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R E S E A R C H

Open Access

Volume-preserving diffeomorphisms with

inverse shadowing

Manseob Lee

*

*Correspondence:

[email protected] Department of Mathematics, Mokwon University, Daejeon, 302-729, Korea

Abstract

Letfbe a volume-preserving diffeomorphism of a closedCn-dimensional Riemannian manifoldM. In this paper, we prove the equivalence between the following conditions:

(a) fbelongs to theC1-interior of the set of volume-preserving diffeomorphisms

which satisfy the inverse shadowing property with respect to the continuous methods,

(b) fbelongs to theC1-interior of the set of volume-preserving diffeomorphisms which satisfy the weak inverse shadowing property with respect to the continuous methods,

(c) fbelongs to theC1-interior of the set of volume-preserving diffeomorphisms

which satisfy the orbital inverse shadowing property with respect to the continuous methods,

(d) fis Anosov.

MSC: Primary 37C50; secondary 34D10

Keywords: shadowing; inverse shadowing; weak inverse shadowing; orbital inverse shadowing; Anosov; volume-preserving

1 Introduction

LetMbe a closedCn-dimensional Riemannian manifold, and letDiff(M) be the space of diffeomorphisms ofMendowed with theC-topology. Denote bydthe distance onM

induced from a Riemannian metric · on the tangent bundleTM. Letf :MMbe a diffeomorphism, and letMbe a closedf-invariant set.

Forδ> , a sequence of points{xi}bi=a(–∞ ≤a<b≤ ∞) inMis called aδ-pseudo orbit

off ifd(f(xi),xi+) <δfor allaib– . We say thatf has theshadowing propertyon

if for any> , there isδ>  such that for anyδ-pseudo orbit{xi}i∈Z⊂off, there

isyMsuch that d(fi(y),x

i) < fori∈Z. Note that in this definition, the shadowing

pointyMis not necessarily contained in. We say thatf belongs to theC-interior

shadowing propertyif there is aC-neighborhoodU(f) off such that for anygU(f),g has the shadowing property.

The shadowing property usually plays an important role in the investigation of stability theory and ergodic theory [].

Now, we introduce the notion of the inverse shadowing property which is a ‘dual’ notion of the shadowing property. The inverse shadowing property was introduced by Corless and Pilyugin in [], and the qualitative theory of dynamical systems with the property was

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developed by various authors (see [–]). In this paper, we introduce the various inverse shadowing properties.

LetMZbe the space of all two-sided sequencesξ={xn:n∈Z}with elementsxnM,

endowed with the product topology. For anyδ> , letf(δ) denote the set of allδ-pseudo

orbits off. A mappingϕ:Mf(δ)⊂MZis said to be aδ-methodforf ifϕ(x)=x,

and eachϕ(x) is aδ-pseudo orbit off throughx, whereϕ(x)denotes the th component

of ϕ(x). For convenience, writeϕ(x) for{ϕ(x)k}k∈Z. The set of allδ-methods forf will

be denoted byT(f,δ). We say thatϕis acontinuousδ-methodforf ifϕ is continuous.

The set of all continuousδ-methods forf will be denoted byTc(f,δ). Ifg:MMis

a homeomorphism with d(f,g) <δ, thenginduces a continuousδ-methodϕg forf by

defining

ϕg(x) =

gn(x) :n∈Z.

LetTh(f,δ) denote the set of all continuousδ-methodsϕg forf which are induced by a

homeomorphismg:MMwithd(f,g) <δ, wheredis the usualC-metric. LetTd(f,δ)

denote the set of all continuousδ-methodsϕgforf which are induced byg∈Diff(M) with

d(f,g) <δ. Then, clearly, we know that

Td(f)⊂Th(f)⊂Tc(f)⊂T(f),

(f) =

δ>(f,δ),α= ,c,h,d. We say thatf has theinverse shadowing propertywith

respect to the class(f),α= ,c,h,d, if for any> , there existsδ>  such that for any

δ-methodϕ(f,δ) and any pointxM, there is a pointyM, such that

dfk(x),ϕ(y)k

<, k∈Z.

