CONVERGENCE AND MODULAR TYPE PROPERTIES OF A TWISTED RIEMANN SERIES
21 pages
English

CONVERGENCE AND MODULAR TYPE PROPERTIES OF A TWISTED RIEMANN SERIES

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21 pages
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Niveau: Supérieur, Master, Bac+5
CONVERGENCE AND MODULAR TYPE PROPERTIES OF A TWISTED RIEMANN SERIES T. RIVOAL AND J. ROQUES Abstract. We consider the series ?(?) = ∑∞ m=1 1 m2 sin(2pim 2?) cot(pim?), a twist of the famous continuous but almost nowhere differentiable sine series defined by Riemann. In a slightly different but equivalent form, this series appeared in the first author's paper [On the distribution of multiple of real numbers, Monatsh. Math 164.3 (2011), 325–360]. We pursue here the study of ?, which is almost everywhere but not everywhere convergent. We first prove that ? enjoys a modular type property, in the following sense (with ?n the n-th partial sum of ?): For all ? ? (0, 1], the sequence ?N (?) ? ??b?Nc(?1/?) has a finite simple limit ?(?) as N ? +∞. Using analytic properties of ?, we then prove that ?(?) converges if and only if ? is irrational and ∑ j log(qj+1)/qj converges (Brjuno's condition), where qj is the j-th denominator in the sequence of convergents to ?. This completes the results obtained in the above mentioned paper, where it was proved that ?(?) converges absolutely under Brjuno's condition.

  • brjuno's condition

  • fraction expansion

  • riemann series

  • j?1 ∑

  • since ? ?

  • see section

  • sin

  • functions

  • convergence properties


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Publié par
Nombre de lectures 15
Langue English

