R E S E A R C H
Open Access
Multiple solutions for a fourth-order
nonlinear elliptic problem which is
superlinear at
+
∞
and linear at
–
∞
Ruichang Pei
1,2*and Jihui Zhang
2*Correspondence: [email protected] 1School of Mathematics and
Statistics, Tianshui Normal University, Tianshui, 741001, P.R. China
2School of Mathematics and
Computer Sciences, Nanjing Normal University, Nanjing, 210097, P.R. China
Abstract
We consider a semilinear fourth-order elliptic equation with a right-hand side nonlinearity which exhibits an asymmetric growth at +∞and at –∞. Namely, it is linear at –∞and superlinear at +∞. Combining variational methods with Morse theory, we show that the problem has at least two nontrivial solutions, one of which is negative.
Keywords: fourth-order elliptic boundary value problems; multiple solutions; critical groups; Morse theory
1 Introduction
Consider the following Navier boundary value problem:
⎧ ⎨ ⎩
u(x) +cu=f(x,u) in,
u=u= on∂, ()
whereis the biharmonic operator, andis a bounded smooth domain inRN (N> ),
andc<λ∗ the first eigenvalue of –inH().
The conditions imposed onf(x,t) are as follows:
(H) f ∈C(¯ ×R,R),f(x, ) = for allx∈andf(x,t) < for allt< and allx∈; (H) there existr∈(,p∗)andA,B> such that|ft(x,t)| ≤A+B|t|r– for allx∈, and
t∈R, wherep∗=NN–, ifN> ;
(H) limt→–∞f(xt,t)=luniformly forx∈, wherelis a nonnegative constant;
(H) there existβ,ξ∈Rsuch that forF(x,t) =
t
f(x,s)ds, we have lim
t→–∞sup
F(x,t) –f(x,t)t≤β uniformly for allx∈, ()
lim
t→+∞
F(x,t)
t = +∞ uniformly for allx∈ ()
and
lim
t→+∞inf
f(x,t)t– F(x,t)≥ξ uniformly for allx∈; ()
(H) there existϑ,ϑ∈L∞()+and an integerk≥such that
λk≤ϑ(x)≤ϑ(x)≤λk+ for allx∈, ()
the first and the last inequality are strict on sets (not necessary the same) of positive measure, and
ϑ(x)≤ft(x, ) =lim t→
f(x,t)
t ≤ϑ(x) uniformly for allx∈. ()
In view of the conditions (H) and equation () in (H), it is clear that for allx∈,f(x,t)
is linear at –∞and superlinear at +∞. Clearly,u= is a trivial solution of problem (). It follows from (H) and (H) that the functional
I(u) =
|u|–c|∇u|dx–
F(x,u)dx ()
isCon the spaceH()∩H() with the norm
u:=
|u|–c|∇u|dx
,
whereF(x,t) =tf(x,s)ds. Under the condition (H), the critical points ofIare solutions
of problem (). Let <λ<λ<· · ·<λk<· · · be the eigenvalues of (+c,H()∩ H
()) andφ(x) > be the eigenfunction corresponding toλ. In fact,λ=λ∗(λ∗–c). Let
Eλk denote the eigenspace associated withλk. Throughout this article, we denoted by| · |p
theLp() norm andE=H()∩H(). The aim of this paper is to prove a multiplicity theorem for problem () when the nonlinearity termf(x,t) exhibits an asymmetric be-havior ast∈Rapproaches +∞and –∞. In the past, some authors studied the following elliptic problem:
–u=f(x,u), u∈H() () with asymmetric nonlinearities by using the Fučík spectrum of the operator (–,H
()).
This approach requires thatf(x,t) exhibits linear growth at both +∞and –∞and that the limitslimt→±∞f(x,t)
t exist and belong toR. See the works of Các [], Dancer and Zhang [],
Magalhães [], de Paiva [], Schechter [] and the references therein. Equations with non-linearities which are superlinear in one direction and linear in the other were investigated by Arcoya and Villegas [] and Perera []. They let the nonlinearityf(x,t) be line at –∞ and satisfy the Ambrosetti-Rabinowitz condition at +∞. Particularly, it is worth noticing paper []. The authors relax several of the above restrictions on the nonlinearityf(x,t). Their nonlinearity is only measurable inx∈. The limit ast→–∞off(xt,t) need not ex-ist and the growth at –∞can be linear or sublinear. Furthermore, their nonlinearityf(x,t) does not satisfy the famous AR-condition. They use the truncated skill of first order weak derivative to verify the (PS) condition and obtain multiple solutions for problem () by combining variational methods and Morse theory.
method in [] cannot be applied directly to the biharmonic problems. For example, for the Laplacian problem,u∈H
() implies|u|,u+,u–∈H(), whereu+=max(u, ),
u–=max(–u, ). We can useu+oru–as a test function, which is helpful in proving a
so-lution nonnegative. While for the biharmonic problems, this trick fails completely since
u∈H
() does not implyu+,u–∈H() (see [, Remark ..] and [, ]). As far as
this point is concerned, we will make use of the new methods to overcome it.
