(x)).

The asymptotic formula is valid

[
\omega_n'(x)=a_n\varphi_{n-1}(x)+O(\ln n),
\tag{2}
]

where (a_n\asymp n), and the constant occurring in (O(\ln n)) does not depend on (x\in[-1+h,\,1-h]), (0<h<1).

On the entire interval ([-1,1]) the asymptotic equality holds

[
\omega_n'(x)=a_n\varphi_{n-1}(x)+O(n^{\sigma+3/2}\ln n),
\tag{3}
]

where (\sigma=\max{\alpha,\beta}); the constant occurring in (O(n^{\sigma+3/2}\ln n)) does not depend on (x\in[-1,1]).

Proof. We first prove equality (2). Represent (\omega_n'(x)) in the form of a linear combination of the polynomials ({\varphi_k(x)}_0^{n-1}):

[
\omega_n'(x)=a_n\varphi_{n-1}(x)+\sum_{k=0}^{n-2} c_k\varphi_k(x).
\tag{4}
]

It is easy to obtain the following expression for (c_k):

[
c_k
=
-\int_{-1}^{1}
(1-t)^{\alpha+1}(1+t)^{\beta+1}q'(t)\omega_n(t)\varphi_k(t)\,dt,
\qquad 0\leqslant k\leqslant n-2.
\tag{5}
]

The sum (\displaystyle \sum_{k=0}^{n-2} c_k\varphi_k(x)), with the aid of the expressions obtained for (c_k), is rep—

takes the form

[
I=\sum_{k=0}^{n-2} c_k\varphi_k(x)
= -\int_{-1}^{1} (1-t)^{\alpha+1}(1+t)^{\beta+1}q'(t)\omega_n(t)
\sum_{k=0}^{n-2}\varphi_k(t)\varphi_k(x)\,dt.
\tag{6}
]

Applying the Christoffel–Darboux formula and taking into account that almost everywhere (q'(t)=O(1)), we obtain:

[
|I|=O(1)\int_{-1}^{1}(1-t)^{\alpha+1}(1+t)^{\beta+1}|\omega_n(t)|
\left|\frac{\varphi_{n-2}(x)\varphi_{n-1}(t)-\varphi_{n-2}(t)\varphi_{n-1}(x)}{t-x}\right|\,dt.
\tag{7}
]

We split the integral on the right-hand side of equality (7) into three integrals according to the scheme

[
\int_{-1}^{1}
=
\int_{-1}^{x-1/n}
+
\int_{x-1/n}^{x+1/n}
+
\int_{x+1/n}^{1}
=I_1+I_2+I_3.
]

Let us first estimate the integrals (I_1) and (I_3). Applying Korous’s theorem (see ((^3)), p. 169), we obtain:

[
\begin{aligned}
I_1={}&
\int_{-1}^{x-1/n}
(1-t)^{\alpha+1}(1+t)^{\beta+1}
\bigl[O(1)|J_n^{(\alpha,\beta)}(t)|+O(1)|J_{n-1}^{(\alpha,\beta)}(t)|\bigr]|t-x|^{-1}
\
&\times
\Bigl{|\varphi_{n-2}(x)|
\bigl[O(1)|J_{n-1}^{(\alpha+1,\beta+1)}(t)|
+O(1)|J_{n-2}^{(\alpha+1,\beta+1)}(t)|\bigr]
\
&\quad
+|\varphi_{n-1}(x)|
\bigl[O(1)|J_{n-2}^{(\alpha+1,\beta+1)}(t)|
+O(1)|J_{n-3}^{(\alpha+1,\beta+1)}(t)|\bigr]\Bigr}\,dt.
\end{aligned}
\tag{8}
]

It is enough to estimate one of the integrals entering the right-hand side of (8), for example the first of them, since the remaining integrals are estimated analogously. For this, note, first, that for (-1+h\le x\le 1-h), (0<h<1), the equality (J_m^{(\alpha+1,\beta+1)}(x)=O(1)) holds (see ((^3)), pp. 80 and 204), whence

[
\varphi_m(x)=O(1),\qquad -1+h\le x\le 1-h,\qquad 0<h<1,
\tag{9}
]

and, secondly, we use the relations

[
\begin{gathered}
(1-t)^{\alpha/2+1/4}(1+t)^{\beta/2+1/4}
|J_m^{(\alpha,\beta)}(t)|=O(1),\
(1-t)^{\alpha/2+3/4}(1+t)^{\beta/2+3/4}
|J_m^{(\alpha+1,\beta+1)}(t)|=O(1),
\end{gathered}
\tag{10}
]

which are valid since (\alpha,\beta\ge -1/2) (see ((^2)), pp. 57, 69, 70; see also ((^3)), p. 177). Then we obtain

[
\int_{-1}^{x-1/n}
(1-t)^{\alpha+1}(1+t)^{\beta+1}
\frac{|J_n^{(\alpha,\beta)}(t)|\,|\varphi_{n-2}(x)|\,|J_{n-1}^{(\alpha+1,\beta+1)}(t)|}{|t-x|}\,dt
=
]

[
=O(1)\int_{-1}^{x-1/n}\frac{dt}{|t-x|}
=O(\ln n).
\tag{11}
]

Thus, (I_1=O(\ln n)). It is proved analogously that (I_3=O(\ln n)).

Consider (I_2). With the aid of Korous’s theorem and equalities (9) and (10), it is not difficult to obtain that (I_2=O(1)). Thus, (I=O(\ln n)).

