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Exponentially long time stability for non-linearizable analytic germs of (C^n,0)

Carletti, Timoteo

Published in:

Annales de l'Institut Fourier

Publication date:

2004

Document Version

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Citation for pulished version (HARVARD):

Carletti, T 2004, 'Exponentially long time stability for non-linearizable analytic germs of (C^n,0)', Annales de

l'Institut Fourier, vol. 54, no. 4, pp. 989-1004.

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TIMOTEOCARLETTI

Abstra t. Westudy the Siegel{S hroder enter problem on the lineariza-tionofanalyti germsofdi eomorphismsinseveral omplexvariables,inthe Gevrey{s, s > 0 ategory. We introdu e a new arithmeti al ondition of Brunotypeonthe linearpartofthegivengerm,whi hensurestheexisten e of a Gevrey{s formallinearization. We usethisfa t to provethe e e tive stability,i.e. stabilityfor nitebutlongtime,ofneighborhoodsoftheorigin fortheanalyti germ.

1. Introdu tion

In this paper we onsider the Siegel{S hroder enter problem [He , CM, Ca℄in some lassofultradi erentiablegermsof(C

n

;0), n1;letus onsidertwo lasses of formal power series A

1  A 2  C n [[z 1 ;:::;z n ℄℄, losed w.r.t. to derivation and omposition, let F 2 A

1 and all DF(0) = A 2 GL(n; C ), we say that F is linearizable in A 2 if there exists H 2 A 2

, normalizedwith DH(0) = I,whi h solves 1 : (1.1) FÆH(z)=HÆR A (z); where R A

(z)=Az. Inthefollowingwewill assumeAto bediagonalwith eigen-valuesofunit modulus

1 ;:::; n ,thusA=diag( 1 ;:::; n ). IfbothA 1 andA 2

oin idewiththeringofformalpowerseriesthengeneri ally theformallinearizationholdsifandonlyifAisnon{resonant,namelyforall 2

N n su hthatj j= P 1in i

2,andforallj2f1;:::;ngthen

 j

6=0(where weusedthestandardnotation

= 1 1 ::: n n ).

When F is a germ of analyti di eomorphisms de ned in a neighborhood of theoriginand wewanttosolve(1.1)in thesame lassofanalyti germs,wehave to onsider several ases. If Ais thePoin are domain, namely sup

1jn j j j <1 or sup 1jn j 1 j

j < 1, then Koenigs [Ko℄ and Poin are [Po℄ proved that every analyti germF 2Diff(C

n

;0)su hthatF(0)=0andDF(0)=A, isanalyti ally linearizable. WhenA isnotin thePoin aredomain,wesaythatitisin theSiegel domain;thequestionisharderandsomeadditionalarithmeti al onditionson(

j )

j areneeded(see[He ℄x17page158).

Date:July20,2004.

Keywordsandphrases. Siegel enterproblem,Gevrey lass,Bruno ondition,e e tive stabil-ity,Nekoroshevlikeestimates.

1

HereFÆHmeansthe ompositionofFandH;inthefollowingwewilldenotethe omposition ofF n-timeswithitself,byF

n

insteadofF Æn

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Letp2 N

,p2andletusde nefornon{resonant 1 ;:::; n : (1.2) (p)= min 1jn inf 2N n 0<j j<p j  j j;

wesay that A veri esaDiophantine ondition of type( ;) if there exist > 0 and n 1su hthatforall 2

N n

nf0gwehave(j j) j j 

. Siegel[Si ℄in 1942forthen=1 aseand thenSternberg[St ℄ andGray[Gr℄in thegeneral ase provedthatifAveri esaDiophantine onditionthenthelinearizationproblemhas ananalyti solution. Bruno[Br℄weakenedthearithmeti al onditionbyaskingthe onvergen eoftheseries

P k log 1 (2 k +1 ) 2 k

. Weremark thatintheonedimensional asetheBruno ondition

2

isoptimal,asprovedbyYo oz[Yo℄.

