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HAL Id: hal-02860568

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Submitted on 5 Apr 2021

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ON GOOD UNIVERSALITY AND THE RIEMANN HYPOTHESIS

Jean-Louis Verger-Gaugry, Radhakrishnan Nair, Michel Weber

To cite this version:

Jean-Louis Verger-Gaugry, Radhakrishnan Nair, Michel Weber. ON GOOD UNIVERSAL- ITY AND THE RIEMANN HYPOTHESIS. Advances in Mathematics, Elsevier, In press,

�10.1016/j.aim.2021.107762�. �hal-02860568v2�

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ON GOOD UNIVERSALITY AND THE RIEMANN HYPOTHESIS

RADHAKRISHNAN NAIR, JEAN-LOUIS VERGER-GAUGRY, AND MICHEL WEBER

ABSTRACT. We use subsequence and moving average ergodic theorems applied to Boole’s transformation and its variants and their invariant measures on the real line to give new characterisations of the Lindel¨of Hypothesis and the Riemann Hypothesis. These ideas are then used to study the value distribution of DirichletL-functions, and the zeta functions of Dedekind, Hurwitz and Riemann and their derivatives. This builds on earlier work of R. L.

Adler and B. Weiss, M. Lifshits and M. Weber, J. Steuding, J. Lee and A. I. Suriajaya using Birkhoff’s ergodic theorem and probability theory.

Keywords: Ergodic Averages, Boole’s Transformation, Dedekind Zeta Function, Dirichlet L-function, L-Series, Hurwitz Zeta Function, Riemann Zeta Function, The Lindel¨of Hy- pothesis, The Riemann Hypothesis.

2020 Mathematics Subject Classification: 11M06, 28D05, 37A44, 11M26, 11M35, 30D35.

CONTENTS

1. Introduction 2

2. Applications of Theorem 1.1 6

2.1. The Riemann zeta function 6

2.2. DirichletL-functions 10

2.3. The Dedekind zeta function of a number field 11

2.4. The Hurwitz zeta function 12

3. Proof of Theorem 1.1 12

4. Proof of Theorems 1.2 to 1.5 14

5. Comparing dynamical and probabilistic models 21

6. Hartman uniformly distributed and good universal sequences 24

7. Moving averages 26

7.1. Stoltz sequences and Theorem 7.2 26

7.2. Applications and moving average ergodic Theorems 27

8. Sublinearity and the Riemann zeta function 28

Acknowledgements 29

References 29

1

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1. INTRODUCTION

Equivalent statements of the Riemann Hypothesis are well-known and can be found e.g. in Titchmarsh [T] or more recently e.g. in Mazur and Stein [MSt]. The Lindel¨of Hypothesis asserts that for everyε >0 we have

(1.1) |ζ(1/2+it)|=O(|t|ε) as|t| →∞,

whereζ(z)is the Riemann zeta funtion, and Landau’s notation “O” means that there exists a neighbourhoodV of∞and a constantc≥0 such that:|ζ(1/2+it)| ≤c|t|ε for allt∈V. Before stating the main Theorems 1.1–1.5, and Theorem 7.2 in the context of moving average ergodic theorems, let us make precise the context in probability theory.

Let(Xi)i≥1be a sequence of independent Cauchy random variables, with characteristic functionφ(t) =e|t|and consider the partial sumsSn=X1+. . .+Xn(n=1,2, . . .).

M. Lifshits and M. Weber [LW3] studied the value distribution of the Riemann zeta functionζ(s)sampled along the random walk(Sn)n≥1showing, forb>2, that

(1.2) lim

N→∞

1 N

N n=1

ζ 1

2+iSn

=1+o

(logN)b N12

.

They also showed that (1.3)

sup

n≥1

|∑nq=1ζ(12+iSq)−n|

n12(logn)b

2

<∞.

Here of course f(x) = o(g(x)) means limx→∞g(x)f(x) =0. This result was extended to L- functions and Hurwitz zeta functions by T. Srichan [Sr]. In [St2] J. Steuding replaced (Sn)n≥1in [LW3] by(Tnx)n≥1for almost allxonRwith respect the Lebesgue measure, for the Boolean dynamical system byT x:=x1x. This result has its roots in the observation, due to G. Boole [Bo], subsequently developed by J.W.L. Glashier [G1] [G2], that if f is integrable on the real numbers, then

Z

−∞f(x)dx= Z

−∞f x−1

x dx.

See [AdW] for a proof of the ergodicity of this dynamical system. In Theorem 3.1 in [LS], the maps

(1.4) Tα,β(x) =

( α 2

x+β

αx−βα

ifx 6=β, β ifx =β,

forα >0 and realβ, are shown to be measure preserving and ergodic with respect to the probability measure

(1.5) µα,β(A) = α

π Z

A

dt α2+ (t−β)2, for any Lebesgue measureable subsetAof the real numbers.

