diff --git "a/INE5T4oBgHgl3EQfWw9u/content/tmp_files/2301.05561v1.pdf.txt" "b/INE5T4oBgHgl3EQfWw9u/content/tmp_files/2301.05561v1.pdf.txt" new file mode 100644--- /dev/null +++ "b/INE5T4oBgHgl3EQfWw9u/content/tmp_files/2301.05561v1.pdf.txt" @@ -0,0 +1,3668 @@ +arXiv:2301.05561v1 [math.NT] 13 Jan 2023 +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND +NUMBER THEORY +CHRISTOPH AISTLEITNER, ISTV´AN BERKES AND ROBERT TICHY +Abstract. In this paper we present the theory of lacunary trigonometric sums +and lacunary sums of dilated functions, from the origins of the subject up to re- +cent developments. We describe the connections with mathematical topics such +as equidistribution and discrepancy, metric number theory, normality, pseudo- +randomness, Diophantine equations, and the subsequence principle. In the final +section of the paper we prove new results which provide necessary and sufficient +conditions for the central limit theorem for subsequences, in the spirit of Nikishin’s +resonance theorem for convergence systems. More precisely, we characterize those +sequences of random variables which allow to extract a subsequence satisfying a +strong form of the central limit theorem. +Contents +1. +Introduction +1 +2. +Uniform distribution and discrepancy +4 +3. +Arithmetic effects: Diophantine equations and sums of common divisors +7 +4. +The central limit theorem for lacunary sequences +12 +5. +The law of the iterated logarithm for lacunary sequences +16 +6. +Normality and pseudorandomness +20 +7. +Random sequences +24 +8. +The subsequence principle +28 +9. +New results: Exact criteria for the central limit theorem for subsequences 36 +Acknowledgments +49 +References +50 +1. Introduction +The word “lacunary” has its origin in the Latin lacuna (ditch, gap), which is a +diminutive form of lacus (lake). +Accordingly, a lacunary sequence is a sequence +with gaps, and a lacunary trigonometric sum is a sum of trigonometric functions +with gaps between the frequencies of consecutive summands. +The origin of the +theory of lacunary sums might lie in Weierstrass’ famous example of a continuous, +nowhere differentiable function (1872). Since then the subject has evolved into many +very different directions, reflecting for example the emergence of modern measure +theory and axiomatic probability theory in the early twentieth century, profound +1 + +2 +C. AISTLEITNER, I. BERKES AND R. TICHY +developments in harmonic analysis and Diophantine approximation, the establish- +ment of ergodic theory as one of the key instruments of number theory, or the +interest in notions of pseudo-randomness which are associated with the evolution +of theoretical computer science. Throughout this paper we will be concerned with +convergence/divergence properties of infinite trigonometric series +∞ +� +k=1 +ck cos(2πnkx) +or +∞ +� +k=1 +ck sin(2πnkx), +as well as with the asymptotic order and the distributional behavior of finite trigono- +metric sums +N +� +k=1 +ck cos(2πnkx) +or +N +� +k=1 +ck sin(2πnkx) +(the latter often in the simple case where ck ≡ 1), and with their generalizations +∞ +� +k=1 +ckf(nkx) +and +N +� +k=1 +ckf(nkx). +Here (ck)k≥1 is a sequence of coefficients, and (nk)k≥1 is a sequence of positive in- +tegers (typically increasing), which satisfies some gap property such as the classical +Hadamard gap condition +nk+1 +nk +> q > 1, +k ≥ 1, +or the “large gap condition” (also called “super-lacunarity property”) +nk+1 +nk +→ ∞, +k → ∞. +Furthermore, f is a 1-periodic function which is usually assumed to satisfy some reg- +ularity properties (such as being of bounded variation, being Lipschitz-continuous, +etc.), and which for simplicity is usually assumed to be centered such that +� 1 +0 f(x) dx = +0. +Early appearances of such lacunary sums include the following. +• Sums of the form �N +k=1 f(2kx), where f is an indicator function of a dyadic +sub-interval of [0, 1], extended periodically with period 1. Borel used such +sums in 1909 to show that almost all reals are “normal”; more on this topic +is contained in Section 6 below. +• Uniform distribution of sequences ({nkx})k≥1 in Weyl’s seminar paper of +1916; more on this in Section 2. Here and throughout the paper, we write +{·} for the fractional part function. +• Kolmogorov’s theorem on the almost everywhere convergence of lacunary +trigonometric series if the sequence of coefficients is square-summable (1924), + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +3 +a result related to his Three Series Theorem for the almost sure conver- +gence of series of independent random variables. Later it turned out that +Kolmogorov’s convergence theorem for trigonometric series actually remains +true without any gap condition whatsoever, a result which was widely be- +lieved to be “too good to be true” before being established by Carleson [77] +in 1966. More on this in Section 2. +• Foundational work on the distribution of normalized lacunary trigonometric +sums, in particular the central limit theorems of Kac (1946) and Salem and +Zygmund (1947), and the laws of the iterated logarithms of Salem and Zyg- +mund (1950) and of Erd˝os and G´al (1955). More on this in Sections 4 and 5. +A fundamental observation is that the unit interval, equipped with Borel sets and +Lebesgue measure, forms a probability space, and that consequently a sequence of +functions such as (cos(2πnkx))k≥1 or (f(nkx))k≥1 can be viewed as a sequence of +random variables over this space; if f is 1-periodic and if (nk)k≥1 is a sequence +of positive integers then these random variables are identically distributed, but in +general they are not independent. However, under appropriate circumstances the +gap condition which is imposed upon (nk)k≥1 can ensure that these random vari- +ables have a low degree of stochastic dependence. Consequently lacunary sums often +mimic the behavior of sums of independent and identically distributed random vari- +ables. This viewpoint was in particular taken by Steinhaus, Kac, and Salem and +Zygmund in their fundamental work on the subject. In a particularly striking situa- +tion, the dyadic functions considered by Borel actually turn out to be a version of a +sequence of Bernoulli random variables which are truly stochastically independent; +accordingly, Borel’s result on the normality of almost all reals is nowadays usually +read as the historically very first version of the strong law of large numbers in prob- +ability theory. +When taking this probabilistic viewpoint, the theory of lacunary sums could be seen +as a particular segment of the much wider field of the theory of weakly dependent +random systems in probability theory, which is associated with notions such as mix- +ing, martingales, and short-range dependence. However, it should be noted that +the precise dependence structure in a lacunary function system (f(nkx))k≥1 is con- +trolled by the analytic properties of the function f, in conjunction with arithmetic +properties of the sequence (nk)k≥1. It is precisely this interplay between probabilis- +tic, analytic and arithmetic aspects which makes the theory of lacunary sums so +interesting, so challenging and so rewarding. In the following sections we want to +illustrate some instances of these phenomena in more detail. + +4 +C. AISTLEITNER, I. BERKES AND R. TICHY +2. Uniform distribution and discrepancy +Let (xn)n≥1 be a sequence of real numbers in the unit interval. Such a sequence is +called uniformly distributed modulo one (in short: u.d. mod 1) if +(1) +1 +N +N +� +n=1 +1A(xn) = λ(A) +for all sub-intervals A ⊂ [0, 1] of the unit interval. The word “equidistributed” is +also used for this property, synonymously with “uniformly distributed modulo one”. +In this definition, and in the sequel, +1 denotes an indicator function, and λ denotes +Lebesgue measure. In informal language, this definition means that a sequence is +u.d. mod 1 if every interval A asymptotically receives its fair share of elements of the +sequence, which is proportional to the length of the interval. Note that (for example +as a consequence of the Glivenko–Cantelli theorem) for a sequence of independent, +uniformly (0, 1)-distributed random variables (Un)n≥1 one has +1 +N +N +� +n=1 +1A(Un) = λ(A) +almost surely +for all intervals A ⊂ [0, 1], so that in a vague sense uniform distribution of a deter- +ministic sequence can be interpreted in the sense that the sequence shows “random” +behavior; more on this aspect in Section 6 below. Uniform distribution theory can +be said to originate with Kronecker’s approximation theorem and with work of Bohl, +Sierpi´nski and Weyl on the sequence ({nα})n≥1 for irrational α. However, the theory +only came into its own with Hermann Weyl’s [222] seminal paper of 1916. Among +many other fundamental insights, Weyl realized that Definition (1), which in ear- +lier work had only be read in terms of counting points in certain intervals, can be +interpreted in a “functional” way and can equivalently be written as +(2) +lim +N→∞ +1 +N +N +� +n=1 +f(xn) = +� 1 +0 +f(x) dx +for all continuous functions f. This viewpoint suggests that uniformly distributed +sequences can be used as quadrature points for numerical integration; in the multi- +dimensional setting and together with quantitative error estimates this observation +forms the foundation of the so-called Quasi-Monte Carlo integration method, a con- +cept which today forms a cornerstone of numerical methods in quantitative finance +and other fields of applied mathematics (more on this below). Furthermore, Weyl +realized that the indicator functions in (1) or the continuous functions in (2) could +also be replaced by complex exponentials, as a consequence of the Weierstrass ap- +proximation theorem; thus by the famous Weyl Criterion a sequence is u.d. mod 1 +if and only if +lim +N→∞ +1 +N +N +� +n=1 +e2πihxn = 0 + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +5 +for all fixed non-zero integers h, thereby tightly connecting uniform distribution the- +ory with the theory of exponential sums. +For the particular sequence ({nα})n≥1 it can be easily seen from the Weyl criterion +that this sequence is u.d. mod 1 if and only if α ̸∈ Q. However, for other parametric +sequences of the form ({nkα})k≥1 the situation is much more difficult, and in general +it is completely impossible to determine whether for some particular value of α the +sequence is u.d. or not. It turns out that in a metric sense the situation is quite +different. Metric number theory arose after the clarification of the concept of real +numbers, the realization that the reals drastically outnumber the integers and the +rationals, and the development of modern measure theory. Loosely speaking, the +purpose of metric number theory is to determine properties which hold for a set +of reals which is “typical” with respect to a certain measure; here “typical” means +that the measure of the complement is small. In the present paper the measure +under consideration will always be the Lebesgue measure, and a set of reals will +be considered typical if its complement has vanishing Lebesgue measure; however, +metric number theory has for example also been intensively studied with respect to +the Hausdorff dimension or other fractal measures. +Returning to Weyl’s results, what he proved in the metric setting is the following. +For every sequence of distinct integers (nk)k≥1, the sequence ({nkα})k≥1 is u.d. mod +1 for (Lebesgue-) almost all reals α. In other words, even if we cannot specify the +set of α’s for which uniform distribution holds, at least we know that the set of such +α’s has full Lebesgue measure. It is amusing that after formulating the result, Weyl +continues to write: +Wenn ich nun freilich glaube, daß man den Wert solcher S¨atze, in +denen eine unbestimmte Ausnahmemenge vom Maße 0 auftritt, nicht +eben hoch einsch¨atzen darf, m¨ochte ich diese Behauptung hier doch +kurz begr¨unden.1 +One should recall that Weyl’s paper was written in a time of intense conflict of +formalists vs. constructivists (with Weyl favoring the latter ones), and only very +briefly after the notion of a set of zero (Lebesgue) measure had been introduced +at all. Today, Weyl’s theorem is seen as one of the foundational results of metric +number theory, together with the work of Borel, Koksma, Khinchin and others. +While uniform distribution modulo one is a qualitative asymptotic property, it is +natural that one is also interested in having a corresponding quantitative concept +which applies to finite sequences (or finite truncations of infinite sequences). Such +1Even if I think that the value of theorems, which contain an unspecified exceptional set of +measure zero, is not particularly high, I still want to give a short justification. + +6 +C. AISTLEITNER, I. BERKES AND R. TICHY +a concept is the discrepancy of a sequence, which is defined by +DN(x1, . . . , xN) = sup +A⊂[0,1] +����� +1 +N +N +� +n=1 +1A(xn) − λ(A) +����� . +Here the supremum is taken over all sub-intervals A ⊂ [0, 1], and it is easy to +see that an infinite sequence (xn)n≥1 is u.d. mod 1 if and only if the discrepancy +DN(x1, . . . , xN) tends to 0 as N → ∞. With a slight abuse of notation, we will +write throughout the paper DN(xn) = DN(x1, . . . , xN) for the discrepancy of the +first N elements of an infinite sequence (xn)n≥1. From a probabilistic perspective, +the discrepancy is a variant of the (two-sided) Kolmogorov–Smirnov statistic, where +one tests the empirical distribution of the point set x1, . . . , xN against the uniform +distribution on [0, 1]. Without going into details, we note that DN(x1, . . . , xN) can +be bounded above in terms of exponential sums by the Erd˝os–Tur´an inequality, and +that the error when using x1, . . . , xN as a set of quadrature points to approximate +� 1 +0 f(x) dx by 1 +N +�N +n=1 f(xn) can be bounded above by Koksma’s inequality in terms +of the variation of f and the discrepancy DN; for details see the monographs [96, 161], +which contain all the basic information on uniform distribution theory and discrep- +ancy. See also [181] for a discussion of equidistribution and discrepancy from the +viewpoint of analytic number theory, and [164, 165, 192] for expositions which put +particular emphasis on the numerical analysis aspects. +Weyl’s metric result from above can be written as +lim +N→∞ DN({nkα}) = 0 +for almost all α, +for any sequence (nk)k≥1 of distinct itegers. Strikingly, the precise answer to the +corresponding quantitative problem is still open more than a hundred years later. +It is known that for every strictly increasing sequence of integers (nk)k≥1 one has +(3) +DN({nkα}) = O +�(log N)3/2+ε +√ +N +� +for almost all α. +This is a result of R.C. Baker [38], who improved earlier results of Cassels [78] and +of Erd˝os and Koksma [104] by using Carleson’s celebrated convergence theorem in +the form of the Carleson–Hunt inequality [140]. In his paper Baker wrote that +[. . . ] probably the exponent 3/2 + ε could be replaced by ε [. . . ] +but it turned out that this is not actually the case. Instead, Berkes and Philipp [64] +constructed an example of an increasing integer sequence (nk)k≥1 for which +(4) +lim sup +N→∞ +��� +�N +k=1 cos(2πnkx) +��� +√N log N += +∞ +for almost every x. +By the Erd˝os–Tur´an inequality this gives a corresponding lower bound for the dis- +crepancy, which implies that the optimal exponent of the logarithmic term in an +upper bound of the form (3) has to be at least 1/2. But the actual size of this opti- +mal exponent, one of the most fundamental problems in metric discrepancy theory, + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +7 +still remains open. Note that