We say that f has theweak inverse shadowing propertywith respect to the class(f),

α= ,c,h,d, if for any> , there existsδ>  such that for anyδ-methodϕ(f,δ) and

any pointxM, there is a pointyMsuch that

ϕ(y)B

Of(x)

,

whereB(A) ={xM:d(x,A)}. Note that iff ∈Diff(M) has the inverse shadowing

property with respect to the class (f) (α= ,c,h,d), then by the definition, it clearly

has the weak inverse shadowing property with respect to the class (f) (α= ,c,h,d).

We say thatf has theorbital inverse shadowing propertywith respect to the class(f),

α= ,c,h,d, if for any> , there is aδ>  such that for anyδ-methodϕ(f,δ) and

any pointxM, there is a pointyMsuch that

Of(x)⊂B

ϕ(y) and ϕ(y)B

Of(x)

.

Note that iff has the inverse shadowing property with respect to the class(f) (α=

,c,h,d), then it has the orbital inverse shadowing property with respect to the classTα(f)

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property with respect to the classTd(f). We say thatf belongs to theC-interior inverse

(weak inverse or orbital inverse) shadowing propertywith respect to the class(f),α=

,c,h,dif there is aC-neighborhoodU(f) offsuch that for anygU(f),ghas the inverse

(weak inverse or orbital inverse) shadowing property with respect to the class(f),α=

,c,h,d.

Lee [], showed that a diffeomorphism belongs to the C-interior inverse shadowing

property with respect to the classTd(f) if and only if it is structurally stable. And Pilyugin

[] proved that a diffeomorphism belongs to theC-interior inverse shadowing property with respect to the classTc(f) if and only if it is structurally stable. Thus, we can restate

the above facts as follows.

Theorem . Let f ∈Diff(M).A diffeomorphism f belongs to the C-interior inverse shad-owing property with respect to the classTd(f) (resp.Tc(f))if and only if it is structurally

stable.

In [] Choi, Lee and Zhang showed that a diffeomorphism belongs to theC-interior weak inverse shadowing property with respect to the classTd(f) if and only if it satisfies

both Axiom A and the no-cycle condition. Moreover, they proved that a diffeomorphism belongs to theC-interior orbital inverse shadowing property with respect to the class

Td(f) if and only if it satisfies both Axiom A and the strong transversal condition. From

the above facts, we get the following.

Theorem . Let f ∈Diff(M).If a diffeomorphism f belongs to the C-interior weak inverse

shadowing property with respect to the classTd(f),then f satisfies both AxiomAand the

no-cycle condition.Moreover,if f belongs to the C-interior orbital inverse shadowing property

with respect to the classTd(f),then it is structurally stable.

By the theorem, even though a diffeomorphism is contained in theC-interior of the set

of diffeomorphisms possessing the weak inverse shadowing property with respect to the classTd(f), it does not necessarily satisfy the strong transversality condition.

A periodic pointpoff ishyperbolicifDfπ(p)has eigenvalues with absolute values

dif-ferent from the one, whereπ(p) is the period ofp. Denote byF(M) the set off ∈Diff(M) such that there is aC-neighborhoodU(f) off such that for anygU(f), everypP(g) is hyperbolic, whereP(g) is the set of periodic points ofg. It is proved by Hayashi [] that fF(M) if and only iff satisfies both Axiom A and the no-cycle condition.

Letbe a closedf ∈Diff(M)-invariant set. We say thatishyperbolicif the tangent bundle TMhas a Df-invariant splittingEsEu and there exist constantsC>  and

 <λ<  such that

Dxfn|Es

x

n and D

xfn|Eu

x

n

for allxandn≥. If=M, then we say thatf is anAnosov diffeomorphism.