As noted in [LS], ifλ denotes Lebesgue measure thenµα(A)≤απ1 λ(A)for allA∈B, where B denotes the Lebesgueσ-algebra. Also ifφα,β(x) =αx+β, withT =T1,0 and

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µ =µ1,0we have

(1.6) Tαα,βT◦φα−1,

which implies the µα-measure preservation and ergodicity of Tα. The referee of this paper has brought to the authors’ attention the paper [MSr], which considers a family of rational maps more general than that in [LS], which we consider in this paper. The suggestion is that our methods in this paper will adapt to the more general framework in [MSr] – at least to a degree. We will not however explore this possibility in this paper, as it would be too much of a digression.

We consider a number of general definitions.

We say(kn)n≥1∈NisLp-good universalif for each dynamical system(X,β,µ,T)and for eachgLp(X,β,µ)the limit

(1.7) ℓT,g(x) = lim

N→∞

1 N

N−1 n=0

g(Tknx) existsµ almost everywhere.

Also throughout the rest of this paperBwill be the Lebesgueσ- algebra onRand when aσ-algebra onRis not explicitly mentioned it is in factB.

We say that a sequencex1, . . .,xN, . . .isuniformly distributed modulo oneif

(1.8) lim

N→∞

1

N#{1≤nN:{xn} ∈I}=|I|

for every intervalI ⊆[0,1). For a real numberywe have used{y}to denote its fractional part and let[y] =y− {y}denote its integer part. We say a sequence of integers isuniformly distributed onZif it is uniformly distributed among the residue classes modulom, for each natural numberm>1. We say a sequence of natural numbers(kn)n≥1isHartman uniformly distributed (onZ)if it is uniformly distributed onZ, and for each irrational numberα, the sequence({knα})n≥1is uniformly distributed modulo one . This condition coincides with (kn)n≥1 being uniformly distributed on the Bohr compactification of Z. Some basics on Hartman uniform distribution can be found in the book of Kuipers and Niederreiter [KN].

Note that if(kn)n≥1is Hartman uniformly distributed onZ, and if forzwith|z|=1 we set

(1.9) F(N,z):= 1

N

N−1 n=0

zkn (N=1,2,· · ·) then

(1.10) lim

N→∞F(N,z) =

1 ifz=1, 0 otherwise.

For ac∈Rwe useHcto denote the half plane{z∈C:ℜ(z)>c}and useLcto denote the line{z∈C:ℜ(z) =c}. We establish the following theorem.

Theorem 1.1. Let f be a meromorphic function onHcsatisfying the following conditions:

(1) there exists a K >0and a c>c such that for any t ∈R, we have (1.11) |f({σ+it|σ >c})| ≤K;

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(2) there exists a non-increasingν :(c,∞)→Rsuch that ifσ is sufficiently near c then ν(σ)≤1+c−σ and that for anyε >0, we have f(σ+it)f,ε |t|ν(σ)+ε as|t| →∞;

(3) f has at most one pole of order m in Hc at s00+it0, that is, we can write its Laurent expansion near s=s0as

a−m

(s−s0)m+ a−(m−1)

(s−s0)(m−1) +. . . a−1

(s−s0)−1+a0+

n=1

an(s−s0)n for m≥0where we set m=0if f has no pole inHc.

Then if (kn)n≥1 is Lp-good universal and Hartman uniformly distributed, for any s ∈ Hc\Lσ0, we have

(1.12) lim

N→∞

1 N

N−1 n=0

f(s+iTα,βkn (x)) = α π

Z

R

f(s+iτ) α2+ (τ−β)2dτ, for almost all x inR.

In the casekn=n(n=1,2, . . .)Theorem 1.1 appears in [LS], where it is shown, using (1), (2) and (3) and contour integration, for

lα(s):= α π

Z

R

f(s+iτ) α2+ (τ−β)2dτ, that if f has a pole ats00+it0,

(1.13) lα,β(s) =







f(s+α+iβ) +Bfm(so), ifc<ℜ(s)<σo, s6=so−α−iβ,

m n=0

a−n

(−2α)n, ifc<ℜ(s)<σo, s=so−α−iβ, f(s+α+iβ), ifℜ(s)>σo,

orlα(s) = f(s−α+iβ)ifs∈Hc and f has no pole. Hereℜ(s)denotes the real part of sand

Bfm(s0) =

m n=1

n a−n

in(β+iα−i(ss0))na−n

in(β−iα−i(ss0))n o.

Moreover, whenm=1, we can extend Theorem 1.1 to the lineLσ0 by setting lα0+it) = f0+α+i(t+β))− a−1α

α2+ (t0t−β)2. Applications will be given in the next section.

As noted earlier Steuding [St2] showed that ifζ denotes the Riemann zeta function

(1.14) lim

N→∞

1 N

N−1

n=0

ζ(s+iTnx) = 1 π

Z

R

ζ(s+iτ) 1+τ2 dτ

existsµ almost everywhere (forx). We can measure the stability of these averages another way. HenceforthC, possibly with subscripts, will denote a positive constant, though non- necessarily the same on each occasion.

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Theorem 1.2. Suppose s=σ+it with 12<σ <1. Let YN(σ) =YN(σ,x):= 1

N

N−1 n=0

ζ(s+iTnx). (N=1,2, . . .) Suppose(Nk)k≥1is a strictly increasing sequence of positive integers. Then there exists an absolute C>0such that

(1.15)

k=1

k sup

Nk≤N<Nk+1

|YN(s)−YNk(s)| k22C πσ

ζ(2σ)

2 +ζ(2σ−1) 2σ−1

.

