R ENDICONTI
del
S EMINARIO M ATEMATICO
della
U NIVERSITÀ DI P ADOVA
F ABIO G IANNONI
L OUIS J EANJEAN
K AZUNAGA T ANAKA
Homoclinic orbits on non-compact riemannian manifolds for second order hamiltonian systems
Rendiconti del Seminario Matematico della Università di Padova, tome 93 (1995), p. 153-176
<http://www.numdam.org/item?id=RSMUP_1995__93__153_0>
© Rendiconti del Seminario Matematico della Università di Padova, 1995, tous droits réservés.
L’accès aux archives de la revue « Rendiconti del Seminario Matematico della Università di Padova » (http://rendiconti.math.unipd.it/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions).
Toute utilisation 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
http://www.numdam.org/
on
Non-Compact Riemannian Manifolds for Second Order Hamiltonian Systems.
FABIO
GIANNONI (*) -
LOUIS JEANJEAN(**)
KAZUNAGA
TANAKA(**)(***)
ABSTRACT - We consider second order Hamiltonian systems on non-compact Rie-
mannian manifolds. We prove the existence of a nontrivial homoclinic orbit under conditions related to the
global superquadratic
condition of Rabinowitz in [17].0. Introduction.
In this paper, we
study
the existence of homoclinic orbits on a com-plete
connectednoncompact
Riemannian manifold M of classC3.
For agiven
functionV(t, x)
E xM, R),
we consider the second order Hamiltoniansystem:
where denotes the derivative of
x(t)
withrespect to t,
the covariant derivative of andgradx V( t, x )
thegradient
ofV(t, x)
withrespect
to the variable x.Let xo E M be a
point
such that(*) Indirizzo dell’A.: Istituto di Matematiche
Applicate
«U. Dini», FacoltAdi
Ingegneria,
Universita di Pisa, Via Bonanno Pisano25/B,
52126 Pisa,Italy.
(**) Indirizzo
degli
AA.: Scuola NormaleSuperiore,
Piazza dei Cavalieri,56100 Pisa,
Italy.
(***) On leave from
Department
of Mathematics,Nagoya University,
Chi- kusa, Nagoya 464,Japan.
We say a solution
x(t)
of(0.1)
is a homoclinic orbitemanating
from xo if andonly
ifOur aim is to derive conditions which ensure the existence of a homo- clinic orbit
emanating
from xo .This kind of
problems
hasrecently
hasrecently
beenextensively
studied via variational methods. See
[1, 2, 5, 7,11,16,17,18, 22, 24]
forhomoclinic orbits or heteroclinic orbits in
RN
and[3, 4, 8, 9,12]
for ho-moclinic orbits on Riemannian manifolds. See also
[6,10,19-21, 23]
for first order Hamiltoniansystems.
To our
knowledge,
so far the existence of homoclinic orbits on Rie- mannian manifold has been studied under twotypes
of conditions.In
[8, 9,12], V(t, x)
isperiodic
in t and satisfieswhile
in [3], V(t, x)
verifies the aboveassumptions
but it is timeindependent.
In
[4] (cf. [1,18]),
thepotential
is timeindependent
and is alocal maximum of
V(x)
such thatV(xo )
= 0. The existence of a homoclin- ic orbitemanating
from xo isproved
under theassumptions
that the setS~ _
~x E M; V(x) 0}
U is open and bounded andgrad V(x) ~
0for all x E a~ .
In this paper, we consider the existence of a homoclinic orbit in the situation where
V(t, x) depends
on t andchanges sign
on M. As far aswe
know,
such a situation is studiedonly
in the case M =RN
and thefollowing global superquadratic
condition isassumed ([7,17])
(GSQ) V(4 x)
is aperiodic
function in t of the formwhere
L(t)
is apositive
definitesymmetric
matrixdepending
ont
continuously
andx) satisfies,
for some 03BC >2,
Our main purpose is to shown the existence of a homoclinic orbit on a Riemannian manifold under a condition which is a
generalization
of(GSQ).
We also show the existence of a homoclinic orbit inRN
underweaker condition than
(GSQ).
See Remark 0.2 andExample
0.4below.
