• Aucun résultat trouvé

Invariant measures for piecewise continuous maps C.R. Acad. Sci. Paris, Ser.I

N/A
N/A
Protected

Academic year: 2023

Partager "Invariant measures for piecewise continuous maps C.R. Acad. Sci. Paris, Ser.I"

Copied!
6
0
0

Texte intégral

(1)

Contents lists available atScienceDirect

C. R. Acad. Sci. Paris, Ser. I

www.sciencedirect.com

Dynamical systems

Invariant measures for piecewise continuous maps

Mesures invariantes pour les applications continues par morceaux

Benito Pires

1

DepartamentodeComputaçãoeMatemática,FaculdadedeFilosofia,CiênciaseLetras,UniversidadedeSãoPaulo, 14040-901, Ribeirão Preto – SP,Brazil

a r t i c l e i n f o a b s t r a c t

Articlehistory:

Received15March2016 Acceptedafterrevision3May2016 Availableonline24May2016 PresentedbyClaireVoisin

We say that f : [0,1]→ [0,1] is a piecewisecontinuous intervalmap if there exists a partition 0=x0<x1<· · ·<xd<xd+1=1 of [0,1] such that f|(xi1,xi) is continuous and thelaterallimits w+0 =limx0+f(x),wd+1=limx1f(x),wi =limxxi f(x) and w+i =limxx+i f(x) exist for eachi.We provethat every piecewisecontinuous interval map withoutconnectionsadmitsan invariant Borelprobability measure. Wealso prove thateveryinjectivepiecewisecontinuousintervalmapwithnoconnectionsandnoperi- odicorbitsistopologicallysemiconjugatetoanintervalexchangetransformation.

©2016Académiedessciences.PublishedbyElsevierMassonSAS.Allrightsreserved.

r é s um é

Onditque f: [0,1]→ [0,1]estuneapplicationd’intervallecontinueparmorceauxs’ilexiste une partition0=x0<x1<· · ·<xd<xd+1=1 de [0,1] telleque f|(xi1,xi) est conti- nue et telle que les limites latérales w+0 =limx0+f(x), wd+1=limx1f(x), wi = limxx

i f(x)etw+i =limxx+i f(x)existentpourchaquei.Onprouvequetouteapplica- tiond’intervallecontinueparmorceauxsansconnexionadmetunemesuredeprobabilité invariante. Onprouveégalementque touteapplicationinjectived’intervallecontinuepar morceauxsansconnexionetsansorbitepériodiqueesttopologiquementsemiconjuguéeà unéchanged’intervalles.

©2016Académiedessciences.PublishedbyElsevierMassonSAS.Allrightsreserved.

1. Introduction

Muchinformationaboutthelong-termbehaviouroftheiteratesofamapisrevealedbyitsinvariantmeasures.Regard- ing piecewisecontinuous intervalmaps,thepresence ofa non-atomicinvariantBorelprobability measurecan beusedto constructtopologicalconjugaciesorsemiconjugacieswithintervalexchangetransformations(IETs).

E-mailaddress:[email protected].

1 PartiallysupportedbySãoPauloResearchFoundation(FAPESP)grant#2015/20731-5.

http://dx.doi.org/10.1016/j.crma.2016.05.002

1631-073X/©2016Académiedessciences.PublishedbyElsevierMassonSAS.Allrightsreserved.

(2)

Transfer operatorshaveproved tobe animportanttool toobtain absolutelycontinuous invariant probabilitymeasures forpiecewisesmoothpiecewisemonotoneintervalmaps(see[1,3–5,9]).Ingeneral,thesetypesofresultsassumethateach branchofthepiecewisecontinuousmapisCr-smooth(r

1),monotoneandhasderivativegreaterthan1.