This fourth-order semilinear elliptic problem can be considered as an analogue of a class of second-order problems which have been studied by many authors. In [], there was a survey of results obtained in this direction. In [], Micheletti and Pistoia showed that (P) admits at least two solutions by a variation of linking iff(x,u) is sublinear. Chipot []
proved that the problem (P) has at least three solutions by a variational reduction method
and a degree argument. In [], Zhang and Li showed that (P) admits at least two
nontriv-ial solutions by Morse theory and local linking iff(x,u) is superlinear and subcritical onu. In this article, under the guidance of [], we consider multiple solutions of problem () with the asymmetric nonlinearity by using variational methods and Morse theory.
2 Main result and auxiliary lemmas
Let us now state the main result.
Theorem . Assume conditions(H)-(H)hold.If l<λ,then problem()has at least two
nontrivial solutions.
Lemma . Under the assumptions of Theorem.,then I satisfies the(PS)condition.
Proof Let{un} ⊂Ebe a sequence such that for everyn∈N,
|un|–c|∇un|
dx–
F(x,un)dx
≤c, ()
(unv–c∇un∇v)dx–
f(x,un)v dx
≤εnv, v∈E, ()
wherec> is a positive constant and{εn} ⊂R+is a sequence which converges to zero. By
a standard argument, in order to prove that{un}has a convergence subsequence, we have
to show that it is a bounded sequence. To do this, we argue by contradiction assuming that for a subsequence, denoted by{un}, we have
un →+∞ asn→ ∞.
Without loss of generality we can assumeun> for alln∈Nand definezn=uunn.
Ob-viously,zn= ∀n∈Nand then it is possible to extract a subsequence (denoted also by {zn}) such that
znz inE, ()
zn→z inL(), ()
zn(x)→z(x), a.e.x∈, ()
wherez∈Eandq∈L(). Dividing both sides of inequality () byun, we obtain
(znv–c∇zn∇v)dx–
f(x,un)
un
v dx≤ εn unv
for allv∈E.
Passing to the limit we deduce from equation () that
lim
n→∞
f(x,un)
un v dx=
(zv–c∇z∇v)dx ()
for allv∈E.
Now we claim thatz(x)≤ a.e.x∈. To verify this, let us observe that by choosing
v=zin equation () we have
lim
n→∞
+ f(x,un)
un
zdx< +∞, ()
where+={x∈|z
(x) > }. But, on the other hand, from (H) and equation () in (H),
we have
f(x,un(x)) un
z(x)≥
lun(x) –K
un
z(x)≥
–lq(x) –K
z(x), a.e.x∈
for some positive constantK> . Moreover, usinglimn→∞un(x) = +∞a.e.x∈+,
equa-tion () and the superlinearity off, we also deduce
lim
n→∞
f(x,un(x)) un
z(x) = lim
n→∞
f(x,un(x)) un
zn(x)z(x) = +∞, a.e.x∈+.
Therefore, if|+|> we will obtain by Fatou’s lemma that
lim
n→∞
+
f(x,un(x)) un
z(x)dx= +∞
which contradicts inequality (). Thus|+|= and the claim is proved.
Clearly,z(x)≡, by (H), there existsC> such that |f(|xu,unn)| | ≤Cfor a.e.x∈. By
using Lebesgue dominated convergence theorem in equation (), we have
(zv–c∇z∇v)dx–
lzv dx= ()
for allv∈E. This contradictsl<λ. Lemma . Let E=V⊕W,where V=Eλ⊕Eλ⊕ · · · ⊕Eλk.If k≥is an integer,ϑ∈
L∞()+,ϑ(x)≤λk+a.e.onand the inequality is strict on a set of positive measure,then
there existsγ > such that
u–
ϑudx≥γu
Proof We claim that there exists a constantϑ< such that
ϑ(x)udx≤ϑu ()
for allu∈W. In fact, if not, there exists a sequence{un}such that
ϑ(x)|un|dx> –
n
un
for alln∈N, which impliesun= for alln. By the homogeneity of the above inequality,
we may assume thatun= and
ϑ(x)|un|dx> –
n ()
for alln. It follows from the weak compactness of the unit ball ofW that there exists a subsequence, say{un}, such thatunweakly converges touinW. Now Sobolev’s embedding
theorem suggests that{un}converges touinL(). From inequality () we obtain
ϑ(x)|u|dx≥.