In[CM ℄authorsstudiedtheSiegel{S hroder enterprobleminthe aseofgeneral algebrasofultradi erentiablegermsof(C;0),in ludingtheGevrey ase. In[Ca℄the multidimensional aseis onsidered: ifA

1 =A

2

andAveri esaBruno ondition, theneveryF2A

1

withF(0)=0andDF(0)=Ais linearizablein A 2 ,whereasif A 1 isproperly ontainedinA 2

new onditionsweakerthanBrunoaresuÆ ientto ensurelinearizabilityin A

2 .

In this paper we onsider in detail the ase where A 1

is the ring of germs of analyti di eomorphismsat theoriginof n 1 omplexvariables, and A

2 is the algebra of Gevrey{s, s > 0, formal power series: the Gevrey{s linearization of analyti germs. Let ^ F = P f z , (f ) 2N n  C n

beaformalpowerseries, then wesaythat it isGevrey{s[Ba,Ra℄,s>0,ifthereexisttwopositive onstantsC

1 ;C 2 su hthat: (1.3) jf jC 1 C sj j 2 (j j!) s 8 2N n :

Wedenotethe lassofallformalve torvaluedpowerseriesGevrey{sby C s

. It is losedw.r.t. derivationand omposition.

IntheGevrey{s asethearithmeti al onditionintrodu edin [CM,Ca℄will be alledBruno{s ondition,s>0: forshortA2B

s

ifthereexistsastri tlyin reasing sequen eofpositiveinteger(p

k ) k su hthat: (1.4) limsup j j!+1 0  2 ( ) X m=0 log 1 (p m+1 ) p m slogj j 1 A <+1; where( )isde ned byp ( ) j j<p ( )+1 .

Remark 1.1. This de nition re all the lassi al one of Bruno [Br℄, where rst one suppose the existen e of astri tly in reasing sequen e of positive integersu h that (1.4) holds, then one anprove (see [Br℄ xIVpage 222) that one an take an exponentially growing sequen e, e.g. p

k =2

k

. This holdsalso inour ase, in fa t we an prove that (1.4)isequivalentto:

limsup N!+1 N X l=0 log 1 (2 l+1 ) 2 l sN2log2 ! <+1: 2

Inthis aselet!2(0;1)nQ su hthat=e 2i!

andlet(q n

) n

bethedenominatorsofthe onvergents[HW℄to!,then the Bruno ondition isequivalentto the onvergen eof theseries P k 0 logq k +1 q .

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Letusgiveasket hofthe proof ofthis laim. Takeasequen e(p k

)for whi h (1.4) holds, then we an nd sequen es of positive integer (m

k ) k and (l k ) k su h that: m 0 =0,l k 1,m k +1 =m k +l k and 2 m k p k <2 m k +1 <<2 m k +l k p k +1 <2 m k +l k +1 : The fun tion 1 (p) is in reasing, hen e: 1 (2 q+1 ) < 1 (p k +1 ) for all q = m k ;:::;m k +l k 1, andso: (1.5) m k +l k 1 X q=m k log 1 (2 q+1 ) 2 q <4 log 1 (p k +1 ) p k :

Takeany j j>1, the orresponding ( )and xN( )=m ( )

+l ( )

2. Then, dividing thesum of (1.4)intopie es fromm

h tom h +l h 1,for h=0;:::;( ), andusingestimate (1.5)for ea h pie e, weget:

2 0  2 ( ) X m=0 log 1 (p m+1 ) p m slogj j 1 A > N( ) X l=0 log 1 (2 l+1 ) 2 l 2slogj j:

Nowthe laimfollows remarkingthat 2slogj j sN( )2log2+ .

