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Abundance of C1C^{1}-robust homoclinic tangencies

Christian Bonatti and Lorenzo J. Díaz This paper was partially supported by CNPq, Faperj, and PRONEX (Brazil) and the Agreement in Mathematics Brazil-France. We acknowledge the warm hospitality of I.M.P.A, Institute de Mathématiques de Bourgogne, and PUC-Rio during the stays while preparing this paper
Abstract

A diffeomorphism ff has a C1C^{1}-robust homoclinic tangency if there is a C1C^{1}-neighbourhood 𝒰{\cal U} of ff such that every diffeomorphism in g𝒰g\in{\cal U} has a hyperbolic set Λg\Lambda_{g}, depending continuously on gg, such that the stable and unstable manifolds of Λg\Lambda_{g} have some non-transverse intersection. For every manifold of dimension greater than or equal to three, we exhibit a local mechanism (blender-horseshoes) generating diffeomorphisms with C1C^{1}-robust homoclinic tangencies.

Using blender-horseshoes, we prove that homoclinic classes of C1C^{1}-generic diffeomorphisms containing saddles with different indices and that do not admit dominated splittings (of appropriate dimensions) display C1C^{1}-robust homoclinic tangencies.

keywords: chain recurrence set, dominated splitting, heterodimensional cycle, homoclinic class, homoclinic tangency, hyperbolic set.

MSC 2000: 37C05, 37C20, 37C25, 37C29, 37C70.


To Carlos Gutierrez (1944 -- 2008), in memoriam


1 Introduction

1.1 Framework and general setting

A homoclinic tangency is a dynamical mechanism which is at the heart of a great variety of non-hyperbolic phenomena: persistent coexistence of infinitely many sinks [22], Hénon-like strange attractors [5, 20], super-exponential growth of the number of periodic points [19], and non-existence of symbolic extensions [15], among others. Moreover, homoclinic bifurcations (homoclinic tangencies and heterodimensional cycles) are conjectured to be the main source of non-hyperbolic dynamics (Palis denseness conjecture, see [23]).

In this paper, we present a local mechanism generating C1C^{1}-robust homoclinic tangencies. Using this construction, we show that the occurrence of robust tangencies is a quite general phenomenon in the non-hyperbolic setting, specially when the dynamics does not admit a suitable dominated splitting.

Let us now give some basic definitions (in Section 2, we will state precisely the definitions involved in this paper). A transitive hyperbolic set Λ\Lambda has a homoclinic tangency if there is a pair of points x,yΛx,y\in\Lambda such that the stable leaf Ws(x)W^{\operatorname{s}}(x) of xx and the unstable leaf Wu(y)W^{\operatorname{u}}(y) of yy have some non-transverse intersection

Given a hyperbolic set Λ\Lambda of a diffeomorphism ff, for gg close to ff, we denote by Λg\Lambda_{g} the hyperbolic set of gg which is the continuation of Λ\Lambda (i.e., Λg\Lambda_{g} is close to Λ\Lambda and the dynamics of ff on Λ\Lambda and gg on Λg\Lambda_{g} are conjugate).

Definition 1.1 (Robust cycles).

  • Robust homoclinic tangencies: A transitive hyperbolic set Λ\Lambda of a CrC^{r}-diffeomorphism ff has a CrC^{r}-robust homoclinic tangency if there is a CrC^{r}-neighborhood 𝒩{\cal N} of ff such that for every g𝒩g\in{\cal N} the continuation Λg\Lambda_{g} of Λ\Lambda for gg has a homoclinic tangency.

  • Robust heterodimensional cycles: A diffeomorphism ff has a CrC^{r}-robust heterodimensional cycle if there are transitive hyperbolic sets Λ\Lambda and Σ\Sigma of ff whose stable bundles have different dimensions and a CrC^{r}-neighborhood 𝒱{\cal V} of ff such that Ws(Λg)Wu(Σg)W^{\operatorname{s}}(\Lambda_{g})\cap W^{\operatorname{u}}(\Sigma_{g})\neq\emptyset and Wu(Λg)Ws(Σg)W^{\operatorname{u}}(\Lambda_{g})\cap W^{\operatorname{s}}(\Sigma_{g})\neq\emptyset, for every diffeomorphism g𝒱g\in{\cal V}.

Note that, by Kupka-Smale theorem, CrC^{r}-generically, invariant manifolds of periodic points are in general position. Hence, generically, the non-transverse intersections in a robust cycle (tangency or heterodimensional cycle) involve non-periodic points (i.e., at least a non-trivial hyperbolic set).

In [21], Newhouse constructed surface diffeomorphisms having hyperbolic sets (called thick horseshoes) exhibiting C2C^{2}-robust homoclinic tangencies. Later, he proved that, in dimension two, homoclinic tangencies of C2C^{2}-diffeomorphisms yield thick horseshoes with C2C^{2}-robust homoclinic tangencies, [22] (see also [24] for a broad discussion of homoclinic bifurcations on surfaces). With the same C2C^{2}-regularity assumption, theorems in [27, 25] extend Newhouse result, proving that homoclinic tangencies in any dimension lead to C2C^{2}-robust homoclinic tangencies. In this paper, we study the occurrence of robust homoclinic tangencies in the C1C^{1}-setting.

Newhouse construction (thick horseshoes with robust tangencies) involves distortion estimates which are typically C2C^{2}. The results in [30] present some obstacles for carrying this construction to the C1C^{1}-topology: C1C^{1}-generic surface diffeomorphisms do not have thick horseshoes. Recent results by Moreira in [17] are a strong indication that there are no surface diffeomorphisms exhibiting C1C^{1}-robust homoclinic tangencies111This question is closely related to the open problem of C1C^{1}-density of hyperbolic diffeomorphisms on compact surfaces (Smale’s density conjecture). In fact, Moreira’s result imply that there are no C1C^{1}-robust homoclinic tangencies associated to hyperbolic basic sets of surface diffeomorphisms. See [1] for a discussion of the current state of this conjecture..

Nevertheless, in higher dimensions, there are examples of diffeomorphisms having hyperbolic sets with C1C^{1}-robust tangencies. For instance, the product of a non-trivial hyperbolic attractor by a normal expansion gives a hyperbolic set Λ\Lambda of saddle type, whose stable manifold has a topological dimension greater than the dimension of its stable bundle. Then the set Λ\Lambda can play the role of thick horseshoes in Newhouse construction. Geometrical constructions using these kind of “thick” hyperbolic sets provide examples of systems with C1C^{1}-robust heterodimensional cycles222A heterodimensional cycle is a cycle associated to saddles having different indices. (see [3]) or C1C^{1}-robust tangencies (see [28, 4]). But these constructions involve quite specific global dynamical configurations, thus they cannot translate to a general setting.

1.2 Robust homoclinic tangencies

The aim of this paper is to show that the existence of C1C^{1}-robust homoclinic tangencies is a common phenomenon in the non-hyperbolic setting. For instance, next result is a consequence of the local mechanism for robust tangencies in Theorem 2.

Theorem 1.

Let MM be a compact manifold with dim(M)3\dim(M)\geq 3. There is a residual subset {\cal R} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that, for every ff\in{\cal R} and every periodic saddle PP of ff such that

  • (index variability) the homoclinic class H(P,f)H(P,f) of PP has a periodic saddle QQ with dim(Es(Q))dim(Es(P))\dim(E^{\operatorname{s}}(Q))\neq\dim(E^{\operatorname{s}}(P)),

  • (non-domination) the stable/unstable splitting Es(R)Eu(R)E^{\operatorname{s}}(R)\oplus E^{\operatorname{u}}(R) over the set of saddles RR homoclinically related with PP is not dominated,

then the saddle PP belongs to a transitive hyperbolic set having a C1C^{1}-robust homoclinic tangency.

For the precise definitions of homoclinic class and dominated splitting see Definitions 2.1 and 2.4. Let us reformulate Theorem 1 by focusing on the homoclinic class of a prescribed periodic orbit:

Corollary 1.

Let MM be a compact manifold with dim(M)3\dim(M)\geq 3. Consider a diffeomorphism ff with a saddle PfP_{f} whose continuation PgP_{g} is defined for all gg in a neighborhood 𝒰{\cal U} of ff in Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M). Assume that

  • (generic index variability) there is a residual subset 𝒢{\cal G} of 𝒰{\cal U} such that, for every g𝒢g\in{\cal G}, the homoclinic class of PgP_{g} of ff contains a saddle QQ of different index,

  • (robust non-domination) for every g𝒰g\in{\cal U}, the stable/unstable splitting Es(R)Eu(R)E^{\operatorname{s}}(R)\oplus E^{\operatorname{u}}(R) over the set of saddles RR homoclinically related with PgP_{g} is not dominated.

Then there is an open and dense subset 𝒞{\cal C} of 𝒰{\cal U} of diffeomorphisms gg such that the saddle PgP_{g} belongs to a transitive hyperbolic set with a C1C^{1}-robust homoclinic tangency.

Remark 1.2.

The diffeomorphisms ff in the residual subset {\cal R} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) in Theorem 1 satisfy the following properties (see [2, Section 2.1] and [13, Appendix B.1.1]):

  • Every homoclinic class H(Pf,f)H(P_{f},f) of ff depends continuously on ff\in{\cal R}. Therefore, if H(Pf,f)H(P_{f},f) has a dominated splitting then H(Pg,g)H(P_{g},g) also has a dominated splitting whose bundles have constant dimension for all gg\in{\cal R} close to ff.

  • Assume that a homoclinic class H(Pf,f)H(P_{f},f) of ff\in{\cal R} contains saddles of stable indices jj and kk, jkj\neq k. Then the homoclinic class H(Pg,g)H(P_{g},g) also contains saddles of stable indices jj and kk for every gg\in{\cal R} close to ff.

In other words, the conditions in Theorem 1 are C1C^{1}-open in the residual set {\cal R} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M).

The index interval of a homoclinic class HH is the interval [i,j][i,j], where ii and jj are the minimum and the maximum of the s{\operatorname{s}}-indices (dimension of the stable bundle) of the periodic points in HH. The homoclinic class HH has index variation if i<ji<j. Given a transitive hyperbolic set Λ\Lambda its s{\operatorname{s}}-index is the dimension of its stable bundle.

Corollary 2.

For every diffeomorphism ff in the residual subset {\cal R} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M), any homoclinic class HH of ff with index variation, and every k[i,j]k\in[i,j], where [i,j][i,j] is the index interval of HH, one has:

  • either there is a dominated splitting E<FE\oplus_{{}_{<}}F (i.e., FF dominates EE) with dim(E)=k\dim(E)=k,

  • or there is a hyperbolic transitive set ΛH\Lambda\subset H with s{\operatorname{s}}-index kk having a C1C^{1}-robust homoclinic tangency.

When we are interested only in the existence of robust homoclinic tangencies, without paying attention to the index of the hyperbolic set involved in their generation, there is the following reformulation:

Corollary 3.

There is a residual subset 𝒢{\cal G} of Diff 1(M)\,\mbox{{\rm Diff\,}}^{1}(M) such that for every diffeomorphism f𝒢f\in{\cal G} and every homoclinic class H(P,f)H(P,f) of ff with index interval [i,j][i,j], j>ij>i,

  • either H(P,f)H(P,f) has a dominated splitting

    TH(P,f)M=Ecs<E1<<Ej<Ecu,T_{H(P,f)}M=E^{\operatorname{cs}}\oplus_{{}_{<}}E_{1}\oplus_{{}_{<}}\cdots\oplus_{{}_{<}}E_{j}\oplus_{{}_{<}}E^{\operatorname{cu}},

    where dim(Ecs)=i\dim(E^{\operatorname{cs}})=i and E1,,EjE_{1},\dots,E_{j} are one-dimensional,

  • or the homoclinic class H(P,f)H(P,f) contains a transitive hyperbolic set with a robust homoclinic tangency.

In the first case of Corollary 3, we say that H(P,f)H(P,f) has an indices adapted dominated splitting.

The previous results have an interesting formulation for tame diffeomorphisms, i.e., the C1C^{1}-open set 𝒯(M){\cal T}(M) of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) of diffeomorphisms having finitely many chain recurrence classes (see Definition 2.3) in a robust way. We define 𝒲(M)=defDiff 1(M)𝒯(M)¯{\cal W}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\mbox{{\rm Diff\,}}^{1}(M)\setminus\overline{{\cal T}(M)} as the set of wild diffeomorphisms. Let us observe that, for an open and dense subset of 𝒯(M){\cal T}(M), a chain recurrence class is either hyperbolic or has index variation, see [2].

Given a chain recurrence class CC of ff we first consider the finest dominated splitting over CC (i.e., the bundles of this splitting can not be decomposed in a dominated way). Then we let EsE^{\operatorname{s}} (resp. EuE^{\operatorname{u}}) be the sum of the uniformly contracting (resp. expanding) bundles of this splitting (these bundles may be trivial, see [14]). The bundles E1,,EkE_{1},\dots,E_{k} are the remaining non-hyperbolic bundles of the finest dominated splitting of CC. In this way, we get a dominated splitting over CC

TCM=Es<E1<<Ek<Eu,T_{C}M=E^{\operatorname{s}}\oplus_{{}_{<}}E_{1}\oplus_{{}_{<}}\cdots\oplus_{{}_{<}}E_{k}\oplus_{{}_{<}}E^{\operatorname{u}},

where EsE^{\operatorname{s}} and EuE^{\operatorname{u}} are uniformly contracting and expanding, and E1,,EkE_{1},\dots,E_{k} are indecomposable and non-hyperbolic. We call this splitting the finest central dominated splitting of the chain recurrence CC.

Remark 1.3.

Let ff be any tame diffeomorphisms and H(P,f)H(P,f) any homoclinic class of ff which is far from robust homoclinic tangencies. Then the finest central dominated splitting of H(P,f)H(P,f) is indices adapted. For tame diffeomorphisms, the corollary below gives a more precise description of the relation between the finest central dominated splitting and the robust homoclinic tangencies associated to a homoclinic class.

Corollary 4.

There is a C1C^{1}-open and dense subset 𝒪{\cal O} of the set 𝒯(M){\cal T}(M) of tame diffeomorphisms such that, for every ff in 𝒪{\cal O} and every chain recurrence class CC of ff whose finest central dominated splitting is

TCM=Es<E1<<Ek<Eu,T_{C}M=E^{\operatorname{s}}\oplus_{{}_{<}}E_{1}\oplus_{{}_{<}}\cdots\oplus_{{}_{<}}E_{k}\oplus_{{}_{<}}E^{\operatorname{u}},

then, for every i=1,,ki=1,\dots,k,

dim(Ei)>1{for all j{1,,dim(Ei)1},there is a transitive hyperbolic set K of s-indexinds(K)=dim(EsE1Ei1)+jhaving a C1-robust homoclinic tangency.\dim(E_{i})>1\Longleftrightarrow\left\{\begin{array}[]{ll}&\mbox{for all $j\in\{1,\dots,\dim(E_{i})-1\}$,}\\ &\mbox{there is a transitive hyperbolic set $K$ of ${\operatorname{s}}$-index}\\ &{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(K)=\dim\left(E^{\operatorname{s}}\oplus E_{1}\oplus\cdots\oplus E_{i-1}\right)+j\\ &\mbox{having a $C^{1}$-robust homoclinic tangency.}\end{array}\right.
Remark 1.4.

  1. 1.

    Under the hypotheses of Corollary 4, [9, Theorem 1.14] implies that (choosing appropriately the open and dense subset 𝒪{\cal O} of 𝒯(M){\cal T}(M)) the hyperbolic set KK with a C1C^{1}-robust homoclinic tangency is also involved in a C1C^{1}-robust heterodimensional cycle.

  2. 2.

    Corollary 4 can also be stated for isolated chain recurrence classes of C1C^{1}-generic diffeomorphisms 333By C1C^{1}-generic diffeomorphisms we mean diffeomorphisms in a residual subset of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M)..

This article proceed a program for studying the generation of robust cycles (homoclinic tangencies and heterodimensional cycles) in the C1C^{1}-topology. In [9] we proved that homoclinic classes containing periodic points with different indices generate (by arbitrarily small C1C^{1}-perturbations) C1C^{1}-robust heterodimensional cycles. Here we show that these robust heterodimensional cycles generate blender-horseshoes, a sort of hyperbolic basic sets with geometrical properties resembling the thick horseshoes, see Section 3.2 and Theorem 6.4. We next see that, in the context of critical dynamics (some suitable non-domination property), blender-horseshoes yield C1C^{1}-robust tangencies, see Theorem 2. In fact, the definition and construction of blender-horseshoes (a special class of cu{\operatorname{cu}}-blenders defined in [8]) and Theorem 2 are the technical heart of our arguments and the main novelty of this paper.

The results in this paper and the ones in [9] support the following conjecture:

Conjecture 1 (Bonatti, [6]).

Every C1C^{1}-diffeomorphism can be C1C^{1}-approximated either by a hyperbolic diffeomorphism (Axiom A and no-cycle property) or by a diffeomorphism exhibiting a C1C^{1}-robust cycle (homoclinic tangency or heterodimensional cycle).

This conjecture is a stronger version of the denseness conjecture by Palis in [23] (dichotomy hyperbolicity versus approximation by diffeomorphisms with homoclinic bifurcations). The novelty here is that the conjecture considers two disjoint open sets whose union is dense in the whole set of C1C^{1}-diffeomorphisms: the hyperbolic ones and those with robust cycles. In the setting of tame diffeomorphisms, a strong version of Conjecture 1 was proved in [9, Theorem 1.14]: every tame diffeomorphism can be C1C^{1}-approximated either by hyperbolic diffeomorphisms or by diffeomorphisms exhibiting robust heterodimensional cycles. Recall that Palis conjecture for surface C1C^{1}-diffeomorphisms was proved in [26] (due to dimension deficiency, for surface diffeomorphisms the conjecture only involves homoclinic tangencies).

1.3 Newhouse domains

Following [19], we say that an open set 𝒩{\cal N} of Diff r(M)\mbox{{\rm Diff\,}}^{r}(M) is a CrC^{r}-Newhouse domain if there is a dense subset 𝒟{\cal D} of 𝒩{\cal N} such that every g𝒟g\in{\cal D} has a homoclinic tangency (associated to some saddle). A preliminary step toward Conjecture 1 is the following question.

Question 1.

Let MM be a closed manifold and 𝒩{\cal N} be a C1C^{1}-Newhouse domain of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M). Are the diffeomorphisms having C1C^{1}-robust homoclinic tangencies dense in 𝒩{\cal N}?

If it is not possible to answer positively this question in its full generality, it would be interesting to provide sufficient conditions for a C1C^{1}-Newhouse domain to contain an open and dense subset of diffeomorphisms with C1C^{1}-robust homoclinic tangencies. If the dimension of the ambient manifold is at least three, one may also ask about the interplay between robust homoclinic tangencies and robust heterodimensional cycles.

We now discuss briefly Question 1. Before going to our setting, lets us review the discussion in [1] about this question for C1C^{1}-surface diffeomorphisms. Let Hyp1(M)\textrm{Hyp}^{1}(M) denote the subset of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) consisting of Axiom A diffeomorphisms. By [26], for surface diffeomorphisms, the open set

𝒩1(M2)=defDiff1(M2)Hyp1(M2)¯{\cal N}^{1}(M^{2})\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\textrm{Diff}^{1}(M^{2})\setminus\overline{\textrm{Hyp}^{1}(M^{2})}

is a Newhouse domain. The set 𝒩1(M2){\cal N}^{1}(M^{2}) is the union of the closure of three pairwise disjoint open sets 𝒪1(M2),𝒪2(M2){\cal O}_{1}(M^{2}),{\cal O}_{2}(M^{2}), and 𝒪3(M2){\cal O}_{3}(M^{2}) defined as follows.

  • The set 𝒪1(M2){\cal O}_{1}(M^{2}) consists of diffeomorphisms having C1C^{1}-robust homoclinic tangencies.

