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Research article Special Issues

Flows with ergodic pseudo orbit tracing property


  • In the manuscript, we deal with a type of pseudo orbit tracing property and hyperbolicity about a vector field (or a divergence free vector field). We prove that a vector field (or a divergence free vector field) of a smooth closed manifold M has the robustly ergodic pseudo orbit tracing property then it does not contain any singularities and it is Anosov. Additionally, there is a dense and open set R in the set of C1 a vector field (or a divergence free vector field) of a smooth closed manifold M such that given a vector field (or a divergence free vector field) has the ergodic pseudo orbit tracing property then it does not contain singularities and it is Anosov.

    Citation: Manseob Lee. Flows with ergodic pseudo orbit tracing property[J]. Electronic Research Archive, 2022, 30(7): 2406-2416. doi: 10.3934/era.2022122

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  • In the manuscript, we deal with a type of pseudo orbit tracing property and hyperbolicity about a vector field (or a divergence free vector field). We prove that a vector field (or a divergence free vector field) of a smooth closed manifold M has the robustly ergodic pseudo orbit tracing property then it does not contain any singularities and it is Anosov. Additionally, there is a dense and open set R in the set of C1 a vector field (or a divergence free vector field) of a smooth closed manifold M such that given a vector field (or a divergence free vector field) has the ergodic pseudo orbit tracing property then it does not contain singularities and it is Anosov.



    In smooth dynamical systems, various pseudo trajectory(orbit) tracing properties have been studied to investigate hyperbolic systems (see [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21]). About the ergodic pseudo orbit tracing property (see [22]), Barzanouni and Honary [23] and Lee [24,25,26] studied that a C1 diffeomorphism f of a smooth closed manifold M has a hyperbolic structure if f has the robustly ergodic pseudo orbit tracing property. The results are a version of discrete smooth dynamic system. In general, many results of discrete smooth dynamic systems can be extended for continuous smooth dynamic systems. However, the results of discrete dynamic systems can not directly lead to the results of successive smooth dynamic systems (see [27,28]). For instance, Sakai [19] proved that a diffeomorphism f has the robustly pseudo orbit tracing property if and only if it is structural stable. But, for continuous dynamical systems, it is still open problem if the system having sinuglar points (see [6]). In the paper, we consider an extended version, that is, continuous dynamic systems, of the result for the ergodic pseudo orbit tracing property of a C1 diffeomorphism f of a smooth closed manifold M.

    Assume that Mn=M is smooth closed n(3) dimensional manifold with Riemannian metric d(,). The flow φ:R×MM satisfies the followings: (i) φ0(x)=x, xM, and (ii) φs(φt(x))=φs+t(x) xM and all s,tR. Denote by X(M) the set of C1-vector fields on M. For any xM, the Orb(x,φ)={φt(x):tR} is called the orbit of φ through x. Let Rep={h:RR:h is an oriented homeomorphism with h(0)=0}. For any ϵ>0, we define Rep(ϵ) as follows:

    Rep(ϵ)={hRep:|h(t)h(s)ts1|<ϵ(ts)}.

    Let ξ={(xi,ti):tiτ,iZ}, and Γδ(ξ)={iZ:d(φti(xi),xi+1)δ}. Then a sequence of points {(xi,ti):tiτ,iZ} is called (δ,τ)-ergodic pseudo orbit of φ if for iZ, tiτ,

    limn#(Γδ(ξ){0,,n1})n=0, and
    limn#(Γδ(ξ){0,1,,n+1})n=0,

    where #(A) is the number of the elements of A. Let s0=0,sn=n1i=0ti, and sn=1i=nti, n=1,2,. Then we define

    Γϵ(ξ,x)+={iN{0}:si+1sid(φh(t)(x),φtsi(xi))dtϵ}, and
    Γϵ(ξ,x)={iN:si+1sid(φh(t)(x),φtsi(xi))dtϵ}.

    We set Γϵ(ξ,x)=Γϵ(ξ,x)+Γϵ(ξ,x).

    Definition 2.1. A vector field φ has the ergodic pseudo orbit tracing property if for any positive ϵ>0, we can find positive δ>0 such that for any (δ,τ)-ergodic pseudo orbit ξ={(xi,ti):tiτ,iZ} there are a point zM and hRep(ϵ) for which

    lim|n|#(Γϵ(ξ,z){0,1,,n1})n=0.