There are other ergodic theoretic measures of the stability of the Riemann zeta function.

In this direction we consider the frequencies associated to the sequences ζ(s+iTnx)

n

n≥1. Evidently

n→∞lim

ζ(s+iTnx)

n =0,

for almost all x. It is possible to make this more precise as follows. Suppose 0<p<∞.

For a sequence of real numbersx={xn:n≥1}set

(1.16) kxkp,∞:= sup

t>0

{tp#{n:|xn|>t}}1p .

Theorem 1.3. (i) Suppose 12 <σ <1. Then

(1.17) lim

m→∞

#{n: |ζ(σ+iTn nx)|m1}

m =ζ(σ+1)− 2

σ(2−σ), for almost all x∈R. and in L1(µ)norm.

(ii) Further (1.18)

|ζ(σ+iTnx)|

n :n≥11,∞

1

<∞.

Moreover,

Theorem 1.4. Suppose s=σ+it with 12 <σ <1. Suppose κ = (kn)n≥1 is Lp- good universal for p>2and let

(1.19) RN(s,x,κ):= 1 N

N−1 n=0

ζ(s+iTknx). (N=1,2, . . .).

Then

(i) there exists a constant C>0such that (1.20)

N=1

RN+1(s, .,κ)−RN(s, .,κ)22C πσ

ζ(2σ)

2 +ζ(2σ−1) 2σ−1

, (ii) there exists C>0

(1.21) µαnx:

N=1

|RN+1(s,x,κ)−RN(s,x,κ)|2≥λoC λ2

ζ(2σ)

2 +ζ(2σ−1) 2σ−1

.

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We will provide additional information about various special families of sequences in Section 4 and Section 8. On the other hand if we consider theL1-norm we have the follow- ing theorem in the opposite direction.

Theorem 1.5. Suppose κ = (kn)n≥1 is Hartman uniformly distributed and Lp- good uni- versal for fixed p≥ 1andσ∈(12,1). Then

(1.22)

N≥1

RN+1(σ,x,κ)−RN(σ,x,κ) = +∞,

almost everywhere in x with respect to Lebesgue measure.

It would be interesting to get good bounds almost everywhere inxfor

J N=1

RN+1(σ,x,κ)−RN(σ,x,κ), (J=1,2. . .)

even for specific cases ofκ.

The paper is organized as follows: in Section 2 new characterisations of the (extended) Lindel¨of Hypothesis are obtained for the Riemann zeta function, and for Dirichlet L- functions, Dedekind zeta functions of number fields, Hurwitz zeta functions, as applica- tions of Theorem 1.1. The sequences here are assumed to be Hartman uniformly distributed and Lp-good universal. Replacing this assumption by being Stoltz leads to similar limit theorems, which are reported in Section 7. The role played by sublinear sequences hav- ing controlled growth is investigated in Section 8 for the Riemann zeta function. Section 6 contains some examples of Lp-good universal sequences and Hartman uniformly dis- tributed sequences. Comparison between the dynamical and probabilistic models of Weber [W], resp. Srichan [Sr], is done in Section 5.

2. APPLICATIONS OFTHEOREM 1.1

From now, we assume that(kn)n≥1satisfies the hypothesis in Theorem 1.1.

In the sequel, for a function f denote f(0)= f and f(k)thek-th derivative of f and set Pk(s):= (−1)kk!

ik+1

1

(β+iα−i(s−1))k+1− 1

(β−iα−i(s−1))k+1

for any non-negative integerk.

2.1. The Riemann zeta function.

Theorem 2.1. Suppose (kn)n≥1 is Lp-good universal for some p ∈[1,∞] and Hartman uniformly distributed. Then for any k≥0and s∈H1

2\L1we have

(2.1) lim

N→∞

1 N

N−1 n=0

ζ(k)(s+iTαkn(x)) = α π

Z

R

ζ(k)(s+iτ) α2+ (τ−β)2dτ for almost all x inR.

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Denote the right hand side of this limit bylα,β(k) . Then

(2.2) lα,β(k) =





ζ(k)(s+α+iβ) +Pk(s), if −12<ℜ(s)<1, s6=1−α−iβ, (−1)kγk(2α)k!k+1, if −12<ℜ(s)<1, s=1−α−iβ,

ζ(k)(s+α+iβ), ifℜ(s)>1, where

(2.3) γk= lim

N→∞

N n=1

logkn

n −logk+1N k+1

! .

In the casek=0 we can extend the result to the lineL1by setting (2.4) lα(0) =lα,β(0)(1+it) =ζ(0)(1+α+i(t+β))− α

α2+ (t22).

If we set kn=n(n=1,2, . . .)Theorem 2.1 appears in [LS] and this is in the caseα = 1,β =0 andk=1 in [St2].