for pure cosine-sums �N +k=1 cos(2πnkx) it is easily seen +that one has a metric upper bound with exponent 1/2 + ε in the logarithmic term; +this follows from the orthogonality of the trigonometric system, together with Car- +leson’s inequality and the Chebyshev inequality. Thus, in connection with (4), the +optimal upper bound in a metric estimate for pure cosine sums is known. For sums +�N +k=1 f(nkx) with f being a 1-periodic function of bounded variation, the optimal +exponent also is 1/2 + ε, but this is a much deeper result than the one for the pure +cosine case, and was established only recently in [15, 169]. By Koksma’s inequality, +an upper bound for the discrepancy implies an upper bound for sums of function +values for a (fixed) function of bounded variation, but the opposite is not true. So +while the case of a fixed function f is solved and is an important test case for the +discrepancy, the problem of the discrepancy itself (which requires a supremum over +a whole class of test functions) is more involved and remains open. +3. Arithmetic effects: Diophantine equations and sums of common +divisors +One of the most classical tools of probability theory is the calculation of expectations, +variances, and higher moments of sums of random variables. Due to trigonometric +identities such as +(5) +cos a cos b = cos(a + b) + cos(a − b) +2 +, +the calculation of moments of sums of trigonometric functions (with integer frequen- +cies) reduces to a counting of solutions of certain Diophantine equations. Indeed, +while the first and second moments +� 1 +0 +N +� +k=1 +cos(2πnkx) dx = 0 +and +� 1 +0 +� N +� +k=1 +cos(2πnkx) +�2 +dx = N +2 +are trivial and do not depend on the particular sequence (nk)k≥1 (as long as the +elements of the sequence are assumed to be distinct), interesting arithmetic effects +come into play when one has to compute higher moments, and it can be clearly seen +how the presence of a gap condition leads to a behavior of the moments which is +similar to that of sums of independent random variables. More precisely, assume +that we try to calculate +� 1 +0 +� N +� +k=1 +cos(2πnkx) +�m +dx +for some integer m ≥ 3. By (5) this can be written as a sum +2−m � +± +� +1≤k1,...,km≤N +1 (±nk1 ± · · · ± nkm = 0) . +Here the first sum is meant as a sum over all positive combinations of “+” and “-” +signs inside the indicator function at the end. Now assume that, for simplicity, we +consider the particular sequence nk = 2k, k ≥ 1, which is a prototypical example + +8 +C. AISTLEITNER, I. BERKES AND R. TICHY +of a sequence satisfying the Hadamard gap condition. Then it is not difficult to see +that +±nk1 ± · · · ± nkm = 0 +is only possible if the elements of the sum cancel out in a pairwise way; that is, after a +suitable re-ordering of the indices, we need to have k1 = k2, k3 = k4, . . . , km−1 = km, +and it only remains to count how many such re-orderings are possible. The result +is a combinatorial quantity, and it is exactly the same that arises when calculating +an m-th moment of a sum of independent random variables. Thus the moments +of the trigonometric lacunary sum converge to those of a suitable Gaussian distri- +bution, which gives rise to the classical limit theorems for lacunary trigonometric +sums. The situation is more delicate if one only has the Hadamard gap condition +nk+1/nk > q > 1 rather than exact exponential growth, and again more delicate if +one considers a sum of dilated functions � f(nkx) instead of a pure trigonometric +sum, but the principle described here is very powerful also in these more general +situations. For a long time this was the key ingredient in most of the proofs of +limit theorems for lacunary sums; see for example [103, 145, 193, 201, 214, 221]. A +different method is based on the approximation of a lacunary sum by a martingale +difference; here the “almost independent” behavior is not captured by controlling +the moments of the sum, but in the fact that later terms of the sum (functions with +high frequency) oscillate quickly in small regions where earlier summands (functions +with much lower frequency) are essentially constant. +As far as we can say, this +method was first used in the context of lacunary sums by Berkes [53] and, indepen- +dently, by Philipp and Stout [196]. We will come back to this topic in Section 4. +Broadly speaking, the “almost independent” behavior of sums of dilated functions +breaks down when the lacunarity condition is relaxed. Many papers have been de- +voted to this effect; see in particular [57, 59, 102, 184]. In order to maintain the +“almost independent” behavior of the sum, there are two natural routes to take. On +the one hand, one could randomize the construction of the sequence (nk)k≥1, and +assume that the undesired effects disappear almost surely with respect to the under- +lying probability measure – it turns out that this is a very powerful method, and we +will come back to it in Section 7 below. On the other hand, when adapting the view- +point that the “almost independence” property is expressed in the small number of +solutions of certain Diophantine equations, one could try to compensate the weaker +growth assumption by stronger arithmetic assumptions. A prominent example of a +class of sequences for which the latter approach has been very successfully used are +the so-called Hardy–Littlewood–P´olya sequences, which consist of all the elements of +the multiplicative semigroup generated by a finite set of primes, sorted in increasing +order. These sequences are in several ways a natural analogue of lacunary sequences; +note that the sequence (2k)k≥1 actually also falls into this framework by consisting +of all elements of the semigroup generated by a single prime. Such sequences gener- +ated by a finite set of primes have attracted the attention of number theorists again +and again, a particularly interesting instance being F¨urstenberg’s [126] paper on +disjointness in ergodic theory. It is known that Hardy–Littlewood–P´olya sequences +(if generated by two or more primes) grow sub-exponentially, and the precise (only + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +9 +slightly sub-exponential) growth rates are known (Tijdeman [216]). What is more +striking (and a much deeper fact) is that also the number of solutions of the rel- +evant linear Diophantine equations can be bounded efficiently – this is Schmidt’s +celebrated Subspace Theorem [207] in a quantitative form such as that of Evertse, +Schlickewei and Schmidt [107] or Amoroso and Viada [30]. By a combination of the +(slightly weaker) growth condition with the (strong) arithmetic information avail- +able for Hardy–Littlewood–P´olya sequences, much of the machinery that is used for +Hadamard lacunary sequences can be rescued for this generalized setup; see [194] as +well as [19, 65, 123]. +We briefly come back to the case of sums of dilated functions � f(nkx) without +the presence of a growth condition on (nk)k≥1. +We assume for simplicity that +� 1 +0 f(x) dx = 0, so trivially +� 1 +0 +N +� +k=1 +f(nkx) dx = 0, +but already the calculation of the variance +(6) +� 1 +0 +� N +� +k=1 +f(nkx) +�2 +dx +is in general quite non-trivial. If f(x) = cos(2πx), then one can simply use the +orthogonality of the trigonometric system. If f is a more general function, then one +can still express f by its Fourier series, expand the square and integrate, and thus +translate the problem of calculating (6) into a problem of counting the solutions +of certain linear Diophantine equations. When carrying out this approach, one is +naturally led to the problem of estimating a certain sum involving greatest common +divisors. For example, assume that f(x) = {x}−1/2. In this case a classical formula +(first stated by Franel and first proved by Landau) asserts that +� 1 +0 +f(mx)f(nx) dx = 1 +12 +(gcd(m, n))2 +mn +, +and consequently +� 1 +0 +� N +� +k=1 +({nkx} − 1/2) +�2 +dx = 1 +12 +� +1≤k,ℓ≤N +(gcd(nk, nℓ))2 +nknℓ +. +The sum on the right-hand side of this equation is called a GCD sum. A similar +identity holds for example for the Hurwitz zeta function ζ(1 − α, ·), where +� 1 +0 +ζ(1 − α, {mx})ζ(1 − α, {nx}) dx = 2Γ(α)2 ζ(2α) +(2π)2α +(gcd(m, n))2α +(mn)α +for α > 1/2, thus leading to a GCD sum +� +1≤k,ℓ≤N +(gcd(nk, nℓ))2α +(nknℓ)α + +10 +C. AISTLEITNER, I. BERKES AND R. TICHY +with parameter α. If f(x) is a general 1-periodic function, then one usually does not +obtain such a nice exact representation of the variance of a sum of dilated function +values, but typically the variance (6) can be bounded above by a GCD sum, which +together with Chebyshev’s inequality and the Borel–Cantelli lemma allows to make +a statement on the almost everywhere asymptotic behavior of a sum of dilated func- +tion values. +This connection between sums of dilated functions and GCD sums is explained in +great detail in Chapter 3 in Harman’s monograph on Metric Number Theory [136], +where mainly the context of metric Diophantine approximation is treated (see also [127, +155]). Recently this connection has also led to a solution of the problem of the al- +most everywhere convergence of series of dilated functions. Recall that Carleson’s +theorem [77] asserts that the series +∞ +� +k=1 +ck cos(2πnkx) +is almost everywhere convergent provided that � +k c2 +k < ∞. It is natural to ask +which assumption on the sequence of coefficients (ck)k≥1 is necessary to ensure the +almost everywhere convergence of the more general series +(7) +∞ +� +k=1 +ckf(nkx), +under some regularity assumptions on f. Gaposhkin [129, 130] obtained some partial +results, but a satisfactory understanding of the problem was only achieved very +recently, when the connection with GCD sums was fully understood and optimal +upper bounds for such sums were obtained. Exploiting this connection with GCD +sums, it was shown in [15, 169] that for 1-periodic f which is of bounded variation +on [0, 1] the series (7) is almost everywhere convergent provided that +∞ +� +k=3 +c2 +k(log log k)γ < ∞ +for some γ > 2, and this result is optimal in the sense that the same assumption +with γ = 2 would not be sufficient. In [16] it was shown that for the class Cα of +1-periodic square integrable functions f with Fourier coefficients aj, bj satisfying +aj = O(j−α), +bj = O(j−α) +for 1/2 < α < 1, a sharp criterion for the almost everywhere convergence of (7) is +that +(8) +∞ +� +k=1 +c2 +k exp +�K(log k)1−α +(log log k)α +� +< ∞ +with a suitable K = K(α). +In the case of 1-periodic Lipschitz α functions f, +Gaposhkin [130] proved that for α > 1/2, the series (7) converges a.e. under +� +k c2 +k < ∞ (just like in the case of Carleson’s theorem) and Berkes [60] showed + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +11 +that this result is sharp, i.e. for α = 1/2 the exact analogue of Carleson’s theorem is +not valid. No sharp convergence criteria exists in the case 0 < α ≤ 1/2; for sufficient +criteria for see Gaposhkin [129]. See also [4, 68, 128] for a general discussion and +several further results for the convergence of series � +k ckf(nkx). +For general periodic f ∈ L2 the direct connection between the integral (6) and GCD +sums breaks down, but upper bounds for (6) as well as for +(9) +� 1 +0 +� N +� +k=1 +ckf(nkx) +�2 +dx +can be given in terms of the coefficients ck, of the Fourier coefficients of f, and +arithmetic functions such as d(n) = � +d|n 1, σs(n) = � +d|n ds, or the Erd˝os-Hooley +function ∆(n) = supu∈R +� +d|n,u≤d≤eu 1. See Koksma [156, 157], Weber [220], and +Berkes and Weber [69, 70]. A typical example (see [220]) is the bound +� 1 +0 +�� +k∈H +ckf(kx) +�2 +dx ≤ +� ∞ +� +ν=1 +a2 +ν∆(ν) +� � +k∈H +c2 +kd(k) +valid for any set H of disjoint positive integers lying in some interval [er, er+1], r ≥ 1. +Here ak are the complex Fourier coefficients of f. Using standard methods, such +bounds lead easily to a.e. convergence criteria for sums � +k ckf(kx), see the papers +cited above. +In Wintner [223] it was proved that if f is a periodic L2 function with Fourier +coefficients ak, bk, then the series � +k ckf(kx) converges in L2 norm for all coefficient +sequences (ck)k≥1 satisfying � +k c2 +k < ∞ if and only if the functions defined by the +Dirichlet series +∞ +� +k=1 +akk−s, +∞ +� +k=1 +bkk−s, +are bounded and regular in the half plane ℜ(s) > 0. There is also a remarkable con- +nection between the maximal order of magnitude of GCD sums with the order of ex- +treme values of the Riemann zeta function in the critical strip; see [72, 94, 138, 209]. +Naturally, estimating the integral (6) provides important information also on the +asymptotic behavior of averages +(10) +1 +N +N +� +k=1 +f(nkx). +By the Weyl equidistribution theorem, for any 1-periodic f with bounded variation +in (0, 1) we have +(11) +lim +N→∞ +1 +N +N +� +k=1 +f(kx) = +� 1 +0 +f(x) dx +a.e. + +12 +C. AISTLEITNER, I. BERKES AND R. TICHY +(actually for every irrational x). Khinchin [150] conjectured that (11) holds for every +1-periodic Lebesgue integrable f as well. This conjecture remained open for nearly +50 years and was finally disproved by Marstrand [178]. An example for a periodic +integrable f and a sequence (nk)k≥1 of positive integers such that the averages (10) +do not converge almost everywhere had already been given earlier by Erd˝os [100]. +On the other hand, Koksma [157] proved that (11) holds if f ∈ L2 and the Fourier +coefficients ak, bk of f satisfy +∞ +� +k=1 + +(a2 +k + b2 +k) +� +d|k +1 +d + + < ∞, +and Berkes and Weber [70] proved that the last condition is optimal. No similarly +sharp criteria are known in the case f ∈ L1. +For further results related to the +Khinchin conjecture, see [37, 50, 70, 74, 185]. +4. The central limit theorem for lacunary sequences +Salem and Zygmund [201] proved the first central limit theorem (CLT) for lacunary +trigonometric sums. More specifically, they showed that for any integer sequence +(nk)k≥1 satisfying the Hadamard gap condition one has +lim +N→∞ λ +� +x ∈ (0, 1) : +N +� +k=1 +cos(2πnkx) ≤ t +� +N/2 +� += Φ(t), +where Φ denotes the standard normal distribution. Note that +� 1 +0 +� N +� +k=1 +cos(2πnkx) +�2 +dx = N +2 , +so the result above contains the “correct” variance for the limit distribution, exactly +as it should also be expected in the truly independent case. This result has been +signi���cantly strengthened since then; for example, Philipp and Stout [196] showed +that under the Hadamard gap condition the function +S(t, x) = +� +k≤t +cos(2πnkx), +considered as a stochastic process over the space ([0, 1], B[0, 1], λ), is a small per- +turbation of a Wiener process, a characterization which allows to deduce many fine +asymptotic results for this sum. It is also known that the central limit theorem +for pure trigonometric lacunary sums remains valid under a slightly weaker gap +condition than Hadamard’s: as Erd˝os [102] proved, it is sufficient to assume that +nk+1/nk ≥ 1 + ck−α, α < 1/2, while such an assumption with α = 1/2 is not suffi- +cient. +The whole situation becomes very different when the cosine-function is replaced +by a more general 1-periodic function, even if it is such a well-behaved one as a + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +13 +trigonometric polynomial. For example, consider +(12) +f(x) = cos(2πx) − cos(4πx), +nk = 2k, k ≥ 1. +In this case the lacunary sum is telescoping, and it can be immediately seen that +there cannot be a non-trivial limit distribution. A more delicate example is attrib- +uted to Erd˝os and Fortet2, and goes as follows. Let +f(x) = cos(2πx) + cos(4πx), +nk = 2k − 1, k ≥ 1. +Then it can be shown that N−1/2 �N +k=1 f(nkx) does indeed have a limit distribution, +but one which is actually non-Gaussian. More precisely, for this example one has +lim +N→∞ λ +� +x ∈ (0, 1) : +N +� +k=1 +f(nkx) ≤ t +� +N/2 +� += +1 +√π +� 1 +0 +� t/2| cos(πs)| +−∞ +e−u2duds. +Thus the limit distribution in this case is a so-called “variance mixture Gaussian”, +which can be seen as a normal distribution whose variance is a function rather than +a constant. This limiting behavior can be explained from the observation that +(13) +f(nkx) = cos((2k+1 − 2)πx) + cos((2k+2 − 4)πx) +and +(14) +f(nk+1x) = cos((2k+2 − 2)πx) + cos((2k+3 − 4)πx). +Combining the second term on the right-hand side of (13) with the first term on the +right-hand side of (14) we obtain +cos((2k+2 − 4)πx) + cos((2k+2 − 2)πx) = 2 cos(πx) cos((2k+2 − 3)πx), +so the whole lacunary sum �N +k=1 f(nkx) can essentially be written as 2 cos(πx) +multiplied with a pure cosine lacunary sum. This is exactly what the “variance +mixture Gaussian” indicates: the limit distribution is actually that of 2 cos(πx) +independently multiplied with a Gaussian. The failure a of Gaussian central limit +theorem in the example above can be seen as a consequence of the fact that the +Diophantine equation +nk+1 − 2nk = 1 +possesses many solutions k for this particular choice of sequence. Equipped with +this observation, one could readily construct similar examples with other trigono- +metric polynomials f, and other variance mixture Gaussians as limit distributions, +by creating situations where there are many solutions k, ℓ to +(15) +ank − bnℓ = c +2The Erd˝os–Fortet example is first mentioned in print in a paper of Salem and Zygmund [202]. +They mention the example without proof, and write: “This remark is essentially due to Erd˝os.”