TheaimofthisarticleistoprovetheexistenceofinvariantBorelprobabilitymeasuresforpiecewisecontinuousinterval maps not embraced bythe transferoperator approach.In thisway,our resultincludesgap maps,piecewise contractions and generalisedinterval exchange transformations(GIETs). No monotonicityandno smoothnessassumptions,beyond the uniform continuityofeach branchofthemap, areassumed. Ourresultisthe naturalversion oftheKryloff–Bogoliouboff Theorem(see[8])forpiecewisecontinuousintervalmaps.

We arealsointerested inconstructingtopologicalsemiconjugacybetweeninjectivepiecewisecontinuous intervalmaps and interval exchange transformations, possibly with flips. In thisregard, it is worth mentioning the result by J. Milnor and W. Thurston(see[12]), whichstatesthat anycontinuous piecewise monotone interval map ofpositive entropyhtop is topologicallysemiconjugate toamap withconstantslope equalto

±

ehtop.Thisresultwasgeneralisedby L. Alsedàand M. Misiurewicz in[2]to piecewise continuous piecewise monotone interval mapsofpositive entropy. Concerningcount- ably piecewise continuous piecewise monotone interval maps,a necessaryandsufficient condition fortheexistence of a non-decreasingsemiconjugacytoamapofconstantslopewasprovidedbyM. MisiurewiczandS. Rothin[13].Theauthor andA. Nogueiraprovedin[14]thateveryinjectivepiecewisecontractionistopologicallyconjugatetoamapwithconstant slopeequalto

±

12.

The proof ofthe Kryloff–Bogoliouboff Theorem failsfor discontinuous maps.In thisarticle, we presenta variation of thisproofthatovercomessuchlimitation.Thehypothesisofnoconnectionscannotberemovedsincethereareexamplesof piecewisecontinuousmapsthathaveconnectionsandadmitnoBorelinvariantmeasure.Theproofpresentedheredoesnot holdforcountablypiecewisecontinuousmapssinceforsuchmapsthelaterallimitsmightnotexistatallpointsof

[

0

,

1

]

.

2. Statementoftheresults

Throughoutthisarticle,assumethat f

: [

0

,

1

] → [

0

,

1

]

isapiecewisecontinuousintervalmap.Hence,thereexistsapar- tition0

=

x0

<

x1

< · · · <

xd

<

xd+1

=

1 of

[

0

,

1

]

suchthat f

|

(xi−1,xi)iscontinuousandthelaterallimitsw+0

=

limx0+ f

(

x

)

, wd+1

=

limx1 f

(

x

)

,wi

=

limxx

i f

(

x

)

andw+i

=

limxx+

i f

(

x

)

existforeach i.Let D

= {

x0

, . . . ,

xd+1

},

W

= {

w+0

,

w1

,

w+1

, . . . ,

wd

,

wd+

,

wd+1

}.

Wesaythat f hasnoconnectionsif

wW

k=0

{

fk

(

w

)} ∩

D

= ∅.

(1)

Wesaythatx

∈ [

0

,

1

]

isaperiodicpointof f ifthereexistsanintegerk

1 suchthat fk

(

x

) =

x.

OurfirstresultturnsouttobeaversionoftheKryloff–BogoliouboffTheorem[8]forpiecewisecontinuousintervalmaps.

Theorem2.1.Letf

: [

0

,

1

] → [

0

,

1

]

beapiecewisecontinuousmapwithnoconnections,thenf admitsaninvariantBorelprobability measure

μ

.Moreover,if f hasnoperiodicpoints,thenthemeasure

μ

isnon-atomic.

The hypothesis ofnoconnections inthestatement ofTheorem 2.1,althoughmore readilycheckable,maysounda bit restrictivebecause,forinstance,itprohibitsthataleft-continuousmap f takesonediscontinuityintoanother.Indeed,what needs tobeavoidedfortheexistenceoftheinvariantmeasureisthepresenceofclosedconnections,amoretechnicalnotion giveninSection3.

Intheworldofgeneralisedintervalexchangetransformations,thehypothesisofnoconnectionscorrespondstothenotion ofhavingan

-completepath.Asremarkedin[11,p. 1586],everyGIETwithsuchpropertyistopologicallysemiconjugate toanIET.Thenextresultextendsthisclaimtopiecewisecontinuousmaps.Itcanalsobeconsideredageneralisationofthe item (a)oftheStructureTheorembyGutierrez[6,p. 18].