We also mention here that the casekn=n(n=1,2, . . .)andT =T1,0of Theorems 2.3 and 2.4 to follow, appeared in [St2], of Theorem 2.4 appeared first in [BSY] and of Theorems 2.6 and 2.7 appeared in [LS].

Proof. Note that fork≥0, we know that ζ(k) is meromorphic and has an absolutely con- vergent Dirichlet series forℜ(s)>1. Thus the condition (1) of Theorem 1.1 is satisfied for c>1. This is because the Laurent expansion ofζ near the pole ats=1 is known [Br] and then that the Laurent expansion ofζ(k)has the form

ζ(k)(s) = (−1)kk!

(s−1)k+1+ (−1)kγk+

n=k

(−1)n+1γn

(n−k+1)!(s−1)n−k+1.

Thus ifk≥0 the functionζ(k) has a pole of orderk+1 ats=1. We can in addition show (Titchmarsh [T], pp. 95–96) that givenε>0 we have

ζ(k)(σ+it)≪ |t|µ(σ)+ε, where

µ(σ) =



0, ifσ >1,

(1−σ)

2 , if 0≤σ≤1,

1

2−σ, ifσ <0,

if k ≥0. Therefore Theorem 2.1 follows from Theorem 1.1 with c =−12, s0 = 1 and

m=k+1 toζ(k)(s)as required.

We now state a formulation of the Lindel¨of Hypothesis in terms ofζ(k)from [LS].

Lemma 2.2. The Lindel¨of Hypothesis(1.1)is equivalent, for everyε >0, to (2.5)

ζ(k)(1

2+it) ≪ |t|ε as|t|tends to∞, for any k≥0.

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We now give a new characterization of the Lindel¨of Hypothesis for the Riemann zeta function, which generalizes the classical one. The classical case kn =n(n=0,1,2, . . .) appears in [LS].

Theorem 2.3. Suppose (kn)n≥1 is Lp-good universal for some p ∈[1,∞] and Hartman uniformly distributed. Suppose k is any non-negative integer. Then the statement, for any natural number l,

(2.6) lim

N→∞

1 N

N−1 n=0

ζ(k)

1

2+iTα,βkn (x)2l= α π

Z

R

(k)(12+iτ)|2l α2+ (τ−β)2 dτ forµα -almost all x inR, is equivalent to the Lindel¨of Hypothesis.

Proof. Via Lemma 2.2 the Lindel¨of Hypothesis implies that givenε>0 we have

ζ(k) 1

2+.

2m

Lp(R,B,µα,β)

for each pair of natural numbers k,m. Here .represents the variablet ∈R. Theorem 1.1 and the ergodicity ofTα implies that

N→∞lim 1 N

N−1 n=0

ζ(k)

1

2+iTαkn(x)

2l

= α π

Z

R

(k)(12+iτ)|2l α2+ (τ−β)2dτ. We now prove the converse. First

ζ(k)(s) = (−1)k−1 Z

1

[x]−x+12

xs+1 (logx)k−1(−slogx+k)dx+ (−1)kk!

(s−1)k+1. Thus there existsCk>0, dependent only onk,α andβ, such that for|t| ≥1 we have

(k)(1

2+it)|<Ck|t|.

Also evidently there existscα,β >0 such that if|τ| ≥1 1

α2+ (τ−β)2cα 1 1+τ2.

Assuming that the Lindel¨of Hypothesis is false, implies there existsη>0 andτm→∞and Cα1 such that

ζ(m)(1

2+it)

>Cα1τmη. Now,|ζ(k)(12+it)|<Ck|t|for any|t| ≥1 withCk>0, and

ζ(k)(1

2+iτ)−ζ(1

2+iτm) =

Z τ τm

(k+1)(1

2+it)dt

<Cα2|τ−τm|τ.

So |ζ(12+iτ)| ≥ 12Cα,β1 τmη for τ with|τ−τm| ≤τm−1 withm large enough. LetL:= 23τm; then the intervalI:= (τm−τm−1mm−1)contains the interval(L,2L)for largem. Hence

Z 2L L

ζ(k)

1

2+iτ2l 1

2 dτ 1+τ2

C1

2 2lZ

Iτm2lη−2dτ=2.

C1 2

2l

m2lη−3,

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which is≫T2lη−3, and this is impossible asl→∞. So our theorem is proved.

We now specialize to the caseT =T1,0and give a condition in terms of ergodic averages equivalent to the Riemann Hypothesis. We denote byρ=β+iγ, a representative complex zeros of the Riemann zeta function. See Titschmarsh [T], p. 30 for instance for details.

Theorem 2.4. Suppose(kn)n≥1 is both Hartman uniformly distributed and Lp-good uni- versal for some p>1. Then for almost all x in R with respect to Lebesgue measure we have

(2.7) lim

N→∞

1 N

N n=1

log ζ

1 2+1

2iTknx=

ρ:ℜ(ρ)>12

log ρ

1−ρ . Evidently, the Riemann Hypothesis follows if either side is zero.

To prove Theorem 2.4, we need the following lemma due to M. Balazard, E. Saias and M. Yor [BSY].