. +Later the example was mentioned in a paper of Kac [146], who wrote: “It thus came as a surprise +when simultaneously and independently of each other, Erd˝os and Fortet constructed an example +showing that the limit [. . . ] need not be Gaussian”, with a footnote: “In Salem and Zygmund this +example is erroneously credited to Erd˝os alone.” No proof is given in Kac’s paper either, but he +writes: “Details will be given in [a forthcoming] paper by Erd˝os, Ferrand, Fortet and Kac”. Such +a joint paper never appeared. + +14 +C. AISTLEITNER, I. BERKES AND R. TICHY +for some fixed a, b, c. However, interestingly, a special role is played by such equations +when c has the particular value c = 0; very roughly speaking, solutions of the +equation for c = 0 effect only the limiting variance (in a Gaussian distribution), +but not the structure of the limiting distribution itself. This is visible in a paper +of Kac [145], who studied the sequence nk = 2k, k ≥ 1, where indeed the only +equations that have many solution are of the form 2mnk − nℓ = 0 for some m (the +solutions being ℓ = k + m). Kac proved that for this sequence and any 1-periodic f +of bounded variation and zero mean one has +(16) +lim +N→∞ λ +� +x ∈ (0, 1) : +N +� +k=1 +f(nkx) ≤ tσf +√ +N +� += Φ(t) +with a limiting variance σ2 +f, provided that +(17) +σ2 +f := +� 1 +0 +f 2(x) dx + 2 +∞ +� +m=1 +� 1 +0 +f(x)f(2mx) dx ̸= 0. +Thus in this case the limit distribution is always a Gaussian, and the failure of the +trivial example in (12) to produce such a Gaussian limit comes from the fact that +the limiting variance is degenerate. +These observations show that there is a delicate interplay between arithmetic, an- +alytic and probabilistic effects; in particular, it is obviously not only the order of +growth of (nk)k≥1 which is responsible for the fine probabilistic behavior of a la- +cunary sum. Takahashi [211] proved a CLT (with pure Gaussian limit) under the +assumption that nk+1/nk → ∞, and Gaposhkin [128] proved that a CLT (with pure +Gaussian limit) holds when nk+1/nk is an integer for all k, or if nk+1/nk → α for +some α such that αr ̸∈ Q, r = 1, 2, . . . (and if additionally the variance does not +degenerate). A general framework connecting Diophantine equations and the dis- +tribution of lacunary sums was established in Gaposhkin’s profound paper [131], +where he proved that a CLT (with pure Gaussian limit) holds if for all fixed positive +integers a, b the number of solutions k, ℓ of the Diophantine equation (15) is bounded +by a constant which is independent of c (where only c ̸= 0 needs to be considered, +provided that the variance does not degenerate). One can check the validity of this +general condition for sequences satisfying the assumptions mentioned earlier in this +paragraph, such as nk+1/nk → ∞ or nk+1/nk → α for αr ̸∈ Q. Finally, an optimal +result was established in [13]: For (nk)k≥1 satisfying the Hadamard gap condition, +the limit distribution of N−1/2 �N +k=1 f(nkx) is Gaussian provided that the number +of solutions (k, ℓ) of (15), subject to k, ℓ ≤ N, is of order o(N) (for all fixed a, b, +uniformly in c ̸= 0). If, on the other hand, for some a, b, c the number of solutions +is Ω(N), then the CLT generally fails to hold. If the number of solutions with c = 0 +also is of order o(N), then the CLT has the “correct” variance +� 1 +0 f(x)2dx, in perfect +accordance with the independent case. Even if the number of solutions is of order +Ω(N) for some a, b, c, then the deviation of the distribution of N−1/2 �N +k=1 f(nkx) +from the Gaussian distribution can be quantified in terms of the ratio “(number of +solutions)/N”. This shows for example that while the CLT generally fails in the + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +15 +case nk+1/nk → p/q, one obtains an “almost CLT” if both p and q are assumed to be +large. Another example for such an “almost CLT” is when the growth constant in +the Hadamard gap condition is assumed to be very large. See the statement of [13, +Theorem 1.3] and the subsequent discussion for more details. +Note that Gaposhkin’s condition implies that the CLT also holds for all subsequences +that are picked out of (nk)k≥1. This is not the case under the assumptions from [13], +where one might be able to extract a subsequence along which the CLT fails (by +choosing a subsequence which allows a large number of solutions of the relevant +Diophantine equations). It is interesting that the probabilistic behavior of lacunary +sums might change when one passes to a subsequence of the original sequence – +this is in clear contrast to the bevahior of sums of independent random variables, +where any subsequence of course is independent as well. A similar remark holds for +permutations of lacunary sums resp. permutations of sums of independent random +variables. These phenomena have received strong attention during the last years; see +for example [17, 18, 19, 21, 114]. To give only one sample result, in [17] the following +is shown. As noted above, the CLT is true for pure trigonometric sums under the +Erd˝os gap condition nk+1/nk ≥ 1 + ck−α for some α < 1/2. However, this is only +true for the unpermuted sequence (i.e. sorted in increasing order). If permutations +of the sequence are allowed, then this gap condition is not sufficient anymore for the +validity of the CLT, as is no other gap conditon weaker than Hadamard’s. More +precisely, for any sequence (εk)k≥1 with εk → 0 there exists a sequence of positive +integers satisfying nk+1/nk ≥ 1 + εk, together with a permutation σ : N �→ N, such +that the permuted (pure trigonometric) sum N−1/2 �N +k=1 cos(2πnσ(k)x) converges in +distribution to a non-Gaussian limit. One can also construct such examples where +the norming sequence N−1/2 has to be replaced by (log N)1/2N−1/2 and the limit is a +Cauchy distribution, and examples where no limit distribution exists at all. See [17] +for details on this particular result, and Chapter 3 of [61] for a detailed discussion +of permutation-invariance of limit theorems for lacunary (trigonometric) systems. +We close this section with some further references. For Hadamard lacunary (nk)k≥1, +the limit distribution of N1/2DN(nkx) was calculated in [14]; under suitable Dio- +phantine assumptions it coincides with the Kolmogorov distribution, which is the +distribution of the range of a Brownian bridge. A central limit theorem for Hardy– +Littlewood–P´olya sequences was established in [124]. In [87] the Erd˝os–Fortet ex- +ample was revisited from the perspective of ergodic theory, and was interpreted in +terms of the limiting behavior of certain modified ergodic sums, and generalized to +cases such as expanding maps, group actions, and chaotic dynamical systems under +the assumption of multiple decorrelation. See also [86, 88]. The limit distribution +of N−1/2 �N +k=1 cos(2πnkx) for the special sequence nk = k2, k ≥ 1, was determined +by Jurkat and Van Horne in [141, 142, 143], and turned out to have finite moments +of order < 4, but not of order 4. The theory of such sums is closely related to theta +sums, and goes back to Hardy and Littlewood [135]. For further related results, +see [80, 108, 219]. For non-Gaussian limit distributions of N−1/2 �N +k=1 cos(2πnkx) + +16 +C. AISTLEITNER, I. BERKES AND R. TICHY +near the Erd˝os gap condition nk+1/nk ≥ 1 + ck−1/2 see [58]. For a multidimensional +generalization of Kac’s results see [112, 120], and for a multidimensional generaliza- +tion of the CLT for Hardy–Littlewood–P´olya sequences (considering a semi-group +generated by powers of matrices instead) see [167, 168]. See also [85, 90] for general- +izations of the CLT for Hardy–Littlewood–P´olya sequences to a very general setup +of sums over powers of transformations/automorphisms. +5. The law of the iterated logarithm for lacunary sequences +Together with the law of large numbers (LLN) and the central limit theorem (CLT), +the law of the iterated logarithm (LIL) is one of the fundamental results of prob- +ability theory. Very roughly speaking, the (strong) law of large numbers says that +when scaling by N−1 one has almost sure convergence of a sum of random variables, +and the central limit theorem says that when scaling by N−1/2 one has a (Gaussian) +limit distribution. The law of the iterated logarithm operates between these two +other asymptotic limit theorems; in its simplest form, it says that for a sequence +(Xn)n≥1 of centered i.i.d. random variables (under suitable extra assumptions, such +as boundedness) one has +lim sup +N→∞ +�N +n=1 Xn +√2N log log N = σ +almost surely, +where σ is the standard deviation. Heuristically, the law of the iterated logarithm +identifies the threshold between convergence in distribution and almost sure conver- +gence for sums of i.i.d. random variables; indeed, while +�N +n=1 Xn +√2N log log N converges to 0 in +distribution by the CLT, it does not converge to 0 almost surely by the LIL. The +first version of the LIL was given by Khinchin in 1924, and a more general variant +was established by Kolmogorov in 1929. Note that the law of large numbers for +trigonometric sums or sums of dilated functions is rather unproblematic: for any +sequence of distinct integers (nk)k≥1 one has +(18) +lim +N→∞ +1 +N +N +� +k=1 +f(nkx) = +� 1 +0 +f(x) dx, +as long as one can assume a bit of regularity for f (such as f being a trigonometric +polynomial, being Lipschitz-continuous, being of bounded variation on [0, 1], etc.). +Only if one is not willing to impose any regularity assumptions upon f the situation +becomes quite different; see the remarks at the end of Section 3. +The most basic law of the iterated logarithm for lacunary systems is +(19) +lim sup +N→∞ +�N +n=1 cos(2πnkx) +√2N log log N += 1 +√ +2 +a.e. +under the Hadamard gap condition on (nk)k≥1; this was obtained by Salem and +Zygmund (upper bound) [203] and Erd˝os and G´al (lower bound) [103]. Generally +speaking, as often in probability theory the lower bound is more difficult to estab- +lish than the upper bound, since the latter can be proved by an application of the + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +17 +first Borel–Cantelli lemma (convergence part), while the former is proved by the +second Borel–Cantelli lemma (divergence part, which needs some sort of stochastic +independence as an extra assumption). Note that (19) is a perfect analogue of (18) +with the “correct” constant on the right-hand side. +As in the case of the CLT, replacing pure trigonometric sums by sums of more +general 1-periodic functions makes the situation much more delicate. +As in the +previous section, a key role is played by Diophantine equations. However, while +for the CLT it is crucial that the number of solutions of Diophantine equations +“stabilizes” in some way to allow for a limit distribution (albeit a potentially non- +Gaussian one), no such property is necessary for the validity of a form of the LIL +(since, as noted above, this is defined as a lim sup, not as a lim). Instructive examples +are the following. In all examples, we assume that f is 1-periodic with mean zero +and bounded variation on [0, 1]. +• If nk+1/nk → ∞ as k → ∞, then +lim sup +N→∞ +�N +n=1 f(nkx) +√2N log log N = +�� 1 +0 +f 2(x) dx +�1/2 +a.e. +• If nk = 2k, k ≥ 1, then +lim sup +N→∞ +�N +n=1 f(nkx) +√2N log log N = σf +a.e., +with +σ2 +f = +� 1 +0 +f 2(x)dx + 2 +∞ +� +m=1 +� 1 +0 +f(x)f(2mx) dx. +• Assume that nk+1/nk ≥ q > 1, k ≥ 1. Then there exists a constant C +(depending on f and on q) such that +(20) +lim sup +N→∞ +�N +n=1 f(nkx) +√2N log log N ≤ C +a.e. +• If nk = 2k − 1, k ≥ 1, and if f(x) = cos(2πx) + cos(4πx), then +(21) +lim sup +N→∞ +�N +n=1 f(nkx) +√2N log log N = +√ +2| cos(πx)| +a.e. +The first result in this list (due to Takahashi [213]) is in perfect accordance with +the LIL for truly independent random sums, in accordance with the fact that +also the CLT holds in the “truly independent” form under the large gap condi- +tion nk+1/nk → ∞. The second result is an analogue of Kac’s CLT in Equations +(16) and (17): as with the CLT, also the LIL holds for the sequence (2k)k≥1, but +the limiting variance deviates from the one in the “truly independent” case. Note +that in contrast to the CLT case we now do not need to require that σf ̸= 0 for the +validity of the statement. The third result (Takahashi [212]) asserts that there is an +upper-bound version of the LIL for lacunary sums (even for sequences where there is +no convergence of distributions, and any form of the CLT fails). Finally, the fourth + +18 +C. AISTLEITNER, I. BERKES AND R. TICHY +result (the Erd˝os–Fortet example for the LIL instead of the CLT) shows the remark- +able fact that the lim sup in the LIL for Hadamard lacunary sums might actually be +non-constant – this is very remarkable, and a drastic deviation from what one can +typically observe for sequences of independent random variables. In particular this +example shows that under the Hadamard gap condition an upper-bound version of +the LIL is in general the best that one can hope for. Not very surprisingly, the source +of all these phenomena are (as in the previous section) Diophantine equations such +as (15), and their number of solutions within the sequence (nk)k≥1. So in the LIL +there is again a complex interplay between probabilistic, analytic and arithmetic +aspects which controls the fine asymptotic behavior of lacunary sums. +In probability theory there is a version of the LIL for the Kolmogorov–Smirnov +statistic of an empirical distribution. This is called the Chung–Smirnov LIL, and +in the special case of a sequence (Xn)n≥1 of i.i.d. random variables having uniform +distribution on [0, 1] (where the Kolmogorov–Smirnov statistic coincides with the +discrepancy) it asserts that +lim sup +N→∞ +NDN(Xn) +√2N log log N = 1 +2 +almost surely. +Here the number 1/2 on the right-hand side arises essentially as the maximal L2 +norm (“standard deviation”) of a centered indicator function of an interval A ⊂ [0, 1] +(namely the