A NNALES DE L ’I. H. P., SECTION C
L ORENZO J. D ÍAZ R AÚL U RES
Persistent homoclinic tangencies and the unfolding of cycles
Annales de l’I. H. P., section C, tome 11, n
o6 (1994), p. 643-659
<http://www.numdam.org/item?id=AIHPC_1994__11_6_643_0>
© Gauthier-Villars, 1994, tous droits réservés.
L’accès aux archives de la revue « Annales de l’I. H. P., section C » (http://www.elsevier.com/locate/anihpc) implique l’accord avec les condi- tions générales d’utilisation (http://www.numdam.org/conditions). Toute uti- lisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
Persistent homoclinic tangencies
and the unfolding of cycles
Lorenzo J.
DÍAZ (1)
and Raúl URES(2)
Departamento de Matematica, PUC-RJ, Brazil
and
IMERL, Facultad de Ingieneria,
Universidad de la Republica, Uruguay
Vol. 11, n° 6, 1994, p. 643-659. Analyse non linéaire
ABSTRACT. - We describe a new mechanism
implying
thepersistence
of homoclinic
tangencies
after theunfolding
of abifurcating cycle.
Thecycles
we consider are heterodimensional: the index of thehyperbolic points
involved in thecycle
are different.Key words : Bifurcation, cycle, heteroclinic point, homoclinic tangency, hyperbolic Nous decrivons un nouveau mecanisme
impliquant
lapersistance
detangences homocliniques apres
ledeploiement
d’uncycle.
Les
cycles
que l’on considere sont heterodimensionnels : 1’ index despoints hyperboliques impliques
dans lecycle
sont differents.1. INTRODUCTION
In this paper we are concerned with the
problem
ofdescribing generic (in
an openset)
bifurcations ofone-parameter
families ofdiffeomorphisms leading
to thephenomenon
ofpersistence
of homoclinictangencies.
1991 Mathematics Subject Classification : 58 F 14, 58 F 10.
(1)
Supported by CNPq Brazil.(~)
Partially supported by CNPq Brazil.Annales de l’Institut Henri Poincaré - Analyse non linéaire - 0294-1449 Vol. 11/94/06/$ 4.00/@ Gauthier-Villars
Since Newhouse
([8]-[9],
see[13]
for a newproof)
it is known that thegeneric unfolding
of a homoclinic(or heteroclinic) tangency
in arcsof surface
diffeomorphisms implies persistence
of homoclinictangencies
in intervals in the
parameter
line. This result was extended tohigher
dimensions first
by
Palis-Viana[14],
who treated the codimension 1 case.The
generalization
to any codimension was morerecently
obtainedby
Romero
[16].
In the
unfolding
of homoclinictangencies
on surfaces there are,essentially,
three differentpossibilities according
to the fractional dimension(Hausdorff
dimension andthickness)
of thehyperbolic
set involved in thecreation of the
tangency:
1. if the Hausdorff dimension of the
hyperbolic
set is less than one, thefamily
of intervals ofpersistent tangencies
hasdensity
zero(in
theLebesgue sense)
at the bifurcation value. Moreprecisely, hyperbolicity corresponds
to a set ofdensity
one at thisparameter value,
see Palis-Takens[12],
2. if the Hausdorff dimension of the
hyperbolic
set isbigger
than one,the
parameter
valuescorresponding
tohyperbolic diffeomorphisms
is not of
density
one at the initial bifurcation value. Indeed thereare
"plenty"
ofparameter
valuescorresponding
todiffeomorphisms exhibiting
homoclinictangencies,
see Palis-Yoccoz[15],
3. if the
hyperbolic
set is a thick set, i. e. theproduct
of its stable and unstable thickness isbigger
than one, the bifurcation value is in theboundary
of aninterval of
persistence
of homoclinictangencies,
see Newhouse([8]-[9]).