Forrealnumber,theBruno{s ondition anbeslightlyweakened(see[CM℄);let !2(0;1)nQ ,thentheBruno{s,s>0, onditionreads:

(1.6) limsup k !+1 0  k X j=0 logq j+1 q j slogq k 1 A <+1; where(q k ) k

arethedenominatorsofthe onvergentsto!. Weremarkthatinboth asesthenew onditionsareweakerthanBruno ondition,whi hisre overedwhen s=0. Indimensiononeweprovethat the set

S s B s isPSL(2; Z ){invariant(see remark3.1). Themainresultof[Ca℄in the aseofGevrey{s lassesreads:

Theorem1.2(Gevrey{slinearization). Let 1

;:::; n

be omplexnumbersofunit modulusand A=diag(

1 ;:::; n ); let D 1 =fz2 C n :jz i j<1;1ingbethe isotropi polydisk of radius 1 and letF :D

1 !

C n

be an analyti fun tion, su h thatF(z)=Az+f(z),withf(0)=Df(0)=0. IfAisnon{resonantandveri esa Bruno{s, s>0, ondition (1.4)(or (1.6)when n=1), then thereexistsa formal Gevrey{slinearization

^

H whi h solves (1.1).

The aim of this paperis to show that the Gevrey hara ter of theformal lin-earization angiveinformation on erningthedynami softheanalyti germ. Let F(z)= Az+f(z) beagerm of analyti di eomorphism verifying thehypothesis of Theorem 1.2, assume moreoverF not to be analyti allylinearizable. We will showthatevenifthereisnotSiegel disk,where thedynami sofF is onjugateto thedynami sofitslinearpart,wehaveanopenneighborhoodoftheoriginwhi h \behavesasaSiegel disk" under theiterates of F for nite but longtime, whi h resultsexponentiallylong: thee e tivestability[GDFGS ℄ofthe xedpoint.

Inthe aseofanalyti linearization,jH 1 i

(z)j,i=1;:::;n,(whi hiswellde ned suÆ iently lose to the origin be ause H is tangent to the identity) is onstant along theorbits, namelyitisa rstintegralandjF

m (z

0

)jisboundedforallmand suÆ ientlysmalljz

0 j.

Wewillprovethatanynon{zeroz 0

belongingtoapolydiskofsuÆ ientlysmall 1=s

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the Gevreyexponent of the formal linearization, and we an nd analmost rst integral: afun tionwhi hvariesbyaquantityoforderrunder mK iterations, whi himpliesthatF

m (z

0

)iswellde nedandboundedformK. Morepre isely weprovethefollowing

Theorem1.3. Let 1

;:::; n

be omplexnumbersofunitmodulusandA=diag( 1 ;:::; n ); letF :D 1 ! C n

beananalyti andunivalentfun tion,su hthatF(z)=Az+f(z), with f(0)=Df(0)=0. If A isnon{resonantandveri es aBruno{s, s>0, on-dition (1.4)(or (1.6)whenn=1),thenforallsuÆ ientlysmall0<r



<1,there existpositive onstants A

 ;B

 ;C



su hthat for all 0<jz 0 j <r  =2,the m{th iterate of z 0

by F is well de ned and veri es jz m j = jF m (z 0 )j  C  r  , for all mK  = j A 1  exp n B  (r  =jz 0 j) 1=s ok .

ThehypothesisonthedomainforF isanaturalnormalization onditionbeing thewholeprobleminvariantbyhomothety.

Inse tion3we ompareourstabilityresultwiththestrongerresultswhi h an beprovedusing Yo oz'srenormalizationmethod [PM2℄ inthe asen=1. More-overwe dis uss therelation between ourBruno{s ondition andthe arithmeti al ondition ofPerez{Mar o[PM1, PM2℄ ensuring that in thenon{linearizable ase the xedpointisa umulatebyperiodi orbits.

A knwoledgements. Iamgratefulto D.Sauzinforaverystimulatingdis ussion on erningGevrey lassesandasymptoti analysis.