Moreover one has
≥ u≥λk+|u|≥
ϑ(x)|u|dx≥.
Hence we have
u=λ
k+|u|
and
λk+–ϑ(x)
udx=
which implies thatu∈Eλk+\ {}andu= on a positive measure subset. It contradicts
the unique continuation property of the eigenfunction.
3 Computation of the critical groups
It is well known that critical groups and Morse theory are the main tools in solving elliptic partial differential equation. Let us recall some results which will be used later. We refer the readers to the book [] for more information on Morse theory.
LetHbe a Hilbert space andI∈C(H,R) be a functional satisfying the (PS) condition or (C) condition, andHq(X,Y) be theqth singular relative homology group with integer
coefficients. Letube an isolated critical point ofIwithI(u) =c,c∈R, andUbe a
neigh-borhood ofu. The group
Cq(I,u) :=Hq
Ic∩U,Ic∩U\ {u}
, q∈Z
LetK:={u∈H:I(u) = }be the set of critical points ofIanda<infI(K), the critical groups ofIat infinity are formally defined by []
Cq(I,∞) :=Hq
H,Ia, q∈Z.
From the deformation theorem, we see that the above definition is independent of the particular choice ofc<infI(K). Ifc<infI(K) then
Cq(I,∞) :=Hq
H,˙Ia, q∈Z. ()
For the convenience of our proof, we first recall two interesting results and prove two important propositions.
Proposition .[] Under(H),if u∈E:=H()∩H()is an isolated critical point of
I,then C∗(I,u)∼=C∗(I|C (),u).
Proposition . [] If D ⊂ D⊂E⊂E ⊂X and for some integer k ≥ we have
Hk(E,D)= and Hk(E,D) = ,then either Hk+(E,E)= or Hk–(D,D)= . Proposition . If the assumptions of Theorem.hold,then
Ck(I,∞) = for all integers k≥.
Proof Under the guidance of [] and [], we begin to prove this result. LetI=I|C(¯).
Indeed, it follows from above Proposition . thatIandI have same critical set. Since
C(¯) is dense inE, invoking Proposition of Palais [], we have
Hk
E,I˙a=Hk
C(¯),I˙a for alla∈Rand all integersk≥. () From equations () and (), we see that in order to prove the proposition, it suffices to show that
Hk
C(¯),Ia= for alla< with|a|large and all integersk≥. () In order to prove equation (), we proceed as follows. We define the sets
∂Bc=u∈C(¯) :uC (¯)=
and
∂Bc,+=u∈∂Bc:u(x) > for somex∈. Consider the maph+: [, ]×∂Bc,+→∂Bc,+defined by
h+(t,u) =
( –t)u+tφ
( –t)u+tφC(¯)
for all (t,u)∈[, ]×∂Bc,+.
Clearly,h+is a continuous homotopy andh(,u) =φfor allx∈∂Bc,+. Therefore,∂Bc,+is
By equation () in (H), given anyγ > , we can findC=C(γ) > such that
F(x,t)≥γ t
for allx∈and allt≥C. ()
Similarly, from condition (H), and by choosingC> even bigger if necessary, we observe
that there is a numberγ> such that
F(x,t)≥–γ t
for allx∈and allt≤–C(γ). ()
Moreover, by condition (H), we have
F(x,t)≤C for allx∈and all|t| ≤C(γ) ()
for someC> .
Letu∈∂Bc,+. By inequalities (), (), and (), for allt> we have
I(tu) =t
u
–
F(x,tu)dx
=t
u
–
tu≥C
F(x,tu)dx–
tu≤–C
F(x,tu)dx–
|tu|≤C
F(x,tu)dx
≤t
+
γ λ
u–γ
tu≥C udx
+C||. ()
Recalling thatγ> is arbitrary, from (), we have
I(tu)→–∞ ast→–∞. ()
Using formula () in condition (H), we see that there exist constantsξandM> such
that
f(x,t)t– F(x,t)≥ξ for allx∈and allt≥M. ()
By (H) and formula () in condition (H), we have
F(x,t) –f(x,t)t≤C for allx∈and allt<M () for someC> . By inequalities () and (), for anyu∈Ewe have
F(x,t) –f(x,t)tdx≤C, ()
whereCis a positive constant. Leti:C
(¯)→Ebe the continuous embedding map. Let
·,·denote the duality brackets for the pair (C(¯)∗,C(¯)). We letI=I◦i, and so
I(u) =i∗Ii(u) for allu∈C(¯),
d dtI(tu) =
I(tu),u=tu–
f(x,tu)u dx≤ t
I(tu) +C∗.