For heteroclinic
tangencies
in surfaces the results are similar. See[13]
for a
comprehensive
information on thesubject
above.In the cases
quoted
above([8]-[9], [14], [16])
theconcept
of thick horseshoeplays
akey
role toget persistence
oftangencies:
there areparameter
valuesarbitrarely
close to thebifurcating
onehaving
a thickhorseshoe with a homoclinic
tangency,
from which thepersistence
oftangencies
is obtained.We also mention that in these cases the creation of a homocli- nic/heteroclinic
tangency implies
the appearence of acycle
in which the index of thehyperbolic
sets(i. e.
dimension of the stablebundle)
areequal.
Suchcycles
are calledequidimensional.
Otherwise thecycle
isheterodimensional,
i. e. there is apair P, Q
ofhyperbolic periodic points
in the
cycle
with Notice that on surfacesevery
cycle
isequidimensional.
Here we deal with heterodimensional
cycles.
We say that an arc ofdiffeomorphisms
defined on a n-dimensional manifold has aheterodimensional
cycle
at t = b if there arehyperbolic
saddlepoints Pt
andQt
with different index so thatWU (Pb)
meetsWS ( Qb) quasitransversely along
the orbit of apoint
and intersectstransversely.
If
WS(Pb)
rh has a connectedcomponent being it-invariant
we say that the
cycle
is connected. When rhW u ( Qb )
contains aconnected
component
so that for every i7~
0 thecycle
isnamed nonconnected. Observe that there are
cycles being simultaneously
connected and nonconnected. The weak
expanding eigenvalue
ofQb
andthe weak
contracting eigenvalue
ofPb
are called the connexioneigenvalues.
In the
present
paper we describe a new mechanismleading
topersistence
of homoclinic
tangencies
after theunfolding
of acycle.
We prove that for alarge
open class of arcs ofdiffeomorphisms ( ft)te I unfolding
a connectedheterodimensional
cycle having
acomplex
connexioneigenvalue,
there isan open interval in the
parameter
linecontaining
the bifurcation value b in its interior where theparameter
valuescorresponding
to homoclinictangencies
are dense. In such a case we say that thepersistence
ofhomoclinic
tangencies
is apersistent phenomenon.
We
point
out that in this paper we do not useconcepts
related to fractional dimensions(namely
Hausdorff dimension andthickness).
The mainnovelty
of our
proof
of thepersistence
oftangencies
is that itonly
involves the twohyperbolic periodic points
in thecycle.
Let us recall that in[8]
toget persistence
oftangencies
it is considered a thickhyperbolic
set witha homoclinic
tangency.
Here to
get persistence
of homoclinictangencies
we analize thegrowth
of the homoclinic
points
ofPt.
Inrough
terms we prove thefollowing:
fort
nearby
b there is a subsetit
of the tranversal homoclinicpoints
ofPt being
dense in a center-stable manifold ofPt,
seeProposition.
The setAt plays
a similar role of the thickhyperbolic
set in[8],
see Section 3.2.Heterodimensional
cycles
were introducedby
Newhouse and Palis inthe
seventies,
see[10].
In([2]-[4])
the connected and nonconnected caseswith real connexion
eigenvalues
in any dimension were studied. Connected heterodimensionalcycles
withcomplex
connexioneigenvalues
remain sofar
unexplored
and here wegive
a contribution to theunderstanding
ofthe
dynamics
in this case.The
unfolding
of homoclinic/heteroclinictangencies
leads to the relevantdynamical phenomenon
of abundance of Henon-likeattractors/repellors ( [ 1 ], [7], [18]).
On the otherhand,
theunique
knowngeometric configurations leading
toprevalence
ofparameter
values with Henon-like attractors arethe
dissipative
critical saddle-nodecycles
studied in[ 11 ],
see[6].
We thinkthat in the
sectionally dissipative
cases considered in this paper ourproof suggests
that the heterodimensionalcycles
considered in this paper may be agood place
to search for Henon-like attractors withpositive density
at the bifurcation value.