Corollary2.2.Let f

: [

0

,

1

] → [

0

,

1

]

beaninjectivepiecewisecontinuousmapwithnoconnectionsandnoperiodicpoints,thenf is topologicallysemiconjugatetoanintervalexchangetransformation,possiblywithflips.

Now we presenta class of piecewise continuous interval mapsfor whichhaving no connections is a generic (in the measure-theoreticalsense)property.Werecallthatanirrationalitycriterion fortheabsenceofconnectionsinIETswithout flipswasprovidedbyM. Keanein[7].

Theorem2.3.Let

φ

1

, . . . , φ

d+1

: [

0

,

1

] → (

0

,

1

)

becontinuousmapsandlet

Rdbetheopenset

= { (

x1

, . . . ,

xd

)

Rd

|

0

<

x1

< · · · <

xd

<

1

}

,thenforLebesguealmostevery

(

x1

, . . . ,

xd

)

,thepiecewisecontinuousmap f

: [

0

,

1

] → (

0

,

1

)

definedby f

(

x

) = φ

i

(

x

)

ifx

Ii,whereI1

= [

0

,

x1

),

I2

= [

x1

,

x2

), . . . ,

Id

= [

xd1

,

xd

)

,Id+1

= [

xd

,

1

]

,hasnoconnectionsandhenceadmitsan invariantBorelprobabilitymeasure.

(3)

3. ProofofTheorem2.1

Henceforth,assumethatthemap f hasnoconnectionsandnoperiodicorbits.

Lemma3.1.Givenx

∈ [

0

,

1

]

andanintegerr

1,thereexistsanopensubinterval Jxof

[

0

,

1

]

containingx suchthat

{

f

(

y

), . . . ,

fr

(

y

) } ∩

Jx

= ∅

for every y

Jx

.

(2)

Proof. Firstletusprovetheresultforx

=

xi,where1

i

d.Let

γ =

r k=1

{

fk1

(

wi

),

fk

(

xi

),

fk1

(

w+i

)}.

Bythe uniformcontinuity of f

|

(xj−1,xj), 1

j

d

+

1,together with thehypothesis of noconnections, we have that for every

>

0,thereexist0

< δ <

andaninterval Jxi

= (

xi

δ,

xi

+ δ) ⊂ [

0

,

1

]

suchthat

d

fk

(

y

), γ <

for every y

Jxi and 1

k

r

,

(3)

whered

fk

(

y

), γ

=

minzγ

|

fk

(

y

)

z

|

.

Let

=

12d

(

xi

, γ )

,then

>

0,otherwise f wouldhaveaconnection ora periodicorbit. Thistogetherwith(3)implies that

|

fk

(

y

)

xi

| > > δ

forall y

Jxi and1

k

r.Hence,(2)holdsforeveryx

=

xi

D.

The casesin which x

=

x0

=

0 or x

=

xd+1

=

1 followslikewise,by considering intervals ofthe form Jx0

= [

0

, δ)

and Jxd+1

= (

1

δ,

1

]

,respectively.

Itremainstoconsiderthecaseinwhichx

∈ { /

x0

, . . . ,

xd+1

}

.Duetothehypothesisofnoconnections,thereareonlytwo possibilities:either

{

fk

(

x

) :

k

0

} ∩ {

x0

, . . . ,

xd+1

} = ∅

orthereexistk

1 (taketheleastvalue)and0

i

d

+

1 suchthat fk

(

x

) =

xi.As forthefirst possibility,take

γ = {

f

(

x

), . . . ,

fr

(

x

) }

,then f iscontinuous on

{

x

} ∪ γ

.Moreover, since f has noperiodicpoints,wehavethat x

/ γ

.Therefore,forevery

>

0,thereexist0

< δ <

andaninterval Jx

= (

x

δ,

x

+ δ)

suchthat (3)holdsfor Jx intheplaceof Jxi.Toconcludetheproof, proceedasbefore.Concerningthesecondpossibility, let Jxi

= (

xi

δ,

xi

+ δ)

beasinthebeginningoftheproof,then,asalreadyproved,

{

f

(

y

), . . . ,

fr

(

y

)} ∩

Jxi

= ∅

for every y

Jxi

.