2 Statement of the results

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stable diffeomorphism is an Axiom A diffeomorphism. And in [], Palis extended this result to-stable diffeomorphisms.

LetMbe a compactCn-dimensional Riemannian manifold endowed with a volume formω. Letμdenote the measure associated withωthat we call the Lebesgue measure, and letddenote the metric induced by the Riemannian structure. Denote byDiffμ(M)

the set of diffeomorphisms which preserves the Lebesgue measureμendowed with the C-topology. In the volume-preserving case, the Axiom A condition is equivalent to the diffeomorphism being Anosov, since(f) =Mby the Poincaré recurrence theorem.

We define the set(M) as the set of diffeomorphismsf ∈Diffμ(M) which has aC

-neighborhoodU(f)⊂Diffμ(M) such that for anygU(f), every periodic point ofg is

hyperbolic. Note that(M)⊂F(M) (see [, Corollary .]).

Very recently, Arbieto and Catalan [] proved that if a volume-preserving diffeomor-phism is contained in(M), then it is Anosov. Indeed, at first they used the Mañé results

([, Proposition II.]). Then they showed thatP(f) is hyperbolic, whereP(f) is the set of periodic points off. And they proved that the nonwandering set(f) =P(f) by Pugh’s closing lemma. Finally, by the Poincaré recurrence theorem,(f) =M. From the above facts, we can restate the theorem as follows.

Theorem . Any diffeomorphism inFμ(M)is Anosov.

In [], Lee showed that if a volume-preserving diffeomorphism belongs to the C

-interior expansive orC-interior shadowing property, then it is Anosov. And [] proved that if a volume-preserving diffeomorphism belongs to theC-interior weak shadowing

property orC-interior weak limit shadowing property, then it is Anosov. From these

re-sults, we study the cases when a volume-preserving diffeomorphismf is inC-interior various inverse shadowing property with respect to the classTd(f), then it is Anosov. Let intISμ(M) denote the set of volume-preserving diffeomorphisms inDiffμ(M) satisfying

the inverse shadowing property with respect to the class Td, and letintWISμ(M)

(re-spect.,intOISμ(M)) denote the set of volume-preserving diffeomorphisms inDiffμ(M)

satisfying the weak inverse shadowing property with respect to the classTd(respect., the

orbital inverse shadowing property with respect to the classTd). From now, we only

con-sider the classTdwhen we mention the inverse shadowing property; that is, the ‘inverse

shadowing property’ implies the ‘inverse shadowing property with respect to the classTd’.

Now we are in a position to state the theorem of our paper.

Theorem . Let f ∈Diffμ(M).We have

intISμ(M) =intOISμ(M) =intWISμ(M) =ANμ(M),

whereANμ(M)is the set of Anosov volume-preserving diffeomorphisms inDiffμ(M).

3 Proof of Theorem 2.2

LetMbe a compactCn-dimensional Riemannian manifold endowed with a volume formω, and letf∈Diffμ(M). To prove the results, we will give the following well-known

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Lemma . Let f ∈Diffμ(M)andU be a C-neighborhood of f inDiff

μ(M).Then there

exist a C-neighborhoodU

⊂Uof f and> such that if gU,for any finite f -invariant

set E={x, . . . ,xm}, any neighborhood U of E and any volume-preserving linear maps

Lj:TxjMTg(xj)M withLjDxjg for all j= , . . . ,m,there is a conservative dif-feomorphism g∈U coinciding with f on E and out of U,and Dxjg=Ljfor all j= , . . . ,m.

Remark . From the Moser theorem (see []), there is a smooth conservative change of coordinatesϕx:U(x)TxMsuch thatϕx(x) =

, whereU(x) is a small neighborhood ofxM.

Proposition . If f ∈intISμ(M),then every periodic point of f is hyperbolic.

Proof Takef ∈intISμ(M) andU(f) is aC-neighborhood off ∈intISμ(M). Let> 

andV(f)⊂U(f) be a corresponding number and aC-neighborhood given by Lemma ..

