A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
C HARLES A. S TUART
Global properties of components of solutions of non-linear second order ordinary differential equations on the half-line
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 2, n
o2 (1975), p. 265-286
<http://www.numdam.org/item?id=ASNSP_1975_4_2_2_265_0>
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Properties Components
of Non-Linear Second Order Ordinary Differential Equations
on
the Half-Line.
CHARLES A. STUART
(*)
1. - Introduction and abstract
setting.
Suppose that p
> 0and q
are continuous real-valued functions on(0, 00)
such that the
symmetric operator
i definedby
(1.1) TU(X) == - (p(x)u’(x))’+
for x > 0on
oo)
has aunique self-adjoint
extension S inL2 (0, oo)
whose do-main is
(u e W2(o, oo) : u(o)
=01
and such that S is bounded below.Let Q
bea lower bound for the essential
spectrum
of S. Someglobal properties
ofthe set of non-trivial real solutions of the non-linear
eigenvalue problem
are established in the
general
case where the essentialspectrum
of S isnon-empty.
Several authors
(for example [1]
to[6])
have treated thecorresponding two-point boundary-value problem
forregular
second orderordinary
dif-ferential
equations
on a finite interval which may be taken to be[0, 1].
There the
appropriate setting
is the scale of Banach spaces of k-timescontinuously
differentiable functions( k
=0, 1, 2 ~ ... )
and theboundary
condition
(1.3)
must bereplaced by
(*)
Battelle Institute, 7 Route de Drize, CH-1227Carouge,
Geneve.Pervenuto alla Redazione il 21 Marzo 1974 ed in forma definitiva il 10 Novem- bre 1974.
where
(a2 + fl2)(62 + y2)
-~ 0. Thencompactness
isreadily
available both in theembeddings
ofCk+1( [o, 1] )
in for 7~ =0, 1, 2,
... and for theresolvent of the linear differential
operator T
which is evencompact
as amapping
fromC°([0, 1])
intoC~([o, 1]). Here,
since we areassuming
that zis in the
limit-point
case atinfinity,
it isappropriate
to seek solutions of theequation (1.2)
in the usual Sobolev spaces of squareintegrable
functionson
(0,00) together
with theboundary
condition(1.3).
Then the continuousembedding
of00)
inL2(0, 00) ( o 00))
is notcompact
for any 1~ =0, 1,2, ... and,
ingeneral, r
does not have acompact
resolvent. Never-theless,
we find that the abstractapproach
devised for the case of boundedintervals can be modified so as to
apply
in cases wherecompactness
is notavailable.
Following
the method laid downby
Rabinowitz for thecompact
case, it is shown in Stuart
[8]
that thetopological degree theory
for k-setcontractions
(l~ 1) developed by
Nussbaum[7]
can be used to this end.The results are obtained
by showing that, given appropriate
behaviour of the functionf,
thesystem (1.2), (1.3)
isequivalent
to anoperator equation
of the
form,
where R denotes the real
numbers, B
denotes a real Banach space withnorm 11 11
and the
operators
A and H have thefollowing properties.
PI)
A : B ~ B is a bounded linearoperator.
P2)
H : B X R - B is abounded,
continuous(non-linear) operator
such thatuniformly
for A in bounded intervals and such thatH(~, - ) :
R - B isuniformly
continuous on bounded intervals for u in bounded subsets of B.P3)
Themapping
G : B X R --~ B definedby
is such that
G( ~ , ~) :
B ~B is a contraction where k : R ~[0, 00)
is a known continuous
mapping.
Alternatively
thehypotheses P2)
can bereplaced by
thefollowing
one.P2 )’ H : B X R ~ B
is a continuouscompact mapping
such thatuniformly
for I in bounded intervals.Under these
hypotheses,
it is clear that is a solution of(1.4)
for all2 c R,
and such solutions are called trivial. Let Q; denote the subset of B X Rconsisting
of all non-trivial solutions of(1.4)
and letis a characteristic value of
A~ .
It is
readily
shownthat,
if 1 and(0, h)
is in the closure of Q withrespect
to the B x Rtopology,
then indeed(0, h)
c-’6’. In other,vords,
inthe range
4,
bifurcation from the curve of trivial solutions of(~1.4)
cantake
place only
at characteristic values of A. LetC,
denote thecomponents
(maximal
connectedsubset)
of i3’(endowed
with the inducedtopology
from
B X R) containing
ThenCl
isnonempty
if andonly
if u is a characteristic value of A.
THEOREM 1. l .
Let It
be a characteristic valueof
Aof
oddalgebraic
multi-plicity
withk(,u) C 1.
Thenep
has at least oneof
thefollowing properties.