(4)

Moreover, since k is the least value, f is locally continuous around

{

x

,

f

(

x

), . . . ,

fk1

(

x

)}

, thus there exists an interval Jx

= (

x

η ,

x

+ η )

suchthat Jx

,

f

(

Jx

), . . . ,

fk

(

Jx

)

arepairwisedisjointintervalsand fk

(

Jx

)

Jxi.Now(4)impliesthat(2) holdsforevery y

Jx,whichconcludestheproof. 2

Letq

∈ [

0

,

1

]

begiven.Since f hasnoperiodicorbits,thereexists

0 suchthat

fk

(

q

) :

k

D

= ∅

.Hereafter,set p

=

f

(

q

)

,then

{

p

,

f

(

p

),

f2

(

p

), . . .} ∩

D

= ∅.

(5)

Denoteby

( μ

n

)

n=1thesequenceofBorelprobabilitymeasureson

[

0

,

1

]

definedby

μ

n

=

1 n

n1 k=0

δ

fk(p)

,

where

δ

fk(p)istheDiracprobabilitymeasureon

[

0

,

1

]

concentratedat fk

(

p

)

.

Bythe Banach–AlaogluTheorem, thespaceof Borelprobability measureson a compactmetric spaceiscompact with respect tothe weak topology. Hence,there exist aBorelprobability measure on

[

0

,

1

]

,denoted henceforthby

μ

,anda subsequenceof

{ μ

n

}

,denotedhenceforthby

{ μ

nj

}

j=1,thatconvergesto

μ

intheweak topology.

Thenextresultisgoingtobeusedtwice,inLemma 3.3aswellasinLemma 3.5.

Lemma3.2.Letx

∈ [

0

,

1

]

.Given

>

0,thereexistanopensubinterval Jxof

[

0

,

1

]

containingx,andanintegerj0

1suchthat

μ

nj

(

Jx

) <

for every j

j0

.

(6)

Proof. Letr

1 beanintegersogreatthat 2

r

<

.Since

{

nj

}

j=1 isasubsequenceof

{

1

,

2

, . . .}

,thereexists j0

1 suchthat nj

>

rforevery j

j0.Let JxbeasinthestatementofLemma 3.1.Let j

j0 and

=

#

{

0

k

nj

1

|

fk

(

p

)

Jx

}

,where

# denotescardinality.By(2),wehavethat

(

1

)

r

nj,thus

μ

nj

(

Jx

) =

1 nj

nj1 k=0

δ

fk(p)

(

Jx

) =

#

{

0

k

nj

1

|

fk

(

p

)

Jx

}

nj

2

r

<

for every j

j0

. 2

(4)

Lemma3.3.Themeasure

μ

isnon-atomic.

Proof. Let x

(

0

,

1

)

. Given

>

0,let Jx be an opensubintervalof

[

0

,

1

]

containing x asinthestatement ofLemma 3.2.

Since the set S

= {

z

∈ [

0

,

1

] : μ ({

z

}) >

0

}

is atmost countable, thereexists a subinterval Jx

Jx containing xsuch that

μ

Jx

=

0,where

Jxdenotestheendpointsoftheinterval Jx.By[15,Theorem6.1,p.40]andby(6),

μ ( {

x

} )μ (

Jx

) =

lim

j→∞

μ

nj

(

Jx

)

lim sup

j→∞

μ

nj

(

Jx

) .

Thefactthat isarbitraryyields

μ ( {

x

} ) =

0.