  • There is a residual subset 2(M2){\cal R}_{2}(M^{2}) of 𝒪2(M2){\cal O}_{2}(M^{2}) such that every f2(M2)f\in{\cal R}_{2}(M^{2}) has a homoclinic class H(P,f)H(P,f) that robustly does not admit any dominated splitting. However, for every hyperbolic set Λ\Lambda contained in H(P,f)H(P,f) the invariant manifolds of Λ\Lambda meet transversely. In this case, we say that the diffeomorphism ff has a persistently fragile homoclinic tangency associated to PP.

  • There is a residual subset 3(M2){\cal R}_{3}(M^{2}) of 𝒪3(M2){\cal O}_{3}(M^{2}) such that for every diffeomorphism f3(M2)f\in{\cal R}_{3}(M^{2}) and every (hyperbolic) periodic point PP of ff the homoclinic class H(P,f)H(P,f) is hyperbolic. But there is a sequence of periodic points (Pn)n(P_{n})_{n} of ff such that the hyperbolic homoclinic classes H(Pn,f)H(P_{n},f) accumulate (Hausdorff limit) to an aperiodic class (i.e., a recurrence class without periodic points).

As mentions above, Moreira’s result in [17] provides strong evidences suggesting that 𝒪1(M2){\cal O}_{1}(M^{2}) is empty. On the other hand, we do not know if the sets 𝒪2(M2){\cal O}_{2}(M^{2}) and 𝒪3(M2){\cal O}_{3}(M^{2}) are empty or not. In fact, Smale density conjecture (hyperbolic diffeomorphisms are dense in Diff1(M2)\textrm{Diff}^{1}(M^{2})) is equivalent to prove that these three sets are empty.

We now explain how the discussion above is translated to higher dimensions. As before, we first consider non-hyperbolic diffeomorphisms, that is, the set Diff1(M)Hyp1(M)¯\textrm{Diff}^{1}(M)\setminus\overline{\textrm{Hyp}^{1}(M)}. If dim(M)3\dim(M)\geq 3 this set is not a Newhouse domain: it contains open sets of diffeomorphisms without homoclinic tangencies. Thus we consider the sets Tang1(M)\textrm{Tang}^{1}(M) of diffeomorphisms having a homoclinic tangency associated to a saddle and 𝒪0(M){\cal O}_{0}(M) of non-hyperbolic diffeomorphisms far from homoclinic tangencies,

𝒪0(M)=defDiff 1(M)(Tang1(M)Hyp1(M))¯.{\cal O}_{0}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\mbox{{\rm Diff\,}}^{1}(M)\setminus\overline{(\textrm{Tang}^{1}(M)\cup\textrm{Hyp}^{1}(M))}.

Note that this set is not-empty and it is an open question whether it is contained in the set of tame diffeomorphisms (in fact, the first author conjectured that 𝒪0(M){\cal O}_{0}(M) consists of tame diffeomorphisms, [6]). The diffeomorphisms in 𝒪0(M){\cal O}_{0}(M) were studied in several papers, let us just refer to [31, 32, 33].

From now on, we will focus on the set

𝒩1(M)=defDiff 1(M)(𝒪0(M)Hyp1(M))¯.{\cal N}^{1}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\mbox{{\rm Diff\,}}^{1}(M)\setminus\overline{\left({\cal O}_{0}(M)\cup\textrm{Hyp}^{1}(M)\right)}.

By definition, this set is a Newhouse domain. As in the case of surface diffeomorphisms, we split the set 𝒩1(M){\cal N}^{1}(M) into three closed sets with pairwise disjoint interiors. We first define the set 𝒪1(M){\cal O}_{1}(M) similarly as the set 𝒪1(M2){\cal O}_{1}(M^{2}),

𝒪1(M)=def{fDiff 1(M) with a transitive hyperbolic set with a robust homoclinic tangency}.{\cal O}_{1}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\{\mbox{$f\in\mbox{{\rm Diff\,}}^{1}(M)$ with a transitive hyperbolic set with a robust homoclinic tangency}\}.

The results in this paper implies that 𝒪1(M){\cal O}_{1}(M) is non-empty, see also [4, 28].

We define the set 𝒪2(M){\cal O}_{2}(M) by

𝒪2(M)=def{f(Diff 1(M)𝒪1(M)¯) with a persistently fragile homoclinic tangency}.{\cal O}_{2}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\{f\in(\mbox{{\rm Diff\,}}^{1}(M)\setminus\overline{{\cal O}_{1}(M)})\mbox{\,with a persistently fragile homoclinic tangency}\}.

Consider the residual set 𝒢{\cal G} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) in Corollary 3. Then if ff is a diffeomorphism in 𝒢𝒪2(M){\cal G}\cap{\cal O}_{2}(M) with a persistently fragile homoclinic tangency associated to PP then the homoclinic class H(P,f)H(P,f) has no index variation (otherwise one gets robust homoclinic tangencies).

Finally, define 𝒪3(M){\cal O}_{3}(M) by

𝒪3(M)=def(Diff 1(M)Hyp1(M)𝒪0(M)𝒪1(M)𝒪2(M)¯).{\cal O}_{3}(M)\stackrel{{\scriptstyle\scriptscriptstyle\rm def}}{{=}}\left(\mbox{{\rm Diff\,}}^{1}(M)\setminus\overline{\textrm{Hyp}^{1}(M)\cup{\cal O}_{0}(M)\cup{\cal O}_{1}(M)\cup{\cal O}_{2}(M)}\right).

Corollary 3 implies that if f𝒢𝒪3(M)f\in{\cal G}\cap{\cal O}_{3}(M) then every homoclinic class of ff has an indices adapted dominated splitting. The description of the accumulation of homoclinic classes of diffeomorphisms in 𝒪3(M){\cal O}_{3}(M) is a subtle issue. For instance, by shrinking 𝒢{\cal G}, for diffeomorphisms f𝒢𝒪3(M)f\in{\cal G}\cap{\cal O}_{3}(M), there are kk and a sequence of saddles PnP_{n} of index kk such that every H(Pn,f)H(P_{n},f) has a dominated splitting E<FE\oplus_{{{}_{<}}}F with dim(E)=k\dim(E)=k and the sequence of homoclinic classes H(Pn,f)H(P_{n},f) accumulates to a set Λ\Lambda that does not admit a dominated splitting E<FE\oplus_{{{}_{<}}}F with dim(E)=k\dim(E)=k (the set Λ\Lambda is the Hausdorff limit of the sequence (H(Pn,f))(H(P_{n},f))).

We observe that, as a consequence of Corollary 4, there is an open and dense subset of 𝒪2(M)𝒪3(M){\cal O}_{2}(M)\cup{\cal O}_{3}(M) consisting of wild diffeomorphisms. Note that we do not known if the sets 𝒪2(M){\cal O}_{2}(M) and 𝒪3(M){\cal O}_{3}(M) are empty or not.

Summarizing, as in the case of surface diffeomorphisms, we have that the Newhouse domain 𝒩1(M){\cal N}^{1}(M) is the closure of the union of the pairwise disjoint open sets 𝒪1(M),𝒪2(M){\cal O}_{1}(M),{\cal O}_{2}(M), and 𝒪3(M){\cal O}_{3}(M).

This paper is organized as follows. In Section 2, we recall some definitions and state some notations we will use throughout the paper. In Section 3, we review the notion of cu{\operatorname{cu}}-blender in [8] and present the notion of blender-horseshoe, a key ingredient of our constructions. In Section 4, we introduce a class of sub-manifolds, called folding manifolds relative to a blender-horseshoe Λ\Lambda. The main result is that folding manifolds and the local stable manifold of the blender-horseshoe Λ\Lambda have C1C^{1}-robust tangencies, see Theorem 2. Using this result, we state a sufficient condition for the generation of robust homoclinic tangencies by homoclinic tangencies associated to hyperbolic sets. In Section 5, we see that strong homoclinic intersections of non-hyperbolic periodic points (i.e., intersections between the strong stable and unstable manifolds) generate blender-horseshoes. We also see that such strong intersections naturally occur in the non-hyperbolic setting. Finally, in Section 6 we conclude the proof of Theorem 1. We also state a result about the occurrence of robust heterodimensional cycles inside non-hyperbolic chain recurrence classes, see Theorem 3, which is an extension of [9, Theorem 1.16].

2 Definitions and notations

In this section, we define precisely the notions involved in this paper and state some notations.

Given a closed manifold MM, we denote by Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) the space of C1C^{1}-diffeomorphisms endowed with the usual uniform topology.

A diffeomorphism ff has a homoclinic tangency associated to a (hyperbolic) saddle RR if the unstable manifold Wu(R,f)W^{\operatorname{u}}(R,f) and the stable manifold Ws(R,f)W^{\operatorname{s}}(R,f) of the orbit of RR have some non-transverse intersection.

The s{\operatorname{s}}-index (resp. u{\operatorname{u}}-index) of a hyperbolic periodic point RR, denoted by inds(R){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(R) (resp. indu(R){\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(R)), is the dimension of the stable bundle EsE^{\operatorname{s}} (resp. dimension of EuE^{\operatorname{u}}) of RR. We similarly define the s{\operatorname{s}}-index and u{\operatorname{u}}-index of a transitive hyperbolic set Λ\Lambda, denoted by inds(Λ){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(\Lambda) and indu(Λ){\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Lambda), respectively.

A heterodimensional cycle of a diffeomorphism ff consists of two hyperbolic saddles PP and QQ of ff of different s{\operatorname{s}}-indices and two heteroclinic points XWu(P,f)Ws(Q,f)X\in W^{\operatorname{u}}(P,f)\cap W^{\operatorname{s}}(Q,f) and YWs(P,f)Wu(Q,f)Y\in W^{\operatorname{s}}(P,f)\cap W^{\operatorname{u}}(Q,f). In this case, we say that the cycle is associated to PP and QQ. Note that (due to insufficient dimensions) at least one of these intersections is not transverse. The heterodimensional cycle has co-index kk if |inds(Q)inds(P)|=k|{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)-{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)|=k (note that k1k\geq 1).

Definition 2.1 (Homoclinic class).

Consider a diffeomorphism ff and a saddle PP of ff. The homoclinic class of PP, denoted by H(P,f)H(P,f), is the closure of the transverse intersections of the stable and unstable manifolds of the orbit of PP.

Remark 2.2.

The homoclinic class H(P,f)H(P,f) can be alternatively defined as the closure of the saddles QQ homoclinically related with PP: the stable manifold of the orbit of QQ transversely meets the unstable manifold of the orbit of PP and vice-versa. Although all saddles homoclinically related with PP have the same s{\operatorname{s}}-index as PP, the homoclinic class H(P,f)H(P,f) may contain periodic orbits of different s{\operatorname{s}}-index as the one of PP (i.e., there are homoclinic classes having index variation). Finally, a homoclinic class is a transitive set with dense periodic points.

Definition 2.3 (Chain recurrence class).

A point xx is chain recurrent if for every ε>0\varepsilon>0 there are ε\varepsilon-pseudo orbits starting and ending at xx. The chain recurrence class of xx for ff, denoted by C(x,f)C(x,f), is the set of points yy such that, for every ε>0\varepsilon>0, there are ε\varepsilon-pseudo orbits starting at xx, passing ε\varepsilon-close to yy and ending at xx.

According to [7], for C1C^{1}-generic diffeomorphisms, the chain recurrence class of any periodic point is its homoclinic class.

Definition 2.4 (Dominated splitting).

Consider a diffeomorphism ff and a compact ff-invariant set Λ\Lambda. A DfDf-invariant splitting TΛM=EFT_{\Lambda}M=E\oplus F over Λ\Lambda is dominated if the fibers ExE_{x} and FxF_{x} of EE and FF have constant dimension and there exists kk\in{\mathbb{N}} such that

Dxfk(u)Dxfk(w)<12,\frac{||D_{x}f^{k}(u)||}{||D_{x}f^{k}(w)||}<\frac{1}{2},

for every xΛx\in\Lambda and every pair of unitary vectors uExu\in E_{x} and wFxw\in F_{x}.

This definition means that vectors in the bundle FF are uniformly more expanded than vectors in EE by the derivative DfkDf^{k}. If it occurs, we say that FF dominates EE and write E<FE\oplus_{{}_{<}}F.

Remark 2.5.

In some cases, one needs to consider splittings with more than two bundles. A DfDf-invariant splitting E1E2EkE_{1}\oplus E_{2}\oplus\cdots\oplus E_{k} over a set Λ\Lambda is dominated if for all j{1,,k1}j\in\{1,\dots,k-1\} the splitting E1jEj+1kE_{1}^{j}\oplus E_{j+1}^{k} is dominated, where Eir=EiErE_{i}^{r}=E_{i}\oplus\cdots\oplus E_{r}, i<ri<r.

We use the notation E1<E2<<EkE_{1}\oplus_{{}_{<}}E_{2}\oplus_{{}_{<}}\cdots\oplus_{{}_{<}}E_{k}, meaning that Ei+1E_{i+1} dominates EiE_{i}, or equivalently that E1j<Ej+1kE_{1}^{j}\oplus_{{}_{<}}E_{j+1}^{k}.

As mentioned before, the main goal of this paper is to construct hyperbolic sets exhibiting homoclinic tangencies in a robust way. We need the following definition.

Definition 2.6 (Robust tangency).

Given a diffeomorphism f:MMf\colon M\to M, a hyperbolic set Γ\Gamma of ff with a hyperbolic splitting EsEuE^{\operatorname{s}}\oplus E^{\operatorname{u}}, and a submanifold NMN\subset M with dimension dim(N)=dim(Eu)\dim(N)=\dim(E^{\operatorname{u}}), we say that the stable manifold Ws(Γ)W^{\operatorname{s}}(\Gamma) of Γ\Gamma and the submanifold NN have a C1C^{1}-robust tangency if for every diffeomorphism gg C1C^{1} close to ff and every submanifold NgN_{g} C1C^{1}-close to NN, the stable manifold Ws(Γg)W^{\operatorname{s}}(\Gamma_{g}) of Γg\Gamma_{g} has some non-transverse intersection with NgN_{g}.

We are specially interested in the case where NN is the unstable manifold Wu(P)W^{\operatorname{u}}(P) of a periodic point PP of a non-trivial hyperbolic set Γ\Gamma and Ng=Wu(Pg)N_{g}=W^{\operatorname{u}}(P_{g}). In that case, one gets C1C^{1}-robust homoclinic tangencies (associated to Γ\Gamma), recall Definition 1.1.


Standing notation: Throughout this paper we use the following notation:

  • Given a diffeomorphism ff and a hyperbolic set Λf\Lambda_{f} of ff there is a C1C^{1}-neighborhood 𝒰{\cal U} of ff such that every g𝒰g\in{\cal U} has a hyperbolic set Λg\Lambda_{g} called the continuation of Λf\Lambda_{f}. The set Λg\Lambda_{g} is close to Λf\Lambda_{f} and the restrictions of ff to Λf\Lambda_{f} and of gg to Λg\Lambda_{g} are conjugate. If PfP_{f} a hyperbolic periodic point, we denote by PgP_{g} the continuation of PfP_{f} for gg close to ff.

  • Given a periodic point PP of ff we denote by π(P)\pi(P) its period.

  • The perturbations we consider are always arbitrarily small. Thus the sentence there is a CrC^{r}-perturbation gg of ff means there is gg arbitrarily CrC^{r}-close to ff.

3 Blender-horseshoes

In this section, we introduce precisely the definition of a blender-horseshoe, a particular case of the blenders in [8]. In fact, blender-horseshoes are the main ingredient of this paper and the key tool for getting robust homoclinic tangencies. We beging by reviewing the notion of a blender.

3.1 Blenders

The notion of a cu{\operatorname{cu}}-blender was introduced in [8] as a class of examples, without a precise and formal definition. Blenders were used to get C1C^{1}-robust transitivity, [8], and robust heterodimensional cycles, [9]. The relevance of blenders comes from their internal geometry and not from their dynamics: a cu{\operatorname{cu}}-blender is a (uniformly) hyperbolic transitive set whose stable set robustly has Hausdorff dimension greater than its stable bundle. In some sense, this property resembles and plays a similar role as the thick horseshoes introduced by Newhouse, [21]. Following [13, Definition 6.11], we now give a tentative formal definition of a cu{\operatorname{cu}}-blender:

Definition 3.1 (cu{\operatorname{cu}}-blender).

Let f:MMf\colon M\to M be a diffeomorphism. A transitive hyperbolic set Γ\Gamma of ff with indu(Γ)=k2{\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Gamma)=k\geq 2 is a cu{\operatorname{cu}}-blender if there are a C1C^{1}-neighborhood 𝒰{\cal U} of ff and a C1C^{1}-open set 𝒟{\cal D} of embeddings of (k1)(k-1)-dimensional disks DD into MM such that, for every diffeomorphism g𝒰g\in{\cal U}, every disk D𝒟D\in{\cal D} intersects the local stable manifold Wlocs(Γg)W^{s}_{{\operatorname{loc}}}(\Gamma_{g}) of the continuation Γg\Gamma_{g} of Γ\Gamma for gg. The set 𝒟{\cal D} is called the superposition region of the blender.

By definition, the property of a diffeomorphism having a cu{\operatorname{cu}}-blender is a C1C^{1}-robust property.

We do not know whether cu{\operatorname{cu}}-blenders yield robust tangencies in the sense of Definition 2.6. This leads to the following questions:

Question 2.

Let f:MMf\colon M\to M be a diffeomorphism having a cu{\operatorname{cu}}-blender Γ\Gamma with k=indu(Γ)k={\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Gamma).

  • Does it exist a submanifold NMN\subset M with dim(N)=k\dim(N)=k such that that Ws(Γ)W^{s}(\Gamma) and NN have a robust tangency?

  • Suppose that a submanifold LL of dimension kk and Ws(Γ)W^{s}(\Gamma) have a tangency. Does this tangency yield robust tangencies? More precisely, does there exist an open set 𝒰{\cal U} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M), ff in the closure of 𝒰{\cal U}, of diffeomorphisms gg with robust tangencies associated to Γg\Gamma_{g} and “continuations” of LL?

We note that, even for the first cu{\operatorname{cu}}-blenders constructed in [8, Section 1], these questions remain open. We will give a partial answer to this question in Theorem 2. For that we will introduce a special class of cu{\operatorname{cu}}-blenders, conjugate to the usual Smale horseshoe, that we call blender-horseshoes.

3.2 Blender-horseshoes

In this section, we give the precise definition of a blender-horseshoe. This definition involves several concepts as invariant cone-fields, hyperbolicity, partial hyperbolicity, and Markov partitions, which we will present separately. Our presentation follows closely [8, Section 1], thus some details of our construction are just sketched.

3.2.1 Cone-fields

Consider n=su{\mathbb{R}}^{n}={\mathbb{R}}^{s}\oplus{\mathbb{R}}\oplus{\mathbb{R}}^{u}, where s>0,u>0s>0,u>0, and n=s+u+1n=s+u+1. For α(0,1)\alpha\in(0,1), denote by 𝒞αs{\cal C}^{{\operatorname{s}}}_{\alpha}, 𝒞αu{\cal C}^{{\operatorname{u}}}_{\alpha}, and 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha} the following cone-fields:

𝒞αs(x)={v=(vs,vc,vu)su=TxM:vc+vuαvs},𝒞αu(x)={v=(vs,vc,vu)su=TxM:vsαvc+vu},𝒞αuu(x)={v=(vs,vc,vu)su=TxM:vs+vcαvu}.\begin{array}[]{ll}{\cal C}^{{\operatorname{s}}}_{\alpha}(x)&=\{v=(v^{s},v^{c},v^{u})\in{\mathbb{R}}^{s}\oplus{\mathbb{R}}\oplus{\mathbb{R}}^{u}=T_{x}M\quad\colon\quad\|v^{c}+v^{u}\|\leq\alpha\,\|v^{s}\|\},\\ {\cal C}^{{\operatorname{u}}}_{\alpha}(x)&=\{v=(v^{s},v^{c},v^{u})\in{\mathbb{R}}^{s}\oplus{\mathbb{R}}\oplus{\mathbb{R}}^{u}=T_{x}M\quad\colon\quad\|v^{s}\|\leq\alpha\,\|v^{c}+v^{u}\|\},\\ {\cal C}^{{\operatorname{uu}}}_{\alpha}(x)&=\{v=(v^{s},v^{c},v^{u})\in{\mathbb{R}}^{s}\oplus{\mathbb{R}}\oplus{\mathbb{R}}^{u}=T_{x}M\quad\colon\quad\|v^{s}+v^{c}\|\leq\alpha\,\|v^{u}\|\}.\end{array}

As α(0,1)\alpha\in(0,1), one gets that 𝒞αs{\cal C}^{{\operatorname{s}}}_{\alpha} is transverse to 𝒞αu{\cal C}_{\alpha}^{{\operatorname{u}}}, that is, 𝒞αs(x)𝒞αu(x)=0xTxM{\cal C}_{\alpha}^{{\operatorname{s}}}(x)\cap{\cal C}_{\alpha}^{{\operatorname{u}}}(x)=0_{x}\in T_{x}M. Moreover, 𝒞αuu(x)𝒞αuu(x){\cal C}_{\alpha}^{{\operatorname{uu}}}(x)\subset{\cal C}_{\alpha}^{{\operatorname{uu}}}(x) for all xx.

