Abstract Generated abstract
This note refines an asymptotic expansion in the central limit theorem for sums of independent identically distributed random variables with finite moment of integer order k at least 3 and a nonlattice type characteristic function condition. It proves a uniform weighted remainder estimate for the difference between the normalized distribution function and its Edgeworth expansion, improving Esseen’s uniform little-o remainder by a factor depending on 1 plus the kth power of the argument. The result yields consequences for global integral forms of limit theorems, including asymptotic estimates in Lp norms for the approximation error and for the distance between the normalized distribution function and the normal law.
Full Text
UDC 519.21
MATHEMATICS
L. V. OSIPOV
ON AN ASYMPTOTIC EXPANSION IN THE CENTRAL LIMIT THEOREM
(Presented by Academician Yu. V. Linnik on 16 IX 1965)
Let \(X_1, X_2,\ldots\) be a sequence of mutually independent identically distributed random variables with mathematical expectation \(m=EX_1\) and positive variance \(\sigma^2=E(X_1-m)^2\). Introduce the notation
\[ F_n(x)=P\left\{\frac{1}{\sigma\sqrt n}\sum_{j=1}^n (X_j-m)<x\right\},\quad \Phi(x)=\frac{1}{\sqrt{2\pi}}\int_{-\infty}^{x} e^{-t^2/2}\,dt. \]
Theorem. Suppose that the following conditions are satisfied:
1) \(E|X_1|^k<\infty\) for some integer \(k\geq 3\);
2) \[ \lim_{|t|\to\infty}\left|Ee^{itX_1}\right|<1. \]
Then there exists a function \(\varepsilon(n)\), independent of \(x\), such that
\[
\lim_{n\to\infty}\varepsilon(n)=0
\]
and
\[ \left|F_n(x)-\Phi(x)-\sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}}\right| \leq \frac{\varepsilon(n)}{(1+|x|^k)n^{(k-2)/2}} \]
for all \(x\) \((-\infty<x<\infty)\). The functions \(P_\nu(-\Phi)\) are defined in the same way as in \((^{1,4})\).
This theorem is a refinement of a theorem of Esseen \((^{1,2})\), according to which, under the conditions of the theorem formulated above, the relation
\[ F_n(x)-\Phi(x)-\sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}} = o\left(\frac{1}{n^{(k-2)/2}}\right) \]
holds as \(n\to\infty\), uniformly with respect to \(x\) \((-\infty<x<\infty)\).
V. V. Petrov \((^3)\) earlier found conditions necessary and sufficient for the validity of the relation
\[ \left| \frac{d}{dx}\left(F_n(x)-\Phi(x)-\sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}}\right) \right| \leq \frac{\varepsilon(n)}{(1+|x|^k)n^{(k-2)/2}} \]
for all \(x\) \((-\infty<x<\infty)\), where \(\varepsilon(n)\) does not depend on \(x\) and
\[
\lim_{n\to\infty}\varepsilon(n)=0.
\]
From the theorem stated above there follows directly a series of consequences concerning the global form of integral limit theorems.
Under the conditions of the theorem, the following assertions are valid:
- For any \(p>1/k\), as \(n\to\infty\) we have
\[ \int_{-\infty}^{\infty} \left| F_n(x)-\Phi(x)-\sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}} \right|^p dx = o\left(\frac{1}{n^{(k-2)p/2}}\right). \]
- For any \(p \geqslant 1\), as \(n \to \infty\) we have
\[ \int_{-\infty}^{\infty} |F_n(x)-\Phi(x)|^p dx = \int_{-\infty}^{\infty} \left| \sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}} \right|^p dx + o\!\left(\frac{1}{n^{(k+p-3)/2}}\right). \]
- For any \(p \geqslant 1\), as \(n \to \infty\) we have
\[ \|F_n(x)-\Phi(x)\| = \left\| \sum_{\nu=1}^{k-2}\frac{P_\nu(-\Phi)}{n^{\nu/2}} \right\| + o\!\left(\frac{1}{n^{(k-2)/2}}\right). \]
Here
\[ \|u(x)\|=\left[\int_{-\infty}^{\infty}|u(x)|^p dx\right]^{1/p} \]
for any function \(u(x)\in L_p(-\infty,\infty)\).
Leningrad State University
named after A. A. Zhdanov
Received
7 IX 1965
REFERENCES
- B. V. Gnedenko, A. N. Kolmogorov, Limit Distributions for Sums of Independent Random Variables, 1949.
- G.-G. Esseen, Acta Math., 77, 1 (1945).
- V. V. Petrov, Theory of Probability and Its Applications, 9, 343 (1964).
- V. V. Petrov, Vestnik Leningrad Univ., No. 19, 150 (1962).