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LXXIV.1 (1996)

On a form of the Erd˝os–Tur´an inequality

by

Jeffrey J. Holt (Houghton, Mich.)

1. Introduction. Let P = {x1, . . . , xN} be a set of points in R, and define the Z-periodic set

P= {x + m : x ∈ P, m ∈ Z}.

The discrepancy D(P) gives a measure of how evenly (or unevenly) dis- tributed P is in R/Z. There are a number of ways to define the discrepancy (see, for instance, [2, 8, 13]); a common form is as follows: Let s, t be real numbers which satisfy s < t < s+1, and let χs,t(x) denote the characteristic function of the interval [s, t]. Then we define

(1.1) D(P) = sup

s<t<s+1

X

x∈P

χs,t(x) − N (t − s) .

In 1948, P. Erd˝os and P. Tur´an [4] established a quantitative connection between D(P) and the exponential sums

XN n=1

e(mxn) ,

where m is a nonzero integer and e(θ) = e2πiθ. Specifically, they showed that there exist absolute constants C1 and C2 such that

(1.2) D(P) ≤ C1N M−1+ C2 XM m=1

m−1

XN n=1

e(mxn)

holds for all integers M ≥ 1. Explicit values for C1and C2are given in ([8], pp. 112–114) and ([12], Theorem 20).

The notion of the discrepancy of a point set has been generalized to a wide variety of settings. Bounds in the style of (1.2) have been given in several cases (see [3, 5, 11]), and are typically referred to as “Erd˝os–Tur´an”

inequalities. Here we establish such an inequality for points distributed on the unit torus Rk/Zk, where k ≥ 2. In a manner analogous to the one- dimensional case, we let P = {x1, . . . , xN} be a set of points in Rkand then

[61]

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define

P= {x + m : x ∈ P, m ∈ Zk}.

For r > 0 and c ∈ R, let Bk(r, c) denote the closed ball of radius r centered at c given by

Bk(r, c) = {x ∈ Rk: |x − c| ≤ r},

where | · | denotes the usual Euclidean metric on Rk. For each such r and c, define

(1.3) ∆[P; Bk(r, c)] = Z[P; Bk(r, c)] − N µ(Bk(r, c)),

where Z[Q; A] denotes the number of points of a discrete set Q ⊂ Rk which fall in a compact set A ⊂ Rk, and µ is the usual Euclidean volume. For each r > 0 we then define the discrepancy Dr(P) by

(1.4) Dr(P) = sup

c∈Rk

|∆[P; Bk(r, c)]|.

By applying an observation of H. L. Montgomery (see [1], Section 2.3) to- gether with functions constructed by J. Vaaler and the author [7], we estab- lish the following bound:

Theorem 1. Let r > 0 and P = {x1, . . . , xN} be a subset of Rk. Then (1.5) Dr(P)

≤ N Ak(r, s) + X0

|m|<s

{Ak(r, s) + (r/|m|)k/2|Jk/2(2πr|m|)|}

XN n=1

e(m · xn) for all s > 0, where

Ak(r, s) = ωks−1rk−1{πrs(J(k−2)/2(πrs)2+ Jk/2(πrs)2)

− (k − 1)J(k−2)/2(πrs)Jk/2(πrs)}−1,

Jν(x) is the ν-th order Bessel function and ωk = 4π(k−2)/2Γ (k/2)−1. In 1969, W. Schmidt [9] showed that the discrepancy cannot be uniformly small. Suppose that ε > 0 and that δ satisfies N δk ≥ 1. Schmidt proved that there exists a ball Bk(r, c) with r ≤ δ such that

|∆[P; Bk(r, c)]| > c1(k, ε)(N δk)(k−1)/2k−ε.

On the other hand, J. Beck ([2], Theorem 14) has shown that there exists an infinite sequence x1, x2, . . . such that for all N ≥ 2 and any ball Bk(r, c) with r ≤ 1 and N rk ≥ 1, we have

(1.6) |∆[{x1, . . . , xN}; Bk(r, c)]| ≤ c2(k)(N rk)(k−1)/2k(log N )3/2. In view of Schmidt’s lower bound, we see that (1.6) must be close to best possible. Applying Theorem 1 and a simple averaging procedure, we may establish the existence of a set of p points in Rk (here p is a prime) which

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has modest discrepancy. (A similar application is given in [8], pp. 154–157.) Although our result is not as sharp as Beck’s, our proof is much simpler and we do not have the requirement that r ≤ 1. For h ∈ Zk, let Ph be the collection of p points of the form (n/p)h, n = 1, . . . , p.