Suppose that there exists a nonhyperbolic periodic pointpP(g) for somegV(f). To simplify the notation of the proof, we may assume thatg(p) =p. Then there is at least one eigenvalueλofDpg such that|λ|= . Denote byEcpthe eigenspace corresponding toλ.

Then we see that ifλ∈R, thendimEc

p= , and ifλ∈C, thendimEcp= .

First, we considerdimEpc= . For simplicity, we may assume thatλ=  (the other case is similar). By making use of Lemma ., we linearizeg atpwith respect to the Moser theorem; that is, by choosingα>  sufficiently small, we constructgC-nearbyg such

that

g(x) =

ϕp–◦Dpgϕp(x) ifx(p),

g(x) ifx∈/Bα(p).

Theng(p) =g(p) =p. Since the eigenvalueλofDpgis one,Dpg(v) =vfor anyvEcp(α).

Takev∈Ecp(α) such thatv=α/. Then we set

Iv={t·v: –≤t≤} ⊂ϕp

(p)

.

Take=α/. Let  <δ<be the number of the inverse shadowing property ofg. Then

by our construction ofg,ϕ–p (Iv)⊂(p). PutJp=ϕ

–

p (Iv). Then we see thatg(Jp) =Jp

and it is the identity map. For the aboveδ> , we can defineTd(g)-method as follows.

For anyxM, we setϕp(x) = (v, . . . ,vn) andDpg(v, . . . ,vn) = (v,A(v, . . . ,vn)). HereAis

corresponding to|λ| = . Then we define

h(x) =ϕ–p (v) +δ/,ϕp–

A(v, . . . ,vn)

=x+δ/,x

,

where ϕ–

p (A(v, . . . ,vn)) =x= (x, . . . ,xn). Clearly, d(g,h) <δ, andhTd(g). Letpbe

identified with = (, . . . , ). Then choosex= (x, , . . . , )∈Jp such that d(,x) = .

Then

dhi(),gi(x)=d(,x) = .

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We take a point y= (y, , . . . , )∈ Jp such that d(y,x) < and hi(y) = (ϕ–p (w) +

iδ/,ϕp–(Ai(w

, . . . ,wn))) = (y+iδ/,yi), whereϕp(y) = (w, . . . ,wn),y=ϕ–p (A(w, . . . ,wn))

andAcorresponding to|λ| = . Thend(gi(x),hi(y)) =d(x,y

+iδ/) and for somek∈Z,

d(x,y+kδ/) >α/ =.

This is a contradiction.

Therefore, we can choose a pointyM\Jpsuch thatd(x,y) <. Sinced(gi(x),hi(y)) =

d((x, , . . . , ), (y+iδ/,yi)), we can findk∈Zsuch that

d(x, , . . . , ),

y+kδ/,yk

>,

whereyk=ϕ–

p (Ak(w, . . . ,wn)). This is a contradiction sincef ∈intISμ(M).

Finally, ifλ∈C, thendimEc

p= . To avoid the notational complexity, we may assume

thatg(p) =p. As in the first case, by Lemma ., there areα>  andg∈V(f) such that

g(p) =g(p) =pand

g(x) =

ϕ–

pDpgϕp(x) ifx(p),

g(x) ifx∈/Bα(p).

With aC-small modification of the mapD

pg, we may suppose that there isl>  (the

minimum number) such thatDpgl(v) =vfor anyvϕp(Bα(p))⊂TpM. Takev∈ϕp(Bα(p))

such thatv=α/, and set

Lp=ϕ–p

{t·v: ≤t≤ +α/}

.

ThenLpis an arc such that

gi

(Lp)∩gj(Lp) =∅for≤i=jl– ,

gl(Lp) =Lp, and

gl

|Lpis the identity map.

Note thatghas the inverse shadowing property if and only ifgkhas the inverse shadowing

property for allk∈Z(see []). As in the first case, we can show thatgdoes not have the

inverse shadowing property, which contradicts the fact thatg∈U(f). Thus, every periodic

point off ∈intISμ(M) is hyperbolic.