2. STATEMENT OF RESULTS
Throughout
this paper M denotes acompact
n-dimensional(n
>3) boundaryless
manifold and the space of arcs of C°°diffeomorphisms equipped
with the usual C°°topology.
We say that exhibits a heterodimensional
cycle
at t = b if thereare
hyperbolic periodic points Pt
andQt
such thatCondition
(2)
means that xb is aquasitranversal
heteroclinicpoint
anddim(W8(Pt)) +dim(Wu(Qt))
=n+1.
We lose nogenerality by assuming
that rb = some
ko
and that b = 0.We say that
( ft)tEl unfolds generically
thecycle
above if there are aC1
curve(rt)t~I
and aC1
map C:I -->R+ with rt
E andC(0) ~
0 such thatspace
spanned by
We
proceed
to describe the set of arcs ofdiffeomorphisms
we considerhere. Let
H(M)
be the subset ofP°°(M) consisting
of arcs that unfoldsgenerically
a heterodimensionalcycle.
From now on, forsimplicity,
weassume that
Pt
andQt
are fixed. We consider arcs( ft)tEr satisfying:
(CI) Linearizing
coordinates : Let{.~i(t)}i-1,...,n
and{,~2(t)}z_1,...,~
be the
eigenvalues
of Dft(Pt)
and Dft(Qt), respectively.
Assume that... 1
pn(o>I
and ...]
1~~n-y0)~ _ ]
where E(C B R).
From now on write
~S
=Àn-2’ ~~ _ Àn-1
andAn.
(1)
isC1-linearizable
atPt
andQt
and
FIG. 1. - Heterodimensional cycle with a complex connexion eigenvalue.
or
By (CI)
there isstrong
stable foliation inWS(Pt)
with= 1. From now on
Ft S (x)
denotes the leave ofcontaining
x.We say that a curve at C
WS(Pt)
does not have s-criticalities if at~h~
in for every x E at.(CII)
There is anf t-invariant
connectedcomponent 03B3t
ofWS(Pt)
rhdepending continuously
on t such that qt has not neither s-criticalities nor radialcriticalities,
see definition below.Let
C(M)
be the subset of1t(M) consisting
of arcs( ft)tEI satisfying (CI-II).
THEOREM. - There is an open and dense subset
T (M) of C(M)
so thatfor
everyT(M)
there is e = > 0 and a dense subsetT~ in [-~, ~]
such thatf s
has a homoclinictangency for
every s ET~.
We
point
out that ourarguments give
that(ft)tEI
unfoldsgenerically
ahomoclinic
tangency
for every s ET~.
3. PERSISTENCE OF
TANGENCIES:
PROOF OF THE THEOREM From now on we assume that
C(M).
We
begin by remarking
that up to a finite number of nonresonanceconditions on the
eigenvalues
off o
atPo
andQo
the linearizations off t
atPt
andQt,
say 03C6Pt and can betaken,
and wedo,
todepend differentially
on theparameter, (see [17]),
and defined onneighbourhoods Up
andUQ
ofPt
andQt independent
of t.We take a metric in M so that
d(x, y)
=e(03C6Rt (x),
03C6Rt(y))
for everyx, y E
UR, (R = P, Q),
where e denotes the euclidean metric. From now ongiven
a curveI, III
means itslenght.
Given a set A and x E
A, C(x, A)
denotes the connectedcomponent
of A
containing x.
Let z = s, ~c,R =
P, Q.
We suppose that EIRn-2,
xc E
{(O,...
xu EE and E
By (CI-II)
we can choose 03C6Pt so that n ELet
H(Pt)
denote the set of transversal homoclinicpoints
related withPt.
We say that6’i
andS2
are~-transverse
at x, denotedby Sl fix S’2,
ifS’1
rhS2
andS2 ) > ~,
where L denotes theangle.