Theorem 2. Let p be a prime number , and suppose that r ≥ p−1/k. Then there exists a lattice point h ∈ Zk such that |h| < p and

(1.7) Dr(Ph) ≤ c3(k)(prk)(k−1)/k.

Notation. We use the definition for Fourier transforms and series of Stein and Weiss [10]. For x ∈ Rk and r > 0, χr(x) denotes the characteristic function of Bk(r, 0). To simplify expressions, we adopt the convention that m appearing in a sum will always be a point in Zk. Finally,P0

means that the term in the sum corresponding to m = 0 is omitted.

2. Proof of theorems

P r o o f o f T h e o r e m 1. We require two auxiliary functions. Combin- ing the results in ([7], Theorem 3) and a k-dimensional form of the Paley–

Wiener theorem ([10], Chapter III, Theorem 4.9), we see that for r > 0 and s > 0 there exist functions Fk(x; r, s) and Gk(x; r, s) that satisfy

Fk(x; r, s) ≤ χr(x) ≤ Gk(x; r, s) for all x ∈ Rk, (2.1)

Fbk(t; r, s) = bGk(t; r, s) = 0 for all |t| ≥ s, (2.2)

R

Rk

(Gk(x; r, s) − Fk(x; r, s)) dx = Ak(r, s), (2.3)

where Ak(r, s) is defined in the statement of the theorem. From (1.3) we see that for c ∈ Rk,

∆[P; Bk(r, c)] = XN n=1

X

m

χr(xn− c + m) − N µ(Bk(r, 0)).

Now suppose that for a given r and c we have ∆[P; Bk(r, c)] ≥ 0. Then by (2.1), the Poisson summation formula and the triangle inequality we have

∆[P; Bk(r, c)] ≤ XN n=1

X

m

Gk(xn− c + m; r, s) − N µ(B(r, 0)) (2.4)

= XN n=1

X

m

Gbk(m; r, s)e(m · (xn− c)) − N bχr(0)

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= X

|m|<s

Gbk(m; r, s)e(−m · c) XN n=1

e(m · xn) − N bχr(0)

≤ N ( bGk(0; r, s) − bχr(0)) + X0

|m|<s

| bGk(m; r, s)|

XN n=1

e(m · xn) . From (2.1) and (2.3) we know that

(2.5) Gbk(0; r, s) − bχr(0) = R

Rk

(Gk(x; r, s) − χr(x)) dx ≤ Ak(r, s).

A general expression for bGk(t; r, s) seems difficult to find. However, we can obtain an estimate that will do for our purposes. First note that

b

χr(t) = R

Rk

χr(x)e(−t · x) dx = (r/|t|)k/2Jk/2(2πr|t|).

Applying the triangle inequality together with (2.5) and the above identity, we see that

| bGk(t; r, s)|

R

Rk

(Gk(x; r, s) − χr(x))e(−t · x) dx +

R

Rk

χr(x)e(−t · x) dx

≤ ( bGk(0; r, s) − bχr(0)) + |bχr(t)|

≤ Ak(r, s) + (r/|t|)k/2|Jk/2(2πr|t|)|.

Thus it follows from (2.4) and (2.5) that (2.6) ∆[P; Bk(r, c)]

≤ N Ak(r, s) + X0

|m|<s

{Ak(r, s) + (r/|m|)k/2|Jk/2(2πr|m|)|}

XN n=1

e(m · xn) . If it should happen that for a given r and c we have ∆[P; Bk(r, c)] < 0, then following the preceding analysis using Fk(x; r, s) in place of Gk(x; r, s) yields inequality (2.6) with a minus sign attached to the left-hand term.

Combining these bounds verifies (1.5) and completes the proof.

P r o o f o f T h e o r e m 2. We begin by using some estimates to simplify the bound given in Theorem 1. If rs ≥ 1, then Ak(r, s) k s−1rk−1 (see [7], Theorem 1). Combining this with the bound |Jν(x)| ≤ 1 for ν > 0 and x > 0 reduces (1.5) to

Dr(P) kN s−1rk−1+ X0

|m|<s

{s−1rk−1+ (r/|m|)k/2}

XN n=1

e(m · xn) .

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For a prime p, if h and m are lattice points, then Xp

n=1

e((n/p)h · m) =

0 if h · m 6≡ 0 (mod p), p if h · m ≡ 0 (mod p).