1 ) ell is
unbounded subsetof
B X R.2)
supf k (2): (u,
> 1.3) C,
contains an element(0,
‘ where~C
=1= fl.In the case where we can choose
k(l)
= 0 for all l E R(corresponding
to
G( ~ , ~,) :
B - Bbeing compact
for each2 c- R)
this result coincides with Theorem ].3 of Rabinowitz[5].
The case where themapping
H has thespecial
formH(u, ~,)
- for some ~: B - B is established as The- oreui J .6 of Stuart[8]. However, given
eitherP2)
orP2 )’,
we seethat,
for a bounded sequence
f(Un,
in B X R with aswhere
a(xn)
denotes the set measure ofnon-compactness
of a bounded sequence in B as defined in Stuart[8]. Hence,
for a bounded sequenceIn))
in B X R such that un =
2n)
for all n and sup{k(2n): n - 1, 2, ...1 1,
we see that
~(un, 2n)l
contains aconvergent subsequence.
With thisnoted,
the
proofs
of Lemma 1.7 and Theorem 1.6 of Stuart[8] immediately yield
the result in the above
generality.
For
applications
to differentialequations,
it is useful tointerpret
Theorem 1.1 in the
following setting.
Let B now be a real Hilbert space withnorm )) ))
and let ~S:~(~S) ~ B
be an unboundedself-adjoint operator
in B which is bounded
below, Q being
a lower bound for the essentialspectrum
of the
complexification
of S. LetH,
withnorm III III,
denote the real Hilbert space obtained from the domain of Sequipped
with thegraph topology.
Then H is
continuously (but
ingeneral
notcompactly)
embedded in B.Consider the non-linear
eigenvalue problem
setby
where J.1f has the
following properties.
P4)
M: H X R --~ B is abounded,
continuousmapping
such thatuniformly
for 2 in bounded intervals and such thatM(u, - ) :
R -~ Bis
uniformly
continuous on bounded intervals for ~c in bounded sub- sets of H.Let 8 denote the set of all non-trivial solutions of
(1. 5)
in .Z~ X R andlet 8’ =
S’u {(O,
 is aneigenvalue
of81.
THEOREM 1.2.
Suppose
that pQ
is aneigenvalue of
oddmultiplicity of
S andthat,
in addition tosatisfying P4),
themapping
M is such thatM( ., 2):
H - B iscompact for
each 2 E R. Letell
den-ote thecomponent of
S’(endowed
with thetopology
inducedfrom H X R) containing (0, p).
Theneft
has at least one
of
thefollowing properties.
1 ) eft
is an unbounded subsetof
H X R.2 )
sup~~, : (u, A)
E3) ell
contains an element(0, ~u)
E S’ wherefi =1= fl.
This result is deduced from Theorem 1.1
by following
the method which is set out in detail for aspecial
case in Stuart[9].
Given any two of the
properties 1 ), 2), 3)
of Theorem1.2,
anexample
can be
provided
in which thehypotheses
of Theorem 1.2 are all satisfied andyet
there is acomponent
which has neither of the two selectedproperties.
See[14].
In the case of a
simple eigenvalue
of S we can say more.THEOREM 1.3.
Suppose
that uQ
is aneigenvalue of multiplicity
1o f
S.Also,
in addition toP4),
suppose that thepartial
derivativesMu
and exist and are continuous in an openneighbourhood of (0, fl)
in H X R. Thenit
follows from P4 )
thatMu(O, 1)
= 0for
all R and assume thatA)
= 0f or
all  E R. Then there exist an openneighbourhood
Uof
in H X
R,
an open interval(- ð, ð)
and continuousfunctions
such that
and
where u
E H, Illulli II =1
and Su =,uu.(Here
M isregarded
as a continuousmapping from
H X R in B and the derivatives are taken in the Fréchetsense. )
That
ell
has the local structure indicated above followsimmediately
from Theorem 1.4 of Crandall and Rabinowitz
[10].
In this case we setwhere and
D§
denote thecomponents
ofS’",,{(O, lz)l containing
aw(a), ,u -]- x c- (0, b))
andaw(a), ,u -f- 0) 1
respectively.
It is not claimed thatC)
ande;
are ingeneral distinct, although
in theapplications
toordinary
differentialequations
consideredbelow this will be seen to be so.
Using
the method introducedby
Rabinowitzin Theorem 1.27 of
[5],
we can deduce thefollowing global
results aboutthe subsets
C,~
ande;~-.
THEOREM 1.4.
Suppose
that all thehypotheses of
Theorem 1.3 aresatisfied
and
that,
inaddition, M( ~ , ~,) :
.H -~ R is acompact macpping for
each  E R.Then the set
~~~
has at least oneof
thefollowing properties.