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4FENAGGAE4A2E;DF;MC2GLYPAPGFPAGLIAI FB2LWIILA;GIAD2EEIAGIAI
T. RIVOAL AND J. ROQUES
P1π=( (in(2,2 ) cot(, ,)taiwtsofthe 5LefdJMf.risehert(esWisedceno ) =π2s famouscontinuousbutalmostnowheredierentiablesineseriesde nedbyRiemann.Ina slightlydierentbutequivalentform,thisseriesappearedinthe rstauthorspaper[On the distribution of multiple of real numbers Math, Monatsh.134eW06.](201.325{31),3 pursueherethestudyof,whichisalmosteverywherebutnoteverywhereconvergent. We rstprovethatenjoysamodulartypeproperty,inthefollowingsense(withn then For-th partial sum of ): all 2(0;1], the sequence N( )  bN c( 1= ) has a nite simple limit ( ) asN!+.Ungsialanicytporpitrefoseew,erpvohtne P that ( ) converges if and only if is irrational andαlog(qα+()q=αconverges (Brjuno’s condition), whereqαis theπ-th denominator in the sequence of convergents to . This completes the results obtained in the above mentioned paper, where it was proved that ( ) converges absolutely under Brjuno’s condition.
1.iaMfNgdaˆfA ˆ This paper deals with the series X 1 ( ) =m+sin(2m+ ) cot(m ).(1.1) m=) (The summand is defined for any real number because sin(2m+z) cot(mz) is an entire P function for any integerm1.ofRiwistisat)Iteissnremenahidpohantinestudyin[1R.]3ameinm=n)semr)i+cis(2insseomnti+ It).nusuo appeared in a different form in t e onRand nowhere differentiable, except at the rational numbers of the formp/qwithp andq6]t[aarmteisDudraHeG,yrpoc(emiodthnddaboerIV]I.),5hCpatitsu;see[rver,Ita showed that these facts are simple consequences of the following modular type functional on, whereR( ) =Pm=)m+and > equatie+im+ 0: +3Z ,(1. R( ) ei/1 0/+R( 1/ ) =6+iei/1p  i2  2ei/(1p R( 1/)d2) which itself can be deduced from the classical modular equation satisfied by the theta series Pm2Zeim+ . The latter was used by Jaffard [7] to compute the multifractal spectrum of
Date: February 28, 2012. 2010atMcstimaheuSjbceCtalss iaction.Primary 11J70, 40A05, Secondary 11F03, 22A30. Keywordsandphrases.Twisted Riemann series, Brjuno’s condition, Modular type equations, Contin-ued fraction expansions. 0
1
Riemann series. The important information in (1.2) is that the right-hand side is much smoother (differentiable with continuous derivative on (0,+)than what is suggested by theleft-handside(continuousbutalmostnowheredierentiable). Weaddressheretwoquestions: When does the series ( ) converge? {Does the series ( ) satisfy a modular type functional equation (like (1.2)that pro-vides some non-trivial analytic information? Although both questions might seem unrelated, it turns out that our answer to the second one is an important step to answer the first one. We shall now make a couple of comments concerning the first question. On the one hand, it is easy to prove that the series diverges for all rational number =p/qwith (p, qin this case, for any integer  Indeed,) = 1.J1, q )q )J )J ) X X X Jsin(2m+ ) cot(m X 1 1 m=)m+(2ins=)k+p/q) cot(q/pk))(jq+k)++ 2j=),qj k=)j= whencealogarithmicdivergenceof(p/qtaht]3.)nOhtoehtreahdn,itwasprovedin[1 ( ) converges absolutely for any irrational number satisfyingBePhab'f BMbcL.agMaF ;baBMgMba Xlog(qj+))<,(1.3) q (j j= whereqjdenotes thejof the sequence of convergents to-th denominator . ()) More precisely, the “absolute convergence" result proved in [13] concerns the series of general termm)+Pmk=)cos(2km ) but this does not change anything since Xmcm+ 1 ) m+k)cos(2 km) = os(m(mm+in)(1+sm ) (n)is = ) sin(m+ )+ =sin(2m+ )2mc+ot(m m+( .4) 1 and the second fraction on the right of (1.4) is the term of an absolutely convergent series for any  proof uses the fact that. Thejsin(2m+ ) cot(m )j jj mm+ jj(wherejxj denotes the distance ofx2RtoZ) and then estimates in terms of the continued fraction expansion of for the growth of the sumsPNm=)mj+m+ mjj,inspired by the estimates found j in Kruse’s paper [9] for the sumsPNm))j also [14].. See =msjm )esriseTvedisprosultheretsehecnrc]no[n31Pn1(os(c=n(n21i)(+ n(1is))n2 )and its simple relation with ns ( ( Eq.(1.4)below.Fui)gsvineybcompmoreli-id[nalectyeh41b]itndcosepsrniioromrehtronujrB,e cated conditionPα)(og+(xaqj1+q=jq;j)αhttaobhtdeni1[]4snotstat.Itwa:tnelaviqueearnsioitndco q j P = ; qα) 2qα indeed, we haveqα+(=qαmax(qα+(qα+(and the seriesαlog(qα)=qαis convergent for any irrational number  is well-known that only Liouville numbers may fail to satisfy Brjuno’s condition,. It which thus holds almost surely.
7iSgdP ,.
Plot of
2((on [0 1 ,
2
In the present paper, a modular type property of ( ) is established and used in order tounderstandmorepreciselytheconvergencepropertiesof( egeryintoran)F.Nand any real number , we denote bN ) theN-th partial sum of ( ) : y  ( N Xsin(2m+ ) cot(m  ( ) = ). N)m+ m= We then consider
N( ) = N( )  ( 1/ ) N c where⌊  c observe that the limit of Ω Wedenotes the floor function.N( ) is. ceMbeM defined almost everywhere on (0, The first part of the paper is1] but not everywhere. devoted to the proof of the following result, which in particular shows that the limit of N( ) exists and is defined everywhere on (0,toroirehF.]1,nemonehonchapofsuncesnsta see [1, 2, 3, 15, 18]. LWTdeTb .1abhFG;aGbFMhgd;FfFfLaTNL.f . fMWcTF TMWMgba(0,1].fN!+. MbeFbiFe, X