To state our
result,
we need some notations:let (., ’)~
be the Rie- mannian structure of M. ForW(x) E C2 (M, R), grad W(x)
andv]
will denote the Riemanniangradient
and the Riemannian Hessian ofW, i.e.,
where
y(s)
is thegeodesic
such thaty( o)
= x,~(0)
= v. In casealso
depends
ont E R,
we denoteby gradx W(t, x)
andHW (t, x)[v, v]
the Riemanniangradient
and the Rie- mannian Hessian of Wrespect
to x.We assume
(VO)
V EC2 (R
xM, R)
is1-periodic in t,
(VI) V(t, xo )
=0, gradx V(t, xo )
for all t E R and(V2) the
set~( t ) _ ~ x E M; V( t, x ) ~ 0 }
iscompact
for all t andgradx V(t, x) ~
0 for all X e andt e R, (V3)
lim inf infV(t, x)
> 0.d(x, xo ) -+ 00 t E R
(V4) V( t, x )
is of the form:where
~(t, x), W(t, x)
EC2 (R
xM, R)
are1-periodic
in t. More-over there is a function such that
(~1 ) grad p(ro )
=0,
(p2)
thereexists g
>0,
co E(0, 1/2), c’
> 0 such that for all x E M and v ETx M,
(1Jl) ~( t, x ) >
0 for all t E R and xE M, (p2)
there exists such thatNow we state our main result.
THEOREM 0.1. Let M be as above and assume
(VO)-(V4).
Then(0.1)-(0.2)
has at least one non- trivial, homoclinic orbitemanating from
xo .The
following
observationsclarify
themeaning
of conditions(VO)-(V4).
REMARK 0.2. Let M =
RN
with a standard Euclidean metric andassume satisfies condition
(GSQ). Setting p(x)
=1/2
and¢(t, x)
=1/2 (L(t)x, x),
we see conditions(VO)-(V4)
are satisfied. We obtain conditions(VO)-(V4)
as a first trial togeneralize
condition(GSQ)
of
Rabinowitz [17].
Wehope
thatthey
may beimproved.
REMARK 0.3.
(i)
In the condition(V4),
we can takep(t, x)
= 0. Inthis case,
V(t, x)
=W(t, x)
and if we take aq;(x)
eC2 (M, R)
suchthat
for some a >
0,
the condition(V4)-(w)
isclearly
satisfied for x EMBA
and it can be
regarded
as a condition on the setA,
thatis,
a condition onthe behavior of
V(t, x)
in aneighborhood
of0(t)’.
SeeExample
0.4below.
(ii) By
the condition(V4)-(w), W(t, x)
cannot take apositive
maxi-mum. Thus
(V4)-(w)
is satisfiedonly
onnon-compact
manifolds.EXAMPLE 0.4. Let M =
RN
with a standard Euclidean metric. Letp(f) e C~([0, oo)~ /:)
be a function such that for1 /2 )
Suppose V(t, x)
EC2 (R
xRN, R)
is1-periodic
in t and satisfiesThen
V(t, x)
satisfies(VO)-(V4)
for = andtp(t, x)
= 0provid-
ed that
We remark in the
set ~ ~ ~ x ~ 1 - ~ }
conditions(vo)-(V4)
are satis-fied if
V(t, x)
isnegative
and1-periodic.
Ingeneral, (GSQ)
is not satis-fied in this case.
REMARK 0.5. In the above
example, putting
a «handle» in the set~ p ~ x ~ 1 - p }, we
see that there exists acouple (M, V) satisfying
conditions
(VO)-(V4)
with the Riemannian manifold M notbeing
diffeo-morphic
toRN .
In the
following sections,
we prove Theorem 0.1. First we consider theproblem
on bounded intervals[ - n, n ] of R
and second we take alimit
1. Preliminaries.
Let
(M, ~ ~, ~ ~)
be acomplete,
connected finite dimensional Riemanni-an manifold of class
C3. By
the well-known Nashembedding
theo-rem
([13]),
M can be embedded inRN (with
a standard Euclidean met-ric)
forsufficiently large
N. Thus we may assume M is a submanifold ofRN
whose Riemannian structure is induced from the standard Eu- clidean metric onRN .
We may also assume xo E M iscorresponding
to0 E RN by
theembedding.
In what
follows,
we denoteby ~ ~ ~ I
the Euclidean norm,by (., .)
theEuclidean s-calar
product, by « - »
the difference inRN , by d(., .)
the distance on M indicedby
the Riemannianstructure,
and we also writeFor a technical reason, we consider the Hamiltonian
system (0.1)
on bounded intervals first. For n eN,
we defmeIt is well-known
(e.g. Palais [15]) that O1n
is a Hilbert manifold of classC2
and itstangent
space at x e isgiven by
We define a scalar
product
and a norm onby
where
Dt
is the covariant derivativealong
the curvex( t )
ES~ n .