Consider the cube

=[1,1]n=[1,1]s×[1,1]×[1,1]u.{\mathbb{C}}=[-1,1]^{n}=[-1,1]^{s}\times[-1,1]\times[-1,1]^{u}.

We split the boundary of {\mathbb{C}} into three parts:

s=([1,1]s)×[1,1]×[1,1]u,c=[1,1]s×{1,1}×[1,1]u,anduu=[1,1]s×[1,1]×([1,1]u).\begin{array}[]{ll}\partial^{\operatorname{s}}{\mathbb{C}}&=\partial\big{(}[-1,1]^{s}\big{)}\times[-1,1]\times[-1,1]^{u},\\ \partial^{\operatorname{c}}{\mathbb{C}}&=[-1,1]^{s}\times\{-1,1\}\times[-1,1]^{u},\quad\mbox{and}\\ \partial^{\operatorname{uu}}{\mathbb{C}}&=[-1,1]^{s}\times[-1,1]\times\partial\big{(}[-1,1]^{u}\big{)}.\end{array}

We also consider

u=[1,1]s×([1,1]×[1,1]u)=cuu.\partial^{\operatorname{u}}{\mathbb{C}}=[-1,1]^{s}\times\partial\big{(}[-1,1]\times[-1,1]^{u}\big{)}=\partial^{c}{\mathbb{C}}\cup\partial^{\operatorname{uu}}{\mathbb{C}}.

We now consider a local diffeomorphism f:nf\colon{\mathbb{C}}\to{\mathbb{R}}^{n} and formulate conditions BH1)BH6) for the maximal invariant set Λ\Lambda of ff in the cube {\mathbb{C}},

Λ=ifi(),\Lambda=\bigcap_{i\in{\mathbb{Z}}}f^{i}({\mathbb{C}}),

to be a blender-horseshoe, see Definition 3.8.

BH1) The intersection f()(s××[1,1]u)f({\mathbb{C}})\cap({\mathbb{R}}^{s}\times{\mathbb{R}}\times[-1,1]^{u}) consists of two connected components, denoted f(𝒜)f({\cal A}) and f()f({\cal B}). Furthermore,

f(𝒜)f()(1,1)s××[1,1]u, and f({\cal A})\cup f({\cal B})\subset(-1,1)^{s}\times{\mathbb{R}}\times[-1,1]^{u},\mbox{ and }
(𝒜)uu()=.({\cal A}\cup{\cal B})\cap\partial^{\operatorname{uu}}({\mathbb{C}})=\emptyset.

We denote f𝒜:𝒜f(𝒜)f_{{}_{\cal A}}\colon{\cal A}\to f({\cal A}) and f:f()f_{{}_{\cal B}}\colon{\cal B}\to f({\cal B}) the restrictions of ff to 𝒜{\cal A} and {\cal B}, respectively. See Figure 1.

\psfrag{C}{${\mathbb{C}}$}\psfrag{Ru}{${\mathbb{R}}^{u}$}\psfrag{B}{${\cal B}$}\psfrag{A}{${\cal A}$}\psfrag{Rc}{${\mathbb{R}}$}\psfrag{dC}{$\partial^{\operatorname{uu}}{\mathbb{C}}$}\includegraphics[height=115.63243pt]{bh1.eps}
Figure 1: Projection in u{\mathbb{R}}\oplus{\mathbb{R}}^{u} of a blender horseshoe. Condition BH1).

BH2) Cone-fields: The cone-field 𝒞αs{\cal C}_{\alpha}^{\operatorname{s}} is strictly Df1Df^{-1}-invariant and the cone-fields 𝒞αu{\cal C}^{{\operatorname{u}}}_{\alpha} and 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha} are strictly DfDf-invariant. More precisely, there is 0<α<α0<\alpha^{\prime}<\alpha such that, for every xf(𝒜)f()x\in f({\cal A})\cup f({\cal B}) one has

Df1(𝒞αs(x))𝒞αs(f1x).Df^{-1}({\cal C}^{\operatorname{s}}_{\alpha}(x))\subset{\cal C}^{{\operatorname{s}}}_{\alpha^{\prime}}(f^{-1}x).

In the same way, for every x𝒜x\in{\cal A}\cup{\cal B}, one has

Df(𝒞αuu(x))𝒞αuu(f(x))andDf(𝒞αu(x))𝒞αu(f(x)).Df({\cal C}^{\operatorname{uu}}_{\alpha}(x))\subset{\cal C}^{{\operatorname{uu}}}_{\alpha^{\prime}}(f(x))\quad\mbox{and}\quad Df({\cal C}^{\operatorname{u}}_{\alpha}(x))\subset{\cal C}^{{\operatorname{u}}}_{\alpha^{\prime}}(f(x)).

Moreover, the cone-fields 𝒞αu{\cal C}^{\operatorname{u}}_{\alpha} and 𝒞αs{\cal C}^{\operatorname{s}}_{\alpha} are uniformly expanding and contracting, respectively.

Note that that property BH2) is open: by increasing slightly α<α\alpha^{\prime}<\alpha, it holds for every diffeomorphism gg in a C1C^{1} neighborhood of ff.

Since f(uu)f(\partial^{\operatorname{uu}}{\mathbb{C}}) is disjoint from s+1×[1,1]u{\mathbb{R}}^{s+1}\times[-1,1]^{u} and f(𝒜)f()(1,1)s××[1,1]uf({\cal A})\cup f({\cal B})\subset(-1,1)^{s}\times{\mathbb{R}}\times[-1,1]^{u}, from condition BH1) one has that

f(())([1,1]s××[1,1]u)f(sc).f(\partial({\mathbb{C}}))\cap\partial([-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u})\subset f(\partial^{\operatorname{s}}{\mathbb{C}}\cup\partial^{\operatorname{c}}{\mathbb{C}}).

Furthermore, this is a C1C^{1}-robust property.

By BH2), the components of f(())([1,1]s××[1,1]u)f(\partial({\mathbb{C}}))\cap\partial([-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u}) are foliated by disks Δ\Delta tangent to 𝒞αuu{\cal C}_{\alpha}^{\operatorname{uu}}, i.e., TxΔ𝒞αuu(x)T_{x}\Delta\subset{\cal C}^{\operatorname{uu}}_{\alpha}(x). Hence these disks are transverse to ([1,1]s××[1,1]u)\partial([-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u}). As a consequence, one gets the following:

Remark 3.2.

Under the (C1C^{1}-robust) hypothesis BH2), hypothesis BH1) is also a C1C^{1}-robust property.

Remark 3.3 (Hyperbolicity).

Consider the maximal invariant set Λ\Lambda of ff in {\mathbb{C}}

Λ=ifi().\Lambda=\bigcap_{i\in{\mathbb{Z}}}f^{i}({\mathbb{C}}).

By BH1) and BH2) the set Λ\Lambda is compact and satisfies

Λint(𝒜)int().\Lambda\subset\mbox{\rm int}({\cal A}\cup{\cal B})\subset\mbox{\rm int}({\mathbb{C}}).

Moreover, the set Λ\Lambda has a dominated splitting TΛM=E<F<FT_{\Lambda}M=E\oplus_{{}_{<}}F\oplus_{{}_{<}}F, where E𝒞sE\subset{\cal C}^{\operatorname{s}}, FG𝒞uF\oplus G\subset{\cal C}^{\operatorname{u}}, and G𝒞uuG\subset{\cal C}^{{\operatorname{uu}}}, and FF is one-dimensional.

By BH2), the set Λ\Lambda has a hyperbolic splitting EsEuE^{\operatorname{s}}\oplus E^{\operatorname{u}}, where Es=EE^{\operatorname{s}}=E and Eu=FGE^{\operatorname{u}}=F\oplus G and dim(Es)=s\dim(E^{\operatorname{s}})=s and dim(Eu)=u+1\dim(E^{\operatorname{u}})=u+1. Furthermore, the set Λ\Lambda also has a partially hyperbolic splitting

TΛM=Es<Ecu<EuuT_{\Lambda}M=E^{\operatorname{s}}\oplus_{{}_{<}}E^{{\operatorname{cu}}}\oplus_{{}_{<}}E^{{\operatorname{uu}}}

with three non-trivial directions, where Ecu=FE^{{\operatorname{cu}}}=F and Euu=GE^{{\operatorname{uu}}}=G and dim(Euu)=u\dim(E^{\operatorname{uu}})=u. Note that Eu=EcuEuuE^{\operatorname{u}}=E^{\operatorname{cu}}\oplus E^{\operatorname{uu}}. We say that EuuE^{\operatorname{uu}} is the strong unstable bundle of Λ\Lambda.

3.2.2 Markov partitions

Write

𝔸=f1(f(𝒜))and𝔹=f1(f()).{\mathbb{A}}=f^{-1}\left(f({\cal A})\cap{\mathbb{C}}\right)\quad\mbox{and}\quad{\mathbb{B}}=f^{-1}\left(f({\cal B})\cap{\mathbb{C}}\right).

BH3) Associated Markov partition:

  • The sets 𝔸{\mathbb{A}} and 𝔹{\mathbb{B}} are both non-empty and connected. That is, the sets 𝔸{\mathbb{A}} and 𝔹{\mathbb{B}} are the connected components of f1()f^{-1}({\mathbb{C}})\cap{\mathbb{C}}.

  • The sets 𝔸{\mathbb{A}} and 𝔹{\mathbb{B}} are horizontal sub-cubes of {\mathbb{C}} and their images f(𝔸)f({\mathbb{A}}) and f(𝔹)f({\mathbb{B}}) are vertical sub-cubes of {\mathbb{C}}. More precisely,

    f(𝔸)f(𝔹)(1,1)s×[1,1]×[1,1]u, andf({\mathbb{A}})\cup f({\mathbb{B}})\subset(-1,1)^{s}\times[-1,1]\times[-1,1]^{u},\mbox{ and}
    𝔸𝔹[1,1]s×(1,1)×(1,1)u.{\mathbb{A}}\cup{\mathbb{B}}\subset[-1,1]^{s}\times(-1,1)\times(-1,1)^{u}.

    In other words, f(𝔸)f(𝔹)f({\mathbb{A}})\cup f({\mathbb{B}}) is disjoint from s\partial^{\operatorname{s}}{\mathbb{C}} and 𝔸𝔹{\mathbb{A}}\cup{\mathbb{B}} is disjoint from u\partial^{\operatorname{u}}{\mathbb{C}}.

As a consequence of BH2) and BH3), one gets that {𝔸,𝔹}\{{\mathbb{A}},{\mathbb{B}}\} is a Markov partition generating Λ\Lambda. Therefore the dynamics of ff in Λ\Lambda is conjugate to the full shift of two symbols. In particular, the hyperbolic set Λ\Lambda contains exactly two fixed points of ff, P𝔸P\in{\mathbb{A}} and Q𝔹Q\in{\mathbb{B}}. See Figure 2.

\psfrag{C}{${\mathbb{C}}$}\psfrag{b}{${\mathbb{B}}$}\psfrag{B}{${\cal B}$}\psfrag{A}{${\cal A}$}\psfrag{a}{${\mathbb{A}}$}\includegraphics[height=115.63243pt]{bh4.eps}
Figure 2: Projection in ×u{\mathbb{R}}\times{\mathbb{R}}^{u}. BH3) Markov partition of a blender-horseshoe.

3.2.3 uu{\operatorname{uu}}-disks and their iterates

Definition 3.4 (s{\operatorname{s}}- and uu{\operatorname{uu}}-disks).

A disk Δ\Delta of dimension ss contained in {\mathbb{C}} is an s{\operatorname{s}}-disk if

  • it is tangent to 𝒞αs{\cal C}_{\alpha}^{\operatorname{s}}, i.e., TxΔ𝒞αs(x)T_{x}\Delta\subset{\cal C}_{\alpha}^{\operatorname{s}}(x) for all xΔx\in\Delta, and

  • its boundary Δ\partial\Delta is contained in s()\partial^{\operatorname{s}}({\mathbb{C}}).

A disk Υs××[1,1]u\Upsilon\subset{\mathbb{R}}^{s}\times{\mathbb{R}}\times[-1,1]^{u} of dimension uu is a uu{\operatorname{uu}}-disk if

  • it is tangent to 𝒞αuu{\cal C}_{\alpha}^{\operatorname{uu}}, i.e. TxΥ𝒞αuu(x)T_{x}\Upsilon\subset{\cal C}_{\alpha}^{\operatorname{uu}}(x) for all xΥx\in\Upsilon, and

  • Υs××([1,1]u)\partial\Upsilon\subset{\mathbb{R}}^{s}\times{\mathbb{R}}\times\partial([-1,1]^{u}).

Given a point xΛx\in\Lambda, there is a unique ff-invariant manifold of dimension uu tangent at xx to the strong unstable bundle Euu(x)E^{\operatorname{uu}}(x), the strong unstable manifold Wuu(x)W^{{\operatorname{uu}}}(x) of xx. For points xΛx\in\Lambda, the local invariant manifolds Wlocs(x)W^{\operatorname{s}}_{\operatorname{loc}}(x), Wlocu(x)W^{{\operatorname{u}}}_{\operatorname{loc}}(x), and Wlocuu(x)W^{{\operatorname{uu}}}_{\operatorname{loc}}(x) are the connected components of the intersections Ws(x)W^{\operatorname{s}}(x)\cap{\mathbb{C}}, Wu(x)W^{{\operatorname{u}}}(x)\cap{\mathbb{C}}, and Wuu(x)W^{{\operatorname{uu}}}(x)\cap{\mathbb{C}} containing xx, respectively.

As a consequence of BH1)–BH3) one gets

Remark 3.5.

For every xΛx\in\Lambda, Wlocs(x)W^{\operatorname{s}}_{\operatorname{loc}}(x) is an s{\operatorname{s}}-disk and Wlocuu(x)W^{\operatorname{uu}}_{\operatorname{loc}}(x) and is a uu{\operatorname{uu}}-disk.

BH4) uu{\operatorname{uu}}-disks through the local stable manifolds of PP and QQ: Let DD and DD^{\prime} be uu{\operatorname{uu}}-disks such that DWlocs(P)D\cap W^{\operatorname{s}}_{\operatorname{loc}}(P)\neq\emptyset and DWlocs(Q)D^{\prime}\cap W^{\operatorname{s}}_{\operatorname{loc}}(Q)\neq\emptyset. Then

Dc()=Dc()=DD=,D\cap\partial^{\operatorname{c}}({\mathbb{C}})=D^{\prime}\cap\partial^{\operatorname{c}}({\mathbb{C}})=D\cap D^{\prime}=\emptyset,

see Figure 3.

\psfrag{D}{$D$}\psfrag{Dp}{$D^{\prime}$}\psfrag{b}{${\mathbb{B}}$}\psfrag{a}{${\mathbb{A}}$}\psfrag{c}{${\mathbb{C}}$}\psfrag{p}{$P$}\psfrag{q}{$Q$}\psfrag{wuuP}{$W^{\operatorname{uu}}_{\operatorname{loc}}(P)$}\psfrag{wuuQ}{$W^{\operatorname{uu}}_{\operatorname{loc}}(Q)$}\psfrag{Cuu}{${\cal C}^{{\operatorname{uu}}}_{\alpha}$}\includegraphics[height=144.54pt]{bh5.eps}
Figure 3: Projection in u{\mathbb{R}}\oplus{\mathbb{R}}^{u}. uu{\operatorname{uu}}-disks. Condition BH4).

Given any s{\operatorname{s}}-disk Δ\Delta, there are two different homotopy classes of uu{\operatorname{uu}}-disks contained in [1,1]s××[1,1]u[-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u} and disjoint from Δ\Delta. We call these classes uu{\operatorname{uu}}-disks at the right and at the left of Δ\Delta. We use the following criterion: the uu{\operatorname{uu}}-disks disjoint from Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) in the homotopy class of Wlocuu(Q)W^{\operatorname{uu}}_{\operatorname{loc}}(Q) are at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). The uu{\operatorname{uu}}-disks disjoint from Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) in the other homotopy class are at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). We define similarly uu{\operatorname{uu}}-disks at the left and at the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q), where uu{\operatorname{uu}}-disks at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) are those in the class of Wlocuu(P)W^{{\operatorname{uu}}}_{\operatorname{loc}}(P).

According to BH4), uu{\operatorname{uu}}-disks at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) are also at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q). Analogously, uu{\operatorname{uu}}-disks at the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) are also at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P).

Summarizing, there are five possibilities for a uu{\operatorname{uu}}-disk DD in [1,1]s××[1,1]u[-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u}:

  • either DD is at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P),

  • or DWlocs(P)D\cap W^{\operatorname{s}}_{\operatorname{loc}}(P)\neq\emptyset,

  • or DD is at the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q),

  • or DWlocs(Q)D\cap W^{\operatorname{s}}_{\operatorname{loc}}(Q)\neq\emptyset,

  • or else DD is at the right of Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and at the left of Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q). In this case, we say that the uu{\operatorname{uu}}-disk DD is in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q).

As a consequence of BH4) one gets the following.

Remark 3.6 (uu{\operatorname{uu}}-disks in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q)).

  1. 1.

    There is a non-empty open subset UU of {\mathbb{C}} such that any uu{\operatorname{uu}}-disk through a point xUx\in U is in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q). In particular, there exist uu{\operatorname{uu}}-disks in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q).

  2. 2.

    Every uu{\operatorname{uu}}-disk Δ[1,1]s××[1,1]u\Delta\subset[-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u} in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q) is contained in {\mathbb{C}} and is disjoint from c()\partial^{\operatorname{c}}({\mathbb{C}}).

Consider a uu{\operatorname{uu}}-disk Δ\Delta\subset{\mathbb{C}} and write

f𝒜(Δ)=f(Δ𝒜)andf(Δ)=f(Δ).f_{{}_{\cal A}}(\Delta)=f(\Delta\cap{\cal A})\quad\mbox{and}\quad f_{{}_{\cal B}}(\Delta)=f(\Delta\cap{\cal B}).

According to BH1) and BH2) one gets,

Remark 3.7.

For every uu{\operatorname{uu}}-disk Δ\Delta\subset{\mathbb{C}}, f𝒜(Δ)f_{{}_{\cal A}}(\Delta) and f(Δ)f_{{}_{\cal B}}(\Delta) are uu{\operatorname{uu}}-disks in [1,1]s××[1,1]u[-1,1]^{s}\times{\mathbb{R}}\times[-1,1]^{u}.