2. Proof of the mainTheorem

Inthis partwe willproveour main result,Theorem 1.3. Theproof will be di-videdinto threesteps: rstweusetheGevrey{s hara teroftheformal lineariza-tion

^

H, given by Theorem 1.2, to nd anapproximate solutionof the onjuga y equation (1.1) up to a (exponentially) small orre tion (paragraph 2.1); then we proveaniterativeLemmaallowingusto ontrolhowthesmallerrorintrodu edin thesolutionpropagates(paragraph2.2). Finallywe olle talltheinformationsto on ludetheproof(paragraph2.3).

2.1. Determinationof anapproximate solution. WeapplyTheorem1.2: the formalpowerseriessolution

^

H belongstoC s

,aswellasitsinverse ^ H 1 whi hsolves (formally): (2.1) ^ H 1 ÆF(z)=R A Æ ^ H 1 (z): Sin e ^ H 1 = P h z 2C s

,thereexistpositive onstantsA 1 andB 1 su h that (2.2) jh jA 1 B sj j 1 (j j!) s 8j j1:

For any positiveintegerN we onsider the ve torial polynomial, sumof homoge-neousve tormonomialsofdegree1lN,de nedby: H

N (z)= P N l=1 P j j=l h z

andtheRemainder Fun tion:

(2.3) R N (z)=H N ÆF(z) R A ÆH N (z):

ThefollowingProposition olle tssomeusefulpropertiesoftheremainderfun tion.

Proposition 2.1. Let R N

(z) be the remainder fun tion de ned in (2.3) and let 2 N n ,then: 1)  R N (0)=0if j jN.

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2) Forall 0<r<1there existsa positive onstants A 2 andB 2 su h that if j jN+1,then: 1 !  z R N (0) A 2 r j j B sN 2 (N!) s :

3) Forall 0<r<1andjzj<r=2 thereexist positive onstants A 3 ;B 3 su h that: (2.4) jR N (z)jA 3 B sN 3 (N!) s  jzj r  N+1 :

Whereweusedthe ompa t notation 1 !  z = 1 1!::: n!  j j  1 z 1 ::: n zn .

Proof. Statement1)isanimmediate onsequen eofthede nitionofR N

. Toprove2)weobservethatR

N

(z)isananalyti fun tion onD 1

,thenonegets byCau hy'sestimatesforall0<r<1andforallj jN+1:

(2.5) 1 !  z R N (0)  1 (2) n 1 r j j+1 max jzj=r jH N ÆF(z)j:

Re allingtheGevreyestimate(2.2)forH N

andtheanalyti ityofF weobtain:

(2.6) 1 !  z R N (0) A 2 B sN 2 (N!) s r j j ;

forsomepositive onstantsA 2

andB 2

dependingontheprevious onstants,onthe dimensionnandonF.

To prove 3) let us write the Taylorseries R N (z) = P j jN+1 1 !  z R N (0)z , thenthebound onderivatives(2.6)impliestheestimate(2.4)foralljzj<r=2and forsomepositive onstantsA

3 andB 3 .  Thebound (2.4)onR N

(z)dependsonthepositiveintegerN,sowe an deter-mine thevalue of N for whi h theright hand side of (2.4) attains its minimum, that'sPoin are'sideaofsummationatthe smallestterm.

Lemma2.2(Summationatthesmallestterm). LetR N

(z)de nedasbeforeandlet 0<r



<1=2thenthereexistpositive onstantsA 4

;B 4

su hthatforall0<jzj<r  wehave: (2.7) jR  N (z)jA 4 exp n B 4  r  jzj  1=s o ; where  N =bB 4 ( r  =jzj) 1=s

andbx denotes the integerpart ofx2 R . Proof. Letus x0<r  <1=2,thenfor0<jzj<r 

byStirlingformulaweobtain:

(2.8) jR N (z)jA 4  NB 1 3 (jzj=r  ) 1=s  Ns e sN ;

for somepositive onstantA 4

. The righthand side of (2.8) attainsits minimum at  N = B 3 (r  =jzj) 1=s

, evaluating the value of this minimum we get (2.7) with

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2.2. Control of the \errors". Letus de neH (z)=H  N (z)andR(z)=R  N (z), being 

Nthe\optimalvalue"obtainedinLemma2.2. WeremarkthatH (z)doesn't solve(2.1)butthe\error",R(z),isverysmall: exponentiallysmall. Wewillprove thatforinitial onditionsinasuÆ ientlysmalldisk,one aniterateanexponentially largenumberoftimeswithoutleavingadisk,say,ofdoublesize.