    Denote by ESP the set of all vector fields possessing the ergodic pseudo orbit tracing property and by int(ESP) the set of all C1 interior of the set of all vector fields possessing the ergodic pseudo orbit tracing property. A closed φt-invariant set ΛM is called hyperbolic for φt if

    (a) Λ have a continuous Dφ-invariant tangent bundle decomposition TΛM=EsΛFEuΛ,

    (b) Dφt|EsxCeλt, xΛ and every t0, and

    (c) m(Dφt|Eux)Ceλt, xΛ and every t0,

    where m(T)=infv=1T(v) is the minimum norm of a linear operator T, and F is generated by X(x). We say that φX(M) is Anosov if M is hyperbolic for φ. Let Sing(φ)={xM:φ(x)=0} and P(φ)={xM: there is T>0 such that φT(x)=x}. Denote by Crit(φ)=Sing(φ)P(φ).

    Theorem A Let φX(M). we have the followings:

    (a) If φint(ESP) then Sing(φ)= and φ is Anosov.

    (b) There is a dense and open set R in X(M) such that given φR, if φESP then Sing(φ)= and φ is Anosov.

    Let Mn=M be a smooth closed n(3)-dimensional Riemannian manifold endowed with a volume form μ(Lebesgue measure). A vector field φ is divergence-free if its divergence is zero. Notice that, by Liouville formula, a flow φt is volume-preserving means that it is the corresponding divergence-free vector field φ. Let Xμ(M) denote the space of C1 divergence-free vector fields on M and we consider the usual C1 Whitney topology on this space. Lee proved in reference [8] that a volume preserving diffeomorphism f of a smooth compact manifold M has the robustly the ergodic pseudo orbit tracing property is equivalent to Anosov, and there is a dense and open set M in the set of all volume preserving diffeomorphisms of a smooth compact manifold M such that given fM, f has the the ergodic pseudo orbit tracing property is equivalent to Anosov. It is a discrete version of volume preserving dynamical systems.

    Denote by ESPμ the set of all divergence-free vector fields possessing the ergodic pseudo orbit tracing property and by int(ESP)μ the set of all C1 interior of the set of all divergence-free vector fields possessing the ergodic pseudo orbit tracing property.

    According the result and the previous results, we have the following.

    Theorem B Let φXμ(M). We have the followings:

    (a) If φint(ESP)μ then it is Anosov.

    (b) There is a dense and open set M in Xμ(M) such that given φM, if φESPμ then it is Anosov.

    Let M be as before, and let φXμ(M). Given δ>0 and τ>0, a sequence of points {(xi,ti):tiτ,iZ} is called (δ,τ)-pseudo orbit of φ if tiτ and d(φti(xi),xi+1)<δ iZ. For x,yM, a finite (δ,τ)-pseudo orbit {(xi,ti):tiτ,i=0,1,,n} of φ is said to be a (δ,τ)-chain of φ from x to y with length n+1 if x0=x and xn=y. A φX(M) is said to be chain transitive if M is a chain transitive set. Let U,V be non-empty open subsets of M. A vector field φ is transitive if φT(U)V, for some T>0. Obviously, if φ is transitive then it is chain transitive (see [31,Proposition 3.3.2]). A closed φt-invariant set ΛM is attracting if Λ equals t0φt(U) for some neighborhood U satisfying ¯φt(U)U, t>0. An attractor of φ is a transitive attracting set of φ and a repeller is an attractor for φ. A closed φt-invariant set ΛM is a proper attractor or repeller if ϕΛM. In [18,Proposition 3], a vector field φ is chain transitive in an isolated set Λ if and only if Λ has no proper attractor for φ. Here Λ is isolated if there exists an open set U of Λ which is called isolated block for which tRφt(U)=Λ.

    A vector field φ has the pseudo orbit tracing property if for any positive η>0, one can find δ>0 such that any (δ,1)-pseudo orbit {(xi,ti):tiT,iZ}, there are a point yM and hRep(ϵ) having the following property;

    d(φh(t)(y),φtsi(xi))<η,

    iZ and sit<si+1, where s0=0,si=t0+t1++ti for i>0 and si=(t1+t2++ti) for i>0.

    Lemma 3.1. If a vector field φESP then φ has the finite pseudo orbit tracing property.