Then, from equation (), we obtain
d
dtI(tu) < for allt> large such thatI(tu) < – C∗
. ()
From conditions (H) and (H), we see that given> , we can findM> such that
F(x,t)≤ (l+)t
+M for allx∈and allt≤. ()
Using inequality (), we have
I(u)≥
u–l|u| –|u|
–M ≥Cu–M
foru∈–C+, whereC+is defined as
u∈C() :u(x)≥ for allx∈
andC> is a positive constant. SoI|–C+is coercive, thus we findC∗∗> such thatI|–C+≥
–C∗∗. We pick
a<min
–C
∗
, –C
∗∗,inf
∂BcI
.
Then inequality () implies that we can findk(u) > such that
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
I(tu) >a ift∈[,k(u)),
I(tu) =a ift=k(u),
I(tu) <a ift>k(u).
Moreover, the implicit function theorem implies thatk∈C(∂Bc
,+, [, +∞)).
By the choice ofa, we have
Ia=tu:u∈∂Bc,+,t≥k(u). ()
We define the setE+={tu:u∈∂Bc,+,t≥}. The maphˆ+: [, ]×E+→E+defined by
ˆ
h+(s,tu) =
⎧ ⎨ ⎩
( –s)tu+sk(u)u if ≤t<k(u),
tu ift≥k(u), s∈[, ], ()
is a continuous deformation ofE+,hˆ+(,E+)⊂Iaandhˆ+(s,·)|Ia=id|Iafor alls∈[, ] (see
equations () and ()). Therefore,Ia is a strong deformation retract ofE+. Hence we
have
Hk
C(¯),Ia=Hk
C(¯),E+
=Hk
Recalling that in the first part of the proof, we established that∂Bc,+is contractible. This yields
Hk
C(¯),∂Bc,+= for all integersk≥.
Combining with equation () leads to equation (), which completes the proof.
Proposition . If the assumptions of Theorem.hold,then Cd(I, )= ,
where d=dimV (V being defined in Lemma.).
Proof By condition (H), given> , we can findδ∗> such that
ϑ(x) –
t≤F(x,t) for allx∈and all|t| ≤δ∗. ()
SinceVis finite dimensional, all norms are equivalent. Thus we can findρ> small such that
u ≤ρ ⇔ u∞≤δ∗ ()
for allu∈V. Taking inequalities () and () into account, for allu∈Vwithu ≤ρwe have
I(u)≤
λk–ϑ(x)
udx+ |u|
. ()
Similar to the proof of Lemma ., there existsC> such that
I(u)≤(–C+)u≤ ()
for allu∈Vandu ≤ρ.
On the other hand, for given> , it follows from (H) and (H) that
F(x,t)≤ϑ(x) + t
+C|t|r ()
for allx∈andt∈R. By () and Lemma ., we have
I(u)≥Cu–Cur ()
for allu∈W. From inequality (), we infer that forρsmall enough we have
4 Proof of the main result
Proof of Theorem. We consider the following problem:
u+cu=f
–(x,u), x∈,
u|∂=u|∂= , where
f–(x,t) =
f(x,t), t< , , t≥.
Define a functionalI–:E=H()∩H()→Rby
I–(u) =
|u|–c|∇u|dx–
F–(x,u)dx,
whereF–(x,t) =
t
f–(x,s)ds, thenI–∈C(E,R). Obviously, by conditions (H) and (H),
we know thatI–is coercive and boundedness from below. Thus we can findv∈Esuch
that
I–(v) =infI–=:m–. ()
Next, we claim thatv= . By condition (H), given∈(,λk–λ), there existsδ> such
that
ϑ(x) –
t≤F–(x,t) for allx∈,t∈[–δ, ]. ()
Forssmall enough, it follows from inequality () that
I–(–sφ) =
s
λ–
F–(x, –sφ)dx
≤s
(λ–λk+) < ,
and thus, by equation (),I–(v)≤I–(–sφ) < , sov= . From condition (H) and strong
maximum principle, we havev< and
Ck(I–,v) =δk,Z for all integersk≥.
Sincevis an interior point of –C+, from Proposition ., we know
Ck(I,v) =Ck(I–,v) =δk,Z for all integersk≥. ()
Letθ∈R,> be such thatθ<m–=I(v) < –. We consider the sublevel sets
Iθ⊂I–⊂I⊂E.