We alsodefine the distance
y )
between andby
We have the
following
relation betweendoj
and d.Since he
1 ], 0 n 1 ),
we have(ahlas)(s)(t)
EC([ 0, 1 ], Wo ~ 2 (n))
with
(ahlas)(s)(t)
ETh(s)(t)M
for allt,
s andahlas(s)( ± n)
= 0. Nowfrom
we have
Therefore
Since
h(s)
isarbitrary,
weget
Similarly,
Thus we
get
the conclusion.We consider on
D;
the functionalWe can establish the
following
lemma in a standard way.LEMMA 1.2.
In (x)
ER)
andx(t)
is a criticalpoint of In (x) if
andonly if x(t)
solvesHere
Dt
is the covariant derivativealong
the curvex( t ).
We also remark that
for all
x(t)
eQ/§
andv(t)
eREMARK 1.3. For let
P(r)(.)
be theorthogonal projection
from
RN
ontoTx M
and let = v - Then we can writeThus
2. The mountain pass structure of
In this
section,
we prove thatIn
eC 1 (~ n , R )
satisfies the assump- tions of the Mountain Pass Theorem.LEMMA 2.1. There exist ao, p o > 0
independent of
n E N such thatif x(t) satisfies
then
Moreover
for x(t)
esatisfying
PROOF.
By
theassumption (VI),
we can choose a > 0 and a > 0 such thatNow
taking 80
> 0sufficiently
small so that(2.1) implies
for such a 60 >
0, clearly
it followsWe can deduce the second assertion in a similar way.
Next we take a
point
Xoo E M such thatV( t,
> 0 for all t and choose a curve such that(Note
that the existence of ~oo follows from(V3).)
For n E
N,
we setThen we can see
easily
Thus there exists an no E N such that
where
so
> 0 is defined in Lem-We fix such an no E N and write
qo ( t )
=q, (t). Setting
we
regard
We define for n * no
By
Lemma2.1,
and formulas(2.2), (2.3),
we can see thefollowing
LEMMA 2.2.
where p o > 0 is
given
in Lemma 2.1. Inparticular
the limitexists.
PROOF. Since we can
regard
Er n¡ c F,,,2
forn2 ~
no , theconclusion of Lemma 2.2 follows from the definition of
bn .
We can also
verify
the Palais-Smalecompactness
condition and wecan see
bn
is a critical value ofIn (x),
thatis,
there exists a non-trivial solution rn( t )
of(1.1)-(1.2).
One mayexpect
after suitable shifts in timexn ( t )
=tn ) ( tn E ~ - n
+1,
...,0,
... , n -1 ~ )
converges to a ho- moclinic orbit.However,
there is apossibility
and
xn ( t )
may converge to a non-trivial solution of(0.1)
in( - m , so )
with
or
To overcome this
problem,
we willget
a homoclinic orbit as a limit of aspecial
sequence ofapproximate
solutions of( 1.1 )-( 1.2)
in thefollowing
section. For this we need.
L E MMA 2.3. There exist constants 81,
Co
> 0independent of
n E Nsuch that
if x(t)
Esatisfies for -
E( o, 1 ]
PROOF.
By
theassumption (VI),
there exist~2 > 0, Ci , C2
> 0 such thatfor all t and x E
B( o, 82 ).
For
x(t)
E0’,
we defineThen
by (1.3)
where
f (x): M ~ RN2 is
an N x N matrix-valued functionsatisfying
Therefore there exist
~3
> 0 andCi , C2
> 0 such thatfor all with
x([ - n, n])
eB(0, a3).
Now we
set al
=min ~ 82 , s3 ~ >
0 and we assume e satisfies(2.4)
and(2.5). By (2.5),
we havethat
is,
Thus
using (2.7), (2.9), (2.10),
weget
where
C3 , C4
> 0 areindependent
of n and c.Using
thesebounds,
weget by (2.8)
3.
Approximate
solutions and their estimates.by
Lemma2.2,
we canchoose nk ;:::
noand yk
Enk
suchthat
For Eo ---
el /2
>0,
where 81 > 0 isgiven
in Lemma2.3,
we setwhere
[ a]
denotes theinteger part
of a E R . Weregard yk
Ernk
Crnk
+ Lkand
by
Lemma 2.2 and1), 2),
we can see thatNow we
apply
thefollowing proposition,
which is a consequence of the usual deformationargument.
PROPOSITION 3.1.
Suppose satisfies
for
some xo , Xl E0 n 1
and setAssume b > 0 and there exists a y E r such that
for
some - > 0Then there exists
x(t)
E0’ n
such thatWe
apply
the aboveproposition
to the case n = nk +lk.
J == =
Ilk
and obtain the existence of such thatWe derive some
properties
ofLEMMA 3.2.