Lemma2.3 (Iterationlemma). Leta;b; andR bepositive realnumbers. Letus onsider the sequen e ofpositive number(

j ) j0 de nedby:  0 =R and  j+1 = j +aexpf b= j g: LetK=bR a 1 expfb=(2R ) g , then j 2Rfor allj K.

Proof. Letusprovebyindu tiononj thatforall0j K wehave

(2.9) 

j

R+jaexpf b=(2R )

g;

thenthe laimwill followfrom(2.9)andthede nitionofK,infa t foralljK:

 j R+jaexpf b=(2R ) gR+R a 1 expfb=(2R ) gaexpf b=(2R ) g2R:

The basis of indu tion is easily veri ed; assume (2.9) for all j  K 1, we will proveitforj=K. Byde nitionof (

j )

j

andtheindu tion hypothesis wehave:

 K =  K 1 +aexpf b= K 1 g  R+(K 1)aexpf b=(2R ) g+aexpf b= K 1 g;

weremarkthatfrom(2.9)withj=K 1,usingK 1<R a 1 expfb=(2R ) g,we get K 1 2Randexpf b= K 1 gexpf b=(2R ) g. Thenwe on lude:  K R+(K 1)aexpf b=(2R ) g+aexpf b=(2R ) g;

whi hendstheindu tion. 

Letr 

asinLemma2.2,de ne(z)=jH (z)jforall0<jzj<r 

,thenLemma2.2 admits the following Corollary, whi h allows us to ontrol the fun tion (z) on onse utivepointsofanorbitofF(z).

Corollary2.4. Let0<r 

<1=2,letr 1

betheradiusofthemaximalpolydiskwhere H (z) is invertible and let r



= min (r 

;r 1

). Then there exist positive onstants A

 ;B



su hthat for all0<jzj<r  wehave: (2.10) (F(z)) (z) A  exp n B   r  (z)  1=s o :

Proof. Byde nition (F(z))=jHÆF(z)j and (z)=jR A

ÆH (z)j, sin ej j

j =1 for1jn,andA=diag(

1 ;:::; n ) ,therefore: (F(z)) (z)  HÆF(z) R A ÆH (z) =jR(z)j;

andfromLemma 2.2weget:

(2.11) (F(z)) (z) A 4 exp n B 4  r  jzj  1=s o :

Wewanttoexpressthis onditionintermsof(z)insteadofjzj,todothiswehave to onsiderthedistortionpropertiesofH (z)andofitsinverse. LetJ(z)=

z H (z) betheJa obianof H (z)and letJ

1 =max jzjr 1 jJ(z)j, where r 1

has beende ned previously. Let0<jzj<r andletus allz

0

=H (z), learlyjz 0

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us allJ 2 =max jz 0 j<r2 j z 0 H 1 (z 0

)j,thenforany0<jz 0

j<r 2

thereexistsonlyone z su hthat z=H 1 (z 0 ),whi hsatis esjzjJ 2 jz 0 j=J 2 jH (z)j. Letr  =min (r  ;r 1

)thenfrom(2.11)forany0<jzj<r  weget: (F(z)) (z) A  exp n B   r  (z)  1=s o ; whereA  =A 4 andB  =B 4 J 1=s 2 . 