    Proof. Firstly, we show that φ is chain transitive. To prove, it is enough to show that Λ is a proper attractor. Since Λ is compact, one can take a positive η> for which ΛB(η,Λ). Set ϵ=η/4 and U=B(η,Λ). We take two points aΛ and bMU. Let δ>0 be the number of the definition of the ergodic pseudo orbit tracing property. Then we construct a (δ,1)-ergodic pseudo orbit of φ as follows: for iZ and ti=1, (i) φi(a)=xi for i0, and (ii) φi(b)=xi for i>0. Clearly, ζ={(xi,ti):ti=1,iZ} is (δ,1)-ergodic pseudo orbit of φ. Since φESP, there are a point zM and hRep(ϵ) having the following property;

    lim|n|#(Γϵ(ζ,z){0,1,,n1})n=0.

    Then we can find τ>0 such that φh(τ)(z)U. Since Λ is an attractor, φt(φh(τ)(z))U, t>0. Set φh(τ)(z)=z. Then we know that

    d(φt(z),φt(b))>η

    t>0. Since d(φt(z),φt(b))>η t>0 and by ergodic pseudo orbit ζ, we have

    i+1id(φh(t)(z),φti(xi))dt>ϵ,

    iN{0}. Thus one can see that

    lim|n|#(Γϵ(ζ,z){0,1,,n1})n0.

    This is a contradiction.

    Now, we prove that φ has the finite pseudo orbit tracing property.

    For any nN, the finite sequence ξn={(xni,ti):ti1,0in} is a (1/n,1)-pseudo orbit of φ. Since φESP, as the above, for any nN, there is a (1/n,1)-chain ζn={(yni,ti):ti1,0in} such that ξnζnξn+1 is a 1/n-pseudo orbit. Clearly, the sequence

    τ={ξ1ζ1ξ2ζ2}={x10,x11,,x1n,y10,y20,,y1n,,}

    is a (1/n,1)-ergodic pseudo orbit of φ. We denote τ={(wi,ti):ti1,i0}. Since φESP, there are a point zM and hRep(ϵ) having the following property;

    limn#(Γϵ(τ,z){0,1,,n1})n=0.

    Then there are tR and wjτ for which d(φt(z),wj)<ϵ. Thus we can find a finite (1/n,1)-pseudo orbit ξnτ such that ξn is ϵ-pseudo orbit traced by the point φt(z). Thus φ has the finite pseudo orbit tracing property which is a contradiction.

    Notice that Thomas proved in [21] that if a flow φt has no singular points then φt has the finite pseudo orbit tracing property with respect to hRep if and only if φt has the pseudo orbit tracing property with respect to hRep. However, if a flow φt has a singular point then it is not true (see [33]). On the other hand, the flow φt has the finite pseudo orbit tracing property if and only if φt has the pseudo orbit tracing property, for some hRep(ϵ).

    Remark 3.2. If vector field φESP then by Lemma 3.1, it has the pseudo orbit tracing property. Then we can easily show that it is transitive.

    Indeed, since φESP, φ is chain transitive and by Lemma 3.1, φ has the pseudo orbit tracing property. Let U,V be given non-empty open sets. We take xU and yV and choose a positive ϵ small enough such that Bϵ(x)U and Bϵ(y)V. Let δ(ϵ)>0 be the number of the pseudo orbit tracing property of φ. Then there is a finite (δ,1)-pseudo orbit {(xi,ti):ti1,0in} such that x0=x and xn=y. Since φ has the pseudo orbit tracing property, there are a point zM and hRep(ϵ) for which d(φh(t)(z),xtsi))<ϵ for all 0in and s0=0,si=t0+t1++tn. Then we know φh(t)(z)V. Put h(t)=T. Then φT(U)V which means that φ is transitive.

    Let γP(φ) be hyperbolic, and let pγ be such that φπ(p)(p)=p. The stable manifold Vs(γ) of γ and the unstable manifold Vu(γ) of γ are defined as follows: Vs(γ)={yM:d(φt(y),φt(γ))0as t}, and Vu(γ)={yM:d(φt(y),φt(γ))0as t}. For any small η>0, the local stable manifold Vsη(p)(p) of p and the local unstable manifold Vuη(p)(p) of p are defined by Vsη(p)(p)={yM:d(φt(y),φt(p))<η(p),if t0}, and Vuη(p)(p)={yM:d(φt(y),φt(p))<η(p),if t0}. Let σSing(φ) be a hyperbolic. Then such as the hyperbolic periodic orbits, the stable/unstable manifold, and local stable/unstable manifold are defined for σSing(φ).

