Abstract Generated abstract
The paper addresses the problem of explicitly constructing, for an arbitrary fixed real number lambda greater than 1, a real number theta such that the fractional parts of theta lambda^x are uniformly distributed. Extending beyond earlier constructions for integer bases and known special noninteger cases, it defines exceptional sets associated with exponential sums, proves computable interval decompositions and measure bounds for them, and uses a Lebesgue-type effective selection procedure to choose nested decimal intervals avoiding their union. The resulting number theta_0 is shown not to belong to the exceptional set, and Weyl’s criterion then yields the uniform distribution of the sequence of fractional parts.
Full Text
Reports of the Academy of Sciences of the USSR
- Volume 143, No. 3
MATHEMATICS
M. F. KULIKOVA
A CONSTRUCTION PROBLEM CONNECTED WITH THE DISTRIBUTION OF THE FRACTIONAL PARTS OF AN EXPONENTIAL FUNCTION
(Presented by Academician I. M. Vinogradov, 17 XI 1961)
Let \(\lambda > 1\) be a fixed number. It is required to construct a real number \(\theta\) such that \(\{\theta \lambda^x\}\), \(x = 1, 2, \ldots\), are uniformly distributed. Many solutions of this problem are known in the case when \(\lambda = g\), \(g \geqslant 2\), is a given natural number. If \(\lambda\) is not equal to a natural number, then the problem has been investigated only for the case when \(\lambda\) is a Pisot number \((^1)\). In the present paper the problem is solved for the general case. It should be noted that the construction which we carry out is much more complicated than the constructions mentioned, although it is theoretically executable. We rely on Koksma’s theorem \((^2)\), which states that for almost all numbers \(\theta\) (in the sense of Lebesgue measure) from a finite interval \((\alpha\beta)\) the fractional parts \(\{\theta \lambda^x\}\) are uniformly distributed, and on Lebesgue’s principle \((^3)\), which makes it possible to render metric theorems effective. We shall construct the number \(\theta\) from the interval \(\{0, 1\}\).
Let \(h \ne 0\) be an integer and \(\nu\) a natural number. Denote by \(E_{(h,\nu)}\) the set of those \(\theta\) from the interval \(0 \leqslant \theta \leqslant 1\) for which
\[ \left| \frac{1}{\nu^2} \sum_{x=1}^{\nu^2} e^{2\pi i h \theta \lambda^x} \right| > \frac{1}{4\sqrt{\nu + 1}} . \]
The following lemmas are easily proved:
Lemma 1. The set \(E_{(h,\nu)}\) consists of a finite number of intervals. The coordinates of the endpoints of these intervals can be computed.
Denote these intervals by
\[ E_1^{(h,\nu)},\ E_2^{(h,\nu)},\ \ldots,\ E_{l(h,\nu)}^{(h,\nu)};\qquad E_{(h,\nu)}=\bigcup_{j=1}^{l(h,\nu)} E_j^{(h,\nu)} . \]
Lemma 2. The inequality holds
\[ \operatorname{mes} E_{(h,\nu)} < \sqrt{\nu+1}\left( \frac{1}{\nu^2} + \frac{1}{\lambda-1}\frac{\log 3\nu^2}{\nu^2} \right). \]