2.3. Endofthe proof. Wearenowableto on ludetheproofofthemain Theo-rem1.3. Takeany0<jz

0 j<r



=2andletusde ne 0 =jz 0 j, m =(F m (z 0 ))for allpositiveintegermforwhi hF

m (z

0

)iswellde ned,byCorollary2.4wehave:

(2.12)  m  m 1 +A  exp n B  (r  = m 1 ) 1=s o : Letus allR=jz 0 j,a=A  ,b=B  r 1=s 

and =1=s,thenwe anapplyLemma2.3, being m  m ,to on ludethat: (2.13)  m r  8mK  = j jz 0 jA 1  exp n B   r  2jz 0 j  1=s ok :

ThisimpliesthatH (z m

)iswellde nedinthisrangeofvaluesofm,itisnot onstant andit evolvesonlyby

jH (z m )j jH (z 0 )j r  . Re alling that z m =F m (z 0 )we alsohavejF m (z 0 )jJ 2 r  and jz m j jz 0 j J 2 r  forall0<jz 0 j<r  =2andall mK  .

This on ludetheproofbysetting A  =2A  r 1  , B  =B  (r  =(2r  )) 1=s and C  =J 2 .

3. Onedimensional ase

Inthis paperwe provedthat anyanalyti germsof di eomorphismsof (C n

;0) withdiagonal,non{resonantlinearparthasane e tivestabilitydomain,i.e. stable up to nite but \long times", lose to the xed point, provided the linear part veri esa new arithmeti al Bruno{like ondition (1.4) depending on aparameter s>0. Remark 3.1 (Invarian eof S s>0 B s

, n=1under thea tionof PSL(2;Z)). The ontinuedfra tiondevelopment[HW,MMY ℄ofanirrationalnumber! givesusthe sequen es: (a k ) k 0 and(! k ) k 0

. Then we introdu e ( k ) k  1 de ned by 1 =1 and for all integerk 0:

k = Q k j=0 ! k , whi h veri es : 1=2< k q k +1 <1and q n n 1 +q n 1 n =1, where q k

's are the denominators of the ontinued fra tion development of !. We laim that ondition Bruno{s (1.6) is equivalent to the followingone: (3.1) limsup k !+1 0  k X j=0 j 1 log! 1 j +slog k 1 1 A <+1:

This an be proved by using the relations between l

and q l

, to obtain the bound, for allinteger k>0:

k X  l 1 log! l + logq l+1 q l   k X l 1 log l q l+1 + l 1 log l 1 + q l 1 q l l logq l+1 18;

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where weused the onvergen eof series q l and q l logq l

(see[MMY ℄ page 272).

To prove the invarian e of S

s B

s

under the a tion of PSL(2;Z), is enough to onsider its generators: T! =!+1andS! =1=!. For any irrational !,T a ts triviallybeing

k

(T!)= k

(!)forallk,whereasforSwehave k

(!)=! k 1

(S!) for all k1. Let ! bean irrational andlet !

0 =!

1

,let usalso denote witha 0 quantitiesgiven by the ontinuedfra tionalgorithm applied to!

0

,thenusing (3.1) one an prove:

! 0 0  k X j=0 0 j 1 log! 0 j 1 +s! 1 0 log 0 k 1 1 A =C(!;s)+ k +1 X j=0 j 1 log! 1 j +slog k ; whereC(!;s)=! 0 log! 1 1 slog! 0  + P 1 l=0 l 1 log! 1 l

,from whi h the laim follows.

Letus onsideraslightlystrongerversionof theBruno{s ondition: !2 R nQ belongsto ~ B s if: (3.2) lim k !+1 k X l=0 logq l+1 q l slogq k ! <+1; where(q n ) n

arethe onvergentsto!.

Remark3.2. This new onditionisstrongerthanBruno{s,be ausethe existen e of the limit isrequired. One an onstru tnumbers ! whi h verify B

s but not ~ B s , asfollows.