Proposition . If f ∈intWISμ(M),then every periodic point of f is hyperbolic.

Proof Takef ∈intWISμ(M), andU(f) is aC-neighborhood off ∈intWISμ(M). Let

>  and V(f)⊂U(f) be a corresponding number and a C-neighborhood given by

Lemma .. Suppose that there exists a nonhyperbolic periodic pointpP(g) for some gV(f). To simplify the notation of the proof, we may assume that g(p) =p. Then, as in the proof of Proposition ., we can takeα>  sufficiently small and a smooth map ϕp:(p)→TpM. Then we can make an arcJp(p) and for someg∈V(f). Take

= (lengthJp)/. Let  <δ< be the number of the weak inverse shadowing property

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Letpbe identified with= (, . . . , ). Then choose a pointx= (x, , . . . , )∈Jpsuch that

d(,x) = . Sinceghas the weak inverse shadowing property,

Oh()⊂B

Og(x)

.

However, for anyyJp,

gi

(y) =y and hi(y) =

y+iδ/,yi

,

whereyi=ϕp–(Ai(w

, . . . ,wn)) is as in the proof of Proposition .. Thus, it is easily seen

that

Oh()⊂B

Og(x)

.

Ify= (y, , . . . , )∈Jp\ {p}, then

hk(y) =y+kδ/,yk

= (y+kδ/, ),

whereyk=ϕp–(Ak(w, . . . ,wn)). Thus, we know that

Oh(y)⊂B

Og(x)

.

This is a contradiction.

Finally, we can choose a pointyM\Jpsuch thatd(x,y) <. Then we know that

hk(y) =y+kδ/,yk

,

whereyk=ϕ–

p (Ak(w, . . . ,wn)). Therefore,

hl(y) /∈B(Jp),

for somel∈Z. Then

Oh(y)⊂B

Og(x)

=B(x).

Thus,gdoes not have the weak inverse shadowing property. This is a contradiction.

Ifλ∈C, then as in the proof of Proposition ., forg∈V(f), we can takel>  such

thatDpgl(v) =vfor anyvϕp(Bα(p))⊂TpM. As in the previous argument, we get a

con-tradiction. Thus, every periodic point off ∈intWISμ(M) is hyperbolic. Consequently, if

f ∈intWISμ(M), thenf(M).

Proposition . If f ∈intOISμ(M),then every periodic point of f is hyperbolic.

Proof The proof is almost the same as that of Proposition .. Indeed, letf ∈intOISμ(M)

andU(f) be aC-neighborhood off ∈intOISμ(M). Let>  andV(f)⊂U(f) be a

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a nonhyperbolic periodic point pP(g) for somegV(f). To simplify the notation of the proof, we may assume thatg(p) =p. Then, as in the proof of Proposition ., we can takeα>  sufficiently small and a smooth mapϕp:(p)→TpM. Then we can make an

arcJp(p) and for someg∈V(f). Take= (lengthJp)/. Let  <δ<be the

num-ber of the orbital inverse shadowing property for someg. Then we can construct a map

h∈Diff(M) as in the proof of Proposition .. Letpbe identified with= (, . . . , ). Then choose a pointx= (x, , . . . , )∈Jpsuch thatd(,x) = . Sinceghas the orbital inverse

shadowing property,

Oh()⊂B

Og(x)

and Og(x)⊂B

Oh()

.

However, for anyyJp,

gi(y) =y and hi(y) =y+iδ/,yi

,

whereyi=ϕp–(Ai(w

, . . . ,wn)) = (y, . . . ,yn) is as in the proof of Proposition .. Thus, it is

easily seen that

Oh()⊂B

Og(x)

.

This is a contradiction sincef ∈intOISμ(M).