1 )
is an unbounded subsetof
H X R.2 )
sup~~, : (u, I)
Ee:} > Q.
3) C)
contains an element(0, p)
E S’ wherep,
=1= fl.4)
There exists an element(u, I)
EC)
such that(-
u,I)
EThe above conclusion remains valid when
e:
isreplaced bye;.
To ensure that the linearisation of
(1.2)
about the trivial solution(0, 1)
isit is assumed that the function
f
which determines thenon-linearity
is con-tinuous and that
f (x,
r, s,~,) = o( (r2 -]- s21’)
as r2+
S2 -0, uniformly
for Ain bounded intervals and
x~---O.
Thisassumption
is statedformally
asA1 )
in Section 2 after the notation for the function spaces to be used and the
hypotheses concerning
the linear differentialoperation
z have been in- troduced. It is shown in Section 2 that under theassumption A1 )
the nodalproperties
of solutions of(1.2)
arepreserved
on connected sets of non-trivial solutions inW2(o, oo)
X R. Theassumption A1 )
is sufficient(*)
toguarantee
that the
Nemytskii operator
inducedby f
mapsW2(0, oo) continuously
into
Z2(o, oo). However,
as may be seenby considering
the mapÂ)
= r2for all
x > 0
and r, s, theassumption A1 )
is not sufficient toimply
that the
Nemytskii operator
is acompact mapping
fromTF~(0~ oo)
intoL2(o, oo) (indeed
it does not even ensure boundedness(**)). Compactness
is
implied by requiring that,
in addition toA1),
we have also thatf (x, r, s, 1)
-j- 0 as x - oo,uniformly
for r, s, A in bounded intervals. This additionalrequirement
of«spatial decay »
in the non-linear term is the content ofA2).
In Theorems 2.8 and 2.9 the results for(1.2)
under theassumption A2)
arepresented. Then,
in Section3,
thisspecial
case is usedto treat
(1.2)
whenonly
the weakerassumption Al)
ismade, provided
that
f
isultimately
almostsign preserving
in the sense of(2.19).
Thisrestriction is
essentially
used to establish thecompactness
of any closed bounded subset U of solutions of(1.2)
such that(u, ~,)
EU~ Q,
which is the content of
Corollary
2.4. The main results for(1.2)
underthese
assumptions
are thengiven
in Theorems 3.3 and 3.7 and it is indicatedhow,
in the usual way, additional structure onf
enables theproperties
of thecomponents
to be furtherspecified.
Such considerationsyield
additionalresults such as Theorem 3.7 on the
multiplicity
of solutions of(1.2)
forprescribed
values of Â.Many
more details of this kind ofanalysis
aregiven
in
[13].
A survey of some related material isgiven
in[15].
2. - Preliminaries.
Let R denote the real numbers and L2 denote the real Hilbert space of all real-valued measurable « functions » u such that
(*)
Indeed, as theproof
ofProposition
2.2(a) shows,I)
=O((r2
+s2)’ )
asr2 + s2 - 0
uniformly
for  in bounded intervals and x > 0 is sufficient to ensure this.(**)
See the remarkfollowing Proposition
2.2.The real Hilbert space of all elements u E L2 such that will be denoted
by W2
where the norm inW2
isgiven by
Here denotes the derivative of u in the sense of distributions. For u E
W2,
both and u’ can be taken to be continuous functions on and we set
H2
=(t+ e -W22: u(o)
=01.
ThusH2
is a real Hilbert space withrespect
tothe
norm III III.
For future reference we note thatfor all u E
H2
and all x:~~0,
where here and henceforth C denotes some, but notalways
the same,positive
constant. Thefollowing
result iseasily
established.
PROPOSITION 2.1. Given s > 0 and
uEH2,
there exist an X >- 0 and an openneighbourhood
Uof u
inH2
such thatHenceforth,
we shall assume that the linear differentialoperator
T hasthe
following properties.
The
coefhcient p
is a continuousnon-negative
function on(0, oo)
such thatThe
coefficient q
is continuous on(0, oo)
andIt is further assumed that the minimal
symmetric operator
T defined in(1.1) by p and q
has aunique self-adjoint
extension whose domainequipped
with the
graph topology
coincides(up
to normequivalence)
with the realHilbert space
H2.
Also the essentialspectrum
of thecomplexification
of 8is assumed to lie
entirely
in the interval[Q, oo).
Then thespectrum
in(- oo, Q)
consists ofsimple eigenvalues
which are indexedThe
eigenfunction corresponding to 2,,
isinfinitely differentiable, belongs
toH2
and has
exactly
n -1 zeros inNumerous sufficient conditions on p
and q
are known which will ensurethe above
properties
of theoperator
T, and we do not select one inparticular
here.