PROOF. Since r 8
(t)(t)
= 0 for all S E[ o, 1 ]
and t E[
- n~ -lk ,
nk +
lk ]~[ - nk , nk ],
we can see from(3.3)
and Lemma 1.1 thatPROPOSITION 3.3. There exist constants
CI, C2
> 0independent of
k E N such that
PROOF. Here we use the
assumption (V4).
We writeSetting v
in(3.2),
we seeSince
H9 (x)[v, w] = (Dv w)
for all v, w ETxM (e.g.
Lemma49
of [14, p.86]),
Thus from
(v4)-(cp2)
that
is,
Therefore, combining (3.4)-(3.6)
and(V4)-(~2),
we haveBy (3.1)
and(3.7),
we have forlarge k
Thus we
by (V4)-(~2)
Thus we
get
from(V4)-(~1)
where
CI
> 0 isindependent
of 1~. Thus we alsoget
from(3.7)
for some
C~
> 0independent
of k. ThereforeLEMMA 3.4. For
large k,
PROOF. Recall that
),
weget
from Lemma 2.3 and(3.2)
thatBut
by
Lemma 2.2 this contradicts(3.1)
forlarge
In the next
section,
we take a limit as t toget
a homoclinicsolution.
4. Limit processes as 1~ --~ 00.
By
Lemmas 3.2 and3.4,
forlarge
we can find a Sk... ,
0,
9 ... , such thatWe defme
We remark
By Proposition 3.3,
we havewhere
Ci , C2
> 0 areindependent
of k E N.By (4.1)
and(4.4), yk (t)
is bounded inRN )
and we can ex- tract asubsequence-still
denoteby
k--such thatweakly
in(R, RN )
andstrongly
inC10c (R, M) .
From(4.4)
and(4.5),
we deduceMoreover LEMMA 4.1.
PROOF. It suffices to prove
for any
~(t)
ECo (R, R).
For a
given ~(t)
ECo (R, R),
we defineand
Since supp
~( t )
c( - tk , lk )
forlarge k, supp Vk ( t )
c( - nk -
+lk ) and vk E
forlarge
k. Nowusing
the fact thatand is bounded in
W o~2 (R, RN ),
we haveTherefore
by (3.2)
By (4.6),
we also haveThus it follows from
(4.10)
On the other
hand,
Here we used the fact
T,,M.
From(4.6), (4.11)
we can deduceThus we
get (4.9).
Using
the aboveLemma,
we can show thefollowing
PROPOSITION 4.2.
y(t) satisfies
PROOF. It suffices to prove
for all
By
forlarge
1~. We can seebounded as I~ --~ 00 and as in the
proof
of Lemma 4.1 vie haveUsing
Lemma4.1,
we haveoo.
Combining (4.12)-(4.14),
weget
the desired result. IEND OF THE PROOF OF THEOREM 0.1.
By (4.1), (4.6),
we ob-serve
In
particular,
To
complete
theproof
of Theorem0.1,
we need to showas t - :t 00 . We deal
only
with the case « + ».(The
case « - » can be treated in a similarway).
First,
we remarky(t)
is bounded on R.Indeed, by (4.7), y(t)
is uni-formly
continuous on I~ andusing (V3)
and(4.8),
our claim fol- lows.From the
equation (0.1),
we have forany h
> 0where m = max
gradx V(z, y(,r) 1.
.i e R
Thus,
if there is a sequence such that-~0.
Set-ting
we see
for
large j
E N. Therefore we haveThis contradicts
(4.7).
ThusNext we set
there exists some
( tj )~ o
such thattj
~ 00,Using
the uniformcontinuity
ofy(t)
on Ragain,
we can see thatLet us show
1]
x For any(s, x)
E Z there exists isuch that
Then
by
the continuousdependence
of solutions ondata,
we havewhere
z(t)
solvesxo ,
using (4.15)
and(V2),
we can seez(t) ~ x
and we havesince
This contradicts
(4.7).
Therefore weget y(t)
Acknowledgements.
This work has been done while the second and the third authors arevisiting
Scuola NormaleSuperiore,
Pisa. The sec-ond author would like tothank Scuola Normale
Superiore
forhosting
him
during
the academic year 1992- 1993 and the Swiss National Fund forallowing
thisexperience.
The third author would like to thank Scuola NormaleSuperiore
for theirsupport
andhospitality
which allow him to take one year leave fromDepartment
ofMathematics, Nagoya
University.
REFERENCES
[1] A. AMBROSETTI - M. L. BERTOTTI, Homoclinics
for
second order conserva- tive systems, in PartialDifferential Equations
and RelatedSubjects
(ed.M. MIRANDA), Pitman Research Note in Math. Ser. (1992).