    Lemma 3.3. Let γ,σCrit(φ) behyperbolic. If a vector field φESP then Vs(σ)Vu(γ) and Vs(γ)Vu(σ).

    Proof. To prove, we consider that γ,σP(φ) are hyperbolic(other case is similar). Since φESP, by Remark 3.2, it is transitive. Thus one can take a point xM for which ¯Orb(x)=M. Let ϵ(σ)>0 and ϵ(γ)>0 be as before with respect to σ and γ. Set η=min{ϵ(σ),ϵ(γ)}. Since, by Lemma 3.1, φ has the pseudo orbit tracing property, we let 0<δ=δ(η)<η be the number of the pseudo orbit tracing property of φ. For a finite (δ,1)-pseudo orbit {(xi,ti):ti1,i=0,,n}. Let ti=1(i=0,,n). Since φ is transitive, there are positive t and s such that

    d(φt(x),σ)<δ  and d(φs(x),γ)<δ.

    Then there are natural number k,lN such that kt<k+1 and ls<l+1, and so d(φk(x),σ)<δ and d(φl(x),γ)<δ.

    Take pσ and qγ such that d(φ1(p),φk(x))<δ and d(φl(x),q)<δ. We may assume that l>k. Then we have a finite (δ,1)-pseudo orbit of φ such that

    {p,φk(x),φk+1(x),,φl1(x),q}.

    Assume that l=k+j for some jR. Then we construct a (δ,1)-pseudo orbit {(xi,ti):ti=1,iZ}={(xi,1):iZ} as follows: (i) xi=φi(p) for i0, (ii) xi+1=φk+i(x) for 0i<j, and (iii) xi=φl+i(q) for i1. Then

    {(xi,ti):ti=1,iZ}={,φ1(p),x0(=p),φk(x),φk+1(x),,φk+j1(x),q,,}={,x1,x0(=p),x1,,xj,xj+1(=q),}

    is a (δ,1)-pseudo orbit of φ. Since φ has the pseudo orbit tracing property, there exist a point zM and hRep(ϵ) such that

    d(φh(t)(z),φtsi(xi))<η iZ,

    where s0=0,si=t0+t1++ti for i>0 and si=t1+t2++ti for i>0. Then d(z,p)<η and

    d(φh(t)(z),φtsi(p))=d(φh(t)(z),φt+i(p))=d(φh(t)(z),φt(φi(p)))<η

    for i0 and sit<si+1. Thus if t then zVuuη(p)Vu(σ).

    Similarly, we obtain zVs(γ). Indeed, for sj+1t<sj+2 we know that

    d(φh(t)(z),φtsj+1(xj+1))=d(φh(t)(z),φtsj+1(q))<η.

    Let φh(t)(z)=z. Then by Lemma 3.1, d(φs(z),φs(φtsj+1(q)))<η for s. One can see that zVuuη(q)Vu(γ). Thus Orb(φ,z)Vu(σ)Vu(γ) and so Vu(σ)Vs(γ).

    A set ΛM is robustly transitive if Λ is closed φt-invariant, and there exist a neighborhood U(φ) of φ and a neighborhood U of Λ such that for any ϕU(φ), Λϕ(U)=tRϕt is transitive. A vector field φ is robustly transitive if Λ=M.

    Remark 3.4. Let φX(M)int(ESP). Since φESP, by Remark 3.2, φ is transitive. Thus if φint(ESP) then φ is robustly transitive. According to Vivier's result [35,Theorem 1], φ has no singularity. Thus if φint(ESP) then Sing(φ)=.

    For a hyperbolic γCrit(φ), we denote index(γ)=dimVs(γ). Note that if γCrit(φ) is hyperbolic then there are a neighborhood U(φ) of φ and a neighborhood U of γ such that for any ϕU(φ), ϕ has a critical hyperbolic orbit γϕU and index(γ)=index(γϕ), where γϕ is called the continuation of γ. We say that a vector field φ is Kupka-Smale if every pCrit(φ) is hyperbolic and their stable and unstable manifolds intersect transversally. It is well known that the Kupka-Smale vector fields form a dense and open set in X(M) (see [29]). Denote by KS the set of all Kupka-Smale vector fields.