Certainly
T has all theseproperties provided
that p,p’ and q
are allcontinuous and bounded on
(0, oo)
withinfp(x)
> 0.However p and q
neednot be bounded on
(0,00). Indeed,
in theimportant special
casep (x)
=-=Iand
q(x) - - x-I
forx > 0,
T has all theproperties
listed above whereQ = 0
and thespectrum
of S is~-1 /~n2 : n =1, 2, ... ~ V [o, oo) .
On theother
hand,
there are cases(e.g. p(x)
=1 andq(x)
= 0 forx > 0)
in whichthe above conditions are satisfied but the
spectrum
of S liesentirely
in theinterval
[Q, oo),
and for such cases thetheory presented
below is vacuous.The
problem
ofdetermining
when there areeigenvalues
in(- oo, Q)
is wellunderstood. See for
example [12].
Turning
now to the non-linear term in( 1. 2 ),
we stateformally
the assump- tions described in the introduction.The function
f : [0,
is continuous andgiven
any bounded interval J and any s > 0 there exists an n > 0 such thatThe
following stronger
conditionrequires
thatf
also hasspatial decay.
A2)
The functionf
satisfiesA1 ) and,
inaddition, given
any bounded interval J and anyE > 0,
there existsan X>0
such thatA consequence of
A2)
which will be useful later isthat, given
a bounded subset K c R3 and there exists anX>0
such thatWe note that if
f (x, r, s, 2)
=y(x)h(r, s, Â)
forand r, s,
2 c- R wherea) [0, oo)
-~ R is continuous andy(x)
--~ 0 as x -~ oo andb)
h : R3 - R is continuous andh(r,
s,Â)
=o((r2 -~- s21’) uniformly
for 2in bounded
intervals,
then
f
satisfies the conditionA2).
In the
following
discussion of theNemytskii operator
inducedby f
itshould be noted that the condition
(2.6)
is instrumental notonly
inguaranteeing
that theNemytskii operator
iso(llIulll)
asIlIulll-+ 0
but evenin
ensuring
theH2
is takencontinuously
into .L2. In the absence of(2.6), growth
estimates would berequired
to ensure this.PROPOSITION 2.2.
(a) Suppose
thatf satisfies
the conditionA1 ) .
Then theNemytskii
oper- atordefined by
is a continuous
from H2
X R into L2. Furthermoreuniformly for
2 in bounded intervals.(b) Suppose
thatf satisfies A2 ) . Then,
in addition to theproperties
in(a),
we have that F:
.H2
X R E2 is acompact mapping
and also thatthe
mapping F(~, ~ ) :
R ~ L2 isuniformly
continuous on bounded intervalsfor
u in bounded subsetsof H 2.
The
proof
isstraight
forward and isgiven
in[13].
REMARK. In connection with the above
results,
it should be noted thatA1 )
is not sufficient to
guarantee
that theNemytskii operator
~I’ takes bounded subsets of~12
X R into bounded subsets of L2. Forexample,
setLet ~c : R --> R be an
infinitely
differentiable function withsupport
containedin
[1, 4]
and such thatu(x) -- 2
forx c- [2, 31. Then,
for eachpositive
in-teger n,
letThus t+n and
liiunll12
=+ U" (X) 2 I
dx oo for all n. Alsof
qatiq--00
fies
A1 ) .
HoweverA) -700
as n - oo .To ensure the boundedness of .~’ it is
enough
tosupplement A1 ) by
the
following assumption.
AB)
Given any bounded interva,lJ,
It is a
pleasant
feature of theapproximation procedure
used in SectiCn 3that it
yields global
results about(1.2)
withoutrequiring
thatthe non-linearity
induces a bounded
Nemytskii operator
from thegraph
space of T into L2.Setting f (x, r, s, A)
= r2 for all x > 0and r, s, 2 c- R,
andconsidering À)
where is the sequence in
H2
definedabove,
shows thatA1 )
andAB)
are not sufficient
hypotheses
off
to ensure that is com-pact.
Of course, when thestronger assumption A2)
ismade, AB)
is auto-matically
satisfied and the boundedness follows o a fortiori» from the com-pactness
as established inProposition
2.2(b).
WTe
give hypotheses
onf
which will ensure that theNemytskii
oper- ator(2.9)
has the smoothnessproperties required
in Theorem 1.3. Partial differentiation withrespect
to the i-th variable is denotedby ai
fori=1,2,3, 4.
AS)
The function and thepartial
derivatives~42 f
and are all continuous on[0, oo)
X R3. Furthermore~2 f ,
and all tend to 0 as
(r 2 + S2)t -70 uniformly
and 2.in bounded intervals.