Suppose that andvare the only critical points ofI. Otherwise, we have a second
non-trivial smooth solution and so we are done. By Proposition ., we have
Hk
We know thatIsatisfies the (PS) condition (see Lemma .). Hence choosing> small enough, we have
Hd
I,I–=C
d(I, )= ()
(see Proposition .). Because of equations () and (), using Proposition ., we obtain
Hd+
E,I= or Hd–
I–,Iθ= .
IfHd+(E,I)= , then there is a critical pointv∗∈EofIsuch that
Iv∗>> and v∗= ,v.
IfHd–(I–,Iθ)= , then there is a critical pointv∗∈EofIsuch that
Cd–
I,v∗= . ()
Sinced≥, from equations () and (), we see thatv∗=v. It is obvious thatv∗= .
Thereforevandv∗are two solutions of problem ().
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
The authors read and approved the final manuscript.
Acknowledgements
The authors would like to thank the referees for valuable comments and suggestions in improving this article. This study was supported by the National NSF (Grant No. 11101319) of China and Planned Projects for Postdoctoral Research Funds of Jiangsu Province (Grant No. 1301038C).
Received: 14 August 2013 Accepted: 16 December 2013 Published:10 Jan 2014
References
1. Các, NP: On nontrivial solutions of a Dirichlet problem whose jumping nonlinearity crosses a multiple eigenvalue. J. Differ. Equ.80, 379-404 (1989)
2. Dancer, EN, Zhang, Z: Fuˇcík spectrum, sign-changing, and multiple solutions for semilinear elliptic boundary value problems with resonance at infinity. J. Math. Anal. Appl.250, 449-464 (2000)
3. Magalhães, CA: Multiplicity results for a semilinear elliptic problem with crossing of multiple eigenvalues. Differ. Integral Equ.4, 129-136 (1991)
4. de Paiva, FO: Multiple solutions for a class of quasilinear problems. Discrete Contin. Dyn. Syst.15, 669-680 (2006) 5. Schechter, M: The Fuˇcík spectrum. Indiana Univ. Math. J.43, 1139-1157 (1994)
6. Arcoya, D, Villegas, S: Nontrivial solutions for a Neumann problem with a nonlinear term asymptotically linear at –∞ and superlinear at +∞. Math. Z.219, 499-513 (1995)
7. Perera, K: Existence and multiplicity results for a Sturm-Liouville equation asymptotically linear at –∞and superlinear at +∞. Nonlinear Anal.39, 669-684 (2000)
8. Motreanu, D, Motreanu, VV, Papageorgiou, NS: Multiple solutions for Dirichlet problems which are superlinear at +∞ and (sub-) linear at –∞. Commun. Pure Appl. Anal.13, 341-358 (2009)
9. Ziemer, WP: Weakly Differentiable Functions. Grad. Texts in Math., vol. 120. Springer, Berlin (1989)
10. Liu, Y, Wang, ZP: Biharmonic equations with asymptotically linear nonlinearities. Acta Math. Sci.27, 549-560 (2007) 11. Pei, RC: Multiple solutions for biharmonic equations with asymptotically linear nonlinearities. Bound. Value Probl.
2010, Article ID 241518 (2010)
12. Lazer, AC, Mckenna, PJ: Large amplitude periodic oscillation in suspension bridges: some new connections with nonlinear analysis. SIAM Rev.32, 537-578 (1990)
13. Micheletti, AM, Pistoia, A: Multiplicity solutions for a fourth order semilinear elliptic problems. Nonlinear Anal. TMA31, 895-908 (1998)
14. Chipot, M: Variational Inequalities and Flow in Porous Media. Springer, New York (1984)
15. Zhang, JH, Li, SJ: Multiple nontrivial solutions for some fourth-order semilinear elliptic problems. Nonlinear Anal. TMA
16. Chang, KC: Infinite Dimensional Morse Theory and Multiple Solutions Problems. Birkhäuser, Boston (1993) 17. Bartsch, T, Li, SJ: Critical point theory for asymptotically quadratic functionals and applications to problems with
resonance. Nonlinear Anal. TMA28, 419-441 (1997)
18. Qian, AX: Multiple solutions for a fourth-order asymptotically linear elliptic problem. Acta Math. Sin.22, 1121-1126 (2006)
19. Perera, K: Critical groups of critical points produced by local linking with applications. Abstr. Appl. Anal.3, 437-446 (1998)
20. Palais, RS: Homotopy theory of infinite dimensional manifolds. Topology5, 1-16 (1966)
10.1186/1687-2770-2014-12