indicator function of an interval of length 1/2). Based on the princi- +ple that lacunary sequences tend to “imitate” the behavior of truly independent +sequences, it was conjectured that an analogue of the Chung–Smirnov LIL should +also hold for the discrepancy of ({nkx})k≥1, where (nk)k≥1 is a Hadamard lacunary +sequence. This was known as the Erd˝os–G´al conjecture, and was finally solved by +Philipp [193], who proved that for any q > 1 there exists a constant Cq such that +for (nk)k≥1 satisfying nk+1/nk ≥ q we have +(22) +1 +√ +32 ≤ lim sup +N→∞ +NDN({nkx}) +√2N log log N ≤ Cq +a.e. +An admissible value of Cq was specified in [193] as Cq = 166/ +√ +2 + 664/(√2q − +√ +2). +The first inequality in (22) follows from (a complex version of) Koksma’s inequality +together with (19), so the novelty is the second inequality (upper bound). Note also +that the upper bound in (22) implies Takahashi’s “upper bound” LIL in (20), again +as a consequence of Koksma’s inequality. +Philipp’s result has been extended and refined into many different directions. The +most precise results, many of which were obtain by Fukuyama, show again a fasci- +nating interplay between arithmetic, analytic and probabilistic effects. As a sample +we state the following results (all from Fukuyama’s paper [113]): +Let nk = θk, k ≥ 1. Then +(23) +lim sup +N→∞ +NDN({nkx}) +√2N log log N + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +19 +exists and is constant (almost everywhere). Denoting the value of this lim sup by +Σθ, we have: +• If θr ̸∈ Q for all r = 1, 2, . . . , then Σθ = 1/2 a.e. +• If r denotes the smallest positive integer such that θr = p/q for some coprime +p, q, then 1/2 ≤ Σθ ≤ +� +(pq + 1)/(pq − 1)/2 a.e. +• If θr = p/q as above and both p and q are odd, then Σθ = +� +(pq + 1)/(pq − 1)/2 +a.e. +• If θ = 2, then Σθ = +√ +42/9 a.e. +• If θ > 2 is an even integer, then Σθ = +� +(p + 1)p(p − 2)/(p − 1)3/2 a.e. +• If θ = 5/2, then Σθ = +√ +22/9 a.e. +All these results were obtained by very delicate calculations involving Fourier anal- +ysis and Diophantine equations. The calculations from [113] were continued by the +same author and his group in [119, 121, 122, 125], so that now we have a relatively +comprehensive picture on the behavior of these lim sup’s in the case when (nk)k≥1 +is (exactly) a geometric progression. +In [7, 8] for general Hadamard lacunary sequences (nk)k≥1 a direct connection was +established which links the number of solutions of (15) with the value of the lim sup +in the LIL, in the same spirit as this was done before in [13] for the CLT (as de- +scribed in the previous section). In particular, if the number of solutions of (15) is +sufficiently small, then the LIL holds with the constant 1/2 on the right-hand side, +exactly as in the truly independent case. Another interesting observation is that +if (nk)k≥1 is Hadamard lacunary with growth factor q > 1, and if Σ denotes the +value of the lim sup in (23), then the difference |Σ − 1/2| can be quantified in terms +of q and tends to zero a.e. as q → ∞. Thus there is a smooth transition towards +the “truly independent” LIL as the growth factor q increases, and under the large +gap condition nk+1/nk → ∞ the value of Σ actually equals 1/2. Another remark- +able fact is that there exist Hadamard lacunary sequences for which the lim sup +in the LIL for the discrepancy is not a constant almost everywhere, but rather a +function of x, similar to what happened in (21) for the LIL for � f(nkx). In some +cases the limit functions in the LIL for the discrepancy can be explicitly calculated, +and are “surprisingly exotic” (in the words of Ben Green’s MathSciNet review of [6]). +As noted above, Philipp’s LIL for the discrepancy has been extended into many +different directions. For example, while it is known that the result can fail as soon +as the Hadamard gap condition is relaxed to any sub-exponential growth condition, +it turns out to be possible to obtain an LIL for the discrepancy when a weaker +growth condition is compensated by stronger arithmetic assumptions. In particu- +lar, an analogue of Philipp’s result has been proved for Hardy–Littlewood–P´olya +sequences [195]; see also [5, 65, 123, 215]. As a closing remark concerning the LIL, +it is interesting that the optimal value of the lower bound in (22) is still unknown; +cf. [25] for more context. + +20 +C. AISTLEITNER, I. BERKES AND R. TICHY +While much effort has been spent towards understanding the probabilistic behavior +of lacunary sums at the scales of the CLT and LIL, it seems that investigations at +other scales (such as in particular at the large deviations scale) were only started +recently. The few results which are currently available point once again towards an +intricate connection between probabilistic, analytic and arithmetic effects; see the +very recent papers [22, 111]. +6. Normality and pseudorandomness +Normal numbers were introduced by Borel [73] in 1909. From the very beginning +the concept of normality of real numbers was associated with “randomness”. While +normality of real numbers was originally defined in terms of counting the number +of blocks of digits, it is not difficult to see3 that a number x is normal in base b if +and only if the sequence ({bnx})n≥1 is equidistributed. As Borel proved, Lebesgue- +almost all real numbers are normal in a (fixed) integer base b ≥ 2, and thus almost +all reals are normal in all bases b ≥ 2 (such numbers are called absolutely normal). +While normal numbers are ubiquitous from a measure-theoretic perspective,4 it is +difficult to construct normal numbers. The most fundamental construction is due +to Champernowne, who proved (using combinatorial arguments) that the number +0.1 2 3 4 5 6 7 8 9 10 11 12 13 14 . . . , +which is obtained by a concatenation of the decimal expansions of the integers, is +normal in base 10. The idea of creating normal numbers by a concatenation of the +(b-ary) expansions of the values of (simple) functions at integers (or primes) is still +the most popular, and probably most powerful, method in this field. We only note +that Copeland and Erd˝os [89] proved that +0.2 3 5 7 11 13 17 19 23 . . . , +which is obtained by concatenating the decimal expansions of the primes, is normal +in base 10, and refer to [92, 93, 171, 174, 186, 187] for more results of this flavor. +It should be noted, however, that there have been earlier constructions of a con- +ceptually very different nature, such as that of Sierpinski [208] in 1917. See [43] +for an exposition of Sierpinski’s construction and more context, and see also [44] on +an early (unpublished) algorithm of Turing for the construction of normal numbers. +We finally mention a very recent idea for the construction of a normal number by +Drmota, Mauduit and Rivat [95], which is not based on the concatenation of deci- +mal blocks as above, but rather on the evaluation of an automatic sequence along +a subsequence of the index set (in this particular case, the Thue–Morse sequences +evaluated along the squares); see also [183, 210]. +3Probably first explicitly mentioned by D.D. Wall in his PhD thesis, 1949. +4Interestingly, while the set of normal numbers is large from a measure-theoretic point of view, it +turns out to be small from a topological point of view. More precisely, the set of normal numbers is +meager (of first Baire category), see e.g. [133]. In the words of Edmund Hlawka [139, p. 78]: “Thus +whereas the normal numbers almost force themselves on to the measure theorist, the topologist is +apt to overlook them entirely.” + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +21 +While Lebesgue-almost all numbers are normal and there are some constructions +of normal numbers, it is generally considered to be completely hopeless to prove +that natural constants such as π, e, +√ +2, . . . are normal in a given base (although +the experimental evidence clearly points in that direction: [189, 218, 224]). Many +such open problems “for the next millennium” are contained in Harman’s survey +article [137]; see also [33]. However, it is quite clear that the mathematical machin- +ery which would be necessary to prove the normality of +√ +2 or other such constants +is completely lacking; compare the rather deplorable current state of knowledge on +the binary digits of +√ +2 as given in [34, 98, 217]. A small spark of hope is provided +by the very remarkable formulas of Bailey, Borwein and Plouffe (now widely known +as BBP formulas), which allow to calculate deep digits of π (and other constants) +without the need of computing all previous digits. See [51] for a very comprehen- +sive “source book” covering computational aspects of π, and see [35] for a very rare +example of a possible strategy of what a proof of the normality of π could possibly +like (cf. also [162]). +Since normality of x in a base b can be expressed in terms of the equidistribution of +the sequence ({bnx})n≥1, it is very natural to consider the discrepancy of DN({bnx}) +and call this (with a slight abuse of language) the discrepancy of x (as a normal +number, with respect to a base b). +Remarkably, it is still unknown how small +the discrepancy of a normal number can be (this is known as Korobov’s problem). +Levin [166] constructed (for given base b) a number x such that +DN({bnx}) = O +�(log N)2 +N +� +; +by Schmidt’s general lower bound the exponent of the logarithm cannot be reduced +below 1, but the optimal size of this exponent remains open. +One of the most interesting, and most difficult, aspects of normal numbers is nor- +mality with respect to two or more different bases. Extending work of Cassels [79], +Schmidt [206] characterized when normality with respect to a certain base im- +plies normality with respect to another base, and when this is not the case. See +also [48, 76]. However, generally speaking it is very difficult to construct numbers +which are normal with respect to several different bases, and the “constructions” +are much less explicit than the ones of Champernowne and Copeland–Erd˝os men- +tioned above. The problem of the minimal order of the discrepancy of normal num- +bers seems to be very difficult when different bases are considered simultaneously. +Aistleitner, Becher, Scheerer and Slaman [12] constructed a number x such that +DN({bnx}) = Ob +� +N−1/2� +for all integer bases b ≥ 2; this is considered to be an “unexpectedly small” order +of the discrepancy by Bugeaud in his MathSciNet review of [12]. It is not known if +the exponent −1/2 of N in this estimate is optimal or not; indeed, no non-trivial +lower bounds whatsoever (beyond the general lower bound (log N)/N of Schmidt) + +22 +C. AISTLEITNER, I. BERKES AND R. TICHY +are known for this problem, but it is quite possible that whenever simultaneous nor- +mality with respect to different (multiplicatively independent) bases is considered, +there must be at least one base for which the discrepancy is “large”. +In a recent years, there has been a special focus on algorithmic aspects of the con- +struction of normal numbers. A particularly striking contribution was a polynomial- +time algorithm for the construction of absolutely normal numbers due to Becher, +Heiber and Slaman [45]. See also [29, 47, 205]. Related to such algorithmic and +computational problems are questions on the complexity of the set of normal num- +bers from the viewpoint of descriptive set theory in mathematical logic; in this +framework, the rank of the set of normal numbers [152] and absolutely normal num- +bers [46] within the Borel hierarchy has been determined. +The notion of normality can be extended in a natural way to many other situa- +tions, where it is always understood that normality should be the typical behaviour. +For example, one can consider normal continued fractions, where the “expected” +number of occurences of each partial quotient is prescribed by the Gauss–Kuzmin +measure; see for example [1, 49]. Other generalizations consider for example normal- +ity with respect to β-expansions [39, 173], a numeration system which generalizes +the b-ary expansion to non-integral bases β, or normality with respect to Cantor ex- +pansions [3, 109, 175], a numeration system which allows a different set of “digits” +at each position. For a particularly general framework, see [172]. Interestingly, in +such generalized numeration systems there can be more than one natural definition +of normality, using as starting point for exampe either the idea of counting blocks +of digits, or the idea of equidistribution of an associated system. The relation be- +tween such different (sometimes conflicting) notions of normality has been studied +in particular detail for Cantor expansions [2, 170, 176]. +Normal numbers feature prominently in the chapter on random numbers in Volume 2 +of Knuth’s celebrated series on The Art of Computer Programming [153]. There he +tries to come to terms with the notion of “random” sequences of numbers, and intro- +duces an increasingly restrictive scheme of “randomness” of deterministic sequences. +The concept of normality is also the starting point for one of the (quantitative) mea- +sures of pseudorandomness, which were introduced by Mauduit and S´ark¨ozy [179] +and then studied in a series of papers. Note in this context that the transformation +T : x �→ bx mod 1, which is at the foundation of the concept of normal numbers, +can in some sense be seen as the continuous analogue of the recursive formula which +defines a linear congruential generator (LCG), one of the most classical devices for +pseudorandom number generation. For this connection between normal numbers +and pseudo-random number generators, see for example [36]. Another very fruitful +aspect of normal numbers is the connection with ergodic theory, which comes from +the observation that the sequence ({bnx})n≥1 is the orbit of x under the transforma- +tion T from above, and that this transformation is measure-preserving (with respect +to the Lebesgue measure) and ergodic. We will not touch upon this connection in + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +23 +any detail, and instead refer to [91, 149]. +Another sequence which is often associated with “randomness” is the sequence +({xn})n≥1 for real x > 1, or more generally ({ξxn})n≥1 for ξ ̸= 0 and x > 1. +This looks quite similar to a (Hadamard) lacunary sequence such as (bnx)n≥1, but +its metric theory is of a very different nature in several respects. Both sequences are +variants of a geometric progression, but while in the lacunary sequence the base b is +fixed and x is assumed to be a “parameter”, now ξ is assumed to be fixed and the +base x of the geometric progression is the parameter. While (bnx)n≥1 can in many +ways be easily interpreted in terms of harmonic analysis, digital expansions, ergodic +theory, etc., such simple interpretations fail for ({xn})n≥1. Note in particular that in +contrast to lacunary sequences there now is no periodicity when replacing x �→ x+1, +there is no “orthogonality”, and the calculation of moments of sums � f(xn) does +not simply reduce to the counting of solutions of Diophantine equations. Still, what +is preserved from the setup of lacunary sequences is that xn (as a function of x) +oscillated quickly on intervals where xm is essentially constant, provided that n is +significantly larger than m, and there are good reasons to consider systems such as +(cos(2πxn))n≥1 to be “quasi-orthogonal” and “almost independent” in some appro- +priate sense. +One of the most fundamental results on this type of sequence is due to Koksma [154]: +assuming that ξ ̸= 0 is fixed, the sequence ({ξxn})n≥1 is uniformly distributed mod +1 for almost