DefineHç(Pt)
asthe subset of
H(Pt) consisting
ofpoints x
so thatWS(Pt)
We say that -yt has no radial criticalities
(see CII)
if(~yt )
is transverseto the
pencil
ofstraighlines through (0,..., 0).
This definition does notdepend
onThe Theorem follows from the
arguments
in theproof
of the nextProposition.
PROPOSITION. -
Suppose
that,Qu(0) _
where B E(8~ ~ Q), ,Q~
E R#
0.and
dt
Àc(O) i=
O.Fixed T > 0 there is
to
> 0 such thatfor
every t E(-to, to)
is dense in where
03C0sst
denotes theprojection from
to 03B3talong
the leaves
of
thestrong
stablefoliation of WS(Pt).
3.1. Proof of the
Proposition
The main tool to
proof
theproposition
is thefollowing
result that extends aprevious
lemma in[3].
LEMMA 1. - Let m ~ N and ~ R so that
...
xl
[x~.
For any I =(Z1,
...,in), 2~
E~~, 1,
... , n >0, (if
n =0,
I= ~ ,
and J =... ) jk
>1
consider the sequencesr, s
E ~ 0,1,
... , so that~
Proof. -
Take x E If xE ~
there isnothing
to prove.Otherwise either
xi+1
xxi
for some iE {I,...,
m -1 ~
orx Let us assume that the first case occurs, the other
one follows
similarly. By (1)
and(2)
therej’i
so that xInductively
weget
asequence {jn}
with xNow
(3) implies
that zn =x~’"’’"2’i
- x as n - oo. This ends theproof
of the lemma. D
Now our
target is, roughly speaking,
thefollowing:
Denote
by «
the naturalordering
in qo so thatPo.
Fixed T > 0we construct a
family
of sequences of T-tranversepoints (x5)
related withPo
so that satisfies thehypotheses
in Lemma 1.To prove the
proposition
we need some technical definitions and constructions. Without loss ofgenerality
we can assume that~~ (o)
>0,
otherwise it isenough
toreplace ,~~ by
andC(0)
> 0. From now onwe write
Ai
instead ofAi(0).
Let B =
,~o ° (?~l~ ) .
Consider the extension of to the wholeB, ~,
., definedby
=,~o ° (cp po (~(~1, ... , a~_l, x~, x
ER})).
WriteUQ).
Vol. 6-1994.
We extend to the whole
By (CI-II),
for every x E where the convergence turns out to be
C1 on compacta.
Now consider a
cl-extension
of to say Let~ro
be theprojection along
the leaves of fromUQ
toDefine
pi
= n E~Z~))~
i =+,-.
We can choose 03C6P0 in such a way that istangent
to(0,..., 0, xu)
at(0,..., 0).
Forsimplicity
let us suppose that(0,
... ,0, xu).
Let us assume that ~yo
spirals
anti-clockwise. LetF+
n ~yo =U Xi,
i>o
where
d(xi+1, Qo) d(xi, Qo).
Otherwise theproof
followssimilarly by considering
the intersections between F- and ,0.Pick the fundamental domain D of ~yo in
Up
so thatf (~~ ... , 0, x, 0), x
E~-l, -~~~~~
.Given x and a curve a let
Let E be the fundamental domain of ~yo bounded
by ~o
andWithout loss of
generality
we can assume, and wedo,
that = D.Write
n(xo)
=k1.
Define
03BA(i) by
the natural number so that( fo 1(xo), x0]
C ’Yo.Remark that ~ is
strictly increasing.
Let 03B3i
be the arc in 03B30 boundedby xi
and There are A and 8 so thatC ~yo
by
the curve oflength
28 centered at x and03A3i(03B4) = 03A3(xi,03B2-03BA(i)u03B4).
Remark that there is$o
such that03A3i(03B4)
is03C4 2-
transversal to Fv for every 0 b
80,
here is the foliationgiven by
vertical lines in the
linerizing
coordinates.Take a small
neighbourhood V
of ~yocontaining
ro. Fixed A cV)
let AS ==
U C(x,
nV) .
xEA
Let xi ==
Wu = u andri (8)
=~i (b)
n For each i > 0 defineprojections along
the leaves of
FIG. 2.