Note that if
f
satisfiesAS)
then bothf
andsatisfy Al).
PROPOSITION 2.3.
Suppose
thatf satisfies AS). Then, for
theNemytskii operator
Fdefined by (2.9),
all the(Préchet) partial
derivativesFli, Fu
andF;.u
exist and are
I)
= 0 andI)
= 0for
all 2 E R.A
proof
isgiven
in[13].
We can now
proceed
with a discussion of(1.2)
in the spaceH2
X R.Henceforth 8 will denote the set of all non-trivial solutions of
(1.2)
inand
The
proof
of Lemma 2.9 in Rabinowitz[6]
showsthat, provided
satisfiesAl),
and
(~c, A)
E8,
the zeros in[0 00)
are allsimple.
LetC,,
denote thecomponent
of S’(endowed
with thetopology
induced fromH2 x R)
con-taining (0
In order to discuss the nodal
properties
of solutions we introduce amapping
N defined on S’ as follows. For(~ Â)
E8, N((u 2))
is the numberof zeros
(possibly infinite)
of u in(0, oo).
On8’U8
we setN(( 0 Ân))
= n -1.When
f
has thespecial
formf (x,
r, s,Â)
=rh(x, r,
s,Â)
for x > 0and r, s, 2
E Rwhere h :
[0, oo)
X R3 - R is continuous andh(x, 0, 0, A)
= 0 for all andall
A e R,
it can be shownsimply, using
the variational characterisation of theeigenvalues
of linear second orderordinary
differentialoperators
whichare
essentially self-adjoint
withrespect
to thegiven boundary condition,
that
N(( u, 2))
= n -1 for all(u, À)
E This method was used in Stuart[8]
and
[9].
To treat thegeneral
case in whichf
satisfiesonly A1),
we mustuse a different
approach.
Both for this and forsubsequent proofs,
it is con-venient to introduce the
following
definition.A
sequence {fk}
of functions is said tosatisfy
the condition(.E)
pro- vided that:a)
the functionsf k satisfy A1 ) uniformly
in k in the sensethat, given
0 and any bounded interval
J,
there exists an n > 0(in- dependent
ofk)
such thatb) f k - f
as k - cxJuniformly
oncompact
subsets of[o, oo) X R3;
c) given
any s > 0 and any bounded intervalJ,
there exists anX > 0 (independent
of1~ )
such thatwhenever and
x > X,
LEMMA 2.3.
Suppose that ffkl satisfies (E).
Let be a boundedsequence in
H2 X R
such that and such thatwhere
H2
X R -> L2 is theNemytskii operator
inducedby
(a)
Then there existpositive
and X(independent of k)
such thatfor
allx ~ X
and all k.(b)
Furthermore~(~ck,
contains asubsequence
which convergesstrongly
in
H2
X R as k - cxJ .PROOF.
Suppose
that(a)
Since we have that andconsequently
inte-gration
of(2.10),
aftermultiplication by
uk,yields
Let be defined
by
It follows from
(E)
thatgiven
any 8> 0 and any bounded intervalJ,
thereexists an
X _> 0
such thatThen, combining (2.12)
with(E) (a),
we seethat, given any s > 0,
thereexists an
X > 0
such thatHence, using (2.3)
and(2.4),
it follows from(2.11)
and( 2 .13 )
that thereexists an
(independent
ofk)
such thatfor all
x > .X
and allk,
where we also have thatq(y) - ltk -1 6 > 0
for ally >X
and all k. This establishes the second statement in(a).
Now
multiplying (2.10) by p(x)uk(x) yields,
7for all
x > X
and allk,
where X has also been chosen such thatp(x) ~ 2 pl >
0for all
x ~ X. But,
for and all k we have thatand so,
given any e > 0
there existsY > X
such thatwhere we have used
(2.14)
and chosen E to besufficiently
small.Combining (2J5)
and(2.16) yields
for all
y > 0, x ~ Y
andall k,
where Y has now been chosensufficiently large
so as to ensure that for all x> Y.Choosing
y =4p, (p, 6) -1
and ~==pi~{16p~(l-)-pi~)}’~
thisgives
Solving (2.17)
shows thatReturning
to(2.14)
andrecalling
that for all~>Y~
wehave that
However,
y since(b) Using part (a)
and(E),
it is easy to seethat,
for eachpositive
in-teger n,
there exists an such thatAlso the
compactness
of theembeddings
for Sobolev spaces over bounded domains and the uniformcontinuity
off
on bounded subsets of[0, oo) X R3, together imply
that asubsequence
can be selected such thatHence, by extracting
a suitablediagonal subsequence
we see that~(u~;,
contains a
subsequence
such thatas
1~’,
l’ ~ oo,where ~ Q
has been chosen so that u -(S - ~) u
is a linearhomeomorphism
ofH2
onto L2. Therefore we have that -*0as and the
proof
iscomplete.