Lemma 2.5. We have

(2.8) 1

2π Z

ℜ(s)=12

log|ζ(s)|

|s|2 |ds|=

ρ:ℜ(ρ)>12

log

ρ 1−ρ

.

Proof. We wish to use Theorem 1.1 to deduce Theorem 2.4 using Lemma 2.5. To show Theorem 1.1 is relevant we need to show that

log ζ

1

2+i.Lp(R,µ1,0), (where.denotest∈R), i.e. that

Z

ℜ(s)=12

|log|ζ(s))|p|

|s|2

|ds|<∞.

We mentioned earlier that there existsC>0 such that if|t|>1,

ζ 1

2+it

C|t|.

Also notice that (log|ζ(s)|)|s|2 p is continuous on an interval onℜ(s) =12centred ons=12. Away from that interval onℜ(s) = 12 we use the observation thatζ(12+it)C|t|. Hence (for s= 12+it), givenδ >0 we have

(log|ζ(s)|)p

|s|2 ≪ 1

|s|2−δ. This means

log ζ

1

2+i.Lp(R,µ1,0),

(11)

as required. Using the fact thatT preserves the measureµ1,0and is ergodic with respect to this measure, we have

N→∞lim 1 N

N n=1

log ζ

1 2+1

2iTknx= 1 2π

Z

ℜ(s)>12

log|ζ(s)|

|s|2 |ds|.

µ1,0 almost everywhere. Theorem 2.4 now follows from Lemma 2.5.

2.2. DirichletL-functions.

Theorem 2.6. Let L(s,χ) denote the L-functions associated to the characterχ. Suppose (kn)n≥1is Hartman uniformly distributed and Lp-good universal for some p>1. Then, for k≥1,

(i) if χis non-principal, for s∈H1

2 we have

N→∞lim 1 N

N−1

n=0

L(k)(s+iTα,βkn (x),χ) = α π

Z

R

L(k)(s+iτ,χ) α2+ (τ−β)2dτ

(2.9) = L(k)(s+α+iβ,χ) for almost all x inR, (ii) if χ(=χ0)is principal, for s∈H1

2\L1we have

(2.10) lim

N→∞

1 N

N−1 n=0

L(k)(s+iTαkn(x),χ) =α π

Z

R

L(k)(s+iτ,χ) α2+ (τ−β)2dτ, for almost all x inR.

Denote this limit, i.e. the right hand side of (2.10), bylα(k)(s,χ0). Then (2.11)

lα(k)(s,χ0) =





L(k)(s+α+iβ,χ0) +γ−10)Pk(s), if −12<ℜ(s)<1, s6=1−α−iβ, γk0)−k!γ(2α)−1k+10), if −12<ℜ(s)<1, s=1−α−iβ, L(k)(s+α+iβ,χ0), ifℜ(s)>1,

where γ−10),γk0), are constants that depend on χ0. These are the coefficients of the Laurent expansion ofL(k)(s,χ0)nears=1. Ifk=0 we can extend the result to the lineL1 by defining

lα,β(0) =lα,β(0)(1+it,χ0) =L(1+α+i(t+β),χ0)− αγ−10) α2+ (t22).

Proof. We know that L(k)(s,χ) has a Dirichlet series expansion for ℜ(s)>1, for each non-negative integerk. From this we can show that

L(k)(s,χ)≪k,ε|t|µ(σ)+ε where

µ(σ) =



0, ifσ >1,

(1−σ)

2 , if 0≤σ≤1,

1

2−σ, ifσ <0.

Ifχ is non-principal thenL(k)(s,χ)is entire for allk≥0, soL(k)(s,χ)satisfies Theorem 1.1 for alls∈H1

2. Ifχ=χ0is principal,L(k)(s,χ0) (k≥1)has a pole of orderk+1 ats=1.

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We can therefore apply Theorem 1.1 withc=−12,s0=1 andm=k+1, toL(k)(s,χ0)with

Laurent coefficients coming from [IK].

2.3. The Dedekind zeta function of a number field. We now consider the Dedekind ζK(s)function of a number field Kof degreedK over the rationalsQwhich is defined by as follows. Fors∈Csuch thatℜ(s)>1, let

ζK(s) =

I⊂OK

1 (NK/Q(I))s.

HereI runs over the ideals contained in the ring of integers ofK denotedOK andNK/Q(I) denotes the absolute norm ofI inK, which is the cardinality of the quotientOK/I. In the caseK=Q, the functionζK(s)reduces to the Riemann zeta functionζ(s). The complex functionζK(s)can be extended meromorphically to the entire complex plane with a simple pole ats=1. See [Coh] p. 216, for more details.

Theorem 2.7. Suppose (kn)n≥1 is Lp-good universal for some p ∈[1,∞] and Hartman uniformly distributed. For any k≥0and any s∈H1

2d1

K

\L1we have

(2.12) lim

N→∞

1 N

N−1

n=0

ζK(k)(s+iTαkn(x)) = α π

Z

R

ζK(k)(s+iτ) α2+ (τ−β)2dτ for almost all x inR.