[2] A. AMBROSETTI - V. COTI ZELATI,
Multiple
homoclinic orbitsfor
a classof
conservative systems, Rend. Sem. Mat. Univ. Padova, 89 (1993), pp. 177- 194. See also
Multiplicité
des orbites homoclines pour desSystèmes
con-servatifs,
C. R. Acad. Sci. Paris, 314 (1992), pp. 601-604.[3] V. BENCI - F. GIANNONI, Homoclinic orbits on compact
manifolds,
J.Math. Anal.
Appl.,
157 (1991), pp. 568-576.[4] M. L. BERTOTTI, Homoclinics
for Lagrangian
systems on Riemannianmanifolds, Dyn. Sys. Appl.,
1 (1992), pp. 341-368.[5] P. CALDIROLI, Existence and
multiplicity of
homoclinic orbitsfor singular potentials
on unbounded domains, Proc.Roy.
Soc.Edinburgh
(to ap-pear).
[6] V. COTI ZELATI - I. EKELAND - E. SÉRÉ, A variational
approach
to ho-moclinic orbits in Hamiltonian systems, Math. Ann., 288 (1990), pp.
133-160.
[7] V. COTI ZELATI - P. H. RABINOEITZ, Homoclinic orbits
for
second order Hamiltonian systemspossessing superquadratic potentials,
J. Amer.Math. Soc., 4 (1991), pp. 693-727.
[8] F. GIANNONI, On the existence
of
homoclinic orbits on Riemannian mani-folds, Ergodic
Theo.Dyn. Sys.,
14 (1994), pp. 103-127.[9] F. GIANNONI - P. H. RABINOWITZ, On the
multiplicity of
homoclinic orbitson Riemannian
manifolds for
a classof second
order Hamiltonian system, Nonlinear Diff.Eq. Appl.,
1 (1994), pp. 1-46.[10] H. HOFER - K. WYSOCKI, First order
elliptic
systems and the existenceof
homoclinic orbits in Hamiltonian system, Math. Ann., 288 (1990), pp.
483-503.
[11] L. JEANJEAN, Existence
of connecting
orbits in apotential
well,Dyn. Sys.
Appl.
(toappear).
[12] V. KOZLOV, Calculus
of
variations in thelarge
and classical mechanics, Russ. Math. Surv., 40 (1985), pp. 37-71.[13] J. NASH, The
embedding problem for
Riemannianmanifolds,
Ann. Math.,63 (1956), pp. 20-63.
[14] B. O’NEILL, Semi-Riemannian
Geometry
withApplications
toRelativity,
Academic Press. (1983).
[15] R. S. PALAIS, Morse
theory
on Hilbertmanifolds, Topology,
2 (1963), pp.299-340.
[16] P. H. RABINOWITZ, Periodic and heteroclinic orbits
for
aperiodic
Hamilto-nian system, Ann. Inst. H. Poincaré:
Analyse
Non Linéaire, 6 (1989), pp.331-346.
[17] P. H. RABINOWITZ, Homoclinic orbits
for
a classof
Hamiltonian systems, Proc.Roy.
Soc.Edinburg,
114 (1990), pp. 33-38.[18] P. H. RABINOWITZ - K. TANAKA, Some results on
connecting
orbitsfor
aclass
of
Hamiltonian system, Math. Zeit., 206 (1991), pp. 473-499.[19] E. SÉRÉ, Existence
of infinitely
many homoclinic orbits in Hamiltonian systems, Math. Zeit., 209 (1992), pp. 27-42.[20] E. SÉRÉ,
Looking for
the Bernoullishift,
Ann. Inst. H. Poincaré: Ana-lyse
Non Linéaire (toappear).
[21] E. SÉRÉ, Homoclinic orbits in compact
hypersurface
in R2Nof
restrictedcontact type,
preprint.
[22] K. TANAKA, Homoclinic orbits
for
asingular
second order Hamiltonian system, Ann. Inst. H. Poincaré:Analyse
NonLinéaire,
7 (1990), pp.427-438.
[23] K. TANAKA, Homoclinic orbits in
a first
ordersuperquadratic
Hamiltonian system:Convergence of
subharmonic orbits, J. Diff.Eq.,
94 (1991), pp.315-339.
[24] K. TANAKA, A note on the existence
of multiple
homoclinic orbitsfor
a per- turbed radialpotential,
Nonlinear Diff.Eq. Appl.
(toappear).
Manoscritto pervenuto in redazione l’ll ottobre 1993.