    Proposition 3.5. Let φint(ESP). Then the index of all hyperbolic γP(φ) isconstant.

    Proof. Let U(φ)X(M) be a neighborhood of φ. Since φESP, by Theorem 3.2 φ is transitive, and so, φ does not admit sink and source. As in the proof of Arbieto, Senos and Sodero [1], assume that there exist two hyperbolic γ,τP(φ) such that index(γ)index(τ). Then we can use Kupka-Smale vector fields and so, we will derive a contradiction. Indeed, assume index(γ)=i and index(τ)=j. If j<i, then we have

    dimVs(γ)+dimVu(τ)dimM.

    Since φint(ESP), we can take ϕKSU(φ) such that ϕESP. Then there exist two hyperbolic γϕ,τϕP(ϕ) such that index(γ)=index(γϕ) and index(τ)=index(τϕ). Thus we know

    dimVs(γϕ)+dimVu(τϕ)dimM.

    We consider the case dimVs(γϕ)+dimVu(τϕ)<dimM. Then we know Vs(γϕ)Vu(τϕ)=.

    We consider other case dimVs(γϕ)+dimVu(τϕ)=dimM. Since ϕESP, by Lemma 3.3, we may assume that xVs(γϕ)Vu(τϕ). Then as in the proof of Arbieto, Senos and Sodero [1], we have

    dim(Tx(Vs(γϕ))+Tx(Vu(τϕ)))<dimVs(γϕ)+dimVu(τϕ)=dimM.

    This means that Vs(γϕ) is not transverse to Vu(τϕ). Since ϕKS, we know Vs(γ)Vu(τ)=. This is a contradiction.

    Finally, we consider j>i. Then as the above arguments, we can get a contradiction.

    Lemma 3.6. [1,Theorem 4.3.] Let φint(ESP). If a periodic orbit γ is not hyperbolic thenthere is ϕ C1-close to φ for which ϕ has twohyperbolic periodic orbits γ1,γ2 with differentindices.

    A vector field φ is star if there exists a neighborhood U(φ)X(M) such that for any ϕU(φ), every γCrit(ϕ) is hyperbolic. Denote by G(M) the set of all star vector fields and G(M) the set of all non-singular star vector fields. Note that if φG(M) then φ is Axiom A without cycles (see [27]) and so φ is Anosov if transitive φG(M).

    Proposition 3.7. If a vector field φint(ESP), then φG(M).

    Proof. Since φint(ESP), by Remark 3.4 we have Sing(φ)=. Assume that φG(M). Then there is ϕ C1-close to φ such that ϕ has a non-hyperbolic periodic orbit γ. By Lemma 3.6, there is ϕ1 C1 close to ϕ (also, C1 close to φ) such that ϕ1 has two hyperbolic periodic orbits γ1,γ2 with index(γ1)index(γ2). Since φint(ESP), by Proposition 3.5, we have index(γ1)=index(γ2). This is a contradiction.

    End of the proof of Item (a). Since φint(ESP), by Remark 3.4, φ is robustly transitive and Sing(φ)=. By Proposition 3.5, for any hyperbolic γ,ηP(φ), we know index(γ)=index(η). By Proposition 3.7, φG(M). According to Remark 3.2, φ is transitive Anosov.

    Lemma 3.8. [1,Lemma 3.4] Let φKS and let γ,τCrit(φ). If dimVs(γ)+dimVu(τ)dimM then Vs(γ)Vu(τ)=.

    Lemma 3.9. There is an dense and open set G1X(M) such that given φG1, if φESP then Sing(φ)= and the index of all γP(φ) is constant.

    Proof. We first show that Sing(φ)=. Let φG1=KS, φESP and let γP(φ) be hyperbolic with index(γ)=j. Assume that there exists a hyperbolic σSing(φ) such that index(σ)=i. We consider two cases: (i) j<i, and (ii) j>i. However, the cases (i) and (ii) have

    dimVs(γ)+dimVu(σ)dimM and dimVu(γ)+dimVs(σ)dimM.

    By Lemma 3.8, this is a contradiction. Thus if a vector field φG1 and φESP then Sing(φ)=.