Denote the right hand side of this limit bylK(k)

α,β. We have (2.13)

lK(k)

α,β(s) =





ζK(k)(s+α+iβ) +γ−1(K)Pk(s), if 12d1

K <ℜ(s)<1, s6=1−α−iβ, k!γk(K)−k!γ(2α)−1k+1(K), if 12d1K <ℜ(s)<1, s=1−α−iβ,

ζ(k)(s+α+iβ), ifℜ(s)>1.

Here γ−1(K)and γk(K)are constants dependent only on K, which are coefficients of the Laurent expansion ofζK(k)nears=1. Also in the casek=0 we can extend the result to the lineL1by setting

(2.14) lK(0)

α,β(1+it) =ζ(0)(1+α+i(t+β))− αγ−1(K) α2+ (t22).

Proof. We refer to [St1] for a bound forLon the half line and to [HIKW] for the coeffi- cients of the Laurent expansionζK(s)near the poles=1. We then proceed as earlier with Theorem 2.1,c= 12d1

K,s0=1 andm=k+1.

Remark 2.8. Results analogous to the ergodic characterisation of the Lindel¨of Hypothesis just given, can be proved forL-functions associated to primitive characters and Dedekind ζ function. In both cases, the statements of ergodic characterisation are of the type: there exist constantsk,ε>0 such that

f 1

2+it

f,k,ε |t|ε,

as|t| →∞, for suitableL-functions f. This inequality when f is anL-function arising from Dirichlet series is called the Generalized Lindel¨of Hypothesis.

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2.4. The Hurwitz zeta function. Recall that the Hurwitz zeta function is defined fora>0 ands∈Cwithℜ(s)>1 by

ζ(s,a) =

n=1

1 (n+a)s.

It is continued meromorphically to the whole ofCwith a single pole ats=1.

Theorem 2.9. Suppose (kn)n≥1 is Lp-good universal for some p ∈[1,∞] and Hartman uniformly distributed. Then for any s such thatℜ(s)>−12,s6=1, with0≤a<1and k a non-negative integer, we have

(2.15) lim

N→∞

1 N

N−1 n=0

ζ(k)(s+iTαkn(x),a) =α π

Z

R

ζ(k)(s+iτ,a) α2+ (τ−β)2dτ, for almost all x inR.

Denote the right hand side of this limit bylα,β(k) (s,a). Then

(2.16) lα(k)(s,a) =





ζ(k)(s+α+iβ,a) +Pk(s), if −12<ℜ(s)<1, s6=1−α−iβ, (−1)kγk(a)−(2αk!)k+1, if −12<ℜ(s)<1, s=1−α−iβ,

ζ(k)(s+α+iβ,a), ifℜ(s)>1, where

(2.17) γk(a) = lim

N→∞

N n=1

logk(n+a)

n+a −logk+1(N+a) k+1

! .

In the casek=0 we can extend the result to the lineL1by setting (2.18) lα(0)(1+it,a) =ζ(0)(1+α+i(t+β),a)− α

α2+ (t22).

If we setkn=n(n=1,2, . . .)Theorem 2.1 appears in [LS] and this is the caseα=1,β=0, andk=1 in [St2].

Proof. Following the proof of Theorem 2.1 choosec=−12,s0=1 andm=k+1. For the bound on|ζ(k)(s,a)|on the half line and the coefficients of the Laurent series ofζ(k)(s,a)

nears=1 we refer to [St1].

3. PROOF OF THEOREM 1.1

The proof is in the continuation, and a generalization, of a Theorem of [LS] in which conditions (1), (2) and (3) are used. We first recall a special case of a Theorem of S. Sawyer [Sa]:

Suppose for a dynamical system(R,B,µα,Tα)thatgLp(R,B,µα,β)and letkgk= (RX|f|pdµα)1p. Set

Mg(x) =sup

N≥1

1

N

N n=1

g(s+iTα,βkn (x)). (N=1,2, . . .)

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If(kn)n≥1isLp-good universal for p>1, then there existsC>0 such that

(3.1) Mg

pCkgkp. Because

N1Nn=1g(s+iTαkn(x))≤Mg(x) (N=1,2, . . .)andMgLp, the dominated con- vergence theorem implies

h(x) = lim

N→∞

1 N

N

n=1

h(s+iTαkn(x))

exists in Lp-norm. Our next order of business is to show that h(s+iTα,β(x)) =h(s+ix).

LetUα,βg(s+ix) =g(s+iTα,β(x)). This is a norm preserving operator onLp asTα,β is µα measure preserving. Also letUα−1 denote theL2 adjoint of Uα. Recall that we say any sequence (cn)n∈Z is positive definite if given a bi-sequence of complex numbers (zn)n∈Z, only finitely many of whose terms are non-zero, we have ∑n,m∈Zcn−mznzm≥0.

Herezis the conjugate of the complex numberz. Letha,bi=RRabdµα,β (i.e. the standard inner product on L2). Notice that D

Uαng,gE

n∈Z is positive definite. Recall that the Bochner-Herglotz theorem [Kt] says that there is a measureωgonT, such that

D

Uαng,gE

= Z

T

zndωg(z). (n∈Z)

This tells us that 1

N

N n=1

g(s+iTαkn+1(x))− 1 N

N n=1

g(s+iTαkn(x))2

= Z

T(2−zz−1)1 N

N

n=1

zkn

2dωg(z) using the parametrizationz=e2πiθ forθ ∈[0,1), this is

=4 Z

T

sin2 θ

2 1

N

N n=1

zkn

2dωg(z).