Notice that
sii
=(recall
the choice ofF+)
and that there areconstants
Ki
andK2
withLet
TIi(8)
= C TOn Up
be the maximalsegment
in TO where the function ~ri i bellow is welldefined,
seeFigure 3,
Remark that
xi
= and that there are constantsKi
andK’2
withIn the
sequel
wetake ~ _ 4 S .
From(2.2)
and(2.0)
there areC1
andC2
Let =
ni(ê)
+2,
whereni(ê)
is definedby
Let
D_1
=fo 1(D).
DefineDi(ê) by
the convex hull ofVol. 11, n° 6-1994.
FIG. 3.
and
From the definition of
mi(c),
U C Hence we candefine every y E
D-l
U Dand j
> 0.By
the definition of -~~ i (~)+1.
On the otherhand,
from(2.3) Cl,~u’~~2~~ (C2~3~’~~2~~. Now,
from(2.4)
From
(2.2-5)
Let
From
(2.6), (2.0)
and the definitions of A and 8Take
The choice of ~ and
(2.7) imply
thatfor every y E
D-i
U D and i EI ( ~ ) .
Sinceby
the definition and DS(recall
the definition ofAs)
the lastinequality
gives
E u Ds for every y ED_1
U Dand j
> 0.We have
proved
thefollowing
Remark. -
Given y
ED-i
UD1 and j
> 1 let~~ - {~i (~i (.~o Z ~~~+~’ (~) ) ) ) ~
Then(1) y;
is well defined for every i > 0and j
>1, (2) yj
EDs-1
u Ds.Take
Since 0 E
(~8 ~ Q)
there is a finite subsetI (~) _ il,
... ,ie(~~ ~, io
=0,
ik
of Z such that(1) is 03BD 2-dense
inD,
where yk =(2) yik+1 yik,
where « means the naturalordering
in 03B30satisfying Po.
Now we are
ready
to construct the sequences~~ J;~’’’ ~~ > i
in the Lemma 1.Let
~~o(xJI’T ,~ )~~>m
where is defined asfollows. For i E
take xi
= For every k E andj >
1 letBy
construction for everyk,
i EGiven I =
(i1, i2,
...,im)
write~I)
= m.Suppose already
definedfor every
(I~
n +l,
n,(I~
_ + 1 and that --~xJ
as j
--~ oo forevery k
EI ( ~ ) .
LetAgain by
construction Z --~ Zas j
~ oo for every r E Now we claimClaim: The sequences
(z
= x,y)
are welldefined
andsatisfies
thehypotheses
in Lemma l.Proof of
the Claim. - Given x, y C write x --~ ymeaning
~r s ( x ) -~
Notice that ~ri i preserves theordering «.
We say that
(a,H)
is apair
if a is a curve in andH is a
family
of 1-disksdepending differentially
on xwith
H(x) x Ws(Po).
Apair (a’, H’)
is asubpair
of(03B1, H)
ifa’
C aand
H’(x)
=H(x)
for every x Ca’.
Remark that there
is J-l
> 0 such that for everypair (a, H)
close to a
subpair
of(where
theCl-proximity
isdefined in the obvious
way)
we can define theprojection p(a,x)
as followsBy shrinking e b
we can assume that preserves theordering «
and
by (2.1-2)
where
~ri
denotes theprojection along
the leaves of from~i (b)
to~i (b) .
A
pair (c~, H)
is called£-pair
ifFor i > 0 define
(ai, ~-LZ) by ai
=fo(a)
and~-l2
={~l2( fo(~))},
wheren
B).
Now let us suppose that
(CI(2a))
occurs, the case(CI(2b))
followsanalogously,
so we omit the details.linearizing
coordinates onegets
that(c~,~)
is to asubpair
of([-~~o],{~(~)Le[ArB~b]~
does notdepend
on
j.