N 1 Ω ( ) = sin(2mm0+ +) N  ) m= jLFeFGNL.f . fMWcTF TMWMgGba[0,1].fN!+.aBj ;bafg.ag Gbe .TT 2[0,1].aB .TTN1. In particular, the function (1Xsin(2m+ )  m=)m0
( (
(1.5)
Mf :bhaBFB :l .a .:fbThgF
(1.6)
3
7iSgdP -.
Plot of Ω
2((on [0.07,1]
i is defined and bounded on [0,.6(1inesrisenesiekil-nnameiRehT.1])scontinuousand behaves like log(1/ ) as !0+(see Lemma 3). These facts will be important for the proof of Theorem 2 stated below. We will provide explicit expressions for the limits G( ) and Ω(  Graphical experiments (see) but they are not easy to study precisely. Figure 2) done with the computer algebra system PARI/GP lead us to formulate the following conjecture: 4dcjTRgheT .1TLF Gha;gMbaGMf ;bagMahbhf ba[0,1]. Fortunately, Theorem 1 provides us enough control on Ω and this conjecture is not required for the proof of our next result. LWTdeTb ..,be .al Mee.gMba.T ahW:Fe 2(0,1), gLF fFeMFf( );baiFeIFf MG .aB baTl MGBePhab'f;baBMgMba(1.3)LbTBf. Ia;.fFbG;baiFeIFa;F,jFL.iF X ( ) =T ( )  Tj )( )Ω(Tj( )(1.7) j=( jLFeFTk( )BFabgFf gLFkfigL MgFe.gF bG :l gLF G.hff W.cT( ) ={1/ }. RFW.eR.By the classical properties of continued fraction expansions, we haveTj( )qqj+)j )  T) =jq and T( j )( )  pj )j q)j. (See Section 3.1 for some properties of j continued fraction expansions.) Hence, since Ω has a logarithmic behavior at the origin, identity (1.7) can be viewed as the quantitative version of the first (qualitative) part of Theorem 2. Similar expansions can be found in [15, 16] for instance and implicitly in [17]. Asmentionedabove,itwasprovedin[13]that( ) converges absolutely if Brjuno’s condition holds. Together with Theorem 2, this leads to the following result.
4dedaaOey
TLF fFeMFf
(
;baiFeIFf MG .aB baTl MG Mg ;baiFeIFf .:fbThgFTl.
4
We observe here that  could be related with “false" Lerch’ sums and “false" theta functions (“false" means here that we replace summations overZby summations overN intheusualdenitionsofLerchsumsandthetafunctions).ForLerchsums,wereferthe reader to Mordell’s papers [11, 12] and Zwegers’ thesis [19] on mock theta functions. It would be interesting to know if an alternative expression for Ω could be deduced from this relationship which would prove Conjecture 1.
Beside Conjecture 1, let us conclude this introduction with a few other problems. For-mally,theFourierseriesexpansionof( ) isS()( ) =)+++Pn=)n+n+cos(2n ) where X X =d+ nifnis a square, =d+otherwise. n n 2 p p
djn )d
djn )d
This is an easy consequence of (1.4). Two problems are to determine for which ’s the Fourier seriesS()( ) converges (+) and for which ones we haveS()( ) = ( ). In the spiritofDavenport-likeproblems(see[4,10]),thenaturalanswerswouldbeifandonly if Brjuno’s condition holds" for both problems but we don’t know what to expect here. It was proved in [13] thatS()( ) = ( ) ifPj=(qj+)/qj+converges, which is an almost sure condition but stronger than Brjuno’s condition. Another problem is the determination of p p the minima of  on [0,1], which seems to be at =+2 )and =0 +2. Finally, it would be interesting to know if our method can be adapted to study the convergence of the series X sin(2m+ ) cot(m ) ms
m=)
for any givens2(1,iressihtrevnocseusiobvros,onasregrseidev,respges,velyecti)2(.oF for every 2Rifs >2, respectively ifs1.)
Wewillfrequentlyworkwithanalyticfunctionshon an open subset Ω ofCdefined as the quotient of analytic functionsh=f /gon Ω. For anyz2Ω, the quotientf(z)/g(z) (which is not well defined ifg(z) = 0) will meanh(z will be implicit in the whole). This paper. We will still denote by⌊c ona modified floor function: [0,+) it coincides with the usual floor function while on (,0) it is set to zero. We will also often treat labels 1 given to certain quantities as mathematical expressions; for instance, if (10.) and (10.2) are such labels, we will freely write things likej(10.1)j ≤1 or (10.2) = 0 when the meaning is obvious.
+Since
(0;1),
()convergestoalmosteverywherebyCarlesonstheorem.
5
2.aRaadPVPdaPTHR, 2.1..ygYgcTYgSeYIROfOPUUg;ydddTpVeWOTgLetf:Rn {0} !C For allbe a map. N2Nand all 2RnQ, we set XNf(2m+ ) cot(m ) ΨN( ) =m=)m+. (The value of an empty sum is set to 0.) Using the classical expansion X 1 1 ++, cot(z) =z2zn=)z n+ which is valid and uniform on any compact subset ofCnZ, we get, for allM, N2Nand all 2(0,+)nQ, + +M ΨN( )  ΨM( 1/  1) =XNf(2mXf( 2m+/ )  +) 0 m=)m m=)m0 N X XMf(2m+ )f( 2n+/ ) 1 + 2 m=)n=)m nm + + n+ +XN1X+f(2m+ )+XM1X+f( 2n+/ ) 2 m+ + n+ 2mn + + n+. m=)mn=M+)n=)m=N+) Iffis the restriction of an analytic function vanishing onZ, then the above equality is meaningful and valid on (0,+htperaitucalcrsae).erThorefine,f= sin, we obtain, for all >0, X + Ncsim+ 2 N( ) = 1XmN)sin(2m+ ) n(/ m(12).) 0 =m 0)= m X Xsin(2n / ) 1 N Ncsin(2m++)+ + 2 n m + + n+(2.2) m=)n=)m +XN1mX+sin(2m+ +))(2.3 2 m=)n= Nc+)m+ + n + 2 +X Nc1X+simn(+ 2n+ +/ n+).(2.4) )nm=N+) n= InordertoproveTheorem1,itissucienttoshowthatthethreesequences(2.,(2.3) 2) and (2.4) converge asNtends to +and that their moduli are bounded by an absolute constant for all 2[0,1] andN will 1. Thisbe proved in Sections 2.2, 2.3 and 2.4 respectively.
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