Now let A1

A2

⊂ · · ·

be asequence ofsubsetsof

[

0

,

1

]

suchthat

k1Ak

= (

0

,

1

)

and

Ak

S

= ∅

foreveryk

1.

By(5),wehavethat

μ

nj

(

Ak

) =

1 forevery j

,

k

1.By[15,Theorem6.1,p.40]oncemore,wehavethat

μ (

Ak

) =

lim

j→∞

μ

nj

(

Ak

) =

1 for every k

1

.

Inthisway,

μ ((

0

,

1

)) =

lim

k→∞

μ (

Ak

) =

1

,

thus

μ ({

0

}) = μ ({

1

}) =

0

. 2

The convergenceof

{ μ

nj

}

j=1 to

μ

intheweak topology impliesthat limj→∞

φ

d

μ

nj

=

φ

d

μ

foreverycontinuous function

φ : [

0

,

1

] →

R.Thenextlemmaextendsthisclaimforthepiecewisecontinuousmap

φ = ϕ

f.

Remark3.4.AspointedoutbyC.Liveraniin[10,p. 4],thepointwheretheproofoftheKryloff–BogoliouboffTheoremfails isLemma 3.5,whichisautomaticforcontinuousfunctions.

Lemma3.5.Foreverycontinuousfunction

ϕ : [

0

,

1

] →

R,

jlim→∞

ϕ

fd

μ

nj

=

ϕ

fd

μ .

Proof. Let

>

0 be arbitrarilysmall.ByLemma 3.3,we havethat

μ ({

xi

}) =

0 forevery 1

i

d.Hence,there existsan open interval Jxi containing xi such that

μ (

Jxi

) <

forevery 1

i

d.By Lemma 3.2,there existan open interval Jxi

containing xi,andaninteger j0

1 suchthat

μ

nj

Jx

i

<

for every j

j0 and 1

i

d

.

Set Jxi

=

Jxi

Jxi.Thefunction

ϕ ◦

f isboundedbysome constantM andcontinuousoneachinterval

(

xi1

,

xi

)

forevery 1

i

d

+

1. In this way, there exists a continuous function h

: [

0

,

1

] → [−

M

,

M

]

such that h

(

x

) = ϕ

f

(

x

)

forevery x

∈ [

0

,

1

] \

d

i=1 Jxi.Puttingitalltogetheryields

ϕ

fd

μ

nj

hd

μ

nj

| ϕ

f

h

|

d

μ

nj

2Md

for every j

j0

,

(7)

and

ϕ

fd

μ

hd

μ

2Md

.

(8)

Finally,sincehiscontinuouson

[

0

,

1

]

and

μ

nj convergesto

μ

intheweak*topology,thereexists j1

j0suchthat

hd

μ

nj

hd

μ

for every j

j1

.

(9)

Itfollowsfromtheequations(7),(8)and(9)that

ϕ

fd

μ

nj

ϕ

fd

μ (

4Md

+

1

)

for every j

j1

,

whichconcludestheproof. 2

Lemma3.6([16,Theorem6.2,p.147]).Letm1andm2betwoBorelprobabilitymeasureson

[

0

,

1

]

.If

ϕ

dm1

=

ϕ

dm2forevery continuousfunction

ϕ : [

0

,

1

] →

R,thenm1

=

m2.

(5)

Givena Borelprobabilitymeasure m on

[

0

,

1

]

andaninteger k

1,letm

fk denotethe Borelmeasuredefinedby

(

m

fk

)(

B

) =

m

fk

(

B

)

foranyBorelsetB.Inparticular,form

= δ

p wehavethat

δ

p

fk

= δ

fk(p).

Lemma3.7([16,Lemma6.6,p.150]).Let

ψ : [

0

,

1

] →

RbeaBorel-measurablefunction,k

1aninteger,andm aBorelprobability measureon

[

0

,

1

]

,then

ψ

fkdm

=

ψ

d

(

m

fk

).

Lemma3.8.Themeasure

μ

isinvariantbyf .