all x > 1. +In particular, when ξ = 1, the sequence ({xn})n≥1 is +uniformly distributed mod 1 for almost all x > 1. +In very sharp contrast with +Koksma’s metric result is the fact that until today not a single example of a number +x is known for which ({xn})n≥1 is indeed uniformly distributed. This problem is +related with Mahler’s problem on the range of ({(3/2)n})n≥1, which also seems to be +completely out of reach for current methods (cf. [97, 110]). The sequence ({xn})n≥1 +is discussed at length in Knuth’s book, where it is conjectured that this sequence is +a good candidate to pass several very strict pseudorandomness criteria for almost +all x. For example, Knuth conjectured that for all sequences of distinct integers +(sn)n≥1 the sequence ({xsn})n≥1 (a subsequence of the original sequence) has a strong +equidistribution property called complete uniform distribution, for almost all x > 1; +this was indeed established by Niederreiter and Tichy [188]. It is also known that +({xn})n≥1 satisfies an law of the iterated logarithm in the “truly independent” form +lim sup +N→∞ +NDN({xn}) +√2N log log N = 1 +2 +a.e., +and similarly satisfies a central limit theorem which is perfectly analogous to the one +for truly independent systems [9]. Note that Knuth’s assertion that the sequence +({xn})n≥1 shows good pseudo-random behavior for almost all x > 1 is of limited +practical use, as long as no such value of x is found. The discrete analogue would +be to study the pseudo-randomness properties of an mod q for n = 1, 2, . . . , where a +and q are fixed integers. Investigations on the pseudo-randomness properties of such +sequence were carried out for example by Arnol’d [32], who experimentally observed + +24 +C. AISTLEITNER, I. BERKES AND R. TICHY +good pseudorandom behavior; cf. also [10]. +To close this section, we note that equidistribution is of course just one property +which can be used to characterize “pseudorandom” behavior (essentially by analogy +with the Glivenko–Cantelli theorem). There are many other statistics which could +be applied to a sequence in [0, 1] to determine whether it behaves in a “random” +way or not. One class of such statistics are gap statistics at the level of the average +gap (which is of order 1/N when considering the first N elements of a sequence +in [0, 1]), such as the distribution of nearest-neighbor gaps, or the pair correlation +statistics. We do not give formal definitions of these concepts here, but note that +they are inspired by investigations of the statistics of quantum energy eigenvalues in +the context of the Berry–Tabor conjecture in theoretical physics; see [177] for more +context. Pseudorandom behavior with respect to such statistics is called “Poisso- +nian”, since it agress with the corresponding statistics for the Poisson process. The +general principle that lacunary systems show pseudorandom behavior is also valid +in this context. For example, Rudnick and Zaharescu [199] showed that for (nk)k≥1 +satisfying the Hadamard gap condition the sequence ({nkx})k≥1 is Poissonian for +almost all x, and Aistleitner, Baker, Technau and Yesha [11] showed that the same +holds for ({xn})n≥1 for almost all x > 1. +This section on normal numbers and sequences of the form ({ξxn})n≥1 gives of course +only a very brief overview of the subject, and has to leave out many interesting +aspects. For a much more detailed exposition we refer the reader to the book of +Bugeaud [75]. +7. Random sequences +In the previous sections we have illustrated the philosophy that gap sequences ex- +hibit many probabilistic properties which are typical for sequences of i.i.d. random +variables. In many cases the large gap condition nk+1/nk → ∞ gives “true” random +limit theorems, the Hadamard gap condition nk+1/nk ≥ q > 1 is a critical transi- +tion point where a mixture of probabilistic, analytic and arithmetic effects comes +into play, and the “almost independent” behavior is lost when the gap condition is +relaxed below Hadamard’s. There are results which hold under weaker gap condi- +tions such as the Erd˝os gap condition nk+1/nk ≥ 1 + ck−α, 0 < α < 1/2, or under +additional arithmetic assumptions, but as a whole the Hadamard gap condition is +the critical point where the “almost independent” behavior of systems of dilated +functions starts to break down. +However, while almost independent behavior is generally lost under a weaker gap +condition (without strong arithmetic information), there is another possible per- +spective on the problem. As noted, for a fixed sequence (nk)k≥1 one cannot ex- +pect “almost independent” behavior of ({nkx})k≥1, say, without assuming a strong +growth condition on (nk)k≥1. However, even without such a growth condition one +might expect that ({nkx})k≥1 shows independent behavior for “typical” sequences +(nk)k≥1. Here the word “typical” of course implies that the sequence has to be taken + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +25 +from a generic set in some appropriate space which possesses a measure, so quite +naturally this idea leads to considering “random” sequences (nk)k≥1 = (nk(ω))k≥1 +which are constructed in a randomized way over some probability space. +Of course there are many possible ways how a random sequence can be constructed. +From results of Salem and Zygmund [204] for trigonometric sums with random signs +it follows easily that if we define a sequence (nk)k≥1 by flipping a coin (independently) +for every positive integer to decide whether it should be contained in the sequence +or not, and let P denote the probability measure on the space over which the “coins” +are defined, then for P-almost all sequences as defined above one has +(24) +1 +√ +N +N +� +k=1 +cos(2πnkx) +D +−→ N(0, 1/4) +and +(25) +lim sup +N→∞ +1 +√2N log log N +N +� +k=1 +cos(2πnkx) = 1 +2 +for almost all x, +where N(0, σ2) denotes the normal distribution with mean 0 and variance σ2 and +D +−→ denotes convergence in distribution. Note that (24) and (25) are not exactly +matching with the truly independent case, where the limit distribution would be +N(0, 1/2) and the limsup in the LIL would be 1/ +√ +2. The “loss” on the right-hand +sides of (24) and (25) comes from the fact that a Dirichlet kernel is “hiding” in this +linearly growing sequence, and this kernel is highly localized near 0 and 1 so that its +contribution is lost in the CLT and LIL. By the strong law of large numbers (SLLN) +clearly nk ∼ 2k as k → ∞, P-almost surely, so the sequences constructed here are +very far from satisfying any substantial gap condition; in contrast, their (typical) +order of growth is only linear. It should be noted that the gaps nk+1 − nk in this +sequence are not bounded: with full P-probability, nk+1 −nk = 1 for infinitely many +k (roughly, in half of the cases), but for infinitely many k, the gap nk+1 − nk has +order of magnitude c log k; this follows from the “pure heads” theorem of Erd˝os and +R´enyi, see [198]. +We call an increasing sequence (nk)k≥1 of positive integers a B2 sequence if there +exists a constant C > 0 such that for any integer ν > 0 the number of representations +of ν in the form ν = nk ±nℓ, k > ℓ ≥ 1, is at most C. By a result of Gaposhkin [131] +already mentioned in Section 4, the sequence (f(nkx))k≥1 satisfies the CLT for all +Hadamard lacunary (nk)k≥1 and all 1-periodic Lipschitz continuous f if and only if +for any m ≥ 1, the set-theoretic union of the sequences (nk)≥1, (2nk)≥1, . . . , (mnk)≥1 +satisfies the B2 condition.5 +No similarly complete result is known for sequences +(nk)k≥1 growing slower than exponentially, but Berkes [54] proved that if (nk)k≥1 is +5Note that the definition of the B2 property used in [131] is slightly different from the standard +usage in number theory (see e.g. [134]) requiring that the number of solutions of ν = nk + nℓ, k > +ℓ ≥ 1, is bounded by C, but this does not affect the discussion below. + +26 +C. AISTLEITNER, I. BERKES AND R. TICHY +a B2 sequence satisfying the gap condition +(26) +nk+1/nk ≥ 1 + ck−α, +k ≥ 1, +for some c > 0, α > 0, then (cos(2πnkx))k≥1 satisfies the CLT and LIL. To verify +the B2 property for a concrete sequence (nk)k≥1 is generally a difficult problem, but +the situation is quite different for random constructions. Let I1, I2, . . . be disjoint +blocks of consecutive integers and let n1, n2, . . . be independent random variables +on some probability space (Ω, F, P) such that nk is uniformly distributed over Ik. +Clearly, the number of different sums ±nk1 ± nk2 ± nk3, 1 ≤ k1, k2, k3 ≤ k − 1, is +at most 8(k − 1)3, and thus if the size of Ik is ≥ k5, then the probability that nk +is equal to any of these sums is ≤ 8k3k−5 = O(k−2). Thus by the Borel-Cantelli +lemma, with P-probability 1, such a coincidence can occur only for finitely many k. +Thus the equation +±nk1 ± nk2 ± nk3 ± nk4 = 0, +k1 ≤ k2 ≤ k3 < k4 +has only finitely many solutions, which implies that (nk)k≥1 is a B2 sequence. +Let us recall now that by a result of Erd˝os [102], (cos(2πnkx))k≥1 satisfies the CLT +with limit distribution N(0, 1/2), provided that (26) holds with α < 1/2, and this +result is sharp, i.e. there exists a sequence (nk)k≥1 satisfying (26) with α = 1/2 such +that the CLT fails for (cos(2πnkx))k≥1. Note that the counterexample is irregular: +while nk+1/nk − 1 is of the order O(k−1/2) for most k, there is also a subsequence +along which nk+1/nk → ∞. One may therefore wonder if regular behavior of nk+1/nk +implies the CLT; in particular, Erd˝os [102] conjectured that the CLT holds for +(cos(2πnkx))k≥1 if nk = ⌊e(kβ)⌋ for some β in the range 0 < β ≤ 1/2. (Note that for +β > 1/2 condition (26) is satisfied with α < 1/2, so the CLT follows from Erd˝os’ +result.) This conjecture was proved by Murai [184] for β > 4/9, but for smaller β the +problem is still open. Random constructions provide here important information. +Kaufman [148] proved that if c is chosen at random, with uniform distribution on a +finite interval (a, b) ⊂ (0, ∞), then (cos(2πnkx))k≥1 with nk = e(ckβ) satisfies the CLT +with probability 1 for any fixed β > 0. An even wider class of random sequences with +the CLT property is obtained by choosing the blocks Ik in the random construction +above as the integers in the interval +(27) +Jk = +� +e(ckβ)(1 − rk), e(ckβ)(1 + rk) +� +, +rk = o(k−(1−β)). +A simple calculation shows that these intervals are disjoint for k ≥ k0 and for nk ∈ Jk +we have (26) with α = 1 − β, in fact we even have +nk+1/nk = 1 + c1(1 + o(1))/k1−β +with some constant c1 > 0. Now if rk decreases like a negative power of k, then the +length of Jk will be ≥ k5 and thus the constructed random sequence (nk)k≥1 will +be a B2 sequence with probability 1, so (cos(2πnkx))k≥1 satisfies the CLT. In other +words, the CLT for (cos(2πnkx))k≥1 holds for a huge class of sequences nk ∼ e(ckβ) +for any c > 0, β > 0. + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +27 +Concerning B2 sequences, it is worth pointing out that Erd˝os [101] proved, decades +before Carleson’s convergence theorem, that �∞ +k=1(ak cos(2πnkx) + bk sin(2πnkx)) +is almost everywhere convergent if (nk)k≥1 is a B2 sequence. The question of how +slowly B2 sequences can grow is a much investigated problem of number theory, +see e.g. Halberstam and Roth [134], Chapters II and III. It is easily seen that +a B2 sequence (nk)k≥1 cannot be o(k2) and Erd˝os and R´enyi [105] proved by a +random construction that for any ε > 0 there exists a B2 sequence (nk)k≥1 with +nk = O(k2+ε). Changing the B2 property slightly and requiring that all numbers +nk ± nℓ, k > ℓ, are actually different, makes the problem considerably harder. The +“greedy algorithm” yields a B2 sequence (nk)k≥1 with nk = O(k3), see [180], and +it took nearly 40 years to improve this to nk = o(k3), see [26]. The best currently +known (random) construction is due to Ruzsa [200], and satisfies nk = k1/( +√ +2−1)+o(1). +Let (ωn)n≥1 be a nondecreasing sequence of positive integers tending to +∞ and let +us divide the set of positive integers into disjoint blocks I1, I2, . . . such that the cardi- +nality of Ik is ωk. Using these blocks in the random construction above, the resulting +random sequence (nk)k≥1 cannot be a B2 sequence if (ωn)n≥1 grows slower than any +power of n, but it is proved in Berkes [55] that with P-probability 1, (cos(2πnkx))k≥1 +still satisfies the CLT and LIL. The limit distribution here is N(0, 1/2) and the lim- +sup in the LIL is 1/ +√ +2, so that the “loss of mass” phenomenon observed in the +case of the random sequence (nk)k≥1 in the Salem-Zygmund paper [204] does not +occur here. The gaps in this sequence satisfy nk+1 − nk ≤ 2ωk+1, i.e. they can grow +arbitrarily slowly. An LIL for the discrepancy of ({nkx})k≥1 under the same gap +condition was given in Fukuyama [118]. In [55] the question was raised if there +exists a sequence (nk)k≥1 with bounded gaps nk+1 − nk = O(1) such that the CLT +holds. Bobkov and G¨otze [71] showed that if we want no loss of mass in the CLT, +the answer is negative: if (nk)k≥1 is any increasing sequence of positive integers +with nk+1 − nk ≤ L, k ≥ 1, such that N−1/2 �N +k=1 cos(2πnkx) has a Gaussian limit +distribution N(0, σ2), then necessarily σ2 < 1/2 and L ≥ 1/(1 − 2σ2). On the other +hand, Fukuyama [115, 116, 117] showed that for any σ2 < 1/2 there exists indeed +a random subsequence (cos(2πnkx))k≥1 of the trigonometric system satisfying the +CLT with limit distribution N(0, σ2) and with bounded gaps nk+1 − nk ≤ L with +L ∼ 4/(1 − 2σ2) as σ2 → 1/2. This shows that the result of Bobkov and G¨otze is +optimal up to a factor 4. This remarkable result is the “small gaps” counterpart of +Erd˝os’ central limit theorem [102]: the latter determines the smallest gap sizes in +(nk)k≥1 implying the CLT for (cos(2πnkx))k≥1, while Fukuyama’s result determines +the smallest gap size which still allows a CLT with limit distribution N(0, σ2) to hold. +It is worth pointing out that the bounded gap sequences in [115, 116, 117] are +obtained by rather complicated random constructions, while using the previously +discussed simple construction and choosing the nk as independent random variables +uniformly distributed over adjoining blocks Ik with equal length results in a random + +28 +C. AISTLEITNER, I. BERKES AND R. TICHY +sequence (nk)k≥1 satisfying almost surely +(28) +1 +√ +N +N +� +k=1 +cos(2πnkx) +D +−→ N(0, Y ), +where Y ≥ 0 is a random variable and N(0, Y ) is a “variance mixture” normal +distribution with characteristic function E exp(−Y t2/2), see [71]. We also note that +there is generally no “loss of mass” phenomenon for the LIL for trigonometric series +with bounded gaps, see [23, 24]. For further results for trigonometric series with +bounded/random gaps, see [42, 41, 62]. +8. The subsequence principle +The purpose of the previous sections was to illustrate the principle that thin subse- +quences of the trigonometric system, or thin subsequences of a more general system +of dilated functions, exhibit properties which are typical for sequences of indepen- +dent random variables. +However, an analogous principle holds in a much wider +framework: it is known that, under suitable technical assumptions, sufficiently thin +subsequences of general systems of random variables behave like genuine indepen- +dent sequences, in the sense that a general sequence of random variables allows +to extract a subsequence showing independent behavior. For example, Gaposhkin +[128, 132] and Chatterji [83, 84] proved that if (Xn)n≥1 is any sequence of random +variables satisfying supn EX2 +n < ∞, then there exist a subsequence (Xnk)k≥1 and +random variables X ∈ L2, Y ∈ L1, Y ≥ 0, such that +(29) +1 +√ +N +� +k≤N +(Xnk − X) +D +−→ N(0, Y ) +and +(30) +lim sup +N→∞ +1 +√2N log log N +� +k≤N +(Xnk − X) = Y 1/2 +a.s., +where as at the end of the previous section N(0, Y ) denotes the “variance mix- +ture”normal distribution with characteristic function E exp(−Y t2/2), and where +again +D +−→ denotes convergence in distribution. A functional (Strassen type) ver- +sion of (30) was proved by Berkes [52]. +By a result of Koml´os [159], from any +sequence (Xn)n≥1 of random variables satisfying supn E|Xn| < ∞ one can select a +subsequence (Xnk)k≥1 such that +(31) +lim +N→∞ +1 +N +� +k≤N +Xnk = X +a.s. +for some X ∈ L1. Chatterji [81] proved that if (Xn)n≥1 is a sequence of random vari- +ables satisfying supn E|Xn|p < ∞ for some 0 < p < 2, then there exist a subsequence + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +29 +(Xnk)k≥1 and a random variable X with E|X|p < ∞ such that +(32) +lim +N→∞ +1 +N1/p +� +k≤N +(Xnk − X) = 0 +a.s. +These results establish the analogues of the central limit theorem (CLT), the law +of the iterated logarithm (LIL), the strong law of large numbers (SLLN) and Mar- +czinkiewicz’ strong law for subsequences (Xnk)k≥1. Note the mixed (or randomized) +character of (29)–(32): the limit X in the strong law of large numbers, the cen- +tering factor X in Marczinkiewicz’ strong law, and the limiting variance Y in the +CLT (which also determines the limsup in the LIL) all become random. For fur- +ther limit theorems for subsequences of arbitrary random variable sequences, see +Gaposhkin [128]. On the basis of these and several other examples, Chatterji [82] +formulated the following heuristic principle: +Subsequence Principle. Let T be a probability limit theorem valid for all se- +quences of i.i.d. random variables belonging to an integrability class L defined by +the finiteness of a norm ∥ ·∥L. Then if (Xn)n≥1 is an arbitrary (dependent) sequence +of random variables satisfying supn ∥Xn∥L < +∞ then there exists a subsequence +(Xnk)k≥1 satisfying T in a mixed form. +In a profound study, Aldous [27] proved the validity of the subsequence principle +for all distributional and almost sure limit theorems subject to minor technical +conditions. To formulate his results, let M denote the class of probability measures +on the Borel sets of R, equipped with the L´evy metric. By [27], a subset A ⊂ M×R∞ +is called a limit statute if: +(a) P((λ, X1(ω), X2(ω), . . .) ∈ A) = 1 provided X1, X2, . . . are i.i.d. random vari- +ables with distribution λ. +(b) (λ, x1, x2, . . .) ∈ A and � |xi − x′ +i| < ∞ implies that (λ, x′ +1, x′ +2, . . .) ∈ A. +An a.s. limit theorem can thus be identified with a limit statute, where the analytic +statement of the theorem is expressed by (a), while relation (b) means that a small +perturbation of the sequence X1, X2, . . . does not change the validity of the limit +theorem. Let us give two examples of limit statutes representing the strong law of +large numbers and the law of the iterated logarithm: +A1 = +� +(λ, x) ∈ A : limN→∞ N−1 �N +k=1 xk = |λ|1 +� +∪ {(λ, x) : |λ|1 = ∞}, +A2 = +� +(λ, x) ∈ A : lim supN→∞(2N log log N)−1/2 ��N +k=1 xk − N|λ|1 +� += |λ|2 +� +∪ {(λ, x) : |λ|2 = ∞}. +Here |λ|1 and |λ|2 denote the mean and variance of λ provided they are finite, and +we write |λ|1 = ∞, resp. |λ|2 = ∞ if +� +R |x|dλ(x) = ∞, resp. +� +R |x|2dλ(x) = ∞. + +30 +C. AISTLEITNER, I. BERKES AND R. TICHY +On the other hand, by the definitions in [27], a weak limit theorem for i.i.d. random +variables is a system +T = (f1, f2, . . . , {Gλ, λ ∈ M0}) +where +(a) M0 is a measurable subset of M. +(b) For each k ≥ 1, fk = fk(λ, x1, x2, . . .) is a real function on M × R∞, measurable +in the product topology, satisfying the smoothness condition +|fk(λ, x) − fk(λ, x′)| ≤ +∞ +� +k=1 +ck,i|xi − x′ +i| +where 0 ≤ ck,i ≤ 1 and limk→∞ ck,i = 0 for each i. +(c) For each λ ∈ M0, Gλ is a probability distribution on the real line such that the +map λ → Gλ is measurable (with respect to the Borel σ-field in M0). +(d) If λ ∈ M0 and X1, X2, . . . are independent random variables with common +distribution λ then +fk(λ, X1, X2, . . . , ) +D +−→ Gλ +as k → ∞. +For example, the central limit theorem corresponds to the case when M0 is the class +of distributions with mean 0 and finite variance, +(33) +fk(λ, x1, x2, . . .) = x1 + . . . + xk − kE(λ) +√ +k +and Gλ = N(0, Var(λ)). +Let now (Xn)n≥1 be a sequence of random variables with supn ∥Xn∥L < ∞ with any +norm ∥ · ∥L on R. Then (Xn)n≥1 is bounded in probability, i.e. +lim +K→∞ P(|Xn| > K) = 0 +uniformly in n. +By an extension of the Helly–Bray theorem (see e.g. [66]), (Xn)n≥1 has a subsequence +(Xnk)k≥1 having a limit distribution conditionally on any event in the probability +space with positive probability, i.e. for any A ⊂ Ω with P(A) > 0 there exists a +distribution function FA such that +lim +k→∞ P(Xnk ≤ t | A) = FA(t) +for all continuity points t of FA. +According to the terminology of [66], such a +subsequence is called determining. Thus when investigating asymptotic properties +of sufficiently thin subsequences of sequences (Xn)n≥1 with bounded norms, we can +assume, without loss of generality, that (Xn)n≥1 itself is determining. As is shown +in [27, 66], for any determining sequence (Xn)n≥1 there exists a random measure µ +(i.e. a measurable map from the underlying probability space (Ω, F, P) to M) such +that for any A with P(A) > 0 and any continuity point t of FA we have +(34) +FA(t) = EA(µ(−∞, t]) + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +31 +where EA denotes conditional expectation given A. This measure µ is called the +limit random measure of (Xn)n≥1; see Section 9 below for more details. +With these preparations, we are now in a position to formulate the subsequence +theorems of Aldous. +Theorem A (Aldous [27]). Let (Xn)n≥1 be a determining sequence with limit ran- +dom measure �� and let A be a limit statute. Then there exists a subsequence (Xnk)k≥1 +such that for any further subsequence (Xmk)k≥1 ⊂ (Xnk)k≥1 we have +P((λ(ω), Xm1(ω), Xm2(ω), . . .) ∈ A) = 1. +Theorem B (Aldous [27]). Let (Xn)n≥1 be a determining sequence with limit ran- +dom measure µ and let +T = (f1, f2, . . . , {Gλ, λ ∈ M0}) +be a weak limit theorem. Assume that P(µ ∈ M0) = 1. Then there exists a sub- +sequence (Xnk)k≥1 such that for any further subsequence (Xmk)k≥1 ⊂ (Xnk)k≥1 we +have +lim +k→∞ P(fk(Xm1(ω), Xm2(ω), . . . µ(ω)) ≤ t) = EGµ(ω)(t) +at all continuity points t of the distribution function on the right hand side. +Writing out Theorem A and B in the case of the limit statutes A1, A2 above and +the weak limit theorem defined by (33), we get the CLT, LIL and SLLN for thin +subsequences of determining sequences, as stated in (29), (30), (31) above. +The proof of Koml´os’ result (31) exemplifies the technique used in the field of sub- +sequence behavior before Aldous’ paper [27], and in particular in proving the results +(29)–(32) mentioned above. As Koml´os showed, if (Xn)n≥1 is a sequence of random +variables with bounded L1 norms, then its sufficiently thin subsequences (Xnk)k≥1 +are, after a random centering and small perturbation, an identically distributed +martingale difference sequence with finite means and thus, by classical martingale +theory, they satisfy the SLLN. Martingale versions of the CLT and LIL yield also +relations (29), (30) and their functional versions. While this method yields several +further limit theorems for lacunary sequences, martingale difference sequences cer- +tainly do not satisfy all i.i.d. limit theorems in a randomized form and thus the +general subsequence principle cannot be proved in such a way. The proof of Theo- +rems A and B in [27] uses a different way and utilizes near exchangeability properties +of subsequences of general sequences of random variables. Let (Xn)n≥1 be a deter- +mining sequence with limit random measure µ and let (Yn)n≥1 be a sequence of +random variables, defined on the same probability space as the Xn’s, conditionally +i.i.d. with respect to µ, with conditional distribution µ. (For the construction of +such an (Yn)n≥1 one may need to enlarge the probability space.) Clearly, (Yn)n≥1 +is exchangeable, i.e. for any permutation σ : N → N of the positive integers, the +sequence (Yσ(n))n≥1 has the same distribution as (Yn)n≥1, and it satisfies limit the- +orems of i.i.d. random variables in a mixed form. For example, if EY 2 +1 < ∞ and + +32 +C. AISTLEITNER, I. BERKES AND R. TICHY +Y = E(Y1 | µ), Z = Var (Y1 | µ), then +N−1/2 +N +� +k=1 +(Yk − Y ) +D +−→ N(0, Z) +and +lim sup +N→∞ +(2N log log N)−1/2 +N +� +k=1 +(Yk − Y ) = Z1/2 +a.s. +This principle holds in full generality, i.e. for all a.s. and distributional limit theorems +in the above formalization. Indeed, if the Yn are conditionally i.i.d. with respect to +µ and with conditional distribution µ (a random probability measure on R) and if +A is a limit statute, then +(35) +P((µ, Y1, Y2, . . .) ∈ A|µ)(ω) = P(µ(ω), Y ∗ +1 , Y ∗ +2 , . . .) ∈ A) +a.e. +where (Y ∗ +n )n≥1 is an i.i.d. sequence with marginal distribution µ(ω). By the definition +of limit statute, the last probability in (35) equals 1 and taking expectations we get +P((µ, Y1, Y2, . . .) ∈ A) = 1, +which is exactly our claim. Specializing to the case of the limit statutes A1 and A2 +above, we get relations (29) and (30). A similar argument works for distributional +limit theorems. Now, as is shown in [27], for every k ≥ 1 we have +(36) +(Xn1, Xn2, . . . Xnk) +D +−→ (Y1, Y2, . . . , Yk) +as +n1 < n2 < . . . < nk, n1 → ∞. +In other words, for large indices the finite dimensional distributions of the sequence +(Xnk)k≥1 are close to those of the limiting exchangeable sequence (Yk)k≥1 and thus +one may expect that limit theorems of (Yk)k≥1 (which, as we have just seen, are +mixed versions of i.i.d. limit theorems) continue to hold for sufficiently thin subse- +quences (Xnk)k≥1 as well. Of course, a limit theorem for (Xnk)k≥1 can describe a +complicated analytic property of the infinite vector (Xn1, Xn2, . . . , Xnk, . . .) which +does not follow from the weak convergence of the finite dimensional distributions +of the sequence, but with a suitable thinning procedure and delicate analytic ar- +guments, Aldous showed an infinite dimensional extension of (36), leading to the +validity of Theorems A and B. +Although the theorems of Aldous are of exceptional generality, there are important +results for lacunary sequences which are not covered by them. As was shown by +Gaposhkin [128], for every uniformly bounded sequence (Xn)n≥1 of random variables +there exists a subsequence (Xnk)k≥1 and bounded random variables X and Y ≥ 0 +such that for any numerical sequence (an)n≥1 satisfying +(37) +AN := +N +� +k=1 +a2 +k → ∞, +aN = o(A1/2 +N ) + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +33 +we have +(38) +1 +AN +N +� +k=1 +ak(Xnk − X) +D +−→ N(0, Y ), +and if the second relation of (37) is replaced by +(39) +aN = o(AN/(log log AN)1/2) +then we have +(40) +lim sup +N→∞ +1 +� +2A2 +N log log AN +N +� +k=1 +ak(Xnk − X) = Y 1/2 +a.s. +The difference of these results from (29) and (30) is that in the CLT and LIL we have +weighted sums �N +k=1 ak(Xnk −X) instead of ordinary sums �N +k=1(Xnk −X). For ev- +ery fixed coefficient sequence (an)n≥1 the CLT and LIL in (38) and (39) follow from +Theorems A and B, but the subsequence (Xnk)k≥1 provided by the proofs depends +on (ak)k≥1 and it is not clear that we can select a subsequence (Xnk)k≥1 satisfying +(38) and (39) simultaneously for all considered coefficient sequences (ak)k≥1. +Another important situation not covered by Aldous’ general theorems is when we +investigate permutation-invariance of limit theorems for subsequences. +Since the +asymptotic properties of an exchangeable sequence (Yn)n≥1 do not change after any +permutation of its terms, it is natural to expect that the conclusions in Theorem A +and B remain valid after an arbitrary permutation of the subsequence (Xnk)k≥1 +in the theorems. However, the proofs of Theorem A and B are not permutation- +invariant and it does not follow that, e.g., any sequence (Xn)n≥1 of random variables +with bounded L1 norms contains a subsequence (Xnk)k≥1 satisfying the strong law +of large numbers after any permutation of its terms. Using ad hoc methods, the +latter result has been proved by Berkes [56] and another classical case, namely the +unconditional a.e. convergence of series � ck(Xnk − X) under � c2 +k < ∞ for subse- +quences (Xnk)k≥1 of L2 bounded sequences (Xn)n≥1, has been settled by Koml´os [160] +(see [27] for another proof via exchangeability). It clearly would be desirable to pro- +vide further general results in this direction. +We now formulate some structure theorems for lacunary sequences enabling one to +handle problems of the kind discussed above. Recall that if (Xn)n≥1 is a determin- +ing sequence with limit random measure µ and (Yn)n≥1 is a sequence conditionally +i.i.d. with respect to the σ-algebra generated by µ and with conditional marginal +distributions µ, then there exists a subsequence (Xnk)k≥1 such that (36) holds. This +shows that, in some sense, for large indices the sequence (Xnk)k≥1 resembles the +sequence (Yk)k≥1, but this property is far too weak to deduce limit theorems for +(Xnk)k≥1 from those valid for the exchangeable sequence (Yk)k≥1. The following +theorem, proved by Berkes and P´eter [63], shows that with a suitable choice of the +subsequence (nk)k≥1, the variables (Xnk)k≥1 can be chosen to be close to the Yk in +a pointwise sense. We call a sequence (Xn)n≥1 of random variables ε-exchangeable + +34 +C. AISTLEITNER, I. BERKES AND R. TICHY +if on the same probability space there exists an exchangeable sequence (Yn)n≥1 such +that P(|Xn − Yn| ≥ ε) ≤ ε for all n. Then we have +Theorem C (Berkes and P´eter [63]). Let (Xn)n≥1 be a sequence of random variables +bounded in probability, and let (εn)n≥1 be a sequence of positive reals tending to zero. +Then, if the underlying probability space is large enough, thee exists a subsequence +(Xnk)k≥1 such that, for all l ≥ 1, the sequence Xnl, Xnl+1, . . . is εl-exchangeable. +Note that Theorem C provides a different approximating exchangeable sequence +(Y (l) +j )j≥1 for each tail sequence (Xnl, Xnl+1, . . .), with termwise approximating error +εl. The following theorem describes precisely the structure of the the sequences +(Y (l) +j )j≥1. +Theorem D (Berkes and P´eter [63]). Let (Xn)n≥1 be a determining sequence of +random variables, and let (εn)n≥1 be a sequence of positive reals. Then there exists +a subsequence (Xmk)k≥1 and a sequence (Yk)k≥1 of discrete random variables such +that +(41) +P +� +|Xmk − Yk| ≥ εk +� +≤ εk +k = 1, 2 . . . , +and for each k > 1 the atoms of the finite σ-field σ{Y1, . . . , Yk−1} can be divided into +two classes Γ1 and Γ2 such that the following holds. Firstly, +(42) +� +B∈Γ1 +P(B) ≤ εk. +Secondly, for any B ∈ Γ2 there exist PB-independent random variables {Z(B) +j +, j = +k, k + 1, . . . } defined on B with common distribution function FB such that +(43) +PB +� +|Yj − Z(B) +j +| ≥ εk +� +≤ εk, +j = k, k + 1, . . . +Here FB denotes the limit distribution of (Xn)n≥1 relative to B and PB denotes +conditional probability given B. +We now give applications of Theorem D to the problems discussed above. First we +note that using Theorem D it is a simple exercise to prove, for suitable subsequences +of a uniformly bounded sequences (Xn)n≥1, the weighted CLT and LIL in (38), +(40) simultaneously for all permitted coefficient sequences (an)n≥1. Next we give a +permutation-invariant form of Theorem B for distributional limit theorems. +Definition 1. We call the weak limit theorem T = (f1, f2, . . . , S, {Gµ, µ ∈ M0}) +regular if there exist sequences pk ≤ qk of positive integers tending