BH5) Positions of images of uu{\operatorname{uu}}-disks (I): Given any uu{\operatorname{uu}}-disk Δ\Delta\subset{\mathbb{C}}, the following holds:

  1. 1.

    if Δ\Delta is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) then f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is a uu{\operatorname{uu}}-disk at the the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P),

  2. 2.

    if Δ\Delta is at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) then f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is a uu{\operatorname{uu}}-disk at the the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P),

  3. 3.

    if Δ\Delta is at the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) then f(Δ)f_{{}_{\cal B}}(\Delta) is a uu{\operatorname{uu}}-disk at the the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q),

  4. 4.

    if Δ\Delta is at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) then f(Δ)f_{{}_{\cal B}}(\Delta) is a uu{\operatorname{uu}}-disk at the the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q),

  5. 5.

    if Δ\Delta is at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) or ΔWlocs(P)\Delta\cap W^{\operatorname{s}}_{\operatorname{loc}}(P)\neq\emptyset then f(Δ)f_{{}_{\cal B}}(\Delta) is a uu{\operatorname{uu}}-disk at the the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), and

  6. 6.

    if Δ\Delta is at the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) or ΔWlocs(Q)\Delta\cap W^{s}_{\operatorname{loc}}(Q)\neq\emptyset then f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is a uu{\operatorname{uu}}-disk at the the right of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q).

Finally, we state the last condition (which will play a key role) in the definition of blender-horseshoe:

BH6) Positions of images of uu{\operatorname{uu}}-disks (II): Let Δ\Delta be a uu{\operatorname{uu}}-disk in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q). Then either f𝒜(Δ)f_{{}_{\cal A}}(\Delta) or f(Δ)f_{{}_{\cal B}}(\Delta) is a uu{\operatorname{uu}}-disk in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q).

Conditions BH5)BH6) are depicted in Figure 4.

\psfrag{D}{$D$}\psfrag{E}{$E$}\psfrag{F}{$F$}\psfrag{a}{${\mathbb{A}}$}\psfrag{b}{${\mathbb{B}}$}\psfrag{wuuP}{$W^{\operatorname{uu}}_{\operatorname{loc}}(P)$}\psfrag{wuuQ}{$W^{\operatorname{uu}}_{\operatorname{loc}}(Q)$}\psfrag{fad}{$f_{{}_{\cal A}}(D)$}\psfrag{fae}{$f_{{}_{\cal A}}(E)$}\psfrag{fbe}{$f_{{}_{\cal B}}(E)$}\psfrag{fbf}{$f_{{}_{\cal B}}(F)$}\psfrag{fbd}{$f_{{}_{\cal B}}(D)$}\psfrag{faf}{$f_{{}_{\cal A}}(F)$}\psfrag{p}{$P$}\psfrag{q}{$Q$}\psfrag{text}{$f_{{}_{\cal B}}(D)$ and $f_{{}_{\cal A}}(F)$ are not in between $W^{\operatorname{s}}_{\operatorname{loc}}(P)$ and $W^{\operatorname{s}}_{\operatorname{loc}}(Q)$}\includegraphics[height=151.76744pt]{bh6.eps}
Figure 4: Projection in u{\mathbb{R}}\oplus{\mathbb{R}}^{u}. Disks in between Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) and their images.

3.2.4 Definition of blender-horseshoe

We are now ready for defining blender-horseshoes444In some cases, we will use the terminology cu{\operatorname{cu}}-blender-horseshoe for emphasizing that the central one-dimensional direction is expanding. Using this terminology, a cs{\operatorname{cs}}-blender-horseshoe is a blender-horseshoe for f1f^{-1}.:

Definition 3.8 (Blender-horseshoe).

Consider a manifold MM of dimension n3n\geq 3 and a diffeomorphism f:MMf\colon M\to M. A hyperbolic set Λ\Lambda of ff is a blender-horseshoe if (in some coordinate system) there are a cube {\mathbb{C}} and families of cone-fields 𝒞s{\cal C}^{\operatorname{s}}, 𝒞u{\cal C}^{\operatorname{u}}, and 𝒞uu{\cal C}^{{\operatorname{uu}}} verifying conditions BH1)BH6 ) above.

We say that {\mathbb{C}} is the reference cube of the blender-horseshoe Λ\Lambda and that the saddles PP and QQ are the reference saddles of Λ\Lambda, where PP is the left saddle and QQ is the right saddle.

Recall that given a hyperbolic set Λ\Lambda of a diffeomorphism ff there is a C1C^{1}-neighborhood 𝒰f{\cal U}_{f} of ff such that every diffeomorphism g𝒰fg\in{\cal U}_{f} has a hyperbolic set Λg\Lambda_{g} which is close and conjugate to Λ\Lambda, called the continuation of Λ\Lambda for gg. Following [8, Lemma 1.11], one can prove the following:

Lemma 3.9.

Let Λ\Lambda be a blender-horseshoe of a diffeomorphism ff with reference cube {\mathbb{C}} and reference saddles PP and QQ. Then there is a neighborhood 𝒰f{\cal U}_{f} of ff in Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that for all g𝒰gg\in{\cal U}_{g} the continuation Λg\Lambda_{g} of Λ\Lambda for gg is a blender-horseshoe with reference cube {\mathbb{C}} and reference saddles PgP_{g} and QgQ_{g}.

Arguing as in [8] (see also [12] for a simple toy model and the example in Section 5.1) one gets the following:

Remark 3.10.

Every uu{\operatorname{uu}}-disk in between in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q) intersects Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda). Therefore the blender-horseshoe Λ\Lambda is a cu{\operatorname{cu}}-blender in the sense of Definition 3.1, where the uu{\operatorname{uu}}-disks in between Wlocs(P)W^{{\operatorname{s}}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{{\operatorname{s}}}_{\operatorname{loc}}(Q) define its superposition region.

4 Robust tangencies

In this section, we introduce a class of sub-manifolds called folding manifolds relative to a blender-horseshoe Λ\Lambda. The main technical step is Proposition 4.4, which claims that folding manifolds are tangent to the local stable manifold Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda) of the blender-horseshoe Λ\Lambda. Moreover, these tangencies are C1C^{1}-robust, see Theorem 2. Finally, using blender-horseshoes, in Theorem 4.8 we give sufficient conditions for the generation of robust tangencies by a homoclinic tangency.

4.1 Folding manifolds and tangencies associated to blender-horseshoes

Let Λ\Lambda be a blender-horseshoe with reference cube {\mathbb{C}} as in Section 3.2. Recall that the dimension of the unstable bundle of Λ\Lambda, Eu=EcuEuuE^{\operatorname{u}}=E^{\operatorname{cu}}\oplus E^{\operatorname{uu}}, is (u+1)(u+1). We say that the u{\operatorname{u}}-index of the blender-horseshoe Λ\Lambda is (u+1)(u+1) (i.e., the u{\operatorname{u}}-index of Λ\Lambda as a hyperbolic set). Define the local stable manifold of Λ\Lambda by

Wlocs(Λ)=xΛWlocs(x),W^{\operatorname{s}}_{{\operatorname{loc}}}(\Lambda)=\bigcup_{x\in\Lambda}W^{\operatorname{s}}_{{\operatorname{loc}}}(x),

where Wlocs(x)W^{\operatorname{s}}_{{\operatorname{loc}}}(x) is the connected component of Ws(x)W^{\operatorname{s}}(x)\cap{\mathbb{C}} containing xx. .

Remark 4.1.

The local stable manifold Wlocs(Λ)W^{\operatorname{s}}_{{\operatorname{loc}}}(\Lambda) of the blender-horseshoe Λ\Lambda is the set of points xx\in{\mathbb{C}} whose forward orbit remains in the reference cube {\mathbb{C}}.

A new ingredient of this section is the notion of folding manifold defined as follows:

Definition 4.2 (Folding manifold).

Consider a blender-horseshoe Λ\Lambda of u{\operatorname{u}}-index (u+1)(u+1) with reference cube {\mathbb{C}} and reference saddles PP and QQ. A sub-manifold 𝒮{\cal S}\subset{\mathbb{C}} of dimension (u+1)(u+1) is a folding manifold of Λ\Lambda (relative to the saddle PP) if there is a family (𝒮t)t[0,1]({\cal S}_{t})_{t\in[0,1]} of uu{\operatorname{uu}}-disks depending continuously on tt such that:

  • 𝒮=t[0,1]𝒮t,{\cal S}=\bigcup_{t\in[0,1]}{\cal S}_{t},

  • 𝒮0{\cal S}_{0} and 𝒮1{\cal S}_{1} intersects Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), and

  • for every t(0,1)t\in(0,1), the uu{\operatorname{uu}}-disk 𝒮t{\cal S}_{t} is in between Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q).

We similarly define a folding manifold (relative to QQ). A folding manifold of the blender-horseshoe Λ\Lambda is a folding manifold relative either to PP or to QQ.

Remark 4.3.

Let 𝒮{\cal S} be a folding manifold of the blender-horseshoe Λ\Lambda. Then there are a point x𝒮x\in{\cal S} and a non-zero vector vTx𝒮v\in T_{x}{\cal S} such that v𝒞s(x)v\in{\cal C}^{\operatorname{s}}(x).

A key property of folding manifolds of blender-horseshoes is the following:

Proposition 4.4.

Let 𝒮{\cal S} be a folding manifold of a blender-horseshoe Λ\Lambda. Then 𝒮{\cal S} and Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda) are tangent at some point zz.

To prove this proposition we need the following lemma:

Lemma 4.5.

Consider a diffeomorphism ff having a blender-horseshoe Λ\Lambda as above. The image by ff of a folding manifold 𝒮{\cal S} of Λ\Lambda contains a folding manifold of Λ\Lambda.

Proof: Let us assume, for instance, that the folding manifold 𝒮{\cal S} is relative to PP. We will prove that either f𝒜(𝒮)f_{{}_{\cal A}}({\cal S}) is a folding manifold relative to PP or f(𝒮)f_{{}_{\cal B}}({\cal S}) contains a folding manifold relative to PP.

If f𝒜(𝒮)f_{{}_{\cal A}}({\cal S}) is a folding manifold relative to PP we are done. So we can assume that f𝒜(𝒮)f_{{}_{\cal A}}({\cal S}) is not a folding manifold. As the uu{\operatorname{uu}}-disks 𝒮0{\cal S}_{0} and 𝒮1{\cal S}_{1} meet Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), by Remark 3.7, their images f𝒜(𝒮0)f_{{}_{\cal A}}({\cal S}_{0}) and f𝒜(𝒮1)f_{{}_{\cal A}}({\cal S}_{1}) are uu{\operatorname{uu}}-disks intersecting Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). Furthermore, by item 1 in BH6), the uu{\operatorname{uu}}-disk f𝒜(𝒮t)f_{{}_{\cal A}}({\cal S}_{t}) is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), for every t(0,1)t\in(0,1).

Since we are assuming that f𝒜(𝒮)f_{{}_{\cal A}}({\cal S}) is not a folding manifold relative to PP, by definition of a folding manifold relative to PP, there is some t0(0,1)t_{0}\in(0,1) such that f𝒜(𝒮t0)f_{{}_{\cal A}}({\cal S}_{t_{0}}) is not at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) (i.e., it is either at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) or it meets Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q)). Thus, by continuity of the disks f𝒜(𝒮t)f_{{}_{\cal A}}({\cal S}_{t}), there is t1(0,t0)t_{1}\in(0,t_{0}) such that f𝒜(𝒮t1)Wlocs(Q)f_{{}_{\cal A}}({\cal S}_{t_{1}})\cap W^{\operatorname{s}}_{\operatorname{loc}}(Q)\neq\emptyset. As 𝒮t1{\cal S}_{t_{1}} is in between Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q), by BH6), the image f(𝒮t1)f_{{}_{\cal B}}({\cal S}_{t_{1}}) is in between Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q).

By the definition of folding manifold relative to PP, every 𝒮t{\cal S}_{t} is at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q). Therefore, by item 4 in BH5), f(𝒮t)f_{{}_{\cal B}}({\cal S}_{t}) is a uu{\operatorname{uu}}-disk at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q), for every t(0,1)t\in(0,1). Moreover, by item 5 in BH5), the images f(𝒮0)f_{{}_{\cal B}}({\cal S}_{0}) and f(𝒮1)f_{{}_{\cal B}}({\cal S}_{1}) are uu{\operatorname{uu}}-disks at the left of Wlocs(P)W^{\operatorname{s}}_{{\operatorname{loc}}}(P).

Now by continuity of the disks f(𝒮t)f_{{}_{\cal B}}({\cal S}_{t}) and since f(𝒮t1)f_{{}_{\cal B}}({\cal S}_{t_{1}}) is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P)), there are parameters t2t_{2} and t3t_{3}, with t2<t1<t3t_{2}<t_{1}<t_{3}, such that f(𝒮t2)f_{{}_{\cal B}}({\cal S}_{t_{2}}) and f(𝒮t3)f_{{}_{\cal B}}({\cal S}_{t_{3}}) are uu{\operatorname{uu}}-disks intersecting Wlocs(P)W^{\operatorname{s}}_{{\operatorname{loc}}}(P) and f(𝒮t)f_{{}_{\cal B}}({\cal S}_{t}) is a uu{\operatorname{uu}}-disk at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), for all t(t2,t3)t\in(t_{2},t_{3}). Since, by item 4 in BH5), these disks are at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q), they are in between Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) and Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q). This implies that

t[t1,t2]f(𝒮t)f(𝒮)\bigcup_{t\in[t_{1},t_{2}]}f_{{}_{\cal B}}({\cal S}_{t})\subset f_{{}_{\cal B}}({\cal S})

is a folding manifold relative to PP, ending the proof of the lemma. \Box

We are now ready to conclude the proof of Proposition 4.4.

Proof of Proposition 4.4: Write 𝒮0=𝒮{\cal S}_{0}={\cal S}. By Lemma 4.5, there is a folding manifold 𝒮1{\cal S}_{1} contained in f(𝒮0)f({\cal S}_{0}). Using Lemma 4.5 and arguing inductively, we define a sequence of folding manifolds (𝒮i)i({\cal S}_{i})_{i} of the blender-horseshoe Λ\Lambda such that, for every i0i\geq 0, 𝒮i+1{\cal S}_{i+1} is contained in f(Si)f(S_{i}). Let

𝒮~i=fi(Si).\tilde{\cal S}_{i}=f^{-i}(S_{i}).

In this way we get a nested sequence (𝒮~i)i(\tilde{\cal S}_{i})_{i}, 𝒮~i+1𝒮~i𝒮\tilde{\cal S}_{i+1}\subset\tilde{\cal S}_{i}\subset{\cal S}, of connected and compact sets. Thus, by construction, the intersection set

𝒮=i=0𝒮~i{\cal S}_{\infty}=\bigcap_{i=0}^{\infty}\tilde{\cal S}_{i}\neq\emptyset

is connected and compact. Moreover, 𝒮𝒮0{\cal S}_{\infty}\subset{\cal S}_{0}.

By construction, the whole forward orbit of the set 𝒮{\cal S}_{\infty} is contained in the reference cube {\mathbb{C}} of the blender. By Remark 4.1, the set 𝒮{\cal S}_{\infty} is contained in Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda). Note that, as Λ\Lambda is totally disconnected (a Cantor set) and 𝒮{\cal S}_{\infty} is connected, hence there is some zΛz\in\Lambda such that

𝒮Wlocs(z).{\cal S}_{\infty}\subset W^{\operatorname{s}}_{\operatorname{loc}}(z).

Since 𝒮i{\cal S}_{i} is a folding manifold for every ii, Remark 4.3 implies that there are a point xi𝒮ix_{i}\in{\cal S}_{i} and a non-zero vector viTxi𝒮iv_{i}\in T_{x_{i}}{\cal S}_{i} such that vi𝒞αs(xi)v_{i}\in{\cal C}^{\operatorname{s}}_{\alpha}(x_{i}).

Consider the point x~i=fi(xi)𝒮~i𝒮\tilde{x}_{i}=f^{-i}(x_{i})\in\tilde{\cal S}_{i}\subset{\cal S} and an unitary vector v~i\tilde{v}_{i} parallel to Dxifi(vi)D_{x_{i}}f^{-i}(v_{i}). Note that v~iTx~i𝒮~i\tilde{v}_{i}\in T_{\tilde{x}_{i}}\tilde{\cal S}_{i}, thus v~iTx~i𝒮\tilde{v}_{i}\in T_{\tilde{x}_{i}}{\cal S}. By the (Df1)(Df^{-1})-invariance of the cone-field 𝒞αs{\cal C}^{\operatorname{s}}_{\alpha}, condition BH2), we have that v~i𝒞αs(x~i)\tilde{v}_{i}\in{\cal C}^{\operatorname{s}}_{\alpha}(\tilde{x}_{i}). We can assume (taking a subsequence if necessary) that

x~ix𝒮𝒮Wlocs(Λ)andv~iv.\tilde{x}_{i}\to x_{\infty}\in{\cal S}_{\infty}\subset{\cal S}\cap W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda)\qquad\mbox{and}\qquad\tilde{v}_{i}\to v_{\infty}.

Hence x𝒮x_{\infty}\in{\cal S}_{\infty} and xWlocs(z)x_{\infty}\in W^{\operatorname{s}}_{\operatorname{loc}}(z). Our construction also implies that vTx𝒮v_{\infty}\in T_{x_{\infty}}{\cal S}. Finally, also by construction, the vector vv_{\infty} belongs to the intersection

i0Dfi(𝒞αs(fi(x)))=TxWlocs(z).\bigcap_{i\geq 0}Df^{-i}({\cal C}^{\operatorname{s}}_{\alpha}(f^{i}(x_{\infty})))=T_{x_{\infty}}W^{\operatorname{s}}_{\operatorname{loc}}(z).

This completes the proof of the proposition. \Box

4.2 Robust tangencies

We now return to the problem of robust tangencies in Question 2. We need the following definition.

Definition 4.6 (Folded submanifolds with respect to a blender-horseshoe).

Let f:MMf\colon M\to M be a diffeomorphism having a blender-horseshoe Λ\Lambda with reference saddles PP and QQ and NMN\subset M be a submanifold of dimension indu(Λ){\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Lambda).

We say that NN is folded with respect to Λ\Lambda if the interior of NN contains a folding manifold 𝒮=(𝒮t)t[0,1]{\cal S}=({\cal S}_{t})_{t\in[0,1]} relative to some reference saddle A{P,Q}A\in\{P,Q\} of the blender, here (𝒮t)t[0,1]({\cal S}_{t})_{t\in[0,1]} is the family of uu{\operatorname{uu}}-disks in Definition 4.2, such that:

  • 𝒮0Wlocs(A){\cal S}_{0}\cap W^{\operatorname{s}}_{\operatorname{loc}}(A) and 𝒮1Wlocs(A){\cal S}_{1}\cap W^{\operatorname{s}}_{\operatorname{loc}}(A) are transverse intersection points of NN with Wlocs(A)W^{\operatorname{s}}_{\operatorname{loc}}(A);

  • There is 0<α<α0<\alpha^{\prime}<\alpha such that the uu{\operatorname{uu}}-disks 𝒮t{\cal S}_{t}, t[0,1]t\in[0,1], are tangent to the cone-field 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha^{\prime}}.

To emphasize the reference saddle AA of the blender we consider, we say that the submanifold NN is folded with respect to (Λ,A)(\Lambda,A).

Remark 4.7.

A submanifold to be folded with respect to a blender-horseshoe is a C1C^{1}-open property.

As a direct consequence of Proposition 4.4 and Remark 4.7 one gets:

Theorem 2.

Let NMN\subset M be a folded submanifold with respect to a blender-horseshoe Λ\Lambda. Then NN and Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda) have a CrC^{r}-robust tangency.

4.3 Robust homoclinic tangencies

In this section we prove that homoclinic tangencies associated to blender-horseshoes yield CrC^{r}-robust homoclinic tangencies.

Theorem 4.8.

Consider a transitive hyperbolic set Σ\Sigma of a CrC^{r}-diffeomorphism ff containing a cu{\operatorname{cu}}-blender-horseshoe and a saddle with a homoclinic tangency. Then there is a diffeomorphism gg arbitrarily CrC^{r}-close to ff such that the continuation Σg\Sigma_{g} of Σ\,\Sigma has a CrC^{r}-robust homoclinic tangency.