    Finally, we show that index(γ)=index(η), for any hyperbolic γ,ηP(φ). Let γ,ηP(φ) be hyperbolic. Assume that index(γ)index(η). Then we have dimVs(γ)+dimVu(τ)dimM. This is a contradiction by Lemma 3.8.

    For any positive δ>0, a point pγP(φ) is δ-hyperbolic if the derivative of the Poincaré map of φ has an eigenvalue λ of p such that (1δ)<|λ|<(1+δ).

    Lemma 3.10. [1,Lemma 5.1,Lemma 5.3] There isa dense and open set G2X(M) suchthat given φG2,

    (a) if any neighborhood U(φ) of φ one can take ϕU(φ) for which ϕ has two hyperbolicperiodic orbits γ1,τ1 with different indices then φ has two hyperbolic periodic orbits γ,τ withdifferent indices.

    (b) for any positive δ>0, if any neighborhood U(φ) of φ one can take ϕU(φ) for which g has a δ-hyperbolic periodic orbit γ1 then φ hasa 2δ-hyperbolic periodic orbit γ.

    Note that if pγP(φ) is a δ- hyperbolic then by [34,Lemma 1.3], one can take ϕ C1-close to φ for which Dϕπ(p)(p) has 1 as an eigenvalue, where π(p) is the period of p.

    Lemma 3.11. There is a dense and open set G3X(M) such that given φG3, if φESP then one can find apositive δ such that every γP(φ) is not δ-hyperbolic.

    Proof. Let φG3=G2G1 and φESP. To derive a contradiction, we may assume that for any δ>0, one can take γP(φ) for which γ is a δ-hyperbolic. Then by [34,Lemma 1.3] and Lemma 3.6, one can take ϕ C1-close to φ such that ϕ has two hyperbolic η1,τ1P(ϕ) with different indices. By Lemma 3.10(a), φ has two hyperbolic η,τP(φ) with different indices. This is a contradiction by Lemma 3.9.

    Proposition 3.12. For φG3, if φ has ESP then φG(M).

    Proof. Let φG3 and φESP. By Lemma 3.9, Sing(φ)=. To prove, it is enough to show that φG(M), that is, for any ϕ C1 close to φ, every γP(ϕ) is hyperbolic. Assume that φG(M). Then one can take ϕ C1 close to φ such that ϕ has a periodic orbit γ which is not hyperbolic. As [34,Lemma 1.3], one can take ϕ1 C1 close to ϕ(also C1 close to φ) for which ϕ1 has a δ/2-hyperbolic γϕ1P(ϕ1). Since φG2, φ has a δ-hyperbolic γP(φ). This is a contradiction by Lemma 3.11.

    End of the proof of Item (b). Let φG3 and φESP. Since φESP, by Remark 3.2, it is enough to show that φG(M). By Lemma 3.9 and Proposition 3.12, every γP(φ) is hyperbolic, and so, φG(M). Thus φ is transitive Anosov.

    Remark 4.1. Let φXμ(M). By Zuppa's Theorem [30], we can find ϕ C1-close to φ such that ϕXμ(M),ϕπ(p)(p)=p and Pπ(p)ϕ(p) has an eigenvalue λ with |λ|=1.

    A φXμ(M) is a divergence-free star if there exists a neighborhood U(φ) of φ in Xμ(M) such that every point in Crit(ϕ) is hyperbolic, for any ϕU(φ)Xμ(M). The set of divergence-free star vector fields is denoted by Gμ(M). Then we get the following.

    Theorem 4.2. [32,Theorem 1] If φGμ(M) then Sing(φ)= and φ is Anosov.

    Proof of Theorem B. To prove Theorem B, it is enough to show that φGμ(M). At first, we assume that φint(ESP)μ. As in the proof of Theorem A, we can easily show that φGμ(M). Thus φ is transitive Anosov. Finally, there is a dense and open set M in Xμ(M) such that given φM, we assume that φESPμ. As in the proof of Theorem A, we can show that φGμ(M). Thus φ is transitive Anosov.

    The authors would like to express thanks to reviewers for their careful reading of the manuscript. This work is supported by the National Research Foundation of Korea(NRF) grant funded by the Korea Government(MSIT) (No. 2020R1F1A1A01051370).

    The authors declare there is no conflicts of interest.



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