Ify= (y, , . . . , )∈Jp\ {p}, then

hk(y) =y+kδ/,yk

= (y+kδ/, ),

whereyk=ϕ–

p (Ak(w, . . . ,wn)). Thus, we know that

Oh(y)⊂B

Og(x)

.

This is a contradiction.

Finally, we can choose a pointyM\Jpsuch thatd(x,y) <. Then we know that

hk(y) =y+kδ/,yk

,

whereyk=ϕ–

p (Ak(w, . . . ,wn)). Therefore,

hl(y) /∈B(Jp),

for somel∈Z. Then

Oh(y)⊂B

Og(x)

=B(x).

Thus,gdoes not have the orbital inverse shadowing property. This is a contradiction.

Ifλ∈C, then as in the proof of Proposition ., forg∈V(f), we can takel>  such that

Dpgl(v) =vfor anyvϕp(Bα(p))⊂TpM. As in the previous argument, in order to reach

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Competing interests

The author declares that they have no competing interests.

Acknowledgements

The author wishes to express their appreciation to the referee for their careful reading of the manuscript and valuable suggestions. This work is supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology, Korea (No. 2011-0007649).

Received: 21 May 2012 Accepted: 13 November 2012 Published: 28 November 2012

References

1. Pilyugin, S: Shadowing in Dynamical Systems. Lecture Notes in Math., vol. 1706. Springer, Berlin (1999) 2. Corless, R, Pilyugin, S: Approximate and real trajectories for generic dynamical systems. J. Math. Anal. Appl.189,

409-423 (1995)

3. Choi, T, Lee, K, Zhang, Y: Chracterisations of-stability and structural stability via inverse shadowing. Bull. Aust. Math. Soc.74, 185-196 (2006)

4. Diamond, P, Lee, K, Han, Y: Bishadowing and hyperbolicity. Int. J. Bifurc. Chaos Appl. Sci. Eng.12, 1779-1788 (2002) 5. Kloeden, P, Ombach, J, Porkrovskii, A: Continuous and inverse shadowing. Funct. Differ. Equ.6, 137-153 (1999) 6. Lee, K: Continuous inverse shadowing and hyperbolicity. Bull. Aust. Math. Soc.67, 15-26 (2003)

7. Pilyugin, S: Inverse shadowing by continuous methods. Discrete Contin. Dyn. Syst.8, 29-38 (2002) 8. Hayashi, S: Diffeomorphisms inF1(M) satisfy Axiom A. Ergod. Theory Dyn. Syst.12, 233-253 (1992)

9. Mañé, R: A proof of theC1-stability conjecture. Publ. Math. IHÉS66, 161-210 (1987)

10. Palis, J: On theC1-stability conjecture. Publ. Math. IHÉS66, 211-215 (1988)

11. Arbieto, A, Catalan, T: Hyperbolicity in the volume preserving scenario. Preprint 12. Lee, M: Volume preserving diffeomorphisms with expansive and shadowing. Preprint 13. Lee, M: Volume preserving diffeomorphisms with weak and weak limit shadowing. Preprint

14. Bonatti, C, Diáz, LJ, Pujals, ER: AC1-generic dichotomy for diffeomorphism: weak forms of hyperbolicity or infinitely

many sinks or sources. Ann. Math.116, 355-418 (2003)

15. Moser, J: On the volume elements on a manifold. Trans. Am. Math. Soc.120, 286-294 (1965) doi:10.1186/1029-242X-2012-275

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  The  aim  of  the  thesis  is  to  reconsider  the  pre-­production  and  production   process  of  narrative  cinema  and  involve  the  rich  and  varied  research  

Indeed, the international community-sponsored state-building agenda in Bosnia - which aims to strengthen state-level institutions to the detriment of the powers of the

Keywords: Continuing Professional Development (CPD); teacher education; Norway; Germany; England; longitudinal study; European Union; in-service teacher development;

The focus o f large-scale e-business developm ent has shifted to the large ‘b lu e-chip’ corporations. H ow ever, large com panies not only have to tackle a new