We need the following lemma.

Lemma 4.9.

Consider a CrC^{r}-diffeomorphism ff with a cu{\operatorname{cu}}-blender-horseshoe Λ\Lambda. Assume that there is a saddle RR with indu(R)=indu(Λ){\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(R)={\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Lambda) and such that Wu(R)W^{\operatorname{u}}(R) has a tangency with Ws(A)W^{\operatorname{s}}(A), where AA is a reference saddle of the blender Λ\Lambda. Then there is a diffeomorphism gg arbitrarily CrC^{r}-close to ff such that Wu(Rg)W^{\operatorname{u}}(R_{g}) is a folded manifold with respect to the continuation Λg\Lambda_{g} of the blender-horseshoe Λ\Lambda.

By Theorem 2 one gets:

Corollary 5.

In Lemma 4.9, the stable manifold Wlocs(Λg)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda_{g}) of the blender-horseshoe and Wu(Rg)W^{\operatorname{u}}(R_{g}) have a CrC^{r}-robust tangency.

Proof of Lemma 4.9: We suppose that A=PA=P is the left reference saddle of the blender. The proof involves a string of CrC^{r}-perturbations of the diffeomorphism ff. For simplicity, we also denote these perturbations by ff.

We begin by noting that the center stable bundle EcsE^{{\operatorname{cs}}} is well defined for every point xx in the local stable manifold Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda). Recall that Wlocs(Λ)W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda) is the set of points whose forward orbit remains in the reference cube {\mathbb{C}} of the blender-horseshoe, Remark 4.1. Given a point xWlocs(Λ)x\in W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda), the subspace Ecs(x)E^{{\operatorname{cs}}}(x) is the set of vectors vTxMv\in T_{x}M such that Dfn(v)(𝒞uu(fn(x)){0})Df^{n}(v)\notin({\cal C}^{\operatorname{uu}}(f^{n}(x))\setminus\{0\}), for every n0n\geq 0. The space Ecs(x)E^{\operatorname{cs}}(x) has dimension inds(Λ)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(\Lambda)+1 and depends continuously on the point xWlocs(Λ)x\in W^{\operatorname{s}}_{\operatorname{loc}}(\Lambda) and on the diffeomorphism ff.

First, after considering forward iterations, we can assume that the tangency intersection point BB between Wu(R)W^{\operatorname{u}}(R) and Ws(P)W^{\operatorname{s}}(P) is in Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). Therefore the whole forward orbit of BB is the reference cube {\mathbb{C}}. Recall that PP is the left reference saddle of the blender-horseshoe, thus PP is in the “rectangle” 𝔸{\mathbb{A}} of the Markov partition. Thus, for any n0n\geq 0, f𝒜n(B)f_{{}_{\cal A}}^{n}(B) is defined and belongs to {\mathbb{C}}. Hence Ecs(fi(B))E^{\operatorname{cs}}(f^{i}(B)) is well defined for all i0i\geq 0 (recall the comment above). Note that

dim(TBWu(R))+dim(Ecs(B))=dim(TBWu(R))+dim(TBWs(P))+1=dim(M)+1.\dim(T_{B}W^{\operatorname{u}}(R))+\dim(E^{\operatorname{cs}}(B))=\dim(T_{B}W^{\operatorname{u}}(R))+\dim(T_{B}W^{\operatorname{s}}(P))+1=\dim(M)+1.

Thus after a perturbation, we can assume that TBWu(R)T_{B}W^{\operatorname{u}}(R) is transverse to Ecs(B)E^{\operatorname{cs}}(B). Hence there is a subspace 𝕍TBWu(R){\mathbb{V}}\subset T_{B}W^{\operatorname{u}}(R) of dimension uu with 𝕍Ecs(B)=TBM{\mathbb{V}}\oplus E^{\operatorname{cs}}(B)=T_{B}M, where (u+1)=indu(Λ)(u+1)={\mbox{\rm{ind}}^{\,{\operatorname{u}}}}(\Lambda).

Consider any α(0,α)\alpha^{\prime}\in(0,\alpha) (α\alpha is the constant in the definition of the cone-fields of the blender). Then, for every n>0n>0 large enough, one has that Dfn(𝕍)Df^{n}({\mathbb{V}}) is contained in the cone 𝒞αuu(fn(B)){\cal C}^{\operatorname{uu}}_{\alpha^{\prime}}(f^{n}(B)). For simplicity, let us assume that n=0n=0, that is 𝕍𝒞αuu(B){\mathbb{V}}\subset{\cal C}^{\operatorname{uu}}_{\alpha^{\prime}}(B). This implies that (up to increase slightly the constant α<α\alpha^{\prime}<\alpha) there is a small submanifold 𝒮~Wu(R)\tilde{\cal S}\subset W^{\operatorname{u}}(R) such that the point BB is in the interior of 𝒮~\tilde{\cal S}, and 𝒮~\tilde{\cal S} is foliated by disks (𝒮~t)t[1,1](\tilde{\cal S}_{t})_{t\in[-1,1]} of dimension uu tangent to the cone-field 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha^{\prime}}.

Using the expansion by DfDf in the cone-field 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha^{\prime}} and considering forward iterations of 𝒮~\tilde{\cal S} by ff, we get k0k\geq 0 and a submanifold 𝒮fk(𝒮~){\cal S}\subset f^{k}(\tilde{\cal S}) such that:

  • 𝒮{\cal S} contains fk(B)f^{k}(B) in its interior and is tangent to Ws(P)W^{\operatorname{s}}(P) at fk(B)f^{k}(B), and

  • 𝒮{\cal S} is foliated by uu{\operatorname{uu}}-disks 𝒮tfk(𝒮~t){\cal S}_{t}\subset f^{k}(\tilde{\cal S}_{t}), t[1,1]t\in[-1,1], where the disks 𝒮t{\cal S}_{t} are tangent to 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha^{\prime}}.

Again for simplicity, we assume that k=0k=0 and that B𝒮0B\in{\cal S}_{0}.

After a new perturbation, we can assume that the contact between 𝒮{\cal S} and Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) at the point BB is quadratic. In particular, there is small ϵ>0\epsilon>0, such that either all the uu{\operatorname{uu}}-disks 𝒮t{\cal S}_{t}, t0t\neq 0 and t[ϵ,ϵ]t\in[-\epsilon,\epsilon], are at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) (case (a)), or all the uu{\operatorname{uu}}-disks 𝒮t{\cal S}_{t}, t0t\neq 0 and t[ϵ,ϵ]t\in[-\epsilon,\epsilon], are at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P) (case (b)). So after discarding some disks and reparametrizing the family 𝒮t{\cal S}_{t}, we can assume that ϵ=1\epsilon=1.

\psfrag{p}{$P$}\psfrag{s}{${\cal S}$}\psfrag{text}{perturbation}\psfrag{proj}{projection in ${\mathbb{R}}^{s}\oplus{\mathbb{R}}^{u}$}\includegraphics[height=144.54pt]{casea.eps}
Figure 5: Folded manifold: case (a).

Case (a): for t0t\neq 0, every 𝒮t{\cal S}_{t} is at the left of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). After a new perturbation, we can assume that 𝒮{\cal S} is a folding manifold relative to PP, see Figure 5. Since, by construction, 𝒮{\cal S} is contained in Wu(R)W^{\operatorname{u}}(R) this concludes the proof in the first case.

Case (b): for t0t\neq 0 every 𝒮t{\cal S}_{t} is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). By considering positive iterations of 𝒮{\cal S} by f𝒜f_{{}_{\cal A}}, one gets a large i>0i>0 such that f𝒜i(𝒮)f_{{}_{\cal A}}^{i}({\cal S}) meets transversely Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q) at some points in f𝒜i(𝒮t1)f_{{}_{\cal A}}^{i}({\cal S}_{t_{1}}) and f𝒜i(𝒮t2)f_{{}_{\cal A}}^{i}({\cal S}_{t_{2}}), where t1<0<t2t_{1}<0<t_{2}. Once again, let us assume that i=0i=0.

\psfrag{p}{$P$}\psfrag{q}{$Q$}\psfrag{s}{${\cal S}$}\psfrag{q}{$Q$}\psfrag{fi}{$f^{i}$}\psfrag{fs}{$f_{{}_{\cal A}}^{i}({\cal S})$}\psfrag{text}{perturbation}\psfrag{proj}{projection in ${\mathbb{R}}^{s}\oplus{\mathbb{R}}^{u}$}\includegraphics[height=173.44756pt]{caseb.eps}
Figure 6: Folded manifold: case (b).

We can choose t1t_{1} and t2t_{2} such that the disks 𝒮t{\cal S}_{t} are at the left of Wlocs(Q)W^{s}_{\operatorname{loc}}(Q) for every t(t1,t2)t\in(t_{1},t_{2}). Recall that, by hypothesis, for all t[t1,t2]{0}t\in[t_{1},t_{2}]\setminus\{0\} the disks 𝒮t{\cal S}_{t} are at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P). Therefore, we can perform a final perturbation so that 𝒮^=t[t1,t2]𝒮t\hat{\cal S}=\bigcup_{t\in[t_{1},t_{2}]}{\cal S}_{t} is a folding manifold relative to QQ, see Figure 6. Since 𝒮^\hat{\cal S} is contained in Wu(R)W^{\operatorname{u}}(R) this ends the proof of the lemma. \Box

We are now ready to prove Theorem 4.8.

Proof of Theorem 4.8: It is enough to observe that after a CrC^{r}-perturbation, one can assume that the homoclinic tangency of Σ\Sigma occurs between the unstable manifold of a periodic point RΣR\in\Sigma and the left reference saddle of the blender-horseshoe. \Box

5 Generation of blender-horseshoes

In this section we see how blender-horseshoes arise naturally in our non-hyperbolic setting. First, in Section 5.1, we review constructions in [12] providing simple examples of blender-horseshoes. In Section 5.2, using these constructions, we see that partially hyperbolic saddles (saddle-node and flip points) with strong homoclinic intersections (intersections between the strong stable and strong unstable manifolds of a non-hyperbolic saddle) yield blender-horseshoes. Finally, following [9], in Sections 5.3 and 5.4 we prove that co-index one heterodimensional cycles generate blender-horseshoes. We will see in Section 6.2 that co-index one cycles occur naturally in the non-hyperbolic setting.

5.1 Prototypical blender-horseshoes

In this section, we consider a local diffeomorphism ff having an affine horseshoe Λ\Lambda with a dominated splitting with three non-trivial bundles, Es<Ecu<EuuE^{{\operatorname{s}}}\oplus_{{}_{<}}E^{\operatorname{cu}}\oplus_{{}_{<}}E^{\operatorname{uu}}, where EcuE^{\operatorname{cu}} is one dimensional and Eu=EcuEuuE^{\operatorname{u}}=E^{\operatorname{cu}}\oplus E^{\operatorname{uu}} is the unstable bundle of Λ\Lambda. We suppose that Λ\Lambda is contained in a hyperplane Π\Pi tangent to EsEuuE^{\operatorname{s}}\oplus E^{{\operatorname{uu}}} and that the expansion along the direction EcuE^{\operatorname{cu}} is close to one. Under these assumptions we prove that there are perturbations gg of ff such that the continuations Λg\Lambda_{g} of Λ\Lambda for gg are blender-horseshoes, see Proposition 5.1. We now go to the details of this construction, we borrow from [12].

Let 𝔻=[1,1]n{\mathbb{D}}=[-1,1]^{n} and n=s+u,s,u1n=s+u,\,s,u\geq 1. Consider a diffeomorphism F:nnF\colon{\mathbb{R}}^{n}\to{\mathbb{R}}^{n} having a horseshoe Σ=kFk(𝔻)\Sigma=\cap_{k\in{\mathbb{Z}}}F^{k}({\mathbb{D}}) such that:

  • F1(𝔻)𝔻F^{-1}({\mathbb{D}})\cap{\mathbb{D}} consists of two connected components 𝔻1=[1,1]s×𝕌1{\mathbb{D}}_{1}=[-1,1]^{s}\times{\mathbb{U}}_{1} and 𝔻2=[1,1]s×𝕌2{\mathbb{D}}_{2}=[-1,1]^{s}\times{\mathbb{U}}_{2}, where 𝕌1{\mathbb{U}}_{1} and 𝕌2{\mathbb{U}}_{2} are disjoint topological compact disks of dimension uu.

  • The map FF is affine on each rectangle 𝔻i{\mathbb{D}}_{i}: there are linear maps Si:ssS_{i}\colon{\mathbb{R}}^{s}\to{\mathbb{R}}^{s} and Ui:uuU_{i}\colon{\mathbb{R}}^{u}\to{\mathbb{R}}^{u}, i=1,2i=1,2, such that

    DF|𝔻i=(Si00Ui),Si,Ui1<1/2,i=1,2,DF|_{{\mathbb{D}}_{i}}=\left(\begin{matrix}S_{i}&0\\ 0&U_{i}\end{matrix}\right),\qquad||S_{i}||,||U_{i}^{-1}||<1/2,\quad i=1,2,

    where A||A|| is the norm of the linear map AA.

We suppose that, in the usual coordinates (xs,xu)(x^{s},x^{u}) in n=s×u{\mathbb{R}}^{n}={\mathbb{R}}^{s}\times{\mathbb{R}}^{u}, the fixed saddles of the horseshoe Σ\Sigma are p=(0s,0u)𝔻1p=(0^{s},0^{u})\in{\mathbb{D}}_{1} and q=(as,au)𝔻2q=(a^{s},a^{u})\in{\mathbb{D}}_{2}.

\psfrag{Ru}{${\mathbb{R}}^{u}$}\psfrag{Rs}{${\mathbb{R}}^{s}$}\psfrag{R}{${\mathbb{R}}$}\psfrag{D1}{${\mathbb{D}}_{1}$}\psfrag{D2}{${\mathbb{D}}_{2}$}\psfrag{I}{$[-1,1]^{n}$}\includegraphics[height=144.54pt]{horseshoe.eps}
Figure 7: An affine horseshoe. The map fλ,0f_{\lambda,0}.

Consider λ(1,2)\lambda\in(1,2) and the family of local diffeomorphisms (fλ,μ)μ[ϵ,ϵ](f_{\lambda,\mu})_{\mu\in[-\epsilon,\epsilon]} of n+1{\mathbb{R}}^{n+1} given by:

fλ,μ(xs,xu,x)={(F(xs,xu),λx),if xu𝕌1,(F(xs,xu),λxμ),if xu𝕌2.f_{\lambda,\mu}(x^{s},x^{u},x)=\left\{\begin{array}[]{lll}&(F(x^{s},x^{u}),\lambda\,x),&\quad\mbox{if $x^{u}\in{\mathbb{U}}_{1}$},\\ &(F(x^{s},x^{u}),\lambda\,x-\mu),&\quad\mbox{if $x^{u}\in{\mathbb{U}}_{2}$}.\end{array}\right.

By definition, for small μ\mu, the diffeomorphism fλ,μf_{\lambda,\mu} has two fixed saddles: P=(0s,0u,0)P=(0^{s},0^{u},0) (independent of λ\lambda and μ\mu) and Qλ,μ=(as,au,μ/(λ1))Q_{\lambda,\mu}=(a^{s},a^{u},\mu/(\lambda-1)).

Let Λλ,0\Lambda_{\lambda,0} be the maximal invariant set of fλ,0f_{\lambda,0} in (𝔻1𝔻2)×[1,1]({\mathbb{D}}_{1}\cup{\mathbb{D}}_{2})\times[-1,1]. Note that Λλ,0=Σ×{0}\Lambda_{\lambda,0}=\Sigma\times\{0\} is a hyperbolic set of fλ,0f_{\lambda,0}. We say that Λλ,0\Lambda_{\lambda,0} is an affine horseshoe of fλ,0f_{\lambda,0} with central expansion λ\lambda. Observe that that the hyperplane n×{0}{\mathbb{R}}^{n}\times\{0\} is not normally hyperbolic for fλ,0f_{\lambda,0}.

We denote by Λλ,μ\Lambda_{\lambda,\mu} the maximal invariant set of fλ,μf_{\lambda,\mu} in (𝔻1𝔻2)×[1,1]({\mathbb{D}}_{1}\cup{\mathbb{D}}_{2})\times[-1,1]. For small μ\mu, the set Λλ,μ\Lambda_{\lambda,\mu} is the continuation of Λλ,0\Lambda_{\lambda,0}. More precisely, fixed small δ>0\delta>0 and the cube δ=[1,1]s×[1,1]u×[δ,δ]{\mathbb{C}}_{\delta}=[-1,1]^{s}\times[-1,1]^{u}\times[-\delta,\delta], for |μ|<(λ1)δ|\mu|<(\lambda-1)\,\delta, the set Λλ,μ\Lambda_{\lambda,\mu} is the maximal invariant set of fλ,μf_{\lambda,\mu} in δ{\mathbb{C}}_{\delta}. Clearly, P,Qλ,μΛλ,μP,Q_{\lambda,\mu}\in\Lambda_{\lambda,\mu}.

Proposition 5.1.

For every λ>1\lambda>1 close to 11 and μ>0\mu>0, the set Λλ,μ\Lambda_{\lambda,\mu} is a blender-horseshoe with reference cube δ{\mathbb{C}}_{\delta} and reference saddles PP and Qλ,μQ_{\lambda,\mu} (PP is the left saddle and Qλ,μQ_{\lambda,\mu} the right one).

In this section, for notational convenience, we write the central coordinates in the third position.

Proof: We fix λ>1\lambda>1 and μ>0\mu>0 and we simply write Λ\Lambda, ff, PP, and QQ, omitting the dependence on the parameters. The hyperbolicity of Λ\Lambda follows from the hyperbolicity of FF and from the normal expansion by λ>1\lambda>1. Consider the constant bundles

Es=(s×{(0u,0)}),Ec=({0s,0u}×),Euu=({0s}×u×{0}).E^{\operatorname{s}}=\left({\mathbb{R}}^{s}\times\{(0^{u},0)\}\right),\quad E^{\operatorname{c}}=\left(\{0^{s},0^{u}\}\times{\mathbb{R}}\right),\quad E^{\operatorname{uu}}=\left(\{0^{s}\}\times{\mathbb{R}}^{u}\times\{0\}\right).

Since λ\lambda is less than 22, then

Txn+1=Es<Ec<Euu,xΛ,T_{x}{\mathbb{R}}^{n+1}=E^{\operatorname{s}}\oplus_{{}_{<}}E^{\operatorname{c}}\oplus_{{}_{<}}E^{\operatorname{uu}},\quad x\in\Lambda,

is a dominated splitting over Λ\Lambda. Furthermore, as the bundles above are constant, the cone-fields 𝒞αcu{\cal C}^{\operatorname{cu}}_{\alpha} and 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha} are DfDf-invariant and 𝒞αs{\cal C}^{\operatorname{s}}_{\alpha} is (Df1)(Df^{-1})-invariant, for every α(0,1)\alpha\in(0,1). Finally, for small α\alpha, 𝒞αs{\cal C}^{\operatorname{s}}_{\alpha} is uniformly contracting and 𝒞αu{\cal C}^{\operatorname{u}}_{\alpha} is uniformly expanding. This gives condition BH2).