Inparticular,
is to asubpair
of From
(2.4)
and|03BBs| |03BBc|2 [see CI(2a)], By shrinking
c, thenincreasing m,(c),
03B2-03BA(i)u~ , where
is defined as above. The choiceof
allow us todefine,
for every z G
7(c) and j ~ 0,
theprojection
where
{ p{a,x) )~
satisfies(2.8).
We define the
i- j-sucessor
of(a, ?-~),
denotedby (a~ , ~h ),
as followsThe choice of c
implies straighforwardly
thata~
C U DS.From
(2.8), (2.4)
and the definitions of A and LBy shrinking c
onegets
By hypothesis, fixi ~i (~),
for every i EI (~) .
Hence there isC6
so thatfo ~2~+~1 (D1
UD)s.
Consider any
C67-pair ( a, ~ ) .
From thearguments above, by shrinking
e, we can assume that the
i-j-sucessor
of(03B1, H)
is also aC6T- pair. Arguing inductively,
suppose that for every I =(il, i2, ... , in),
ik
E and J =(~1, ~2, ... , jn), j~ > 1,
is aC6T-pair.
Vol. 6-1994.
We define as
the in+1-jn+1-sucessor
of(03B1IJ, HIJ).
Fromthe construction
above,
isa C6T-pair
andsatisfies (2.8) 2 1 I I (1 2) |I||03B1|.
1
Now we are
ready
to finish theproof
of the Claim. Forsimplicity
letus assume that
I(~) _ ~0, l, 2; ... , e~.
Take theC6T-pair (c~, ~C),
wherea is a curve
joining xi’2
andH(xi’2)
= nV)
and= n
1>).
From thearguments
aboveFIG. 4.
where
xi;~’T -~
Now the inductivepattern
toget (2)
in Lemma 1 isobvious,
so we omit the details.Finally,
--~ 0as III
2014~ oo follows from thearguments
in theproof
of(2.9) by reduzing
e. Now theproof
of our claim iscomplete.
DNow we prove the
Proposition.
Our construction allow us to definez = x, y, for every I =
(il, ... , in,
E~0, ... , e}
and n >0,
andJ =
( jl , ... , ~n ), j~
>1, n
> 0 in the natural way forevery t
E[-to , to],
to
is small. Moreover these sequencessatisfy
Lemma 1.Fix I and
J,
now the definition of = x, y,only
involvescompact parts
of the invariant manifolds ofPt, hence zIJ : [-to , to]
~M, t
~z J (t) depends C1 on
t.Moreover, by construction,
contains a fundamental domainof 03B3t
forevery t
E[-to, to].
From the A-lemma estimates with
eigenvalue depending differentially
ont one
gets
that if e is taken smallenough
Let =
U C(x ,
Observe thatx~03B3t~uP
contains a
family
of curves(,(0)
as inFigure
5. Fixed i there ist(i)
E(0, to]
FIG. 5.
Vol. 11, n 6-1994.
such that we can define the continuation
~~(t)
of(,(0) depending differentially
on t forevery t
E(-t(i),t(i)).
Letwi(t)
be thepoint
ofquadratic
contact between~2(t,)
and the.~’t u.
Write =see
Figure
5.Since
(yie(0), yo(~))
contains a fundamental domain of ~y~ there isNi
so that E
(yi~(0), yO(O)).
Observe that oo as i - oc.By shrinking t(i),
EyO(t))
for every t E(-t(i), t(i)).
Let 0 follows
where
Cg
does notdepend
on t and i.Take i so that
C7
forevery t
E(-t(i), t(i)).
GivenV > 0 we
get
I and J as above and s E(t -
+V)
such that_ ~ J ( s ) .
Now it is not hard to see that fixed t E( - t ( i ) , t ( i ) )
and V > 0 there is s E
( t - ~ , t
+V)
such that istangent
toC (x J ( s ) , Up).