Using the fact that sinθ2 =0 ifθ =0 and the fact that(kn)n≥1 is Hartman uniformly dis- tributed, by (1.9) and (1.10), we see that g(s+iTα(x)) =g(x). A standard fact from ergodic theory is that if Tα,β is ergodic and g(s+iTα(x)) =g(x)for measurable gthen g(x)is constant, which must beRRgdµα,β. This extends to theLp-norm for allp>1.

All we have to do now is to show that the pointwise limit is the same as the norm limit, i.e. that g(x) =g(x) =RRgdµα. We consider the sequence of natural numbers(Nt)t≥1

such that

1

Nt

Nt

n=1

g(s+iTαkn(x))− Z

Rg(x)dµα

p≤ 1 t. Thus

t=1

Z

X

1

Nt

Nt

n=1

g(s+iTαkn(x))− Z

Rg(x)dµα,βpdµ<∞.

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Fatou’s lemma gives Z

R

t=1

1

Nt

Nt

n=1

g(s+iTαkn(x))− Z

Rg(x)dµα,βpdµ <∞.

This implies

t=1

1

Nt

Nt

n=1

g(s+iTα,βkn (x))− Z

Rg(x)dµαp<∞.

almost everywhere. This means

1 Nt

Nt

n=1

g(s+iTα,βkn (x))− Z

X

g(x)dµα=o(1).

µα almost everywhere. As(kn)n≥1isLp-good universal we must have

N→∞lim 1 N

N−1 n=0

g(s+iTαknx) = Z

Rg(s+ix)dµα,β µα almost everywhere as required to prove Theorem 1.1.

4. PROOF OFTHEOREMS 1.2 TO1.5

We begin by recalling the spectral regularization method of Lifshits and Weber [LW1]

[LW2], and some technical preliminaries. Assume (X,β,ν)is a measure space with fi- nite measure ν and that S is a ν measure preserving transformation of (X,β,ν). For

fL1(X,β,ν)let

(4.1) BN(f) = 1

N

N−1 k=0

fTk. (N=1,2, . . .)

We need the following lemma, due to R. Jones, R. Kaufman, J. Rosenblatt and M. Wierdl [JKRW].

Lemma 4.1. Suppose(Np)p≥ is a strictly increasing sequence of positive integers. Then there exists an absolute constant C>0such that

(4.2)

p=1

sup

Np≤N<Np+1

|BN(f)−BNp(f)|2

2Ckfk2.

Write log+(u) =max(1,log(u))foru≥1. Letω denote the spectral measure associated to the element f and define its regularised measure ˆω via its Radon-Nykodim derivative by

dωˆ dx(x) =

Z π

−πQ(θ,x)ω(dθ), where

Q(θ,x) =

|θ|−1log2+(θx) if|x|<|θ|, θ2|x|−3 if|θ| ≤ |x| ≤π. The following is a theorem of Lifshits and Weber [LW1].

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Lemma 4.2. Suppose N0 and N1with N0<N1 are positive integers. Then there exists an absolute constant C>0such that

(4.3) sup

N0≤N<N1

|BN(f)−BN0(f)|2

2Cωˆ [ 1 N1

1 N0)

.

Suppose 0<p<∞. For a sequence of real numbersx={xn:n≥1}the quantitykxkp,∞

is defined in (1.16). Also ifr<pwe have kxkp,∞≤ kxkp

p pr

1p

kxkp,∞.

We also consider

Nx=sup

m≥1

#{n:xnn > m1}

m .

In our considerations,xn= fn(x)) (n=1,2, . . .)and x=Of(x) = (fn(x))n≥1which is the value of f along the orbit of a point xX. Also let Nf(x) = NO

f(x). We have the following Lemma due to I. Assani [As] (see also [W] - we refer to Jamison, Orey and Pruitt [JOP] for more on the random variable case, and [RR] for Birnbaum-Orlicz spaces and the

“Llog+L” notation).

Lemma 4.3. (i) For any non-negative fL1(µ)the function Nf(x)is weak-(p,p) for all p∈(1,∞). Further

(4.4) lim

m→∞

#{n: f(τnn(x)) > m1}

m =

Z

X

f dµ, µ almost everywhere and also in L1(µ)-norm.

(ii) For fLlog+L

(4.5)

fn(x)) n

1,∞

1

<∞.

Note that, for two positive constantsC1,C2, C1Nf(x)≤

fn(x))

n ,n≥11,∞C2Nf(x).

We now turn to the proof of Theorem 1.2.

By Lemma 4.1,

k=1

sup

Nk≤N<Nk+1

|YN(σ)−YNk(σ)|2

2C π

Z

R

|ζ(σ+iτ)|2 1+τ2 dτ, where as beforeCis universal. We note that, forσ ∈(12,1),

Z

R

|ζ(σ+it)|2 1+t2 dt=

Z 0

{x}

x+1dx=−1 σ

ζ(2σ)

2 +ζ(2σ−1) 2σ−1

.