To get conditions BH1) and BH3) just let

𝒜=[1,1]s×U11([1,1]u)×[δ,δ],=[1,1]s×U21([1,1]u)×[δ,δ],{\cal A}=[-1,1]^{s}\times U^{-1}_{1}([-1,1]^{u})\times[-\delta,\delta],\qquad{\cal B}=[-1,1]^{s}\times U^{-1}_{2}([-1,1]^{u})\times[-\delta,\delta],
𝔸=[1,1]s×U11([1,1]u)×[λ1δ,λ1δ],𝔹=[1,1]s×U21([1,1]u)×[δ+μλ,δ+μλ],{\mathbb{A}}=[-1,1]^{s}\times U^{-1}_{1}([-1,1]^{u})\times[-\lambda^{-1}\,\delta,\lambda^{-1}\,\delta],\qquad{\mathbb{B}}=[-1,1]^{s}\times U^{-1}_{2}([-1,1]^{u})\times\left[\frac{-\delta+\mu}{\lambda},\frac{\delta+\mu}{\lambda}\right],

and observe that

f(𝔸)=S1([1,1]s)×[1,1]u×[δ,δ] and f(𝔹)=S2([1,1]s)×[1,1]u×[δ,δ].f({\mathbb{A}})=S_{1}([-1,1]^{s})\times[-1,1]^{u}\times[-\delta,\delta]\quad\mbox{ and }\quad f({\mathbb{B}})=S_{2}([-1,1]^{s})\times[-1,1]^{u}\times[-\delta,\delta].
\psfrag{Cd}{${\mathbb{C}}_{\delta}$}\psfrag{cB}{${\cal B}$}\psfrag{cA}{${\cal A}$}\psfrag{BB}{${\mathbb{B}}$}\psfrag{AA}{${\mathbb{A}}$}\psfrag{flm}{$f_{\lambda,\mu}$}\includegraphics[height=130.08621pt]{prototypal.eps}
Figure 8: Prototypical blender-horseshoe.

Observe that the local invariant manifolds of PP and QQ are:

Wlocs(P,f)=[1,1]s×{(0u,0)},Wlocs(Q,f)=[1,1]s×{(au,μλ1)},Wlocuu(P,f)={0s}×[1,1]u×{0},Wlocuu(Q,f)={as}×[1,1]u×{μλ1}.\begin{array}[]{lll}&W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f)=[-1,1]^{s}\times\{(0^{u},0)\},&W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f)=[-1,1]^{s}\times\{(a^{u},\frac{\mu}{\lambda-1})\},\\ \\ &W^{{\operatorname{uu}}}_{{\operatorname{loc}}}(P,f)=\{0^{s}\}\times[-1,1]^{u}\times\{0\},&W^{{\operatorname{uu}}}_{{\operatorname{loc}}}(Q,f)=\{a^{s}\}\times[-1,1]^{u}\times\{\frac{\mu}{\lambda-1}\}.\end{array}

It is immediate to check that vertical disks of the form {xs}×[1,1]u×{xc}\{x^{s}\}\times[-1,1]^{u}\times\{x^{c}\} satisfy condition BH4). To get BH4) for uu{\operatorname{uu}}-disks it is enough to take α(0,1)\alpha\in(0,1) small enough in the definition of the cone-fields.

Condition BH5) follows from the fact that f𝒜f_{{}_{\cal A}} and ff_{{}_{\cal B}} are affine maps preserving the dominated splitting and whose center eigenvalue λ\lambda is positive.

\psfrag{wuuP}{$W^{\operatorname{uu}}_{\operatorname{loc}}(P,f)$}\psfrag{wuuQ}{$W^{\operatorname{uu}}_{\operatorname{loc}}(Q,f)$}\psfrag{de}{$\Delta$}\psfrag{I1}{$I_{1}$}\psfrag{I2}{$I_{2}$}\includegraphics[height=130.08621pt]{onedim.eps}
Figure 9: uu{\operatorname{uu}}-disks and one-dimensional reduction.

It remains to check condition BH6). We first consider vertical disks Δ\Delta parallel to EuuE^{\operatorname{uu}}

Δ={xs}×[1,1]u×{xc}\Delta=\{x^{s}\}\times[-1,1]^{u}\times\{x^{c}\}

which are in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f). This means that xc(0,μλ1)x^{c}\in(0,\frac{\mu}{\lambda-1}). We consider two cases:

Case 1: xcI1=(0,μλ(λ1))x^{c}\in I_{1}=(0,\frac{\mu}{\lambda\,(\lambda-1)}). In this case, one has that

f𝒜(Δ)={x¯s}×[1,1]u×{λxc}whereλxc(0,μλ1).f_{{}_{\cal A}}(\Delta)=\{\bar{x}^{s}\}\times[-1,1]^{u}\times\{\lambda\,x^{c}\}\quad\mbox{where}\quad\lambda\,x^{c}\in\left(0,\frac{\mu}{\lambda-1}\right).

Thus f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f).

Case 2: xcI2=(μλ,μλ1)x^{c}\in I_{2}=(\frac{\mu}{\lambda},\frac{\mu}{\lambda-1}). Note that in this case one gets

f(Δ)={x¯s}×[1,1]u×{λxcμ}whereλxcμ(0,μλ1).f_{{}_{\cal B}}(\Delta)=\{\bar{x}^{s}\}\times[-1,1]^{u}\times\{\lambda\,x^{c}-\mu\}\quad\mbox{where}\quad\lambda\,x^{c}-\mu\in\left(0,\frac{\mu}{\lambda-1}\right).

Hence f(Δ)f_{{}_{\cal B}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f).

This completes the proof of BH6) for disks parallel to EuuE^{\operatorname{uu}}.

We next consider general uu{\operatorname{uu}}-disks. We begin with two claims.

Claim 5.2.

Consider τ1<μλ(λ1)\tau_{1}<\frac{\mu}{\lambda\,(\lambda-1)} and any uu{\operatorname{uu}}-disk Δ\Delta (i.e. tangent to the cone-field 𝒞αuu{\cal C}^{\operatorname{uu}}_{\alpha}) through a point (xs,xu,xc)(x^{s},x^{u},x^{c}) with xcτ1x^{c}\leq\tau_{1}. Then, for every α(0,1)\alpha\in(0,1) small enough,

  • f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q),

  • assume that Δ\Delta is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P), then f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f).

Proof: The first statement follows from the compactness of the set of vertical disks with xcτ1x^{c}\leq\tau_{1} and the uniform convergence in α\alpha of the uu{\operatorname{uu}}-disks to the vertical disks (parallel to EuuE^{\operatorname{uu}}) as α0\alpha\to 0.

From the first part of the claim we know that f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is at the left of Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f). It remains to check that f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is at the right of Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f). The disk Δ\Delta contains a point of the form (xs,0u,xc)(x^{s},0^{u},x^{c}) with xc>0x^{c}>0. Thus f𝒜(Δ)f_{{\cal A}}(\Delta) contains the point (S1(xs),0u,λxc)(S_{1}(x^{s}),0^{u},\lambda\,x^{c}). This implies that f𝒜(Δ)f_{{\cal A}}(\Delta) is at the right of Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f). \Box

Arguing as above and using Case 2, one also deduces the following:

Claim 5.3.

Consider τ2>μλ\tau_{2}>\frac{\mu}{\lambda} and any uu{\operatorname{uu}}-disk Δ\Delta through a point (xs,xu,xc)(x^{s},x^{u},x^{c}) with xcτ2x^{c}\geq\tau_{2}. Then, for every α(0,1)\alpha\in(0,1) small enough,

  • f(Δ)f_{{}_{\cal B}}(\Delta) is at the right of Wlocs(P)W^{\operatorname{s}}_{\operatorname{loc}}(P),

  • assume that Δ\Delta is at the left of Wlocs(Q)W^{\operatorname{s}}_{\operatorname{loc}}(Q), then f(Δ)f_{{}_{\cal B}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f).

To get condition BH6), note that, since that (λ1)(0,1)(\lambda-1)\in(0,1), one has μλ<μλ(λ1)\frac{\mu}{\lambda}<\frac{\mu}{\lambda\,(\lambda-1)}. Now it is enough to note that, for α(0,1)\alpha\in(0,1) small enough, for every point (xs,xu,xc)(x^{s},x^{u},x^{c}) in a uu{\operatorname{uu}}-disk Δ\Delta in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f) one has:

  • either xc<μλ(λ1)x^{c}<\frac{\mu}{\lambda\,(\lambda-1)} and then, by Claim 5.2, f𝒜(Δ)f_{{}_{\cal A}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f),

  • or xc>μλx^{c}>\frac{\mu}{\lambda} and then, by Claim 5.3, f(Δ)f_{{}_{\cal B}}(\Delta) is in between Wlocs(P,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(P,f) and Wlocs(Q,f)W^{{\operatorname{s}}}_{{\operatorname{loc}}}(Q,f).

We have checked that the set Λ\Lambda satisfies conditions BH1)BH6). Therefore the set Λ\Lambda is a blender-horseshoe and the proof of Proposition 5.1 is complete. \Box

5.2 Strong homoclinic intersections and generation of blender-horseshoes

In this section, we state the generation of blender-horseshoes by saddle-node and flip periodic points with strong homoclinic intersections.

Let ff be a diffeomorphism with a periodic point SS such that the tangent bundle of MM at SS has a Dfπ(S)Df^{\pi(S)}-invariant dominated splitting TSM=Ess<Ec<EuuT_{S}M=E^{{\operatorname{ss}}}\oplus_{{}_{<}}E^{\operatorname{c}}\oplus_{{}_{<}}E^{\operatorname{uu}}, where EssE^{{\operatorname{ss}}} is uniformly contracting, EuuE^{\operatorname{uu}} is uniformly expanding, and EcE^{\operatorname{c}} is one-dimensional. We say that SS is a saddle-node (resp. flip) if the eigenvalue of Dfπ(S)Df^{\pi(S)} corresponding to the (one-dimensional) central direction EcE^{c} is 11 (resp. 1-1).

Consider the strong stable and unstable manifolds of the orbit of SS (denoted by Wss(S)W^{\operatorname{ss}}(S) and Wuu(S)W^{\operatorname{uu}}(S)). We say that the SS has a strong homoclinic intersection if there is a point XWss(S)Wuu(S)X\in W^{\operatorname{ss}}(S)\cap W^{\operatorname{uu}}(S) such that Xfi(S)X\neq f^{i}(S) for all ii. The point XX is a strong homoclinic point of ff associated to SS.

Let ff be a diffeomorphism with a strong homoclinic intersection associated to a saddle-node SS. In [9, Section 4.1] it is shown that there are k1k\geq 1 and a C1C^{1}-perturbation gg of ff such that gkg^{k} has an a affine horseshoe Λ\Lambda associated to SS whose central expansion is arbitrarily close to 11 (recall Section 5.1). Considering perturbations similar to the ones in Proposition 5.1, [9, Sections 4.1.1-2] gives the following:

Proposition 5.4.

Consider a diffeomorphism ff having a strong homoclinic intersection associated to a saddle-node SS. There is a diffeomorphism gg arbitrarily C1C^{1}-close to ff with a cu{\operatorname{cu}}-blender-horseshoe having SS as a reference saddle.

The same statement holds for cs{\operatorname{cs}}-blender-horseshoes, i.e. cu{\operatorname{cu}}-blender-horseshoes for f1f^{-1}.

We observe that in [9] the terminology blender-horseshoe it is not used. However, the constructions in [9] provide prototypical blender-horseshoes exactly as the ones in Section 5.1. In fact, these constructions are the main motivation (and model) for our definition of blender-horseshoe. Thus Proposition 5.4 just reformulates some results in [9] using this new terminology of blender-horseshoes.

For diffeomorphisms having flip points we need the following lemma (see [9, Remark 4.6]):

Lemma 5.5.

Consider a diffeomorphism ff having a strong homoclinic intersection associated to a flip point SS. There is a diffeomorphism gg arbitrarily C1C^{1}-close to ff having a saddle node SS^{\prime} with a strong homoclinic intersection and such that the orbit of SS^{\prime} remains in an arbitrarily small neighborhood of the orbit of the initial flip point SS.

Proof: Consider a 22-parameter family of deformations fs,tf_{s,t} of f=f0,0f=f_{0,0} such that

  • the parameter ss corresponds to a (non-generic) unfolding of the flip, generating a saddle-node SS^{\prime} close to the flip SS of period twice the period of SS, and

  • the parameter tt corresponds to the unfolding of the strong homoclinic intersection of the flip SS, the local strong stable manifold of SS “passing from the left to the right” of the local unstable manifold of SS.

Then for every s0s\neq 0 small enough, there is a small parameter t=t(s)t=t(s), t(s)0t(s)\to 0 as s0s\to 0, such that the saddle-node SS^{\prime} has a strong homoclinic intersection. \Box

5.3 Co-index one cycles and blender horseshoes

In this section, we borrow some arguments and results from [2, 9] in order to prove that diffeomorphisms with co-index one heterodimensional cycles yield blender-horseshoes.

Proposition 5.6.

Let ff be a diffeomorphism with a heterodimensional cycle associated to saddles PP and QQ with inds(P)=inds(Q)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)+1. Then there is gg arbitrarily C1C^{1}-close to ff with a saddle RR such that:

  1. 1.

    inds(R)=inds(Q){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(R)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q), the orbit of RR has a dominated splitting Ess<Ec<EuuE^{\operatorname{ss}}\oplus_{{}_{<}}E^{\operatorname{c}}\oplus_{{}_{<}}E^{\operatorname{uu}} with three non-trivial bundles such that EssE^{\operatorname{ss}} and EuuE^{\operatorname{uu}} are uniformly contracting and expanding, respectively, dim(Ess)=inds(Q)\dim(E^{\operatorname{ss}})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q), and dim(Ec)\dim(E^{\operatorname{c}}) has dimension one and is expanding,

  2. 2.

    there is cu{\operatorname{cu}}-blender-horseshoe of gg having RR as a reference saddle,

  3. 3.

    Ws(R)W^{\operatorname{s}}(R) intersects transversely Wu(Q)W^{\operatorname{u}}(Q), and

  4. 4.

    Wuu(R)W^{\operatorname{uu}}(R) meets transversely Ws(P)W^{\operatorname{s}}(P).

The arguments for proving this proposition can be found scattered along several constructions in [9]. But, unfortunately, this result is not stated explicitly there and its prove involves some adaptations of the constructions in [9]. As the proof of Proposition 5.6 is somewhat technical, we next explain the sequence of arguments we borrow from [9] and their adaptations in order to prove this proposition. The proof of Proposition 5.6 consists of several reductions to simpler cases we proceed to explain. Let us begin with a definition.

Definition 5.7 (Strong-intermediate saddles).

Let ff be a diffeomorphism having two periodic saddles PP and QQ of indices inds(P)=inds(Q)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)+1. A periodic point RR is strong-intermediate with respect to PP and QQ, denoted by Qu,ssRuu,sPQ\prec_{{\operatorname{u}},{\operatorname{ss}}}R\prec_{{\operatorname{uu}},{\operatorname{s}}}P, if:

  • the orbit of RR is partially hyperbolic and has a dominated splitting Ess<Ec<EuuE^{\operatorname{ss}}\oplus_{{}_{<}}E^{\operatorname{c}}\oplus_{{}_{<}}E^{\operatorname{uu}} with three non-trivial bundles such that EssE^{\operatorname{ss}} and EuuE^{\operatorname{uu}} are uniformly contracting and expanding, dim(Ess)=inds(Q)\dim(E^{\operatorname{ss}})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q), and dim(Ec)=1\dim(E^{\operatorname{c}})=1,

  • the strong stable manifold of RR meets transversely the unstable manifold of QQ and the strong unstable manifold of RR meets transversely the stable manifold of PP, in a formula,

    Wss(R)Wu(Q)andWuu(R)Ws(P).W^{\operatorname{ss}}(R)\pitchfork W^{\operatorname{u}}(Q)\neq\emptyset\quad\mbox{and}\quad W^{\operatorname{uu}}(R)\pitchfork W^{\operatorname{s}}(P)\neq\emptyset.

Note that if a (hyperbolic) saddle RR with inds(R)=inds(Q){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(R)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q) is strong-intermediate with respect to PP and QQ then it satisfies items 3 and 4 in Proposition 5.6.

We need the following lemma:

Lemma 5.8.

Consider two saddles PP and QQ in the same chain recurrence class CC and a periodic point RR which is strong-intermediate with respect to PP and QQ. Then RCR\in C.

Proof: We construct a pseudo-orbit going from RR to PP (the other pseudo-orbits are obtained similarly). Take a point XWss(R)Wu(Q)X\in W^{\operatorname{ss}}(R)\cap W^{\operatorname{u}}(Q). Note that there are arbitrarily large nn and mm such that {fn(X),,fm(X)}\{f^{-n}(X),\dots,f^{m}(X)\} is a segment of orbit starting (arbitrarily) close to RR and ending close to QQ. Since QQ and PP are in the same chain recurrent class, there is a finite pseudo-orbit going from QQ to PP. A pseudo-orbit going from RR to PP is obtained concatenating these two pseudo-orbits. This concludes the sketch of the proof of the lemma. \Box

We now explain the generation of strong-intermediate saddles.

5.3.1 Reduction to the case of cycles associated to saddles with real central eigenvalues

Given a periodic point RR of a diffeomorphism ff, write λ1(R),,λn(R)\lambda_{1}(R),\dots,\lambda_{n}(R) the eigenvalues of Dfπ(R)(R)Df^{\pi(R)}(R) counted with multiplicity and ordered in increasing modulus (|λi(R)||λi+1(R)||\lambda_{i}(R)|\leq|\lambda_{i+1}(R)|). We say that λi(R)\lambda_{i}(R) is the ii-th multiplier of RR.

Consider a diffeomorphism ff having a co-index one cycle associated to period points AA and BB with inds(P)=inds(Q)+1=s+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)+1=s+1. The cycle has real central eigenvalues if λs+1(A)\lambda_{s+1}(A) and λs+1(B)\lambda_{s+1}(B) are both real and

|λs(A)|<|λs+1(A)|<1<|λs+2(A)|and|λs(B)|<1<|λs+1(B)|<|λs+2(B)|.|\lambda_{s}(A)|<|\lambda_{s+1}(A)|<1<|\lambda_{s+2}(A)|\quad\mbox{and}\quad|\lambda_{s}(B)|<1<|\lambda_{s+1}(B)|<|\lambda_{s+2}(B)|.

Before proving Proposition 5.6, we recall the following two facts:

Fact 1: [9, Theorem 2.1] claims that, if ff has a co-index one cycle associated to AA and BB then there is gg arbitrarily C1C^{1}-close to ff with a co-index one cycle with real central eigenvalues. Moreover, this cycle can be chosen associated to saddles AgA^{\prime}_{g} and BgB^{\prime}_{g} homoclinically related to the continuations AgA_{g} and BgB_{g} of AA and BB, respectively.

Fact 2: Assume that there is a diffeomorphism hh arbitrarily C1C^{1}-close to gg having a cu{\operatorname{cu}}-blender-horseshoe Λ\Lambda with a reference saddle RhR_{h} which is strong-intermediate to AhA^{\prime}_{h} and BhB^{\prime}_{h}. Since two saddles being homoclinically related is a C1C^{1}-robust relation, one has RhR_{h} is strong-intermediate with respect to AhA_{h} and BhB_{h}. In this case, the proof of Proposition 5.6 is complete.

In view of these two facts, to prove Proposition 5.6 it is enough to consider the case where the saddles PP and QQ in the cycle have real central eigenvalues and to check that these cycles generate strong-intermediate saddles as in Fact 2, see Proposition 5.9. We now go to the details of this construction.

5.3.2 Reduction to the generation of saddle-node or flip points

In this section, we show that Proposition 5.6 is a consequence of the following result.

Proposition 5.9.

Let ff be a diffeomorphism with a co-index one cycle associated to saddles PP and QQ with real central eigenvalues. Then there is gg arbitrarily C1C^{1}-close to ff having a saddle-node or flip periodic point RgR_{g} such that:

  • RgR_{g} has a strong homoclinic intersection and

  • RgR_{g} is strong-intermediate to PgP_{g} and QgQ_{g}.

This proposition is a stronger version of [9, Theorem 2.3], adding the strong-intermediate property of RR with respect to PP and QQ.

Proposition 5.9 implies Proposition 5.6: First, observe that the strong unstable and strong stable manifolds of RgR_{g} depend continuously on the diffeomorphism (while there is defined a continuation of RgR_{g}).

If R=RgR=R_{g} is a saddle-node then Proposition 5.4 gives a diffeomorphism hh arbitrarily C1C^{1}-close to gg (thus arbitrarily close to ff) with a blender-horseshoe having RR as a reference saddle. Therefore, for hh close enough to gg, one gets the announced intersections between the strong invariant manifolds (intermediate intersections).