Proof. ByLemma 3.6andLemma 3.7(taking

ψ = ϕ

,k

=

1 andm

= μ

),itsufficestoshowthat

ϕ

fd

μ =

ϕ

d

μ

(10)

foreverycontinuousfunction

ϕ : [

0

,

1

] →

R.ByLemma 3.5,foreverycontinuous function

ϕ : [

0

,

1

] →

R,

ϕ

fd

μ

ϕ

d

μ =

lim

j→∞

ϕ

fd

μ

nj

ϕ

d

μ

nj

.

(11)

ByLemma 3.7oncemore(nowtaking

ψ = ϕ

f andm

= δ

p),wereach

ϕ

fd

μ

nj

=

1 nj

nj1 k=0

ϕ

fd

p

fk

) =

1 nj

nj1 k=0

ϕ

fk+1d

δ

p

.

(12)

Likewise,

ϕ

d

μ

nj

=

1 nj

nj1 k=0

ϕ

d

p

fk

) =

1 nj

nj1 k=0

ϕ

fkd

δ

p

.

(13)

Itfollowsfrom(11),(12)and(13)that

ϕ

fd

μ

ϕ

d

μ =

lim

j→∞

n1j

nj1

k=0

ϕ

fk+1

ϕ

fk

d

δ

p

=

lim

j→∞

n1j

ϕ

fnj

ϕ

d

δ

p

lim

j→∞

2

f

nj

=

0

.

Hence,(10)holds,whichconcludestheproof. 2

Remark3.9.TheproofofTheorem 2.1followsfromLemmas 3.3 and3.8.

4. Proofoftheotherresults

Corollary2.2.Letf

: [

0

,

1

] → [

0

,

1

]

beaninjectivepiecewisecontinuousmapwithnoconnectionsandnoperiodicorbits,then f is topologicallysemiconjugatetoanintervalexchangetransformation,possiblywithflips.

Proof. ByTheorem 2.1, f admitsanon-atomicBorelprobabilitymeasure

μ

invariantby f.Leth

: [

0

,

1

] → [

0

,

1

]

bedefined byh

(

x

) = μ ( [

0

,

x

] )

,thenhisacontinuousnon-decreasingsurjectivemap.Let1

i

d

+

1 andx

,

y

(

xi1

,

xi

)

besuchthat h

(

x

) =

h

(

y

)

.Weclaimthath

(

f

(

x

)) =

h

(

f

(

y

))

.Assumethat x

y and f

(

x

)

f

(

y

)

,then,theinjectivity of f togetherwith thecontinuityof f

|

(xi−1,xi)yields

[

x

,

y

] =

f1

([

f

(

x

),

f

(

y

)])

.Hence,since

μ

isnon-atomic,

|

h

(

f

(

y

))

h

(

f

(

x

)) | = μ ([

f

(

x

),

f

(

y

) ]) = μ

f1

([

f

(

x

),

f

(

y

) ])

= μ ([

x

,

y

]) = |

h

(

y

)

h

(

x

) | .

(14) Asfortheothercases,toproceed likewisetoshowthat(14)stillholds.Hence,theclaimistrue.

LetT

: [

0

,

1

] → [

0

,

1

]

bedefinedby T

(

h

(

x

)) =

h

(

f

(

x

))

.Bytheclaim, T iswell defined. Lett0

,

t1

, . . . ,

td+1 bedefinedby t0

=

0,td+1

=

1 andti

=

h

(

xi

)

forevery1

i

d.By(14),wehavethatforeveryt

,

s

(

ti1

,

ti

)

,thereexistx

,

y

(

xi1

,

xi

)

suchthatt

=

h

(

x

)

,s

=

h

(

y

)

and

(6)

|

T

(

t

)

T

(

s

) | = |

h

(

f

(

x

))

h

(

f

(

y

)) | = |

h

(

x

)

h

(

y

) | = |

t

s

|

for every t

,

s

(

ti1

,

ti

).