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Here again{x}=x−[x]denotes the fractional part ofx. The quantity in the bracket on the right hand side is negative. Further,

1 2π

Z

R

|ζ(12+it)|2

1

4+t2 dt=log(2π)−γ.

whereγ is Euler’s constant. See Prop. 7, Cor. 8 and (1.26) in Coffey [C]. Thus

(4.6) C

π Z

R

|ζ(σ+iτ)|2

1+τ2 dτ≤ C πσ

ζ(2σ)

2 +ζ(2σ−1) 2σ−1

. completing the proof of Theorem 1.2.

We now turn to the proof of Theorem 1.3. The first assertion is a consequence of Lemma 4.3 (i). The limit is

1 π

Z

R

|ζ(σ+it)|2 1+τ2 dt.

This integral is a special case of integrals calculated in [St1]. As a consequence of Theorem 1.1 in [St2],

1 π

Z

R

|ζ(σ+it)|2

1+τ2 dt=ζ(σ+1)− 2 σ(2−σ).

For the second assertion, it follows from Lemma 4.3 (ii). The function ζ(s)∈Llog+L is integrable, with respect to the Cauchy measure, because of the estimate

ζ(σ+it)εt1−σ2 .

See Titchmarsh, [T] section 5.1, for the details of this. Therefore Theorem 1.3 is proved as required.

To prove Theorem 1.4 we need the following two lemmas.

Suppose(X,β,µ)is a measure space and thatT :XX is a measure preserving map.

Let(ak)k=0be a sequence of natural numbers and for any measurable f onX set

(4.7) CNf(x) := 1

N

N−1 k=0

f(Takx), (N=1,2,· · ·) that is the ergodic averages corresponding to the sequence and let

M f(x) := sup

N≥1

|CNf(x)|.

Further from the data(X,β,µ,T)and f we construct the ergodicq-variation function Vqf(x) = (

N≥1

|CN+1f(x)−CNf(x)|q)1q. (q ≥ 1) Our first lemma is Theorem 1 from [NW1].

Lemma 4.4. Suppose for a sequence of natural numbers(ak)k=0that for some p > 1and f

Cp > 0depending only on p and(X,β,µ,T)we have

(4.8) M fpCfpkfkp.

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Then there exists another constant Dp > 0depending only on p and(X,β,µ,T)such that if q > 1then

(4.9) Vqf

pDpkfkp.

Further suppose there is a constantCb > 0depending only on (X,β,µ,T) such that we have

(4.10) µ({x:M f(x) > λ}) ≤ Cb λ Z

X|f|dµ.

Then there is a constant D > 0depending only on(X,β,µ,T)such that if q > 1then (4.11) µ({x:Vqf(x) > λ}) ≤ D

λ Z

X|f|dµ.

Proof. Suppose(X,L,η)denote a finite measure space i.e. η(X)<∞. Now, let(Tn)n≥1

denote a sequence of linear transformations ofLp(X,L,η)into measurable functions on X, such that each Tn is continuous in measure, that is, such that if ||ffm||p tends to 0 as m tends to ∞, then ||TnfTnfm||p also tends to 0 as m tends to ∞. Set Tf(x) = supn≥1|Tnf(x)| for fLp(X,L,η). We will say the family (Tn)n≥1 commutes with w: XX ifTf(w(x))≤Tg(x)where g(x) = f(w(x)) onX. Now supposeF is a family of ergodic η preserving transformations on X, closed under composition. We will call (Tn)n≥1distributive if it commutes with all the elements of some familyF onX. We have the following result of S. Sawyer [Sa].

Lemma 4.5. Let (Tn)n≥1 be a distributive sequence of linear operators on Lp(X,L,η), where each Tnis continuous in measure and maps Lp(X,L,η)to measurable functions on X . If p∈[1,2]and if Tf(x)<∞ηalmost everywhere, then there exists a uniform constant C>0such that

(4.12) η {x:Tf(x)≥λ}

C λp

Z

X|f(x)|pdη, for allλ >0and fLp(X,L,η).

The conclusion of Lemma 4.5 is that if Tf(x) <∞ η almost everywhere, then the operator T satisfies a weak(p,p). If there is a C>0 such that ||Tf||pC||f||p we sayTsatisfies astrong(p,p)inequality. It is easy to check that strong(p,p)inequalities imply the corresponding weak(p,p)inequalities for the operatorT. On the other hand it follows from the Marcinkiewicz interpolation theorem [SW] that a weak(p,p)inequality implies a strong(q,q)inequality ifq>p. We now specialize (4.1) to the situation where f is defined onX=R,L is the Lebesgue algebra onX =Randη=µα,β:

TNf(x):= 1 N

N n=1

f(Tα,βkn (x)) (n=1,2, . . .) with f(x) =ζ(σ+ix). One checks readily that(TN)N≥1 commutes with(Tαn)n≥1 and is therefore distributive. In light of Lemma 4.5, we see that Theorem 1.4 follows by recalling

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