If RR is a flip then Lemma 5.5 gives a perturbation hh of gg with a saddle-node with a strong homoclinic intersection and with the strong-intermediate property. Thus we are in the first case. This completes the proof of our claim. \Box

Therefore it is enough to prove Proposition 5.9. The proof of the proposition is similar to the one of [9, Theorem 2.3] and consists of several steps. We next explain and adapt these steps.

5.3.3 Reduction to the creation of weak hyperbolic saddles

We now see that Proposition 5.9 (hence of Proposition 5.6) follows from:

Proposition 5.10.

Let ff be a diffeomorphism having a co-index one cycle associated to saddles PP and QQ, inds(P)=inds(Q)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)+1, with real central eigenvalues. Then there are a constant C>1C>1 and a sequence of diffeomorphisms (fn)(f_{n}), fnC1ff_{n}\stackrel{{\scriptstyle C^{1}}}{{\longrightarrow}}f, such that every fnf_{n} has a periodic point RnR_{n} such that:

  • RnR_{n} has a one-dimensional center-unstable direction whose corresponding multiplier λnc\lambda_{n}^{c} satisfies |λnc|[1C,C]|\lambda_{n}^{c}|\in[\frac{1}{C},C],

  • Wuu(Rn)W^{\operatorname{uu}}(R_{n}) and Wss(Rn)W^{\operatorname{ss}}(R_{n}) have a quasi-transverse intersection, therefore RnR_{n} has strong homoclinic intersections

  • the periods of RnR_{n} go to infinity as nn\to\infty, and

  • RnR_{n} is strong-intermediate with respect to PnP_{n} and QnQ_{n} (the continuations of PP and QQ for fnf_{n}).

This proposition is a stronger version [9, Proposition 3.3], adding the intersection property of the strong invariant manifolds.

Proposition 5.10 implies Proposition 5.9: We proceed exactly as in [9, page 484] (proof of Theorem 2.3 using Proposition 3.3). We just perform a local C1C^{1}-perturbation of fnf_{n} supported in a small neighborhood of RnR_{n}, turning the the central eigenvalue of RnR_{n} equal to ±1\pm 1 while keeping the strong homoclinic point of RnR_{n} and the transverse intersections Wss(Rn)Wu(Qn)W^{\operatorname{ss}}(R_{n})\pitchfork W^{\operatorname{u}}(Q_{n})\neq\emptyset and Wuu(Rn)Ws(Pn)W^{\operatorname{uu}}(R_{n})\pitchfork W^{\operatorname{s}}(P_{n})\neq\emptyset.

In this way, we get diffeomorphisms gg (arbitrarily close to ff) with saddle-node or flip points RgR_{g} (depending if λnc\lambda_{n}^{c} is positive or negative) with strong homoclinic intersections and being strong-intermediate with respect to PgP_{g} and QgQ_{g}. This completes the proof of Proposition 5.9. \Box

5.4 Proof of Proposition 5.10

The following steps of the proof of [9, Proposition 3.3] are described in [9, page 484]:

Step 1: One first puts the cycle in a kind of normal form called simple cycle. In fact, [9, Proposition 3.5] implies that, after a C1C^{1}-perturbation, one can assume that the cycle is simple.

Step 2: One shows that the dynamics in a simple cycle is given (up to a renormalization) by a model family, denoted by Fλ,β,t±,±F^{\pm,\pm}_{\lambda,\beta,t}. Moreover, perturbations of this model family correspond to perturbations of the initial dynamics.

Therefore, to prove Proposition 5.10, it is enough to consider model families Fλ,β,t±,±F^{\pm,\pm}_{\lambda,\beta,t} and their perturbations. Hence it is enough to adapt the perturbations of these normal families in order to get the intersection properties between the strong invariant manifolds.

Proposition 3.8 in [9] claims that the unfolding of co-index one cycles generates sequences of saddles An,mA_{n,m} whose orbits are contained in a neighborhood of the cycle. We now see that these saddles can be taken with the strong-intermediate property (relative to saddles in the initial cycle).

Lemma 5.11.

In [9, Proposition 3.8], for every integer n,mn,m large enough, (in fact larger that the integer NN in the statement), all periodic points An,mA_{n,m} in the proposition are strong-intermediate with respect to PP and QQ.

Note that we have the following string of implications:

Lemma 5.11Proposition 5.10Proposition 5.9Proposition 5.6.\mbox{Lemma~\ref{l.intermediate}}\Rightarrow\mbox{Proposition~\ref{p.weak}}\Rightarrow\mbox{Proposition~\ref{p.saddleblenders}}\Rightarrow\mbox{Proposition~\ref{p.coindexblenders}}.

Therefore to prove Proposition 5.6 it remains to prove Lemma 5.11.

Proof: The model maps Fλ,β,t±,±F^{\pm,\pm}_{\lambda,\beta,t} are defined on some cubes and their restrictions to each of these cubes are affine maps 𝒜λ{\cal A}_{\lambda}, β{\cal B}_{\beta}, 𝒯1,t±{\cal T}^{\pm}_{1,t}, and 𝒯2±{\cal T}^{\pm}_{2} which preserve a constant dominated splitting: the strong stable bundle is the horizontal space s×{(0,0u)}{\mathbb{R}}^{s}\times\{(0,0^{u})\}, the strong unstable bundles is the vertical one {(0s,0)}×u\{(0^{s},0)\}\times{\mathbb{R}}^{u}, and the center bundle is one dimensional {0s}××{0u}\{0^{s}\}\times{\mathbb{R}}\times\{0^{u}\}. More precisely (see Figure 10):

\psfrag{Yp}{$Y$}\psfrag{Xp}{$f^{N_{2}}(X)$}\psfrag{Yq}{$f^{N_{1}}(Y)$}\psfrag{Xq}{$X$}\psfrag{Yq}{$f^{N_{1}}(Y)$}\psfrag{Xq}{$X$}\psfrag{A}{${\cal A}_{\lambda}$}\psfrag{B}{${\cal B}_{\beta}$}\psfrag{Es}{$E^{ss}$}\psfrag{Eu}{$E^{uu}$}\psfrag{Ec}{$E^{c}$}\psfrag{P}{$P$}\psfrag{Q}{$Q$}\psfrag{T1}{${\mathfrak{T}}_{1,t}$}\psfrag{T2}{${\mathfrak{T}}_{2}$}\includegraphics[height=130.08621pt]{transitions.eps}
Figure 10: The model maps Fλ,β,t±,±F^{\pm,\pm}_{\lambda,\beta,t}.
  • The maps 𝒜λ{\cal A}_{\lambda} and β{\cal B}_{\beta} are Dfπ(P)(P)Df^{\pi(P)}(P) and Dfπ(Q)(Q)Df^{\pi(Q)}(Q) and correspond to iterates of ff close to PP and QQ, respectively.

  • The sub-scripts λ\lambda and β\beta correspond to the central multipliers of Dfπ(P)(P)Df^{\pi(P)}(P) and Dfπ(Q)(Q)Df^{\pi(Q)}(Q).

  • The maps 𝒯1,t±{\cal T}^{\pm}_{1,t} and 𝒯2±{\cal T}^{\pm}_{2} are the transitions of the cycle. The map 𝒯2±{\cal T}^{\pm}_{2} corresponds to a fixed number N2N_{2} of iterates from a neighborhood of QQ to a neighborhood of PP following a segment of orbit of a transverse heteroclinic point XX in Ws(P)Wu(Q)W^{\operatorname{s}}(P)\pitchfork W^{\operatorname{u}}(Q).

    Similarly, the map 𝒯1,t±{\cal T}^{\pm}_{1,t} corresponds to a fixed number N1N_{1} of iterates from a neighborhood of PP to a neighborhood of QQ following a segment of orbit of a fixed quasi-transverse heteroclinic point YY in Wu(P)Ws(Q)W^{\operatorname{u}}(P)\pitchfork W^{\operatorname{s}}(Q). The parameter tt of 𝒯1,t±{\cal T}^{\pm}_{1,t} corresponds to the unfolding of the cycle.

  • The super-script ±\pm is positive if the transition map preserves the orientation in the central bundle and negative if otherwise.

For details see [9, page 488].

\psfrag{Yp}{$Y$}\psfrag{Xp}{$f^{N_{2}}(X)$}\psfrag{Yq}{$f^{N_{1}}(Y)$}\psfrag{Xq}{$X$}\psfrag{Yq}{$f^{N_{1}}(Y)$}\psfrag{Xq}{$X$}\psfrag{A}{${\cal A}_{\lambda}$}\psfrag{amn}{$A_{m,n}$}\psfrag{B}{${\cal B}_{\beta}$}\psfrag{Es}{$E^{ss}$}\psfrag{Eu}{$E^{uu}$}\psfrag{Ec}{$E^{c}$}\psfrag{wsp}{$W^{s}(P)$}\psfrag{wuq}{$W^{u}(Q)$}\psfrag{P}{$P$}\psfrag{Q}{$Q$}\psfrag{T1}{${\mathfrak{T}}_{1,t}$}\psfrag{T2}{${\mathfrak{T}}_{2}$}\includegraphics[height=144.54pt]{amn.eps}
Figure 11: The intermediate saddle Am,nA_{m,n}.

By definition, the points Am,n=(as,a,au)A_{m,n}=(a^{s},a,a^{u}) are fixed points of the composition βn𝒯1,t±𝒜λm𝒯2±{\cal B}_{\beta}^{n}\circ{\cal T}^{\pm}_{1,t}\circ{\cal A}_{\lambda}^{m}\circ{\cal T}^{\pm}_{2}. In particular, the point Am,nA_{m,n} belongs to domain of definition ΣQ\Sigma_{Q} of 𝒯2±{\cal T}^{\pm}_{2}, see Figure 11. This domain (defined in [9, page 488]) is the cube

ΣQ=[1,1]s×[bQδ,bQ+δ]×[1,1]u,\Sigma_{Q}=[-1,1]^{s}\times[b_{Q}-\delta,b_{Q}+\delta]\times[-1,1]^{u},

where

[1,1]s×[bQδ,bQ+δ]×{0u}Ws(P)and{0s}×[bQδ,bQ+δ]×[1,1]uWu(Q).[-1,1]^{s}\times[b_{Q}-\delta,b_{Q}+\delta]\times\{0^{u}\}\subset W^{\operatorname{s}}(P)\quad\mbox{and}\quad\{0^{s}\}\times[b_{Q}-\delta,b_{Q}+\delta]\times[-1,1]^{u}\subset W^{\operatorname{u}}(Q).

Moreover, the local strong stable and strong unstable manifolds of the point Am,n=(as,a,au)A_{m,n}=(a^{s},a,a^{u}) are (see [9, page 495, first paragraph]):

Wlocss(Am,n)=[1,1]s×{(a,au)}andWlocuu(Am,n)={(as,a)}×[1,1]u.W^{\operatorname{ss}}_{\operatorname{loc}}(A_{m,n})=[-1,1]^{s}\times\{(a,a^{u})\}\quad\mbox{and}\quad W^{\operatorname{uu}}_{\operatorname{loc}}(A_{m,n})=\{(a^{s},a)\}\times[-1,1]^{u}.

This means that

Wss(Am,n)Wu(Q)andWlocuu(Am,n)Ws(P).W^{\operatorname{ss}}(A_{m,n})\pitchfork W^{\operatorname{u}}(Q)\neq\emptyset\quad\mbox{and}\quad W^{\operatorname{uu}}_{\operatorname{loc}}(A_{m,n})\pitchfork W^{\operatorname{s}}(P)\neq\emptyset.

Therefore the saddle Am,nA_{m,n} is strong-intermediate with respect to PP and QQ, ending the proof of the lemma. \Box

6 Robust tangencies and heterodimensional cycles for C1C^{1}-generic diffeomorphisms

In this section, we prove Theorem 1. First, in Section 6.1, we state some properties about C1C^{1}-generic diffeomorphisms. In Section 6.2, we state the C1C^{1}-generic occurrence of blender-horseshoes in homoclinic classes containing saddles of different indices (Theorem 6.4). Finally, in Section 6.3, we state the existence of robust homoclinic tangencies inside homoclinic classes with index variation and lack of domination (Proposition 6.11), completing the proof of Theorem 1. We close this paper presenting and extension of [9, Theorem 1.16] about the occorrence of robust heterodimensional cycles inside chain recurrence classes (see Theorem 3 in Section 6.4).

6.1 C1C^{1}-generic properties of C1C^{1}-diffeomorphisms

We now collect some properties of C1C^{1}-generic diffeomorphisms. According to [7, Remarque 1.10] and [2, Theorem 1], there is a residual subset set 𝒢{\cal G} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that, for every f𝒢f\in{\cal G},

  • every periodic point of ff is hyperbolic,

  • for every periodic point PP of ff, its homoclinic class H(P,f)H(P,f) and its chain recurrence class C(P,f)C(P,f) are equal,

  • any homoclinic class H(P,f)H(P,f) containing periodic points of u{\operatorname{u}}-indices α\alpha and β\beta also contains saddles of u{\operatorname{u}}-index τ\tau, for every τ[α,β]\tau\in[\alpha,\beta]\cap{\mathbb{N}}.

Lemma 6.1.

([2, Lemma 2.1]) There is a residual subset 𝒢0𝒢{\cal G}_{0}\subset{\cal G} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that, for every f𝒢0f\in{\cal G}_{0} and every pair of periodic points PfP_{f} and QfQ_{f} of ff, there is a neighborhood 𝒰f{\cal U}_{f} of ff in 𝒢0{\cal G}_{0} such that:

  • either H(Pg,g)=H(Qg,g)H(P_{g},g)=H(Q_{g},g) for all g𝒰f𝒢0g\in{\cal U}_{f}\cap{\cal G}_{0},

  • or H(Pg,g)H(Qg,g)=H(P_{g},g)\cap H(Q_{g},g)=\emptyset for all g𝒰f𝒢0g\in{\cal U}_{f}\cap{\cal G}_{0}.

Remark 6.2 (Proof of Claim 2.2 in [2]).

Using a filtration given by Conley theory, one has that the property of two hyperbolic saddles to be in different chain recurrence classes is C1C^{1}-robust.

Next lemma claims that, for C1C^{1}-generic diffeomorphisms, the property of the chain recurrence classes of two periodic points to be equal is also a C1C^{1}-robust property.

Lemma 6.3.

Let 𝒢0{\cal G}_{0} be the residual set of of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) in Lemma 6.1. For every f𝒢0f\in{\cal G}_{0} and every pair of periodic points PfP_{f} and QfQ_{f} of ff, the property of QfQ_{f} belonging to the chain recurrence class C(Pf,f)C(P_{f},f) of PfP_{f} is C1C^{1}-robust: if QfC(Pf,f)Q_{f}\in C(P_{f},f) then QgC(Pg,g)Q_{g}\in C(P_{g},g) for all gg C1C^{1}-close to ff.

Proof: Let f𝒢0f\in{\cal G}_{0} and suppose that QfC(Pf,f)Q_{f}\in C(P_{f},f). Since f𝒢f\in{\cal G} one has that C(Pf,f)=H(Pf,f)C(P_{f},f)=H(P_{f},f). As f𝒢0f\in{\cal G}_{0}, by Lemma 6.1, there is a C1C^{1}-open neighborhood 𝒰f{\cal U}_{f} of ff such that H(Pg,g)=H(Qg,g)H(P_{g},g)=H(Q_{g},g) for every g𝒰f𝒢0g\in{\cal U}_{f}\cap{\cal G}_{0}. In particular, QgH(Pg,g)Q_{g}\in H(P_{g},g) for all g𝒰f𝒢0g\in{\cal U}_{f}\cap{\cal G}_{0}.

Assume that there is g𝒰fg\in{\cal U}_{f} such that QgC(Pg,g)Q_{g}\notin C(P_{g},g). By Remark 6.2, one has that QhC(Ph,h)Q_{h}\notin C(P_{h},h) for every hh in a small neighborhood 𝒱g{\cal V}_{g} of gg contained in 𝒰f{\cal U}_{f}. Choosing h𝒢0𝒱gh\in{\cal G}_{0}\cap{\cal V}_{g} one gets that QhC(Ph,h)=H(Ph,h)Q_{h}\not\in C(P_{h},h)=H(P_{h},h), a contradiction. \Box

6.2 Generation of blender-horseshoes

In this section, we prove that blender-horseshoes occur C1C^{1}-generically for homoclinic classes with index variability (i.e., containing saddles with different indices).

Theorem 6.4.

There is a residual subset {\cal R} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) of diffeomorphisms ff such that for every homoclinic class H(P,f)H(P,f) containing a hyperbolic saddle QQ with inds(Q)>inds(P){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P) there is a transitive hyperbolic set Σ\Sigma containing PP and a cu{\operatorname{cu}}-blender-horseshoe Λ\Lambda.

Applying Theorem 6.4 to f1f^{-1} one gets the following.

Remark 6.5.

Under the assumptions of Theorem 6.4, every C1C^{1}-generic diffeomorphism ff has a cs{\operatorname{cs}}-blender-horseshoe containing QQ and contained in a transitive hyperbolic set.

We first prove a version of Theorem 6.4 for a given fixed saddle PfP_{f}:

Proposition 6.6.

Let 𝒰{\cal U} be an open subset of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) and fPff\mapsto P_{f} be a continuous map defined on 𝒰{\cal U} associating to each f𝒰f\in{\cal U} a hyperbolic periodic point PfP_{f} of ff.

There is a residual subset =P{\cal R}={\cal R}_{P} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) with the following property. For every diffeomorphism f𝒰f\in{\cal R}\cap{\cal U} such that H(Pf,f)H(P_{f},f) contains a saddle BfB_{f} with inds(Bf)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(B_{f})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}) there is a transitive hyperbolic set Σf\Sigma_{f} containing PfP_{f} and a cu{\operatorname{cu}}-blender-horseshoe Λf\Lambda_{f}.

Theorem 6.4 will follow from this proposition using standard genericity arguments (the details can be found in the end of this subsection).

Proof of Proposition 6.4: Consider the residual subset 𝒢0{\cal G}_{0} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) in Lemma 6.1. Given any f𝒢0𝒰f\in{\cal G}_{0}\cap{\cal U}, if H(P,f)H(P,f) contains a saddle BfB_{f} with inds(Bf)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(B_{f})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}), then there is a saddle QfH(Pf,f)Q_{f}\in H(P_{f},f) with inds(Qf)=inds(Pf)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f})+1. Furthermore, by Lemma 6.3, if f𝒢0f\in{\cal G}_{0} the point QfQ_{f} belongs robustly to the chain recurrence class C(Pf,f)C(P_{f},f). Moreover, C(Pf,f)=H(Pf,f)C(P_{f},f)=H(P_{f},f).

Let 𝒲{\cal W} be the set of diffeomorphisms:

𝒲={f𝒰:there is a saddle QfPer(f) withinds(Qf)=inds(Pf)+1,andQf is C1-robustly in C(Pf,f)}{\cal W}=\left\{f\in{\cal U}\colon\mbox{there is a saddle $Q_{f}\in\mbox{{\rm Per}}(f)$ with}\quad\begin{array}[]{ll}&{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f})+1,\\ &\mbox{and}\\ &\mbox{$Q_{f}$ is $C^{1}$-robustly in $C(P_{f},f)$}\end{array}\right\}

By definition, the set 𝒲{\cal W} is an open subset of 𝒰{\cal U}. Let

𝒰1=𝒰𝒲¯.{\cal U}_{1}={\cal U}\setminus\overline{{\cal W}}.

By construction the set 𝒰1{\cal U}_{1} is open and 𝒰1𝒲{\cal U}_{1}\cup{\cal W} is dense in 𝒰{\cal U}.

Claim 6.7.

Let f𝒢0𝒰1f\in{\cal G}_{0}\cap{\cal U}_{1}. Then C(Pf,f)C(P_{f},f) does not contain any hyperbolic periodic point Q~\tilde{Q} with inds(Q~)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(\tilde{Q})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}).