Thisprovesthat T

|

(ti1,ti)isanisometry;therefore,T isanintervalexchangetransformation,possiblywithflips.Bydefini- tion, T

h

=

h

f,thus f istopologicallysemiconjugatetoT. 2

Theorem2.3.Let

φ

1

, . . . , φ

d+1

: [

0

,

1

] → (

0

,

1

)

becontinuousmapsandlet

Rdbetheopenset

= { (

x1

, . . . ,

xd

)

Rd

|

0

<

x1

< · · · <

xd

<

1

}

,thenforLebesguealmostevery

(

x1

, . . . ,

xd

)

,thepiecewisecontinuousmap f

: [

0

,

1

] → (

0

,

1

)

definedby f

(

x

) = φ

i

(

x

)

ifx

Ii,whereI1

= [

0

,

x1

),

I2

= [

x1

,

x2

), . . . ,

Id

= [

xd1

,

xd

)

,Id+1

= [

xd

,

1

]

,hasnoconnectionsandhenceadmitsan invariantBorelprobabilitymeasure.

Proof. Denoteby Idtheidentitymapon

[

0

,

1

]

.SetC0

= {

Id

}

.Let Ck

= {φ

i

h

|

1

i

d

+

1

,

h

Ck1

},

k

1

.

Foreach 0

i

d

+

1,1

j

d,wi

∈ {

wi

,

w+i

}

andh

k0Ck,theset

{ (

x1

, . . . ,

xd

) |

xj

=

h

(

wi

) }

isthegraphofa continuous function definedon

[

0

,

1

]

,thusit isaLebesguenullset.Thistogether withthefactthat x0

=

0 andxd+1

=

1 donotbelongtotherangeofanyh

k1Ckimplies thatthesetofparameters

(

x1

, . . . ,

xd

)

forwhichthemap f has connections isaLebesguenullset,denotedby N.Let

(

x1

, . . . ,

xd

) \

N,theneither f hasaperiodicpointor f hasno periodicpointsandnoconnections.Inthefirstcase, f hasan invariantBorelprobabilitymeasuresupportedonitsperiodic orbits, whileinthesecondcase,byTheorem 2.1, f admitsaninvariantnon-atomicBorelprobabilitymeasure. 2

3. Finalremarks

The claimofTheorem 2.1 keepstrueifin itsstatement theterm“noconnections” isreplaced bythe term“no closed connections” definedbelow. Let f

: [

0

,

1

] → [

0

,

1

]

be asin(1) andlet

¯

f

:

P

( [

0

,

1

] )

P

( [

0

,

1

] )

bethe map definedon eachset A

⊂ [

0

,

1

]

by

¯

f

(

A

) =

xA

lim

0+f

(

x

),

lim

0+f

(

x

+ )

,

wherelim0+ f

( ) :=

f

(

0

)

andlim0+ f

(

1

+ ) :=

f

(

1

)

.Wesaythat themap f hasaclosedconnectionifthereexist 0

i

d

+

1 andk

1 suchthat xi

k1

¯

fk

({

xi

})

.

Theexistenceofconnectionsneitherimpliesnorisimpliedbytheexistenceofperiodicpoints.Infact,let f1

,

f2

: [

0

,

1

] → [

0

,

1

]

bethepiecewisecontinuousmapsdefinedby

f1

(

x

) =

⎧ ⎪

⎪ ⎨

⎪ ⎪

x 2

+

1

8 if 0

x

<

1 2 x

2

+

3 8 if 1

2

x

1

,

f2

(

x

) =

⎧ ⎪

⎪ ⎨

⎪ ⎪

x 2

+

1

4 if 0

x

<

1 2 x

2 if 1

2

x

1

.

The map f1 hastwo periodicpoints andnoconnections. Themap f2 hasaclosedconnection butnoperiodicpoints.

Moreover,itdoesnotadmitanyinvariantBorelprobabilitymeasure.

Acknowledgements

IamverygratefultoKleyberCunhaandCarlangeloLiveraniforthepromptreplytomyquestions.Iamequallythankful fortheprecisecommentsprovidedbytheanonymousreferee.