COROLLARY 2.4.
Suppose that f satisfies A1 )
andthat, given
any e > 0 ,and any bounded intervalJ,
there exists anX > 0
such thatLet U be a closed bounded subset
of
S’ such that(u, ~,)
EU~ Q.
Then U is
compact
and there exists aY>0
such thatu(x)u’(x)
0for
allx ~ Y
and allPROOF. This follows
immediately
from Lemma2.3(b) by choosing fk
=f
for all k.
LEMMA 2.5.
Suppose
thatf satisfies A1 ) .
Then there exists an openneighbourhood
Uof (0,
inH2
X R such thatN((u, ~,~)
= n -1for
all~u, 2) c
U n 8’.PROOF.
Suppose
that there exists a sequence(Vk,
in Sconverging
to(0,
inH2
X R and such thatN~w,~, ,uk~~ ~
n -1 for all k.Setting
- for
x ; 0,
we have thatf or where is defined
by
It is
easily
checked that satisfies the condition(E)
and that indeedgk -+0
asuniformly
oncompact
subsets ofHence, using
Lemma2.3(b),
we may assume that{2u~, ,uk)
contains asubsequence converging strongly
to an element(w, ~C)
inH2
X R. But then we havep = and
showing
thatN((w, In))
= n -1.Furthermore there exists N > 0 such that all of the zeros of w
and w,
lie in the interval
[0, X)
for all k. Therefore there exists an openneigh-
bourhood V of w in
H 2
such that v hasexactly
n -1 zeros(all
of whichare
simple)
in[0, N)
for all v E V. Howeverfwkl
lieseventually
in V but w,~does not have
exactly
n -1 zeros in[0, X)
for any k.This contradiction establishes the result.
LEMMA 2.6.
Suppose
thatf satisfies A1 ) .
Then I(u,A)ECn.
f or
allPROOF. In view of Lemma
2.5,
it is sufficient to provethat, given 2)
e 8 with2))
oo there exists an openneighbourhood
V of(u, Â)
in
H2
X R such that,u~~
=N((u, A))
for all(v, p)
E V n S. With this inmind,
choose(u, A) c- 8
withN((u, A))
00. Thenusing (2.3), (2.4)
andProposition 2.1,
we see that there exist an 0 and an openneighbourhood
V19 - Annali della Scuola Norm. Sup. di Pisa
such that
where X also has the
property
thatand If this
yields
Thus we have shown that there exists an open
neighbourhood
V of(u, Å)
in
.H2
X R such that all the zeros of v lie in[0, X)
whenever(v, ~C)
e V r1 8.Choosing
V smallenough,
we can ensure that v has the same number ofzeros as u in
[0, X)
for all(v, p)
E V and so theproof
iscomplete.
For smooth
enough f,
we can say more.LEMMA 2.7.
(Smoothness) Suppose
thatf satisfies AS).
Then there existan open
neihgbourhood
Uof (0, A~)
inH 2
XR,
an open interval(- ð, ð)
andcontinuous
functions
such that
and
where un is the
unique eigen f unction
withI’urthermore,
and
where
5)’
and:0;
denote thecomponents of S’"",{(O, containing
the setsaw,
~,~ + qJ(a)): aE(O, 6)1
andaw(a), qJ(a): O)l
respectively.
PROOF. Note that
(0, Àn)
is theonly
trivial solution of(1.2 )
inen.
This follows from Lemmas 2.5 and 2.6.Also, given
any(u, Â)
ES, u’(0) =A
0 andso there exists an open
neighbourhood
TT of(u, Â)
inH2
X(-
oo,Q)
suchthat > 0 for all
(v, fl)
E V. The lemma now follows fromPropo-
sition 2.3 and Theorem .3.
Henceforth, whenever f
satisfiesAS),
we shall denote5)+u
and5)-r) {(O, A,,,)l by e;:-
ande; respectively.
Thenen
=e:
ue;
andO,t
r1~n =
A.)I.
We end this section
by stating
theglobal
results for(1.2)
in the case ofspatial decay
inf.
THEOREM 2.8.
(Spatial decay). Suppose
thatf satisfies A2).
Then thecomponent Cn of
S’ has at least oneof
thefollowing properties.
1) Cn
is an unbounded subsetof H2
X R.2 )
sup(u, A)
E =Q.
Furthermore -
PROOF. The
assumptions
madeconcerning
Ttogether
withProposi-
tion
2.2 (b)
are sufficient toguarantee
that Theorem 1.2 isapplicable
to(1.2)
in
H2 X R.