Proof: The proof is by contradiction. Suppose that there is a saddle Q~C(Pf,f)\tilde{Q}\in C(P_{f},f) with inds(Q~)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(\tilde{Q})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}). As f𝒢0f\in{\cal G}_{0}, there is a saddle QfC(Pf,f)=H(Pf,f)Q_{f}\in C(P_{f},f)=H(P_{f},f) with inds(Qf)=inds(Pf)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f})+1. As f𝒢0f\in{\cal G}_{0}, the saddle QfQ_{f} belongs C1C^{1}-robustly to C(Pf,f)C(P_{f},f). Therefore f𝒲f\in{\cal W}, contradicting the definition of 𝒰1{\cal U}_{1}. \Box

Thus, by Lemma 6.3, it is enough to prove Proposition 6.6 for diffeomorphisms in 𝒲{\cal W}. In other words, next lemma implies Proposition 6.6.

Lemma 6.8.

The open set of diffeomorphisms ff having a transitive hyperbolic set Σf\Sigma_{f} containing PfP_{f} and a cu{\operatorname{cu}}-blender-horseshoe Λf\Lambda_{f} is dense in 𝒲{\cal W}.

Proof: Consider f𝒲f\in{\cal W} and a saddle QfQ_{f} with inds(Qf)=inds(Pf)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f})+1 which belongs robustly to C(Pf,f)C(P_{f},f). Next lemma is an immediate consequence of Hayashi connecting lemma in [18]:

Lemma 6.9 ([18]).

Let ff be a diffeomorphism having a pair of (hyperbolic) saddles AfA_{f} and BfB_{f} whose orbits are different and such that BfH(Af,f)B_{f}\in H(A_{f},f). Then there is gg arbitrarily C1C^{1}-close to ff such that Wu(Ag,g)Ws(Bg,g)W^{\operatorname{u}}(A_{g},g)\cap W^{\operatorname{s}}(B_{g},g)\neq\emptyset.

Note that as f𝒲f\in{\cal W} we have QfC(Pf,f)Q_{f}\in C(P_{f},f) in a robust way. After a first perturbation, we can assume that f𝒢0f\in{\cal G}_{0} so that QfH(Pf,f)Q_{f}\in H(P_{f},f). We apply Lemma 6.9 to the saddles PfP_{f} and QfQ_{f} to get a diffeomorphism gg close to ff with a transverse intersection between Wu(Pg,g)W^{\operatorname{u}}(P_{g},g) and Ws(Qg,g)W^{\operatorname{s}}(Q_{g},g). Note that this transverse intersection persists after perturbation, so that we can assume that g𝒲𝒢0g\in{\cal W}\cap{\cal G}_{0}. After a new application of Lemma 6.9 we can suppose that Ws(Pg,g)Wu(Qg,g)W^{\operatorname{s}}(P_{g},g)\cap W^{\operatorname{u}}(Q_{g},g)\neq\emptyset. Therefore there is gg arbitrarily C1C^{1}-close to ff, having a co-index one cycle associated to PgP_{g} and QgQ_{g}.

Applying Proposition 5.6 to the diffeomorphism gg with a co-index one cycle (associated to PgP_{g} and QgQ_{g}), we get hh close to gg, thus close to ff, with a periodic point RhR_{h} such that

  • RhR_{h} is strong-intermediate with respect to PhP_{h} and QhQ_{h},

  • RhR_{h} has the same index as PhP_{h}, and

  • RhR_{h} is a reference saddle of a cu{\operatorname{cu}}-blender-horseshoe Λh\Lambda_{h}.

Recall that, by Lemma 3.9, the continuation of this blender-horseshoe is defined in a neighborhood of hh. Thus we can assume that h𝒢0h\in{\cal G}_{0}.

As the saddle RhR_{h} is (robustly) intermediate with respect to PhP_{h} and QhQ_{h} and QhC(Ph,h)Q_{h}\in C(P_{h},h), Lemma 5.8 implies that RhC(Ph,h)R_{h}\in C(P_{h},h). Thus, from Lemma 6.3, we have that RhR_{h} belongs robustly to C(Ph,h)C(P_{h},h). As RhR_{h} and PhP_{h} have the same index, Lemma 6.9 gives a perturbation φ\varphi of hh with transverse intersections between the invariant manifolds of these saddles. That is, the saddles RφR_{\varphi} and PφP_{\varphi} are homoclinically related, thus their homoclinic classes are equal. Therefore there is a transitive hyperbolic set Σφ\Sigma_{\varphi} containing PφP_{\varphi} and the cu{\operatorname{cu}}-blender-horseshoe Λφ\Lambda_{\varphi} (the continuation of Λh\Lambda_{h}). This ends the proof of the lemma. \Box

The proof of Proposition 6.6 is now complete. \Box

Proof of Theorem 6.4: Given a diffeomorphism ff, denote by Pern(f)\mbox{{\rm Per}}_{n}(f) the set of periodic points PP of ff of period π(P)n\pi(P)\leq n. To prove Theorem 6.4 it is enough to see that, for every nn\in{\mathbb{N}}, there is a residual set n{\cal R}_{\leq n} of diffeomorphisms ff such that the conclusion of the theorem holds for every periodic orbit PPern(f)P\in\mbox{{\rm Per}}_{n}(f). Then it is enough to take =nn{\cal R}=\cap_{n}{\cal R}_{\leq n}.

Note that there is a C1C^{1}-open an dense subset 𝒪nDiff 1(M){\cal O}_{n}\subset\mbox{{\rm Diff\,}}^{1}(M) of diffeomorphisms ff such that every periodic point PPern(f)P\in\mbox{{\rm Per}}_{n}(f) is hyperbolic. In particular, the cardinal of Pern(f)\mbox{{\rm Per}}_{n}(f) is finite an locally constant in 𝒪n{\cal O}_{n}. Moreover, each periodic point PPern(f)P\in\mbox{{\rm Per}}_{n}(f) has a hyperbolic continuation in each (open) connected component 𝒰{\cal U} of the open set 𝒪n{\cal O}_{n}. That is, there are a constant k=k(𝒰)k=k({\cal U}) and continuous maps fPi,ff\mapsto P_{i,f}, i=1,,ki=1,\dots,k, such that Pern(f)={P1,f,,Pk,f}\mbox{{\rm Per}}_{n}(f)=\{P_{1,f},\dots,P_{k,f}\}, for every f𝒰f\in{\cal U}.

Note that the set cc(𝒪n)\mbox{cc}({\cal O}_{n}) of connected components of 𝒪n{\cal O}_{n} is countable. Therefore to prove Theorem 6.4 for periods πn\pi\leq n it is enough to see that this result holds in each connected component 𝒰{\cal U} of 𝒪n{\cal O}_{n}. More precisely, for each connected component 𝒰{\cal U} of 𝒪n{\cal O}_{n}, we first build a residual subset 𝒰~\widetilde{{\cal R}_{\cal U}} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that the conclusion holds in the set 𝒰~𝒰\widetilde{{\cal R}_{\cal U}}\cap{\cal U}. We now consider the set

𝒰=𝒰~(𝒪n𝒰).{\cal R}_{\cal U}=\widetilde{{\cal R}_{\cal U}}\cup({\cal O}_{n}\setminus{\cal U}).

Note that the set 𝒪n𝒰{\cal O}_{n}\setminus{\cal U} is the union of the open connected components of 𝒪n{\cal O}_{n} different from 𝒰{\cal U}. Thus the set 𝒪n𝒰{\cal O}_{n}\setminus{\cal U} is open (and closed) in 𝒪n{\cal O}_{n} and therefore the set 𝒰{\cal R}_{\cal U} is residual in Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M). Finally, the announced residual subset n{\cal R}_{\leq n} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) is the countable intersection of the residual subsets 𝒰{\cal R}_{\cal U} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M):

n=𝒰cc(𝒪n)𝒰.{\cal R}_{\leq n}=\bigcap_{{\cal U}\in\mbox{cc}({\cal O}_{n})}{\cal R}_{\cal U}.

To complete the proof of the theorem it remains to define 𝒰~\widetilde{{\cal R}_{\cal U}} for each component 𝒰{\cal U} of 𝒪n{\cal O}_{n}. Given f𝒰f\in{\cal U} consider Pern(f)={P1,f,,Pk,f}\mbox{{\rm Per}}_{n}(f)=\{P_{1,f},\dots,P_{k,f}\}. For each i=1,,ki=1,\dots,k, Proposition 6.6 gives a residual subset Pi{\cal R}_{P_{i}} of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) where the conclusion holds. The residual set 𝒰~\widetilde{{\cal R}_{\cal U}} is the finite intersection of the residual sets Pi{\cal R}_{P_{i}}. The proof of Theorem 6.4 is now complete. \Box

6.3 Robust homoclinic tangencies under lack of domination

In this section, we conclude the proof of Theorem 1 about C1C^{1}-generic existence of robust homoclinic tangencies inside homoclinic classes with index variation and lack of domination. We first recall a key result stating the relation between lack of domination and homoclinic tangencies.

Theorem 6.10 (Theorem 1.1 in [16]).

Let PfP_{f} be a saddle of a diffeomorphism ff such that the stable/unstable splitting defined over the set of periodic points homoclinically related with PfP_{f} is not dominated. Then there is a diffeomorphism hh arbitrarily C1C^{1}-close to ff with a homoclinic tangency associated to PhP_{h}.

As in Section 6.2, we begin with a version of Theorem 1 for a given fixed saddle.

Proposition 6.11.

Consider a diffeomorphism gg and a hyperbolic saddle PgP_{g} of gg. Let 𝒰{\cal U} be an open subset of Diff 1(M)\mbox{{\rm Diff\,}}^{1}(M) such that the map fPff\mapsto P_{f} (PfP_{f} a hyperbolic saddle) is continuous and well defined. Then there is a residual subset 𝒢𝒰{\cal G}_{\cal U} of 𝒰{\cal U} with the following property. Let f𝒢𝒰f\in{\cal G}_{\cal U} be any diffeomorphism such that:

  • the chain recurrence class C(Pf,f)C(P_{f},f) has a periodic point QfQ_{f} with inds(Qf)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}) and

  • C(Pf,f)C(P_{f},f) does not admit a dominated splitting E<FE\oplus_{{}_{<}}F with dim(E)=inds(Pf)\dim(E)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}).

The C(Pf,f)C(P_{f},f) has a transitive hyperbolic set containing PfP_{f} with a C1C^{1}-robust homoclinic tangency.

Proof: Let 𝒲0𝒰{\cal W}_{0}\subset{\cal U} be the set of diffeomorphisms ff such that the chain recurrence class C(Pf,f)C(P_{f},f) of PfP_{f} contains robustly a hyperbolic periodic point QfQ_{f} with inds(Qf)>inds(Pf){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{f})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}) (i.e., QgC(Pg,g)Q_{g}\in C(P_{g},g) for all gg C1C^{1}-close to ff). By definition and Remark 6.2, the set 𝒲0{\cal W}_{0} is open and non-empty. Let

𝒰0=𝒰𝒲0¯.{\cal U}_{0}={\cal U}\setminus\overline{{\cal W}_{0}}.

Note that 𝒰0𝒲0{\cal U}_{0}\cup{\cal W}_{0} is an open and dense subset of 𝒰{\cal U}.

Let 𝒰1𝒰{\cal U}_{1}\subset{\cal U} be the set of diffeomorphisms ff such that C(Pf,f)C(P_{f},f) has a dominated splitting E<FE\oplus_{{}_{<}}F with dim(E)=inds(Pf)\dim(E)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{f}). Since the map fC(Pf,f)f\mapsto C(P_{f},f) is upper-semi-continuous and a dominated splitting persists in a neighborhood of C(Pf,f)C(P_{f},f) by perturbations (for instance, see [13, Chapter B.1]), one gets that the set 𝒰1{\cal U}_{1} is open. Let

𝒲1=𝒰𝒰1¯.{\cal W}_{1}={\cal U}\setminus\overline{{\cal U}_{1}}.

Then the set 𝒰1𝒲1{\cal U}_{1}\cup{\cal W}_{1} is open and dense in 𝒰{\cal U}. As a consequence, the open sets 𝒰0𝒰1{\cal U}_{0}\cup{\cal U}_{1} and 𝒲0𝒲1{\cal W}_{0}\cap{\cal W}_{1} are disjoint and their union is dense in 𝒰{\cal U}.

Note that we are interested in the subset of 𝒰{\cal U} of diffeomorphisms ff whose chain recurrence class C(Pf,f)C(P_{f},f) contains points of different indices and has not an appropriate dominated splitting, that is, the set set 𝒲0𝒲1{\cal W}_{0}\cap{\cal W}_{1}. Thus next lemma implies the proposition.

Lemma 6.12.

The set 𝒯{\cal T} of diffeomorphisms gg having a hyperbolic set Σg\Sigma_{g} containing PgP_{g} and with a C1C^{1}-robust homoclinic tangency is open and dense in 𝒲0𝒲1{\cal W}_{0}\cap{\cal W}_{1}.

Proof: It is enough to prove the density of the set 𝒯{\cal T}. Let g𝒲0𝒲1g\in{\cal W}_{0}\cap{\cal W}_{1}. As g𝒲0g\in{\cal W}_{0} there is a saddle QgQ_{g} with inds(Qg)>inds(Pg){\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q_{g})>{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P_{g}) such that QgQ_{g} belongs robustly to C(Pg,g)C(P_{g},g). After a C1C^{1}-perturbation, we can assume that the diffeomorphism gg simultaneously belongs to the residual set 𝒢{\cal G} where C(Pg,g)=H(Pg,g)C(P_{g},g)=H(P_{g},g) and to the residual set {\cal R} in Theorem 6.4. Note that:

  • By Theorem 6.4, the set of diffeomorphisms gg having a cu{\operatorname{cu}}-blender horseshoe Λg\Lambda_{g} which is contained in a transitive hyperbolic set containing PgP_{g} is open and dense in 𝒲0{\cal W}_{0}.

  • As g𝒲1g\in{\cal W}_{1} and H(Pg,g)=C(Pg,g)H(P_{g},g)=C(P_{g},g), one has that the stable/unstable splitting defined over the set of periodic points homoclinically related with PgP_{g} is not dominated. Otherwise, this dominated splitting could be extended to the closure of these points (the whole H(Pg,g)H(P_{g},g)) in a dominated way (see [13, Chapter B.1]), which is a contradiction.

  • Since the stable/unstable splitting defined over the set of periodic points homoclinically related with PgP_{g} is not dominated, Theorem 6.10 implies that there is a diffeomorphism hh arbitrarily C1C^{1}-close to gg with a homoclinic tangency associated to PhP_{h}.

Theorem 4.8 now implies that there is a diffeomorphism φ\varphi arbitrarily close to gg with a transitive hyperbolic set containing PφP_{\varphi} and having a robust homoclinic tangency. This ends the proof of the lemma. \Box

The proof of Proposition 6.11 is now complete. \Box

6.3.1 End of the proof of Theorem 1

The proof of Theorem 1 using Proposition 6.11 is almost identical to the proof of Theorem 6.4 using Proposition 6.6. It is enough to see that, for every nn\in{\mathbb{N}}, there is a residual set 𝒢n{\cal G}_{\leq n} of diffeomorphisms ff for which the conclusion of the theorem holds for the points in Pern(f)\mbox{{\rm Per}}_{n}(f).

This proof is similar to the one of Theorem 6.4. So we will omit some details. As in Theorem 6.4, we consider the C1C^{1}-open an dense subset 𝒪nDiff 1(M){\cal O}_{n}\subset\mbox{{\rm Diff\,}}^{1}(M) of diffeomorphisms ff such that every periodic point in Pern(f)\mbox{{\rm Per}}_{n}(f) is hyperbolic. Recall that the number of elements of Pern(f)\mbox{{\rm Per}}_{n}(f) is finite and locally constant, and that each periodic point in Pern(f)\mbox{{\rm Per}}_{n}(f) has a hyperbolic continuation on each (open) connected component of 𝒪n{\cal O}_{n}.

To state Theorem 1 for periodic points in Pern(f)\mbox{{\rm Per}}_{n}(f), it is enough to prove it in each connected component 𝒰cc(𝒪n){\cal U}\in\mbox{cc}({\cal O}_{n}) (recall that cc(𝒪n)\mbox{cc}({\cal O}_{n}) is countable): for each connected component 𝒰{\cal U}, we construct a residual subset 𝒢𝒰~\widetilde{{\cal G}_{\cal U}} such that the conclusion holds in the set 𝒢𝒰~𝒰\widetilde{{\cal G}_{\cal U}}\cap{\cal U}. Then we let

𝒢𝒰=𝒢𝒰~(𝒪n𝒰){\cal G}_{\cal U}=\widetilde{{\cal G}_{\cal U}}\cup({\cal O}_{n}\setminus{\cal U})

and define

𝒢n=𝒰cc(𝒪n)𝒢𝒰.{\cal G}_{\leq n}=\bigcap_{{\cal U}\in\mbox{cc}({\cal O}_{n})}{\cal G}_{\cal U}.

To define 𝒢𝒰~\widetilde{{\cal G}_{\cal U}} for a component 𝒰{\cal U} of 𝒪n{\cal O}_{n}, given f𝒰f\in{\cal U} write Pern(f)={P1,f,,Pk,f}\mbox{{\rm Per}}_{n}(f)=\{P_{1,f},\dots,P_{k,f}\} (k=k(𝒰)k=k({\cal U})) and consider the continuous maps fPi,ff\mapsto P_{i,f}, i{1,,k}i\in\{1,\dots,k\}, defined on 𝒰{\cal U}. For each ii, Proposition 6.11 provides a residual subset where the conclusion of the theorem holds for Pi,fP_{i,f}. Now it is enough to define 𝒢𝒰~\widetilde{{\cal G}_{\cal U}} as the intersection of these residual sets. The proof of Theorem 1 is now complete. \Box

6.4 Robust cycles in non-hyperbolic chain recurrence classes

We close this paper by stating an extension of [9, Theorem 1.16]. The novelty of this version is that the hyperbolic sets involved in the robust cycle are contained in a prescribed chain recurrence class. We note that [9] does not give information about the relation between the hyperbolic set involved in the robust cycle and the saddles in the initial cycle.

Theorem 3.

There is a residual subset Diff 1(M){\cal R}\subset\mbox{{\rm Diff\,}}^{1}(M) with the following property. Consider any diffeomorphism ff\in{\cal R} having a chain recurrence class CC with two saddles PP and QQ such that inds(P)=inds(Q)+1{\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(P)={\mbox{\rm{ind}}^{\,{\operatorname{s}}}}(Q)+1. Then ff has a C1C^{1}-robust heterodimensional cycle associated to hyperbolic sets Λ\Lambda and Σ\Sigma containing PP and QQ.

Since this result follows from arguments similar to the ones in the previous sections and as robust heterodimensional cycles is not the main topic of this paper, we just give some hints for the proof.

As in the proofs above, it is enough to state a local version of the theorem for a given saddle PP. Then the general version follows using standard genericity arguments identical to the ones in Sections 6.2 and 6.3.

To get the local version of the theorem, note that for generic diffeomorphisms ff, the saddle QQ is robustly in the chain recurrence class C(P,f)C(P,f) and there is a cu{\operatorname{cu}}-blender-horseshoe Σ\Sigma associated to QQ. In this step, the strongly intermediate points given by Proposition 5.6 play a key role. Finally, a perturbation gives a robust cycle with a transverse intersection between Ws(P)W^{\operatorname{s}}(P) and Wu(Q)W^{\operatorname{u}}(Q) and a robust intersection of Wu(P)W^{\operatorname{u}}(P) with Ws(Σ)W^{\operatorname{s}}(\Sigma). This completes the brief skecth of the proof.

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Christian Bonatti   (bonatti@u-bourgogne.fr)

Institut de Mathématiques de Bourgogne

B.P. 47 870

21078 Dijon Cedex

France