References

[1]R.Adler,L.Flatto,Geodesicflows,intervalmaps,andsymbolicdynamics,Bull.Amer.Math.Soc.25(1991)229–334.

[2]L.Alsedà,M.Misiurewicz,Semiconjugacytoamapofconstantslope,DiscreteContin.Dyn.Syst.,Ser.B20(2015)3403–3413.

[3]V.Baladi,PositiveTransferOperatorsandDecayofCorrelations,AdvancedSeriesinNonlinearDynamics,WorldScientificPublishingCompany,2000.

[4]R.Bowen,InvariantmeasuresforMarkovmapsoftheinterval,Commun.Math.Phys.69(1979)1–17.

[5]A.Boyarsky,P.Góra,LawsofChaos:InvariantMeasuresandDynamicalSystemsinOneDimension,Birkhäuser,1997.

[6]C.Gutierrez,Smoothingcontinuousflowsontwo-manifoldsandrecurrences,Ergod.TheoryDyn.Syst.6 (1)(1986)17–44.

[7]M.Keane,Intervalexchangetransformations,Math.Z.141 (1)(1975)25–31.

[8]N.Kryloff,N.Bogoliouboff,Lathéoriegénéraledelamesuredanssonapplicationàl’étudedessystèmesdynamiquesdelamécaniquenonlinéaire, Ann.ofMath.(2)38 (1)(1937)65–113.

[9]A.Lasota,J.A.Yorke,Ontheexistenceofinvariantmeasuresforpiecewisemonotonictransformations,Trans.Amer.Math.Soc.186(1973)481–488.

[10]C.Liverani,Invariantmeasuresandtheirproperties.A functionalanalyticpointofview,in:DynamicalSystems.PartII,Pubbl.Cent.Ric.Mat.Ennio Giorgi,ScuolaNorm.Sup.,Pisa,2003,pp. 185–237.

[11]S.Marmi,P.Moussa,J-C.Yoccoz,Linearizationofgeneralizedintervalexchangemaps,Ann.ofMath.(2)176(2012)1583–1646.

[12]J.Milnor,W.Thurston,Oniteratedmapsoftheinterval,in:LectureNotesinMathematics,vol. 1342,Springer,Berlin,1988,pp. 465–563.

[13]M.Misiurewicz,S.Roth,Nosemiconjugacytoamapofconstantslope,Ergod.TheoryDyn.Syst.36(2016)875–889.

[14]A.Nogueira,B.Pires,Dynamicsofpiecewisecontractionsoftheinterval,Ergod.TheoryDyn.Syst.35(2015)2198–2215.

[15]K.Parthasarathy,ProbabilityMeasuresonMetricSpaces,AmericanMathematicalSociety,2005.

[16]P.Walters,AnIntroductiontoErgodicTheory,GraduateTextsinMathematics,vol. 79,Springer-Verlag,2000.

Références

Documents relatifs

Let E f denote the set of ergodic, f -invariant Borel probability mea- sures, Per f the set of invariant measures supported on a single periodic orbit, and O f denote the set

In [Sar02, Gou04a], this theorem is applied by taking R n to be the “first return transfer operators” to Y = (1/2, 1], acting on the space of Lipschitz continuous functions on Y...

We define also the arrival partition of f associated with P, denoted f (P), the partition of [0, 1[ composed of all right-open and left-closed intervals such that their interior

Regardless, to first order the electron wavefunction (whose transverse coherence is many atoms in width) will exhibit a deBroglie phase-shift (relative to nearby columns) which is

- We consider piecewise affine expanding non-renormalizable interval maps, and prove the stability in L1-norm of densities of their invariant measures.. This based on

(To verify condition (II) and (III) we possibly have to divide [0, ε] into smaller intervals.) Knowing that conditions (II) and (III) hold for a one-parameter family, we can

Our main result, Theorem 2.5, is an upper bound on the essential spectral radius of weighted transfer operators associated to cone hyperbolic systems satisfying the bunching

[r]