Therefore we have

(2.7) Dr(Ph) k ps−1rk−1+ X0

|m|<s h·m≡0

{s−1rk−1+ (r/|m|)k/2}p.

The sum above is difficult to handle alone, but the problem simplifies if we average over all lattice points h such that |h| ≤ p. On doing so, the right side of (2.7) is equal to

(2.8) ps−1rk−1+ p(Z[Zk; Bk(p, 0)])−1 X

|h|≤p

X0

|m|<s h·m≡0

{s−1rk−1+ (r/|m|)k/2}

= ps−1rk−1+ p(Z[Zk; Bk(p, 0)])−1 X0

|m|<s

{s−1rk−1+ (r/|m|)k/2} X

|h|≤p h·m≡0

1.

For each m in the outer sum on the right side of (2.8), there is at least one nonzero component mg. We fix such an m, and consider the inner sum. For a given h, once the components h1, . . . , hg−1, hg+1, . . . , hkare set, there is only one choice for hg (mod p) for which h · m ≡ 0 (mod p). Since |h| ≤ p, there are at most three possible choices for hg. Furthermore, the other components h1, . . . , hg−1, hg+1, . . . , hkmust satisfy |hj| ≤ p for each appropriate j. Thus for m 6= 0,

(2.9) X

|h|≤p h·m≡0

1 k pk−1.

We also note that for each i ≥ 2, there exist constants c4(i) and c5(i) such that

(2.10) c4(i)pi≤ Z[Zi; Bi(p, 0)] ≤ c5(i)pi.

(See [6], Theorem 339, for a discussion of the case i = 2.) As we are averag- ing, we see that (2.7)–(2.10) imply there exists a lattice point h with |h| ≤ p such that

Dr(Ph) kps−1rk−1+ X0

|m|<s

{s−1rk−1+ (r/|m|)k/2}.

Applying the inequality

X0

|m|<s

|m|−k/2k sk/2

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and assuming that rs ≥ 1 (required for our bound on Ak(r, s) to be valid), we find that

Dr(Ph) k ps−1rk−1+ (sr)k−1.

The expression on the right above is minimized upon setting s = p1/k, which yields

Dr(Ph) k(prk)(k−1)/k, and completes the proof.

References

[1] R. C. B a k e r, Diophantine Inequalities, Oxford University Press, New York, 1986.

[2] J. B e c k and W. W. L. C h e n, Irregularities of Distribution, Cambridge University Press, 1987.

[3] T. C o c h r a n e, Trigonometric approximation and uniform distribution modulo 1, Proc. Amer. Math. Soc. 103 (1988), 695–702.

[4] P. E r d ˝o s and P. T u r ´a n, On a problem in the theory of uniform distribution, I , Indag. Math. 10 (1948), 370–378.

[5] P. J. G r a b n e r, Erd˝os–Tur´an type discrepancy bounds, Monatsh. Math. 111 (1991), 127–135.

[6] G. H. H a r d y and E. M. W r i g h t, An Introduction to the Theory of Numbers, 5th ed., Oxford University Press, Oxford, 1979.

[7] J. J. H o l t and J. D. V a a l e r, The Beurling–Selberg extremal functions for a ball in Euclidean space, to appear.

[8] L. K u i p e r s and H. N i e d e r r e i t e r, Uniform Distribution of Sequences, Wiley, New York, 1974.

[9] W. M. S c h m i d t, Irregularities of distribution, IV , Invent. Math. 7 (1969), 55–82.

[10] E. M. S t e i n and G. W e i s s, Introduction to Fourier Analysis on Euclidean Spaces, Princeton University Press, Princeton, N.J., 1971.

[11] P. S z ¨u s z, ¨Uber ein Problem der Gleichverteilung, in: Comptes Rendus du Premier Congr`es des Math´ematiciens Hongrois, 1950, 461–472.

[12] J. D. V a a l e r, Some extremal functions in Fourier analysis, Bull. Amer. Math. Soc.

12 (1985), 183–216.

[13] —, Refinements of the Erd˝os–Tur´an inequality, in: Number Theory with an Empha- sis on the Markoff Spectrum, W. Moran and A. Pollington (eds.), Marcel Dekker, New York, 1993, 263–269.

DEPARTMENT OF MATHEMATICS

MICHIGAN TECHNOLOGICAL UNIVERSITY HOUGHTON, MICHIGAN 49931

U.S.A.

Received on 2.11.1994 (2688)

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