Denoting by (\beta_{n,0}) the leading coefficient of the polynomial (\omega_n(x)) ((\beta_{n,0}>0)), and by (\gamma_{n-1,0}) the leading coefficient of the polynomial (\varphi_{n-1}(x)) ((\gamma_{n-1,0}>0)), from equality (4) we have

[
a_n=n\beta_{n,0}/\gamma_{n-1,0}.
\tag{12}
]

Under the conditions of the theorem the following equalities hold

[
\beta_{n,0} \simeq \pi^{-1/2}\cdot 2^n \exp\left{-\frac{1}{2\pi}\int_{-1}^{1}\ln p(x)\frac{dx}{\sqrt{1-x^2}}\right},
\tag{13}
]

[
\gamma_{n-1,0} \simeq \pi^{-1/2}\cdot 2^{n-1}\exp\left{-\frac{1}{2\pi}\int_{-1}^{1}\ln\bigl[p(x)(1-x^2)\bigr]\frac{dx}{\sqrt{1-x^2}}\right}
\tag{14}
]

(see (³), p. 317).

From equalities (12), (13), and (14) it follows easily that (\alpha_n \simeq n). Equality (2) is proved. Equality (3) is proved similarly; one need only take into account the equality (|J_n^{(\alpha+1,\beta+1)}(x)|_{C([-1,1])}=O(n^{\sigma+3/2})).

Corollary. The following equalities hold

[
\omega_n^{(k)}(x)=\gamma_n^{(k)}\delta_{n-k}(x)+O(n^{k-1}\ln n)
\tag{15}
]

(here (-1+h\le x\le 1-h,\ 0<h<1); the constant entering into (O(n^{k-1}\ln n)) does not depend on (x\in[-1+h,1-h]); (\gamma_n^{(k)}\simeq n^k); (\delta_{n-k}(x)) is a polynomial of degree (n-k) from the sequence of polynomials orthonormal with weight (p(x)(1-x^2)^k));

[
\omega_n^{(k)}(x)=\gamma_n^{(k)}\delta_{n-k}(x)+O(n^{\sigma+3/2+2(k-1)}\ln n)
\tag{16}
]

(here (-1\le x\le 1); the constant entering into (O(n^{\sigma+3/2+2(k-1)}\ln n)) does not depend on (x\in[-1,1])).

  1. For a system of polynomials ({\omega_k(x)}) satisfying the conditions of Theorem 1, the following holds.

Theorem 2. If

[
\sum_{k=1}^{\infty} c_k^2 k^{2j}\ln^2 k<\infty,
]

then the series

[
\sum_{k=1}^{\infty} c_k\omega_k^{(j)}(x)
]

converges almost everywhere on the interval ([-1,1]), (j=1,2,\ldots).

Corollary 1. If

[
\sum_{k=1}^{\infty} c_k^2<\infty,
]

then almost everywhere on the interval ([-1,1]) the equality

[
s_n(x)=\sum_{k=1}^{n}c_k\omega_k'(x)=o_x(n\ln n)
]

holds.

Corollary 2. If (\lambda_n\uparrow\infty), then from the condition

[
\sum_{n=1}^{\infty}\left[c_n^2\Big/\lambda_n\sum_{k=1}^{n}c_k^2\right]<\infty
]

it follows that almost everywhere on the interval ([-1,1])

[
s_n(x)=o_x\left[\left(\lambda_n(\ln n)^2n^2\sum_{k=1}^{n}c_k^2\right)^{1/2}\right].
]

  1. Definition. A system of functions ({A_n(x)}_1^\infty) will be called quasi-orthonormal with weight (r(x)) on the interval ([a,b]) if, for any real numbers (c_1,c_2,\ldots,c_n), the equality

[
\int_a^b r(x)\left[\sum_{k=1}^{n}c_kA_k(x)\right]^2dx
=
O(1)\sum_{k=1}^{n}c_k^2,
]

holds, where (O(1)) depends neither on (n) nor on the numbers (c_1,c_2,\ldots,c_n).

It is clear that a system of functions orthonormal with weight (r(x)) on ([a,b]) is quasi-orthonormal. It is also easy to see that if ({A_n(x)}_1^\infty) —

orthonormal with weight (r(x)) on ([a,b]), then the system of functions

[
\left{\sum_{k=0}^{j}\alpha_n^{(k)} A_{n-k}(x)\right}_{n=j+1}^{\infty},
]

where (\alpha_n^{(0)}=O(1),\ \alpha_n^{(1)}=O(1),\ldots,\alpha_n^{(j)}=O(1)), is a quasi-orthonormal system of functions with weight (r(x)) on the interval ([a,b]).

Theorem 3. Let ({\omega_n(x)}_{0}^{\infty}) be a system of polynomials satisfying the conditions of Theorem 1, and let the constants (\alpha_k) ((k=1,2,\ldots)) be taken from equality (2).

The system of polynomials ({\omega_n'(x)/\alpha_n}_{1}^{\infty}) is quasi-orthonormal with weight (p(x)(1-x^2)) on the interval ([-1+h,1-h]), (0<h<1).

For quasi-orthonormal systems the Menshov–Rademacher theorem, the theorem on the equivalence of (A)-summability and ((C,\gamma))-summability, (\gamma>0), etc., are valid.

I express my deep gratitude to Prof. V. S. Videnskii for his help in preparing the article for publication.

Leningrad Financial-Economic Institute
named after N. A. Voznesensky

Received
3 II 1966

REFERENCES

  1. G. Aleksich, Problems of Convergence of Orthogonal Series, IL, 1963.
  2. S. N. Bernstein, Collected Works, 2, 1954.
  3. G. Szegő, Orthogonal Polynomials, Moscow, 1962.

Submission history

UDC 517.512.7