Letus all for shorts k = P k l=0 logql+1 q l slogq k . Fix > >0,Æ>0andto simplify takes>(2+Æ)=log2. We laimthatone an hooselargeenoughpositive integers k 1 anda 1 ;:::;a k1+1 su hthat: s k s k 1 Æ and s k1 2( ;2 );

forinstan etakek 1 >( logq 1 )Æ 1 andindu tivelya l+1   e Æql  ql 1 q l 2  2ql q l 1  q 1 l , for all l = 1;:::;k 1

. Then one an take suÆ iently many a l 's equal to one, a k 1 +1+l =1for l=1;:::;2k 2

+1,and verifythat:

s k1+1+2j s k1+1+2j 2 < Æ;8j=0;:::;k 2 and s k1+1+2k2 < :

Then one iterate taking asuÆ iently large blo k of largeenough a k

's, followed by a suÆ iently large blo k of a

k

= 1. The real number whose ontinued fra tion development is given by x =[0;a

1 ;:::;a

n

;:::℄, veri es by onstru tion Bruno{s, with s>(2+Æ)=log2, being(s

k )

k

bounded by2 , butitdoesn'tverify ~ B s ,in fa t (s k ) k

os illatesfromvalueslargerthan tovaluessmallerthan ,withoutrea hing any limit.

Letusintrodu etwootherarithmeti al onditions. LetusdenotebyB 0 s

theset ofirrationalnumberswhose onvergentsverify:

(3.3) lim k !+1 logq k +1 q k logq k =s:

And ase ond onditionas follows, let( m ) m1 and (s m ) m1

betwopositive se-quen esofrealnumberssu hthat:

P +1 m = <+1and P +1 s m =<+1,

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thenwede ne onditionB ; by: (3.4) logq m+1 q m s m logq m + m 8m1:

Proposition 3.3. Let ! 2 (0;1)nQ and let s > 0 then we have the following in lusions:

1) let!2 ~ B s

,if ! isnotaBruno number then!2B 0 s ,otherwise !2B 0 0 . 2) Letsand!2B ; then!2 ~ B s ;

Proof. Toprovethe rststatementletuswritethefollowingidentity:

(3.5) k X l=0 logq l+1 q l slogq k =C+ k X l=2  logq l+1 q l s(logq l logq l 1 )  ; where C =(1 s)logq 1 + logq 2 q 1 . By ondition ~ B s

, this series onvergesand then itsgeneri termgoestozero,fromwhi hweget:

(3.6) lim k !+1 logq k +1 q k logq k =s  1 lim k !+1 logq k 1 logq k  : Letusdenotebys 0

bevalueoftherighthand sideof (3.6),then learlys 0

2[0;s℄. Letussupposes

0

>0,butthenwehaveforallsuÆ ientlylargek: C 1 q k  logq k logq k +1  C 2 q k ;

forsomepositive onstantsC 1

;C 2

,from whi hweget logq k logq k +1 !0,andfrom(3.6) we on ludethat s 0 =s. Ifs 0 =0,namely logq k logqk +1

!1,thenitiseasyto he kthat!isaBrunonumber. Letusprovethese ondstatement. Foranypositiveintegerk,usingthede nition ofB ; we an write: (3.7) k X l=0 logq l+1 q l slogq k  k X l=0 s l logq l + k X l=0 l slogq k ;

forall0lkwehavelogq l

logq k

thentherighthandsideof (3.7)isbounded by: logq k  s P k l=0 s l  + P k l=0 l . Byhypothesis P k l=0 s l

s, for allk, then using logq k  logq 1 weobtain: k X l=0 logq l+1 q l slogq k  logq 1 s k X l=0 s l ! + k X l=0 l ;

thenpassingto thelimitonkwehave:

lim k !+1 k X l=0 logq l+1 q l slogq k  logq 1 (s )+ <+1: 

Remark 3.4. These new arithmeti al onditionsareweaker thanthe Bruno one, forinstan e onditionB

0 s

isveri edbynumbers! whosedenominators(q k

) k

satisfy a growth ondition like q

k +1  (q k !) s . Condition B ;

implies onvergen e of the series: P k 0 logq k +1 qklogqk .