Then Lemma 2.6 shows that for and sowe have the desired result.
THEOREM 2.9.
(Spatial decay
andsmoothness). Suppose
thatf satisfies A2)
andAS).
Then the conclusionsof
Theorem 2.8 remacin valid when thecomponent en of
S’ isreplaced by
eitherof
the subsets~n
ore; .
3. - The
general
case.We maintain the notation introduced in the
previous
sectiontogether
with the
assumptions concerning
the linear diffPrentialoperator
T madethere. For each
positive integer 7~,
setThen, assuming
thatf
satisfiesAl ) ,
the Theorem :J.8applies
to theproblem
for each k. Our aim is to show that the set obtained
by «taking
the limit » as k of thecomponents
of solutions of(3.1)
discussed in Theorem 2.8 contains acomponent
with the desiredproperties.
LEMMA 3.1.
Suppose
thatf satisfies A1 )
and(2.19).
Let V be ail open bounded subsetof
such that(O,Àn)EV
andsup (2:
Then S’
(a V
denotes theboundary of
VH~ x R.)
PROOF. It follows from Theorem 2.8 that there exists a sequence
~(uk, ,uk)~
in 8V such that(Uk’ !lk)
is a non-trivial solution of(3.1),
Ukhaving exactly
n -1 zeros in(0, c>o).
But it iseasily
checked that thedefined
by
satisfies
(E). Hence, according
to Lemma2.3,
there exists asubsequence converging strongly
inH2 x R
to an elementClearly (u, fl)
satisfies(1.2 )
and(u, p)
E avo If(u, Â)
c- 8 theproof
is com-plete
and so we suppose that ~ 0 as k’- oo and setThen and is a solution of
= 1, where gk
is definedby,
and i
However also satisfies
(E)
andindeed gk
-+ 0 as k - oouniformly
oncompact
subsets of[0,00)
X R3.Hence, again referring
to Lemma2.3,
~Tecan select the
subsequence I’k’)l
such that convergesstrongly
in
H2 X R
to an element whereThis shows that /-l is an
eigenvalue
of ~S and so(0, /-l)
ES’, completing
theproof
of the lemma.As usual we find it convenient to
employ
thefollowing
resultproved
in
Whyburn [11 ] .
LEMMA 2.2.
Suppose
that~’1
andT2
are closed subsetsof
acompact
metric space T stteh that there is no connected subsetof
T which intersects bothTl
ared
T2.
Then there existdisjoint compact
setsI~1 K2
such thatTHEOREM 3. 3.
Suppose
thatf satisfies A1 )
and(2.1 J ) .
Then thecomponent en of
8’ has at least oneof
thefollowing properties..
.: ’tL---
1) en
is an unbounded subsetof H2
X RFurthermore,
PROOF. Let U be an open bounded subset of
H2
X R such that(0, ~,n)
E ~’and sup
~~1: (~, Â)
EQ.
It follows fromCorollary
2.4 thatT = U
n S’is a
compact
metric space whereU
denotes the closure of U inH2 X
R. Alsoand
T2::= {(O,
are closedsubspaces
of T.Suppose
thatthere is not a connected subset of T which intersects both
T1
andT2. Then, by
Lemma 3.2 there existdisjoint compact
setsK1
and.K2
such thatand Let Tr
= ((t1,
+ 1 - p ) 2 ( 1 j1 6 ) y2
for some whereThen V is an open bounded subset of
H2 X R
such thatand
S’naV==0.
This contradicts Lemma 3.1 andso we have that
Cn
n 0.Recalling
Lemma2.6,
we see that theproof
is
complete.
REMARK 1. The
hypotheses A1 )
and(2.19 )
arc satisfiedby f provided
thatwhere
fi
satisfiesA2)
andf2
satisfiesAl)
andf 2(x,
r, s,I)r 0
for alland In
particular,
thefunction f
2 has the desiredproperties provided
that it is in the formwhere h : is a
non-negative
continuous function such thatREMARK 2. The
hypotheses
of Theorem 3.3 do notimply
that theNemytskii operator
inducedby
thenon-linearity
in(1.2)
isnecessarily
abounded
mapping
from.~2
into L2. However it is often the case that thisNemytskii operator
is indeed a bounded continuousmapping
ofH2
withsome
topology
even weaker than that inducedby III III.
Forexample,
iff
is
independent
of sand, given
a bounded intervalJ,
then,
as in the remarkfollowing Proposition 2.2,
we have thatF( ~, 2): H2 -+L2
is a bounded and continuous
mapping
for each  E R where we can con-sider
H2
to have thetopology
inducedby
the normConsequently, under
theseassumptions,
theproperty 1 )
in Theorem 3.3 canbe
replaced by
Let us consider now the
improvements
available whenf
is smooth.LEMMA 3.5.