Now theproof
of theProposition
iscomplete.
D3.2 Proof of the Theorem
To
get
the Theoremjust
observe that in theproof
of theProposition
thehypothesis
(9 E(R B Q)
isonly
used to obtain the--dense
in D for suitable v.
However,
if 9 E R is closeenough
to 03B8 we candefine continuations ... ,
being
a03BD-dense
subset of D. Now the Theorem follows from thearguments
inthe proof
of theProposition.
. DACKNOWLEDGMENTS
We are
grateful
to J. Palis for useful conversations andencouragement.
Both authors
acknowledge
the warmhospitality
of IMPA. The first author thanks M. I. Camacho and M. J. Pacifico for their kindhospitality during
his
stay
at the Dto. de MatematicaAplicada
of IM-UFRJ fromAugust
1991to
July
1993 when this work was done.REFERENCES
[1] M. BENEDICKS and L. CARLESON, The dynamic of the Hénon map, Ann. of Math.,
Vol. 133, 1991, pp. 73-169.
[2] L. J. DIAZ, Robust nonhyperbolic dynamics and the creation of heterodimensional cycles, Erg. Th. and Dyn. Sys. (to appear).
[3] L. J. DIAZ, Persistence of heteroclinic cycles and nonhyperbolic dynamics at the unfolding of heteroclinic bifurcations, preprint.
[4] L. J. DIAZ, and J. ROCHA, Non-connected heterodimensional cycles: bifurcation and stability, Nonlinearity, Vol. 5, 1992, pp. 1315-1341.
[5] L. J. DIAZ, Hyperbolicity and the creation of heterodimensional cycles, in preparation.
[6] L. J. DIAZ, J. ROCHA and M. VIANA, Prevalence of strange attractors and critical saddle-node cycles, preprint.
[7] L. MORA and M. VIANA, The abundance of strange attractors, Acta Math., Vol. 171, 1993, pp. 1-72.
[8] S. NEWHOUSE, Nondensity of Axiom
A(a)
onS2,
Proc. Symp. Pure Math. Am. Math.Soc., Vol. 14, 1970.
[9] S. NEWHOUSE, The abundance of wild hyperbolic sets and non smooth stable sets for
diffeomorphisms, Publ. I.H.E.S., Vol. 50, 1979, pp. 101-151.
[10] S. NEWHOUSE and J. PALIS , Cycles and bifurcation theory, Publ. Asterisque, Vol. 31, 1976 pp. 44-140.
[11] S. NEWHOUSE, J. PALIS and F. TAKENS , Bifurcations and stability of families of diffeomorphisms, Publ. I.H.E.S. , Vol. 57, 1983, pp. 5-71.
[12] J. PALIS and F. TAKENS , Hyperbolicity and the creation of homoclinic orbits, Ann. of Math., Vol. 125, 1987, pp. 337-374.
[13] J. PALIS and F. TAKENS , Hyperbolicity and Sensitive-Chaotic Dynamics at Homoclinic Bifurcations, Fractal Dimensions and Infinitely Many Attractors, Cambridge University Press, 1993.
[14] J. PALIS and M. VIANA, High dimension diffeomorphisms displaying infinitely many sinks, Ann. of Math. (to appear).
[15] J. PALIS and J. C. Yoccoz, Homoclinic bifurcations: Large Haussdorf dimension and
non-hyperbolic behaviour, Acta Math., Vol. 172, 1994, pp. 91-136.
[16] N. ROMERO, Persistence of homoclinic tangencies in higher dimension, Erg. Th. and Dyr.
Sys. (to appear).
[17] F. TAKENS, Partially hyperbolic fixed points, Topology, Vol. 8, 1971, pp. 133-147.
[18] M. VIANA, Strange attractors in higher dimensions, Bol. Soc. Bras. Mat., Vol. 24, 1993, pp. 13-62.
(Manuscript received September 30, 1993;
accepted January, 1994. )