Since the series
\[ \sum_{\nu=1}^{\infty} \sqrt{\nu+1}\left( \frac{1}{\nu^2} + \frac{1}{\lambda-1}\frac{\log 3\nu^2}{\nu^2} \right) \]
converges, for a given integer \(h \ne 0\) we can find \(\nu_0(h)\) such that
\[ \sum_{\nu=\nu_0(h)}^{\infty} \sqrt{\nu+1}\left( \frac{1}{\nu^2} + \frac{1}{\lambda-1}\frac{\log 3\nu^2}{\nu^2} \right) < \frac{1}{4^{|h|}}; \qquad \mathfrak{R}^{(h)}_{\nu} = \bigcup_{j=\nu}^{\infty} E_{(j,h)} . \]
Since \(E_{(h,\nu)}\) is the sum of a finite number of intervals, the set \(\mathfrak{R}^{(h)}_{\nu}\) consists of no more than a countable number of nonintersecting intervals. This, in particular, also applies to \(\mathfrak{R}^{(h)}_{\nu_0(h)}\). For the measure of \(\mathfrak{R}^{(h)}_{\nu_0(h)}\) we have the estimate
\[ \operatorname{mes} \mathfrak{N}_{\nu_0(h)}^{(h)} \leq \sum_{\nu=\nu_0(h)}^{\infty} \sqrt{\nu+1} \left( \frac{1}{\nu^2} + \frac{1}{\lambda-1}\frac{\log 3\nu^2}{\nu^2} \right) < \frac{1}{4^{|h|}} . \]
Define the set \(\mathfrak{M}\) in the following way:
\[ \mathfrak{M} = \bigcup_{\substack{h=-\infty\\ h\ne 0}}^{\infty} \mathfrak{N}_{\nu_0(h)}^{(h)} . \]
The set \(\mathfrak{M}\) consists of a countable number of intervals. Denote them by
\(E_1, E_2, \ldots\). For the measure of \(\mathfrak{M}\) the estimate
\[ \operatorname{mes}\mathfrak{M} \leq 2 \sum_{h=1}^{\infty}\frac{1}{4^{(h)}} = \frac{2}{3} <1 \quad\text{(strictly!)}. \]
holds.
Let \(\alpha_j\) be the length of the interval \(E_j\). Denote
\[ S=\sum_{j=1}^{\infty}\alpha_j;\qquad S_P=\sum_{j=1}^{P}\alpha_j;\qquad r_P=S-S_P . \]
Consider the following 10 segments:
\[ [0,\,{}^{1}/_{10}],\ [^{1}/_{10},\,{}^{2}/_{10}],\ [^{2}/_{10},\,{}^{3}/_{10}],\ \ldots,\ [^{9}/_{10},\,1]. \]
Let \(p_1\) be some number. Take the first \(p_1\) terms of the system
\(E_1, E_2, \ldots, E_{p_1}\). Let
\(S_0^{(p_1)}, S_1^{(p_1)}, \ldots, S_9^{(p_1)}\) be the total lengths of the intersections of
\(E_1\cup E_2\cup\cdots\cup E_{p_1}\), respectively, with
\([0,{}^{1}/_{10}], [^{1}/_{10},{}^{2}/_{10}], \ldots, [^{9}/_{10},1]\). Then
\[ S_0^{(p_1)}+S_1^{(p_1)}+\cdots+S_9^{(p_1)}=S_{p_1}. \]
Hence
\[ (S_0^{(p_1)}+r_{p_1})+(S_1^{(p_1)}+r_{p_1})+\cdots+(S_9^{(p_1)}+r_{p_1}) = S_{p_1}+10r_{p_1} = S+9r_{p_1}. \]
Let \(p_1\) be chosen so large that \(S+9r_{p_1}<1\). Then there exists a segment
\[
\left[\frac{i}{10},\,\frac{i+1}{10}\right]
\]
for which
\[ S_i^{(p_1)}+r_{p_1} \leq \frac{S+9r_{p_1}}{10} < \frac{1}{10} \quad\text{(strictly!)}. \]
Take for \(i_1\) the smallest number \(0\leq i\leq 9\) such that this inequality is satisfied.
Divide the segment
\[
\left[\frac{i_1}{10},\,\frac{i_1+1}{10}\right]
\]
into 10 segments
\[
\left[\frac{i_1}{10},\,\frac{i_1}{10}+\frac{1}{100}\right],
\left[\frac{i_1}{10}+\frac{1}{100},\,\frac{i_1}{10}+\frac{2}{100}\right],
\ldots,
\left[\frac{i_1}{10}+\frac{9}{100},\,\frac{i_1+1}{10}\right].