to +∞ and a +sequence ωk → +∞ such that +(i) fk(λ, x1, x2, . . .) depends only on λ, xpk, . . . , xqk. +(ii) fk satisfies the Lipschitz condition +|fk(λ, xpk, . . . , xqk) − fk(λ′, x′ +pk, . . . , x′ +qk)| ≤ +≤ 1 +ωk +qk +� +i=pk +|xi − x′ +i|α + ̺∗(λ, λ′) + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +35 +for some 0 < α ≤ 1, where ̺∗ is a metric on M0 generating the same topology +as the Prohorov metric ̺. +For example, the central limit theorem can be formalized by the functions +fk(λ, x[k1/4], . . . , xk) = x[k1/4] + . . . + xk − kE(λ) +√ +k +, +leading to a regular limit theorem. Note that originally we formalized the CLT with +the functions fk in (33) containing all variables x1, x2, . . ., but under bounded second +moments the first k1/4 terms here are irrelevant and hence we can always switch to +the present version. The same procedure applies in the general case. +Theorem E (Aistleitner, Berkes and Tichy [20]). Let (Xn)n≥1 be a determining +sequence with limit random measure ˜µ. Let T = (f1, f2, . . . , S, {Gµ, µ ∈ M0}) be a +regular weak limit theorem and assume that P(˜µ ∈ M0) = 1. Then there exists a +subsequence (Xnk)k≥1 such that for any permutation (X∗ +k)k≥1 of (Xnk)k≥1 we have +(44) +fk(X∗ +1, X∗ +2, . . . , ˜µ) →d +� +G˜µdP. +In case of the CLT formalized above, assuming supn EX2 +n < +∞ implies easily that +˜µ has finite variance almost surely, and thus denoting its mean and variance by X +and Y , respectively, we see that the integral in (44) is the distribution N(0, Y ). +Hence (44) states in the present case that +1 +√ +N +N +� +k=1 +(X∗ +k − X) +D +−→ N(0, Y ), +which is the permutation-invariant form of the CLT. +Concerning a.s. limit theorems, a permutation-invariant form of the strong law of +large numbers for subsequences of an L1-bounded sequence was proved, as already +mentioned, in Berkes [56], and a similar argument yields the corresponding result for +the LIL. No permutation-invariant version of the general result in Theorem A has +been proved in the literature, but there is no need for that, since a.s. limit theorems +can be reformulated in a distributional form and thus the proof of Theorem B applies +with obvious changes. For illustration, we give here the reformulation of the LIL: +Theorem F. Let (Xn)n≥1 be a sequence of random variables with E|Xn| ≤ 1, n = +1, 2, . . . Put Sn = �n +i=1 Xi, Sk,l = �l +i=k+1 Xi, and L(N) = (2N log log N)1/2. Then +lim supN→∞ SN/L(N) = 1 a.s. iff for any ε > 0 there exists a sequence m1 < m2 < +· · · of positive integers such that mk ≥ 5k and +P +� +max +mk≤j≤mk+1 +Sk,j +L(j) > 1 + ε +� +≤ 2−k, +k ≥ k0, +and +P +� +max +mk≤j≤mk+1 +Sk,j +L(j) < 1 − ε +� +≤ 2−k, +k ≥ k0. + +36 +C. AISTLEITNER, I. BERKES AND R. TICHY +It is worth pointing out that given a sequence (Xn)n≥1 of random variables, find- +ing a subsequence (Xnk)k≥1 satisfying the permutation-invariant form of some limit +theorem generally requires a much faster growing sequence (nk)k≥1 than to find a +subsequence to satisfy the original limit theorem. This is a phenomenon which also +occurs for lacunary trigonometric sums or lacunary sums of dilated functions; com- +pare the last paragraph of Section 4 above. +In conclusion we note that if (Xn)n≥1 is a sequence of random variables with fi- +nite means over the probability space (0, 1) equipped with the Borel σ-algebra and +Lebesgue measure such that for all n ≥ 1 and (a1, . . . , an) ∈ Rn we have +(45) +C1 +� n +� +k=1 +|ak|p +�1/p +≤ E +����� +n +� +k=1 +akXk +����� ≤ C1 +� n +� +k=1 +|ak|p +�1/p +for some p ≥ 1 and positive constants C1, C2, then the closed subspace of L1(0, 1) +spanned by the Xn is isomorphic with the ℓp space (Hilbert space if p = 2). Relation +(45) holds, in particular, if the Xn are i.i.d. symmetric p-stable random variables with +p > 1, i.e. their characteristic function (Fourier transform) is given by exp(−c|t|p) +with some c > 0. Thus applying the subsequence principle to the “limit theorem” +(45) provides important information on the subspace structure of L1(0, 1). Using this +method, Aldous [28] proved the famous conjecture that every infinite dimensional +closed subspace of L1(0, 1) contains an isomorphic copy of ℓp for some 1 ≤ p ≤ 2. For +a further application of this method, see an improvement of the classical theorem of +Kadec and Pe�lczy´nski [147] on the subspace structure on Lp, p > 2, in Berkes and +Tichy [67]. +9. New results: Exact criteria for the central limit theorem for +subsequences +By the classical resonance theorem of Landau [163], for a real sequence (xn)n≥1 +the series �∞ +n=1 anxn converges for all (an)n≥1 ∈ ℓp (1 ≤ p ≤ ∞) if and only if +(xn)n≥1 ∈ ℓq, where 1/p + 1/q = 1. A deep extension of this result to the case of +function series was given by Nikishin [190]. We call a sequence (fn)n≥1 of measurable +functions on (0, 1) a convergence system in measure for ℓp if for any real sequence +(an)n≥1 ∈ ℓp the series �∞ +n=1 anfn converges in measure. In the case p = 2 Nikishin +proved the following result. +Theorem G (Nikishin [190, 191]). A function system (fn)n≥1 over (0, 1) is a conver- +gence system in measure for ℓ2 if and only if for any ε > 0 there exists a measurable +set Aε ⊂ (0, 1) with measure exceeding 1 − ε and a constant Kε > 0 such that for all +N ≥ 1 and all (a1, . . . , aN) ∈ RN we have +(46) +� +Aε +� N +� +n=1 +anfn +�2 +dx ≤ Kε +N +� +n=1 +a2 +n. +The sufficiency of (46) is obvious, so the essential (and highly remarkable) state- +ment is the converse: if a sequence (fn)n≥1 is a convergence system in measure for + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +37 +ℓ2, then, except for a subset of (0, 1) with arbitrary small measure, (fn)n≥1 behaves +like an orthonormal sequence. +In the previous section we discussed the subsequence principle stating that suffi- +ciently thin subsequences of arbitrary sequences of random variables, subject to +mild boundedness conditions, satisfy “all” limit theorems for i.i.d. random variables +in a mixed (randomized) form. A typical special case of this principle is the following +result: +Theorem H (Gaposhkin [132]). Let (Xn)n≥1 be a sequence of random variables +satisfying +(47) +sup +n +EX2 +n < +∞. +Then there exists a subsequence (Xnk)k≥1 together with random variables X and +Y ≥ 0 such that for any further subsequence (Xmk)k≥1 of (Xnk)k≥1 we have +(48) +1 +√ +N +N +� +k=1 +(Xmk − X) +D +−→ N(0, Y ), +where N(0, Y ) denotes the “variance mixture” normal distribution with characteris- +tic function E exp(−Y t2/2). +If (X2 +n)n≥1 is uniformly integrable then by well-known compactness results (see e.g. +[99]) there exist a subsequence (Xmk)k≥1 and random variables X ∈ L2 and Y ∈ L1/2, +Y ≥ 0, such that +(49) +Xmk → X weakly in L2, +(Xmk − X)2 → Y 2 weakly in L1.6 +As Gaposhkin [128] showed, in this case the random variables X, Y in (48) can be +chosen as in (49). +In Theorem H, condition (47) is not necessary: simple examples show (see below) +that there exist sequences (Xn)n≥1 of random variables without any finite moments, +but having subsequences satisfying (48). The purpose of this section is to give nec- +essary and sufficient conditions for the existence of subsequences (Xnk)k≥1 satisfying +the randomized CLT (48), and it will turn out that our conditions have the same +character as Nikishin’s conditions for the existence of a subsequence being a con- +vergence system, i.e. “nice” behavior of the sequence on subsets of the probability +space with measure as close to 1 as we wish. +To formulate our results, call a sequence (Xn)n≥1 of random variables nontrivial if +it has no subsequence converging with positive probability. It is easily seen that +for non-degenerate sequences the random variable Y in Theorem H is almost surely +6A sequence (ξn)n≥1 of random variables in Lp, p ≥ 1, is said to converge weakly to ξ ∈ Lp +if E(ξnη) → E(ξη) for any η ∈ Lq, where 1/p + 1/q = 1. This type of convergence should not +be confused with weak convergence of probability measures and distributions, called generally +convergence in distribution, and denoted by +D +−→. + +38 +C. AISTLEITNER, I. BERKES AND R. TICHY +positive and Gaposhkin’s theorem can be rewritten in a form involving a pure (i.e. +not mixed) Gaussian limit distribution. +Theorem J. Let (Xn)n≥1 be a nontrivial sequence of random variables satisfying +(47). Then there exists a subsequence (Xnk)k≥1 and random variables X, Y with +Y > 0 such that for all subsequences (Xmk)k≥1 of (Xnk)k≥1 and for any set A in the +probability space with P(A) > 0 we have +(50) +PA +��N +k=1(Xmk − X) +Y +√ +N +< t +� +→ Φ(t) +for all t. +Here PA denotes the conditional probability with respect to A, and Φ is the cumulative +distribution function of the standard normal distribution. +The nontriviality of (Xn)n≥1 is assumed here to avoid degenerate cases. If Xnk → X +on some set A with positive probability then for any sufficiently thin subsequence +(Xmk)k≥1 of (Xnk)k≥1 we have � |Xmk − X| < +∞ a.s. on A, and consequently +a−1 +N +N +� +k=1 +(Xmk − X) → 0 +a.s. on A +for any norming sequence aN → ∞ (random or not). Since for any sequence (Xn)n≥1 +satisfying (47) (and in fact any tight sequence (Xn)n≥1) there is a subsequence +(Xnk)k≥1 and a measurable partition A ∪ B of the probability space such that Xnk +converges on A and is nontrivial on B, there is no loss of generality in assuming that +(Xn)n≥1 is nontrivial. +Clearly, if (Xn)n≥1 satisfies the conclusion of Theorem J, then so does the sequence +(Xn + 2−nZ)n≥1 for any a.s. finite random variable Z, and thus the assumption (47) +is, as stated above, not necessary in Theorem J. Below we will give necessary and suf- +ficient condition for the CLT for lacunary subsequences of a given sequence (Xn)n≥1 +of random variables without any moment assumption on (Xn)n≥1. To formulate our +results, let us note that if all subsequences (Xmk)k≥1 of a sequence (Xn)n≥1 satisfy +(50) for some random variables X, Y , then (Xn)n≥1 is bounded in probability (see +Lemma 2 below). As mentioned in the previous section, every sequence (Xn)n≥1 of +random variables bounded in probability has a subsequence (Xnk)k≥1 which has a +limit distribution relative to every set A of the probability space with P(A) > 0. +Such a sequence was called determining. This concept is the same as that of stable +convergence, introduced by R´enyi [197]; our terminology follows that of functional +analysis. Hence in our investigations we can assume without loss of generality that +the original sequence (Xn)n≥1 is determining. Now if (Xn)n≥1 is determining and FA +denotes its limit distribution relative to the set A, then, as we noted in the previous +section, there exists a random measure µ (called the limit random measure of (Xn)) +such that +(51) +FA(t) = EA(µ(−∞, t]) + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +39 +for any continuity point t of FΩ, where EA denotes conditional expectation relative +to A. Let F• denote the distribution function of µ; we shall call it the limit random +distribution of (Xn)n≥1. We can state now our first new theorem. +Theorem 1. Let (Xn)n≥1 be a nontrivial sequence of random variables. Then the +following statements are equivalent: +A) There exist a subsequence (Xnk)k≥1 and random variables X, Y with Y > 0 such +that (50) holds for all subsequences (Xmk)k≥1 of (Xnk)k≥1 and for any set A ⊂ Ω +with P(A) > 0. +B) For every ε > 0 there is a subsequence (Xnk)k≥1 and a set Aε ⊂ Ω with P(Aε) ≥ +1 − ε such that +(52) +sup +k +� +Aε +X2 +nkdP < +∞. +If (Xn)n≥1 is determining, then two further equivalent statements are: +C) We have +(53) ++∞ +� +−∞ +x2dF•(x) < +∞ +almost surely. +D) For every ε > 0 there exists a set Aε ⊂ Ω with P(Aε) ≥ 1 − ε such that +(54) ++∞ +� +−∞ +x2dFAε(x) < +∞. +Our second new theorem characterizes sequences (Xn)n≥1 for which (50) holds with +X ∈ L2, Y ∈ L1/2. +Theorem 2. Let (Xn)n≥1 be a nontrivial sequence of random variables defined on an +atomless probability space (Ω, F, P). Then the following statements are equivalent: +A) There exists a subsequence (Xnk)k≥1 and random variables X, Y with Y > 0, +X ∈ L2, Y ∈ L1/2 such that (50) holds for all subsequences (Xmk)k≥1 of (Xnk)k≥1 +and all sets A ⊂ Ω with P(A) > 0. +B) There exists a subsequence (Xnk)k≥1 and sequences (Yk)k≥1, (τk)k≥1 of random +variables satisfying +(55) +Xnk = Yk + τk, +where +(56) +sup +k +EY 2 +k < +∞, +� +k +|τk| < +∞ +a.s. + +40 +C. AISTLEITNER, I. BERKES AND R. TICHY +If (Xn)n≥1 has a limit distribution F, then a third equivalent statement is: +C) We have +(57) ++∞ +� +−∞ +x2dF(x) < +∞. +In other words, for the validity of (50) with X ∈ L2, Y ∈ L1/2, assumption (47) is +necessary and sufficient after a small perturbation of (Xn)n≥1, and for identically +distributed (Xn)n≥1 even this perturbation is not needed. A particularly simple case +when X ∈ L2, Y ∈ L1/2 is satisfied is when X, Y are nonrandom. +A trivial example showing the difference between condition (D) of Theorem 1 and +condition (C) of Theorem 2 is the following. Let {Hk, k ≥ 1} be a partition of +the probability space with P(Hk) = 2−k for k = 1, 2, . . . , and let (Xn)n≥1 be a +sequence of random variables on this space which is conditionally i.i.d. given each +Hk with mean 0 and variance 2k. +Then (Xn)n≥1 is nontrivial, determining and +clearly satisfies condition (D) of Theorem 1, but since it is identically distributed +(in fact exchangeable) and since EX2 +1 = +∞, condition (C) of Theorem 2 is not +satisfied. +9.1. Some lemmas. The key for the proof of our theorems is a general structure +theorem for lacunary sequences which was proved in [63], and which was stated as +Theorem D in the previous section. Furthermore, we need the following lemmas. +Lemma 1. Let (Xn)n≥1 be a sequence of random variables such that for some ran- +dom variables X, Y with Y > 0 and for all subsequences (Xnk)k≥1 we have +(58) +N� +k=1 +(Xnk − X) +Y +√ +N +D +−→ N(0, 1). +Then (Xn)n≥1 is bounded in probability. +Proof. Clearly (58) implies that the sequence (XnN − X)/(Y +√ +N) is bounded in +probability as N → ∞, and thus XnN/ +√ +N is bounded in probability for any sub- +sequence (nk)k≥1. If (Xn)n≥1 were not bounded in probability then one could find +a subsequence (mk)k≥1 and a constant c > 0 such that P(|Xmk| ≥ k) ≥ c for +k = 1, 2, . . . , i.e. Xmk/ +√ +k would not be bounded in probability, a contradiction. +□ +Lemma 2. Let (Xn)n≥1 be a sequence of random variables and assume that for some +random variables X and Y > 0 and all sets A ⊂ Ω with P(A) > 0 we have +(59) +PA + + + + + +N� +k=1 +(Xk − X) +Y +√ +N +< t + + + + + → Φ(t) +for all t. + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +41 +Assume further that (59) remains valid if we replace X, Y by some random variables +X∗ and Y ∗ > 0. Then X = X∗ a.s. and Y = Y ∗ a.s. +Proof. From the assumption it follows that the sequences +N−1/2 +N +� +k=1 +(Xk − X) +and +N−1/2 +N +� +k=1 +(Xk − X∗) +are bounded in probability, and thus the same holds for their difference +√ +N(X−X∗), +whence X = X∗ a.s. To prove Y = Y ∗, fix c > 1 and set A = {Y ∗ ≥ cY }. If +P(A) > 0 then clearly we cannot have both (59) and the analogous relation with +Y replaced by Y ∗. Thus P(A) > 0 for all c > 1 whence Y ∗ ≤ Y a.s. The same +argument yields Y ≤ Y ∗ a.s., completing the proof. +□ +Lemma 3. Let X1, X2, . . . , Xn be i.i.d. random variables with distribution function +F and set Sn = X1 + · · · + Xn. Then for any t > 0 we have +(60) +P(|Sn| ≤ 2t) ≤ A t +√n + + + +� +|x|≤t +x2dF(x) − 2 + + + +� +|x|≤t +xdF(x) + + + +2 + + +−1/2 +, +provided the difference on the right-hand side is positive and +� +|x|≤t +dF(x) ≥ 1/2. Here +A is an absolute constant. +Proof. Let F ∗ denote the distribution function obtained from F by