Suppose
thatf satisfies AS)
and(2.19).
Let V be an open bounded subsetof ~I2
X R such that(0, ~, n )
E V and(u, 2)
Ejr~ Q.
Thenwhere
PROOF. Given that
f
satisfiesAS),
it follows from Theorem 2.9 thatthe sequence in 8V chosen at the
beginning
of Lemma 3.1 canbe selected so as to have the additional
property
that for all k.As in Lemma
3.1,
it then follows that it contains asubsequence converging
to an element
(u, I)
in 8’. HoweverS’
isclearly
a closed subset of S’ andso indeed
(~, A)
ES’
*Similarly
we see that8)
r’1a
99.THEOREM 3.6.
Suppose
thatf satisfies AS)
and(2.19).
Then the con-clusions
of
Theorem 3.3 remacin valid when thecomponent en of
S’ isreplaced by
eitherof
its subsetsC.+
ore;.
PROOF.
Replacing S’ by S)
ofS’ respectively
in theproof
of Theorem 3.3 andusing
Lemma 3.5 instead of Lemma3.1,
proves the result.REMARK 3. As in the case of a
compact interval, [1]-[6],
theproperties
of the
components
can be furtherinvestigated
if more is assumed about the structure off.
Forexample, comparison arguments
can be used to findbounds on the range of J. covered
by components
and « apriori »
L2-boundscan be found under
appropriate hypotheses.
Details aregiven
in[13].
Herewe
give only
one result which can be obtained from such considerations.THEOREM 3.7.
Suppose
thatwhere is a continuous
function
such thatuniformly for 2
in boundedintervals.,
uniformly f or
and 2 incompact
sub-In
addition,
suppose thatf satisfies AS)
and that aÂn Âm po Then, for
eachfixed
A E(2,,+i, Àn+i+1]
where i =0,1,
... , m -n -1,
theequation (1.2 )
has at least 2
(i + 1)
distinct non-trivial solutionstu:~ : i
=0, 1,
...,i}
in.~12
where Uj has
exactly
n+ j -1
zeros in( 0, oo), u+’(0)
> 0 andu-’(0)
0.REFERENCES
[1] J. WOLKOWISKY, Non-linear Sturm-Liouville
problems,
Arch. Rational Mech.Anal., 35
(1969),
pp. 299-320.[2] M. G. CRANDALL - P. H. RABINOWITZ, Non-linear Sturm-Liouville
eigenvalue problems
andtopological degree,
J. Math. Mech., 19 (1970), pp. 1083-1102.[3] P. H. RABINOWITZ, Non-linear Sturm-Liouville
eigenvalue problems for
secondorder
ordinary differential equations,
Comm. PureApplied
Math., 23 (1970),pp. 939-962.
[4] R. E. L. TURNER, Non-linear
eigenvalue problems
with non-local operators, Comm. PureApplied
Math., 23 (1970), 963-972.[5] P. H. RABINOWITZ, Some
global
resultsfor
non-lineareigenvalue problems,
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[6] P. H. RABINOWITZ, A
global
theoremfor
non-lineareigenvalue problems
andapplications,
in Contributions to Non-linear FunctionalAnalysis,
Edit. E. Za-rantonello, Academic Press, New York, 1971.
[7] R. D. NUSSBAUM, The
fixed point
indexfor
localcondensing
maps, Ann. Mat.Pura
Appl.,
89 (1971), pp. 217-258.[8] C. A. STUART, Some
bifurcation theory for
k-set contractions, in Proc. London Math. Soc., 27 (1973), pp. 531-550.[9]
C. A. STUART, Existencetheory for
the Hartreeequation,
Arch. Rational Mech.Anal., 51 (1973), pp. 60-69.
[10]
M. G. CRANDALL - P. H. RABINOWITZ,Bifurcation from simple eigenvalues,
J. Functional Anal., 8 (1971), pp. 321-340.
[11]
G. T. WHYBURN,Topological Analysis,
PrincetonUniversity
Press, Princeton,1958.
[12]
N. DUNFORD - J. T. SCHWARTZ, LinearOperators,
Part II, Interscience, New York, 1963.[13]
C. A. STUART, Globalproperties of
componentsof
solutionsof
non-linear second orderordinary differential equations
on thehalf-line,
Battelle MathematicsReport
No. 75, June 1973.
[14] C. A. STUART, An
example in
non-linearfunctional analysis -
the Hartreeequation,
J. Math. Anal.
Appl.,
49(1975),
725-733.[15] C. A. STUART, Set contractions in the