\]
Choose a number \(p_2>p_1\) so large that the inequality
\[ S+9r_{p_1}+90r_{p_2}<1 \quad\text{(strictly!)} \]
will hold.
Let \(i\) be a number, \(0\leq i\leq 9\). Denote by \(S_{i_1 i}^{(p_2)}\) the length of the intersection of
\(E_1\cup E_2\cup\cdots\cup E_{p_2}\) with
\[
\left[\frac{i_1}{10}+\frac{i}{100},\,\frac{i_1}{10}+\frac{i+1}{100}\right].
\]
Then
\[ \sum_{i=0}^{9}\left(S_{i_1 i}^{(p_2)}+r_{p_2}\right) = \sum_{i=0}^{9}S_{i_1 i}^{(p_2)}+10r_{p_2} = S_{i_1}^{(p_2)}+10r_{p_2} = \]
\[ = S_{i_1}^{(p_1)}+r_{p_1}-r_{p_2}+10r_{p_2} = S_{i_1}^{(p_1)}+r_{p_1}+9r_{p_2} \leq \frac{1}{10}(S+9r_{p_1})+9r_{p_2} = \]
\[ = \frac{1}{10}\left(S+9r_{p_1}+90r_{p_2}\right) < 1 \quad\text{(strictly!)}. \]
There will be found such an index \(l_2\) that
\[ S^{(p_2)}_{i_1 i_2}+r_{p_2}\leqslant \frac{1}{100}\left(S+9r_{p_1}+90r_{p_2}\right)<\frac{1}{100} \quad \text{(strictly!)}. \]
Then we define an index \(p_3\) such that
\[ S+9r_{p_1}+90r_{p_2}+900r_{p_3}<1, \]
and an interval of length \(\frac{1}{1000}\) such that
\[ S^{(p_3)}_{i_1 i_2 i_3} < \frac{S+9r_{p_1}+90r_{p_2}+900r_{p_3}}{1000} < \frac{1}{1000}. \]
This process can be continued if the series
\[ S+9r_{p_1}+90r_{p_2}+900r_{p_3}+\cdots \]
converges and its sum is less than 1.
This can be done as follows. For \(p_1\) take the first number such that
\[ r_{p_1}<\frac{1-S}{2\cdot 9}; \]
for \(p_k\) take the first number such that
\[ r_{p_k}<\frac{1-S}{2^k\cdot 9\cdot 10^{k-1}}. \]
Then
\[ S+9r_{p_1}+90r_{p_2}+900r_{p_3}+\cdots \]
\[ < S+\frac{1-S}{1}+\frac{1-S}{2^2}+\cdots = S+(1-S)=1. \]
Define the number \(\theta_0\) by the equality
\[ \theta_0=\frac{i_1}{10}+\frac{i_2}{100}+\frac{i_3}{1000}+\cdots \]
It is obvious that the number \(\theta_0\) does not belong to \(\mathfrak M\).
It is easy to prove that for every integer \(h\ne 0\)
\[ \lim_{N\to\infty}\frac{1}{N}\sum_{x=1}^{N} e^{2\pi i h\theta_0\lambda^x}=0. \]
Hence, by Weyl’s criterion \((^4)\), it follows that the fractional parts \(\{\theta_0\lambda^x\}\) are uniformly distributed.
Chechen-Ingush State
Pedagogical Institute
Received
9 XI 1961
REFERENCES
\(^{1}\) N. M. Korobov, UMN, 6, no. 4, 151 (1951).
\(^{2}\) I. F. Koksma, Compositio Math., 2, 250 (1935).
\(^{3}\) H. Lebesgue, Bull. Soc. Math. de France, 45, 132 (1917).
\(^{4}\) H. Weyl, Math. Ann., 77, 313 (1961).