symmetrization. +From a well-known concentration function inequality of Esseen [106, Theorem 2] it +follows that the left-hand side of (60) cannot exceed +A1 +t +√n + + + +� +|x|≤2t +x2dF ∗(x) + + + +−1/2 +, +where A1 is an absolute constant. +Hence to prove (60) it suffices to show that +� +|x|≤t +dF(x) ≥ 1/2 implies +(61) +� +|x|≤2t +x2dF ∗(x) ≥ +� +|x|≤t +x2dF(x) − 2 + + + +� +|x|≤t +xdF(x) + + + +2 +. +Let ξ and η be independent random variables with distribution function F, and set +C = {|ξ − η| ≤ 2t}, +D = {|ξ| ≤ t, |η| ≤ t}. +Then +� +|x|≤2t +x2dF ∗(x) = +� +C +(ξ − η)2dP + +42 +C. AISTLEITNER, I. BERKES AND R. TICHY +≥ +� +D +(ξ − η)2dP += 2 +� +|ξ|≤t +ξ2dP · P(|η| ≤ t) − 2 + + + +� +|ξ|≤t +ξdP + + + +2 +≥ +� +|ξ|≤t +ξ2dP − 2 + + + +� +|ξ|≤t +ξdP + + + +2 +, +provided P(|η| ≤ t) ≥ 1/2. Thus (61) is valid. +□ +Lemma 4. Let (Ω, F, P) be an atomless probability space and X1, X2, . . . a se- +quence of random variables on (Ω, F, P) with limit distribution F. Then there exist +a subsequence (Xnk)k≥1 and sequences (Yk)k≥1 and (τk)k≥1 of random variables on +(Ω, F, P) such that Xnk = Yk + τk, k = 1, 2, . . . , such that the random variables Yk +have distribution function F, and such that � +k |τk| < +∞ a.s. +Proof. Let ( ˆXn)n≥1 be discrete random variables such that P(|Xn − X′ +n| ≥ 2−n) ≤ +2−n, n = 1, 2, . . . , and denote by Fn the distribution function of Xn. Clearly Fn → F +and thus εn := ̺(Fn, F) → 0, where ̺ denotes the Prohorov distance. By a theorem +of Strassen [8] there exists a probability measure µn on R2 with marginals Fn and +F such that +µn((x, y) : |x − y| ≥ εn) ≤ εn. +Let c be a possible value of ˆXn. Since the probability space restricted to A = { ˆXn = +c} is atomless, there exists a random variable Vn on this space such that +PA(Vn < t) = µn((x, y) : x = c, y < t) +µn((x, y) : x = c) +for all t. Carrying out this construction for all possible values of c in the range of +ˆXn, we get a random variable Vn defined on the whole probability space such that +the joint distribution of ˆXn and Vn is µn. Clearly the distribution of Vn is F and +P(| ˆXn − Vn| ≥ εn) ≤ εn. Choosing (nk)k≥1 so that εnk ≤ 2−k we get +P +� +| ˆXnk − Vnk| ≥ 2−k� +≤ 2−k, +i.e. +P +� +|Xnk − Vnk| ≥ 2 · 2−k� +≤ 2 · 2−k +and thus � +k |Xnk − Vnk| < +∞ a.s. by the Borel–Cantelli lemma. Thus the de- +composition Xnk = Yk + τk, where Yk = Vnk and τk = Xnk − Vnk, satisfies the +requirements. +□ +Our final two lemmas concern the properties of the limit random distribution of +determining sequences. + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +43 +Lemma 5. Let (Xn)n≥1 be a determining sequence of random variables with limit +random distribution F. Then for any set A ⊂ Ω with P(A) > 0 we have +(62) +EA + + ++∞ +� +−∞ +x2dF•(x) + + = ++∞ +� +−∞ +x2dFA(x), +in the sense that if one side is finite then the other side is also finite and the two +sides are equal. The statement remains valid if in (62) we replace the interval of +integrations by (−t, t), provided t and −t are continuity points of FA. +Proof. This lemma follows easily from (51) by integration by parts. +□ +Lemma 6. Let X, X1, X2, . . . be random variables such that both sequences (Xn)n≥1 +and (Xn − X)n≥1 are determining; let F• and G• denote, respectively, their limit +random distributions. Then ++∞ +� +−∞ +x2dG•(x) < +∞ a.s. implies ++∞ +� +−∞ +x2dF•(x) < +∞ +a.s. and conversely. +Proof. Let ε > 0 and choose a set A ⊂ Ω such that P(A) ≥ 1 − ε and on A +both X and ++∞ +� +−∞ +x2dF•(x) are bounded. Let FA and GA denote the limit random +distribution of (Xn)n≥1 resp. (Xn − X)n≥1 relative to A. Replacing Xn by Xn + τn +where τn → 0 a.s. clearly does not change the limit distributions FA, GA, F•, G•, and +thus by passing to a subsequence and using Lemma 4 we can assume, without loss +of generality, that the Xn are identically distributed on A. Then +EAX2 +1 = EAX2 +2 = · · · = ++∞ +� +−∞ +x2dFA(x), +where the last integral is finite by the boundedness of ++∞ +� +−∞ +x2dF•(x) on A and +Lemma 5. By Minkowski’s inequality and the boundedness of X on A it follows +that EA((Xn − X)2) is also bounded, and thus Fatou’s lemma implies that ++∞ +� +−∞ +x2dGA(x) ≤ lim inf +n→∞ EA +� +(Xn − X)2� +< +∞. +Using Lemma 5 again it follows that ++∞ +� +−∞ +x2dG•(x) < +∞ a.s. on A. As the measure +of A can be chosen arbitrarily close to 1, we get +� +x2dG•(x) < +∞ a.s., as required. +□ +9.2. Proof of the theorems. We begin with the proof of Theorem 1. Using diag- +onalization and Chebyshev’s inequality it follows that if a sequence (Xn)n≥1 satisfies +(B), then it has a subsequence bounded in probability and thus also a determining +subsequence. By Lemma 1 the same conclusion holds if (Xn)n≥1 satisfies (A). Thus + +44 +C. AISTLEITNER, I. BERKES AND R. TICHY +to prove our theorem it suffices to prove the equivalence of (A), (B), (C), (D) for +determining sequences (Xn)n≥1. In what follows we shall prove the implications +(A) =⇒ (C) =⇒ (D) =⇒ (B); since (B) =⇒ (A) follows easily from Theorem D in +the previous section by diagonalization, this will prove Theorem 1. +Assume that (Xn)n≥1 is a determining sequence satisfying (A), i.e. there exists a +subsequence (Xnk)k≥1 and random variables X, Y with Y > 0 such that for any +further subsequence (Xmk)k≥1 of (Xnk)k≥1 and any set A ⊂ Ω with P(A) > 0 we +have +(63) +PA + + + + + +N� +k=1 +(Xmk − X) +Y +√ +N +< t + + + + + → Φ(t) +for all t. +We claim that (Xn)n≥1 satisfies (C). Clearly we can assume without loss of generality +that (Xnk)k≥1 = (Xk)k≥1 and since (Xn−X)k≥1 contains a determining subsequence, +we can assume also that (Xn − X)n≥1 itself is determining. Moreover, since (Xn − +X)n≥1 satisfies (C) if and only if (Xn)n≥1 does (see Lemma 6), we can assume that +X = 0. Assume indirectly that (Xn)n≥1 does not satisfy (C), i.e. there exists a set +B ⊂ Ω with P(B) > 0 such that +(64) +lim +t→∞ +t +� +−t +x2dF•(x) = +∞ +on B. +Then there exists a set B∗ ⊂ B with P(B∗) ≥ P(B)/2 such that on B∗ the random +variable Y is bounded and (63) holds uniformly, i.e. there exists a constant K > 0 +and a numerical sequence Kt → +∞ such that +t +� +−t +x2dF•(x) ≥ Kt and Y ≤ K on B∗. +Also, 1 − F•(t) + F•(−t) → 0 a.s. as t → ∞, and thus we can choose a set B∗∗ ⊂ +B∗ with P(B∗∗) ≥ P(B∗)/2 such that on B∗∗ the last convergence relation holds +uniformly, i.e. there exists a positive numerical sequence εt ց 0 such that +(65) +1 − F•(t) + F•(−t) ≤ εt on B∗∗. +We show that there exists a subsequence (Xmk)k≥1 of (Xnk)k≥1 such that (63) fails +for A = B∗∗. Since our argument will involve the sequence (Xn)n≥1 only on the set +B∗∗, in the sequel we can assume, without loss of generality, that B∗∗ = Ω. That is, +we may assume that (65) holds on the whole probability space. + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +45 +Let C be an arbitrary set in the probability space with P(C) > 0. Integrating (65) +and using (51) and Lemma 5 we get +(66) +t +� +−t +x2dFC(x) ≥ Kt, +1 − FC(t) + FC(−t) ≤ εt, +t ∈ H, +where H denotes the set of continuity points of FΩ. Choose t0 ∈ H so large that +εt0 ≤ 1/16 and then choose t1 so large that +K1/2 +t +/4 ≥ 2t2 +0 for t ≥ t1, t ∈ H. +Then for t ≥ t1, t ∈ H we have, using the second relation of (66), +������ +t +� +−t +xdFC(x) +������ +≤ +2t2 +0 + +� +t0≤|x|≤t +|x|dFC(x) +≤ +2t2 +0 + + + + +� +|x|≥t0 +dFC(x) + + + +1/2  + + +� +|x|≤t +x2dFC(x) + + + +1/2 +≤ +2t2 +0 + 1 +4 + + + +� +|x|≤t +x2dFC(x) + + + +1/2 +≤ +1 +2 + + + +� +|x|≤t +x2dFC(x) + + + +1/2 +, +and thus we proved that for any C ⊂ Ω with P(c) > 0 we have +(67) +t +� +−t +x2dFC(x) − 2 + + +t +� +−t +xdFC(x) + + +2 +≥ 1 +2Kt, +t ≥ t1, t ∈ H. +Since (Xn)n≥1 is bounded in probability, there exists a function ψ(x) ր ∞ such +that +(68) +sup +n Eψ(Xn) ≤ 1 +(see [9]). Let (ak)k≥1 be a sequence of integers tending to +∞ so slowly that ak ≤ +log k and +(69) +δk := ak/ψ(k1/4) → 0. +Let further (εn)n≥1 tend to 0 so rapidly that εak ≤ 2−k. By Theorem D there exists +a subsequence (Xmk)k≥1 and a sequence (Yk)k≥1 of discrete random variables such + +46 +C. AISTLEITNER, I. BERKES AND R. TICHY +that (41) holds and for each k > 1 the atoms of the finite σ-field σ{Y1, . . . , Yak} can +be divided into two classes Γ1 and Γ2 such that +(70) +� +B∈Γ1 +P(B) ≤ εak ≤ 2−k +and for each B ∈ Γ2 there exist i.i.d. random variables Z(B) +ak+1, . . . , Z(B) +k +on B with +distribution FB such that +(71) +PB +� +|Yj − Z(B) +j +| ≥ 2−k� +≤ 2−k, +j = ak + 1, . . . , k. +We show that +(72) +P + + + + + +N� +k=1 +Xmk +Y +√ +N +< t + + + + + → Φ(t) +for all t +cannot hold; this will complete our indirect proof of (A) =⇒ (C). Set +S(B) +ak,k = +k +� +j=ak+1 +Z(B) +j +, +B ∈ Γ2, +Sak,k = +� +B∈Γ2 +S(B) +ak,k +1B, +where +1B denotes the indicator function of B. By (71), +PB +������ +k +� +j=ak+1 +Yj − +k +� +j=ak+1 +Z(B) +j +����� ≥ 1 +� +≤ 2−ak, +B ∈ Γ2, +and thus using (70) we get +(73) +P +������ +k +� +j=ak+1 +Yj − Sak,k +����� ≥ 1 +� +≤ 2 · 2−k. +By (68), (69) and the Markov inequality we have +P +������ +ak +� +j=1 +Xmj +����� ≥ akk1/4 +� +≤ +ak sup +1≤j≤ak +P +� +|xmj| ≥ k1/4� +≤ +akψ(k1/4)−1 += +δk, +which, together with (73) and (41), yields +(74) +P +������ +k +� +j=1 +Xmj − Sak,k +����� ≥ 2akk1/4 +� +≤ 3 · 2−ak + δk. + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +47 +Applying Lemma 3 to the i.i.d. sequence {Z(B) +j +, ak + 1 ≤ j ≤ k} and using (67) we +get +PB +������ +S(B) +ak,k +√ +k +����� ≤ 1 +� +≤ PB +� +S(B) +ak,k +√k − ak +≤ 2 +� +≤ const. K−1/2 +√ +k , +where the constant is absolute. Thus using (70) and Y ≤ K it follows that +(75) +P +����� +Sak,k +Y +√ +k +���� ≤ 1 +K +� +≤ const. K−1/2 +√ +k ++ 2−k. +If (72) were true then by (74) and ak ≤ log k we would also have +Sk,ak/Y +√ +k +D +−→ N(0, 1), +which clearly contradicts (75) for large k, since the right-hand side tends to zero. +This completes the proof of (A) =⇒ (C). +The remaining implications (C) =⇒ (D) and (D) =⇒ (B) of Theorem 1 are easy. +Assume first that (C) holds, then for any ε > 0 there exists a set A ⊂ Ω with +P(A) ≥ 1 − ε and a constant K = Kε such that ++∞ +� +−∞ +x2dF•(x) ≤ K on A. +Integrating the last relation on A and using Lemma 5 we get (52), i.e. (D) holds. +Assume now that (D) holds, i.e. for any ε > 0 there exists a set A ⊂ Ω with +P(A) ≥ 1 − ε such that (52) is valid. Applying Lemma 4 for (Xn)n≥1 on the set +A it follows that there exists a subsequence (Xnk)k≥1 and random variables Yk and +τk, k = 1, 2, . . . , defined on A such that Xnk = Yk + τk, k = 1, 2, . . . , and such that +the random variables Yk have distribution FA on A and τk → 0 a.s. on A. Choose +a set B ⊂ A with P(B) ≥ 1 − 2ε such that τk → 0 uniformly on B. Then clearly +(τn)n≥1 is uniformly bounded on B, and further +� +B +Y 2 +k dP +≤ +� +A +Y 2 +k dP += +P(A) ++∞ +� +−∞ +x2dFA(x) +≤ ++∞ +� +−∞ +x2dFA(x) < +∞ +for each k ≥ 1 by the identical distribution of the Yk’s and (52). Thus on B the +sequences (Yk)k≥1 and (τk)k≥1 have bounded L2 norms and thus the same holds for + +48 +C. AISTLEITNER, I. BERKES AND R. TICHY +Xmk = Yk + τk, i.e. +sup +k +� +B +X2 +mkdP < +∞. +In view of P(B) ≥ 1 − 2ε this shows that (Xn)n≥1 satisfies statement (B). This +completes the proof of Theorem 1. +Proof of Theorem 2. Theorem 2 follows from Theorem 1 and a slightly sharper form +of Theorems H and J which was proved in [147]. We already mentioned the fact that +in Theorem H the random variables X, Y appearing in (50) actually satisfy X ∈ L2, +Y ∈ L1/2. Moreover, if instead of (47) we make the slightly stronger assumption +that the sequence (X2 +n)n≥1 is uniformly integrable then by the weak compactness +criteria in L1 and L2 it follows that there exists a subsequence (Xnk) and random +variables X ∈ L2, Y ∈ L1/2 such that +(76) +Xnk → X weakly in L2, +(Xnk − X)2 → Y 2 weakly in L1. +As is shown in [163], in this case (50) holds with the random variables X, Y de- +termined by (76). +We turn now to the proof of Theorem 2. +As in the case of +Theorem 1, it suffices to prove the equivalence of statements (A), (B), (C) in the +case when (Xn)n≥1 is determining. +Also, since replacing Xn by Xn + τn where +� |τn| < +∞ a.s. does not affect the validity of (50), the conclusion (B) =⇒ (A) +of Theorem (2) is contained in the stronger form of Theorem H mentioned above. +Thus it suffices to verify the implications (A) =⇒ (C) and (C) =⇒ (B). To prove +(A) =⇒ (C) let us assume that (Xn)n≥1 is determining with limit distribution F, and +that there exist a subsequence (Xnk)k≥1 and random variables X ∈ L2, Y ∈ L1/2, +Y > 0, such that for all subsequences (Xmk)k≥1 of (Xnk)k≥1 and any set A ⊂ Ω with +P(A) > 0 equation (50) holds. We show ++∞ +� +−∞ +x2dF(x) < +∞. Clearly we can assume +without loss of generality that (Xnk)k≥1 < (Xk)k≥1. Fix ε > 0. By the implication +(A) =⇒ (B) =⇒ (D) of Theorem 1 there is a set A ⊂ Ω with P(A) ≥ 1 − ε and a +subsequence (Xnk)k≥1 such that +(77) +sup +k +� +A +X2 +nkdP < +∞ and +� +A +x2dFA(x) < +∞, +where FA is the limit distribution of (Xn)n≥1 on A. Applying Lemma 4 for (Xnk)k≥1 +on A it follows that there exists a subsequence (Xmk)k≥1 of (Xnk)k≥1 admitting the +decomposition +(78) +Xmk = Yk + τk on A, +where the Yk are identically distributed on A with distribution function FA and +� |τk| < +∞ a.s. on A. Being an identically distributed sequence with finite expec- +tation, the sequence (Y 2 +k )k≥1 is uniformly integrable on A, and thus by the sharper +form of Theorem H mentioned above it follows that there exists a subsequence +(Ypk)k≥1 of (Yk)k≥1 such that +Ypk → U weakly in L2(A), +(Ypk − U)2 → V 2 weakly in L1(A), + +LACUNARY SEQUENCES IN ANALYSIS, PROBABILITY AND NUMBER THEORY +49 +and for any B ⊂ A with P(B) > 0 we have +PB +��N +k=1(Ypk − U) +V +√ +N +< t +� +→ Φ(t) for all t, +where U, V are random variables such that U ∈ L2(A), V ∈ L1/2(A), V > 0. Thus +by (78) and � |τk| < +∞ a.s. on A we get +PB +��N +k=1(Xmpk − U) +V +√ +N +< t +� +→ Φ(t) for all t +for any B ⊂ A with P(B) > 0. Comparing with (50) and using Lemma 2 we get +U = X, V = Y a.s. on A, and thus we proved that +Ypk → X weakly in L2(A), +(Ypk − X)2 → Y 2 weakly in L1(A). +Hence +EAY 2 = lim +k→∞ EA(Ypk − X)2 = lim +k→∞(EAY 2 +pk − 2EAYpkX + EAX2) += lim +k→∞ EAY 2 +pk − EAX2 = ++∞ +� +−∞ +x2dFA(x) − EAX2, +(79) +where in the last step we used the fact that the Yk’s have distribution FA on A. +Hence +(80) +P(A)−1 +� +A +Y 2dP = ++∞ +� +−∞ +x2dFA(x) − P(A)−1 +� +A +X2dP. +Since X ∈ L2(Ω), Y 2 ∈ L1(Ω), the left-hand side of (80) and the second term on +the right-hand side approach finite limits as P(A) → 1 and thus +� +∞ +−∞ x2dFA(x) also +converges to a finite limit. On the other hand, FA → F as P(A) → 1 and thus +Fatou’s lemma implies ++∞ +� +−∞ +x2dF(x) ≤ lim inf +P (A)→1 ++∞ +� +−∞ +x2dFA(x) < +∞, +proving the implication (A) =⇒ (C). Now if (C) holds then by Lemma 4 there exists +a subsequence (Xnk)k≥1 permitting the decomposition (55) where � |τk| < +∞ a.s. +and Yk are identically distributed with distribution F; since F has finite variance +by (C), the first relation of (56) holds. Thus (Xn)n≥1 satisfies (B) and the proof of +Theorem 2 is completed. +Acknowledgments +Christoph Aistleitner is supported by the Austrian Science Fund (FWF), projects F- +5512, I-3466, I-4945, I-5554, P-34763, P-35322 and Y-901. Istvan Berkes is supported +by Hungarian Foundation NKFI-EPR No. K-125569. + +50 +C. AISTLEITNER, I. BERKES AND R. TICHY +References +[1] R. Adler, M. Keane, and M. Smorodinsky. A construction of a normal number for the con- +tinued fraction transformation. J. Number Theory, 13(1):95–105, 1981. +[2] D. Airey and B. Mance. Normality of different orders for Cantor series expansions. Nonlin- +earity, 30(10):3719–3742, 2017. +[3] D. Airey, B. Mance, and J. Vandehey. 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