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Let us on lude re alling a stability result of Perez{Mar o [PM1, PM2℄ and ompareitwithourresult. In[PM2℄authorproved(TheoremV.2.1Annexe2xf) usingageometri renormalizations heme"alaYo oz"validintheonedimensional ase,astabilityresultthat anbestatedasfollows:

Theorem3.5 (Perez{Mar o,Contr^ole deladi usion). Let! 2(0;1)nQ andlet (q

k )

k

be the denominators of its onvergents. Let F be an analyti andunivalent fun tion de nedin the unit disk fz2

C

:jzj<1g su h thatF(z)=z+O(jzj 2

), where=e

2i!

. Thereexisttwopositive onstants C 1

;C 2

su hthat if:

(3.8) jzjC 1 e P k 1 j=0 logq j+1 q j ; thenfor all integer0mq

k wehave: (3.9) jF m (z)jC 2 e P k 1 j=0 logq j+1 q j :

The meaning of the Theorem is lear: if westart inside a disk of radius r =

C 1 e P k 1 j=0 logq j+1 q j

thenwe anapply F, up to q k

times, without leavingadisk of radius rC

2 =C

1

. To ompare thisresult with oure e tivestabilityresult we have tomakeexpli ittherelationbetweenr andq

k

,whi hgivethetimeof "stability". Using our Bruno{s ondition (3.2) we an say that C  rq

s k 1  C 0 for some positive onstantsC ;C 0

. But from (3.3)weget logq k C 3 q k 1 logq k 1 for some positive onstantC 3

,namelythereexist positive onstantsC 0 3 ;C 4 su hthat: q k exp n C 0 3 r 1=s log C 4 r 1=s o :

We anthenrestateTheorem3.5asfollows: ifjzjr,thenjF m (z)jrC 2 =C 1 for allinteger0m expf

C 0 3 r 1=s log C 4 r 1=s

g, obtainingabetterestimate onthetime of e e tivestability.

This improvement has been obtained thanks to a good understanding of the geometryofthedynami s,ifonewouldliketoobtainthesebetterestimatesalsofor germsinhigherdimensions,oneshouldextendthePerez{Mar oideastounderstand thegeometryofdynami sofgermsinhigherdimension. This ouldbeverydiÆ ult whereasourresultsareeasytoadapttoanydimension.

Weendwithalast remarkrelatedagaintotheworkofPerez{Mar o.

Remark 3.6. Perez{Mar o proved in [PM1, PM2℄ that any non{analyti ally lin-earizable analyti germ, univalent in the unit disk, whose multiplier at the xed point,veri es the following arithmeti al ondition:

(3.10) X k 0 loglogq k +1 q k <+1;

hasasequen eofperiodi orbitsa umulatingthe xedpoint,whoseperiods,(q nk

) k

, make the Brunoseriesdiverging.

OurBruno{s onditionimplies (3.10),infa t from (3.2)weget: N X k =0 loglogq k +1 q k  N X k =0  logC 3 q k + logq k q k + loglogq k q k  ;

we anletN grow andusingstandardnumbertheoryresults on erningthe onver-gents, we obtain the Perez{Mar o ondition. Then we an suppose these periodi

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orbits from atoo fast es ape", a situation similarto the one holding in the Neko-roshevTheoremfor Hamiltoniansystems[Ne℄,wherethe resonantweb on nesthe ow for exponentially long times. It would be very interesting to know whether a similar phenomenontakes pla einhigher dimension.

We on lude by pointing out that our method gives us a stability exponent de-pending on the Gevrey exponent and independent of the dimension: the bigger is the exponent, longer is the time interval of stability, we an always take s small enough tohaveavery longtimeofstability.

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(TimoteoCarletti)S uolaNormaleSuperiore,piazzadeiCavalieri7,56126Pisa,Italy, andAstronomieet

Syst

emesDynamiques,Institutde M

e anique C

eleste, 77Av. Den-fertRo hereau,75014Paris,Fran e

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