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 closedC∞n-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 closedC∞n-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 :M→Mbe a diffeomorphism, and let⊂Mbe 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 alla≤i≤b– . We say thatf has theshadowing propertyon
if for any> , there isδ> such that for anyδ-pseudo orbit{xi}i∈Z⊂off, there
isy∈Msuch that d(fi(y),x
i) < fori∈Z. Note that in this definition, the shadowing
pointy∈Mis not necessarily contained in. We say thatf belongs to theC-interior
shadowing propertyif there is aC-neighborhoodU(f) off such that for anyg∈U(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
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 elementsxn∈M,
endowed with the product topology. For anyδ> , letf(δ) denote the set of allδ-pseudo
orbits off. A mappingϕ:M→f(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:M→Mis
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:M→Mwithd(f,g) <δ, wheredis 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),
Tα(f) =
δ>Tα(f,δ),α= ,c,h,d. We say thatf has theinverse shadowing propertywith
respect to the classTα(f),α= ,c,h,d, if for any> , there existsδ> such that for any
δ-methodϕ∈Tα(f,δ) and any pointx∈M, there is a pointy∈M, such that
dfk(x),ϕ(y)k
<, k∈Z.
We say that f has theweak inverse shadowing propertywith respect to the classTα(f),
α= ,c,h,d, if for any> , there existsδ> such that for anyδ-methodϕ∈Tα(f,δ) and
any pointx∈M, there is a pointy∈Msuch that
ϕ(y)⊂B
Of(x)
,
whereB(A) ={x∈M:d(x,A)≤}. Note that iff ∈Diff(M) has the inverse shadowing
property with respect to the class Tα(f) (α= ,c,h,d), then by the definition, it clearly
has the weak inverse shadowing property with respect to the class Tα(f) (α= ,c,h,d).
We say thatf has theorbital inverse shadowing propertywith respect to the classTα(f),
α= ,c,h,d, if for any> , there is aδ> such that for anyδ-methodϕ∈Tα(f,δ) and
any pointx∈M, there is a pointy∈Msuch that
Of(x)⊂B
ϕ(y) and ϕ(y)⊂B
Of(x)
.
Note that iff has the inverse shadowing property with respect to the classTα(f) (α=
,c,h,d), then it has the orbital inverse shadowing property with respect to the classTα(f)
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 classTα(f),α=
,c,h,dif there is aC-neighborhoodU(f) offsuch that for anyg∈U(f),ghas the inverse
(weak inverse or orbital inverse) shadowing property with respect to the classTα(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 anyg∈U(f), everyp∈P(g) is hyperbolic, whereP(g) is the set of periodic points ofg. It is proved by Hayashi [] that f ∈F(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 splittingEs⊕Eu and there exist constantsC> and
<λ< such that
Dxfn|Es
x≤Cλ
n and D
xf–n|Eu
x≤Cλ
n
for allx∈andn≥. If=M, then we say thatf is anAnosov diffeomorphism.
2 Statement of the results
stable diffeomorphism is an Axiom A diffeomorphism. And in [], Palis extended this result to-stable diffeomorphisms.
LetMbe a compactC∞n-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 setFμ(M) as the set of diffeomorphismsf ∈Diffμ(M) which has aC
-neighborhoodU(f)⊂Diffμ(M) such that for anyg∈U(f), every periodic point ofg is
hyperbolic. Note thatFμ(M)⊂F(M) (see [, Corollary .]).
Very recently, Arbieto and Catalan [] proved that if a volume-preserving diffeomor-phism is contained inFμ(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 compactC∞ n-dimensional Riemannian manifold endowed with a volume formω, and letf∈Diffμ(M). To prove the results, we will give the following well-known
Lemma . Let f ∈Diffμ(M)andU be a C-neighborhood of f inDiff
μ(M).Then there
exist a C-neighborhoodU
⊂Uof f and> such that if g∈U,for any finite f -invariant
set E={x, . . . ,xm}, any neighborhood U of E and any volume-preserving linear maps
Lj:TxjM→Tg(xj)M withLj–Dxjg ≤ 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 ofx∈M.
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 pointp∈P(g) for someg∈V(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 constructg C-nearbyg such
that
g(x) =
ϕp–◦Dpg◦ϕp(x) ifx∈Bα(p),
g(x) ifx∈/Bα(p).
Theng(p) =g(p) =p. Since the eigenvalueλofDpgis one,Dpg(v) =vfor anyv∈Ecp(α).
Takev∈Ecp(α) such thatv=α/. Then we set
Iv={t·v: –≤t≤} ⊂ϕp
Bα(p)
.
Take=α/. Let <δ<be the number of the inverse shadowing property ofg. Then
by our construction ofg,ϕ–p (Iv)⊂Bα(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 anyx∈M, 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, andh∈Td(g). Letpbe
identified with = (, . . . , ). Then choosex= (x, , . . . , )∈Jp such that d(,x) = .
Then
dhi(),gi(x)=d(,x) = .
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 pointy∈M\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–
p ◦Dpg◦ϕp(x) ifx∈Bα(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 anyv∈ϕp(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=j≤l– ,
• gl(Lp) =Lp, and
• gl
|Lpis the identity map.
Note thatghas the inverse shadowing property if and only ifgkhas the inverse shadowing
property for allk∈Z(see []). As in the first case, we can show thatgdoes 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 pointp∈P(g) for some g∈V(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:Bα(p)→TpM. Then we can make an arcJp⊂Bα(p) and for someg∈V(f). Take
= (lengthJp)/. Let <δ< be the number of the weak inverse shadowing property
Letpbe identified with= (, . . . , ). Then choose a pointx= (x, , . . . , )∈Jpsuch that
d(,x) = . Sinceghas the weak inverse shadowing property,
Oh()⊂B
Og(x)
.
However, for anyy∈Jp,
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 pointy∈M\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,gdoes 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 anyv∈ϕp(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∈Fμ(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
a nonhyperbolic periodic point p∈P(g) for someg∈V(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:Bα(p)→TpM. Then we can make an
arcJp⊂Bα(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) = . Sinceghas the orbital inverse
shadowing property,
Oh()⊂B
Og(x)
and Og(x)⊂B
Oh()
.
However, for anyy∈Jp,
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 pointy∈M\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,gdoes 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 anyv∈ϕp(Bα(p))⊂TpM. As in the previous argument, in order to reach
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
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