R E S E A R C H
Open Access
Existence and multiplicity of solutions for
some second-order systems on time scales
with impulsive effects
Jianwen Zhou
1, Yanning Wang
2and Yongkun Li
1**Correspondence: [email protected] 1Department of Mathematics, Yunnan University, Kunming, Yunnan 650091, People’s Republic of China
Full list of author information is available at the end of the article
Abstract
In this paper, we present a recent approach via variational methods and critical point theory to obtain the existence of solutions for the nonautonomous second-order system on time scales with impulsive effects
⎧ ⎪ ⎨ ⎪ ⎩
u2(t) +A(σ(t))u(σ(t)) +∇F(σ(t),u(σ(t))) = 0,
-a.e.
t∈[0,T]κT;u(0) –u(T) =u(0) –u(T) = 0,
(ui)(t+j) – (ui)(t–j) =Iij(ui(tj)), i= 1, 2,. . .,N,j= 1, 2,. . .,p,
wheret0= 0 <t1<t2<· · ·<tp<tp+1=T,tj∈[0,T]T(j= 0, 1, 2,. . .,p+ 1),
u(t) = (u1(t),u2(t),. . .,uN(t))∈RN,A(t) = [dlm(t)] is a symmetricN×Nmatrix-valued function defined on [0,T]Twithdlm∈L∞([0,T]T,R) for alll,m= 1, 2,. . .,N,Iij:R→R (i= 1, 2,. . .,N,j= 1, 2,. . .,p) are continuous andF: [0,T]T×RN→R. Finally, two examples are presented to illustrate the feasibility and effectiveness of our results.
MSC: 34B37; 34N05
Keywords: nonautonomous second-order systems; time scales; impulse; variational approach
1 Introduction
Consider the nonautonomous second-order system on time scales with impulsive effects
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩
u(t) +A(σ(t))u(σ(t)) +∇F(σ(t),u(σ(t))) = , -a.e.t∈[,T]κ T; u() –u(T) =u() –u(T) = ,
(ui)(t+
j) – (ui)(t–j) =Iij(ui(tj)), i= , , . . . ,N,j= , , . . . ,p,
(.)
wheret= <t<t<· · ·<tp<tp+=T,tj∈[,T]T(j= , , , . . . ,p+ ),
uit+j=
⎧ ⎨ ⎩
limt→t+
j(u
i)(t), tis right-dense;
(ui)(σ(t
j)), tis right-scattered,
uit–j=
⎧ ⎨ ⎩
limt→t–
j (u
i)(t), tis left-dense;
(ui)(ρ(t
j)), tis left-scattered,
u(t) = (u(t),u(t), . . . ,uN(t)),A(t) = [d
lm(t)] is a symmetricN×N matrix-valued
func-tion defined on [,T]T with dlm ∈L∞([,T]T,R) for all l,m= , , . . . ,N, Iij :R→R
(i= , , . . . ,N,j= , , . . . ,p) are continuous andF: [,T]T×RN →Rsatisfies the fol-lowing assumption:
(A) F(t,x)is-measurable intfor everyx∈RN and continuously differentiable inxfor -a.e.t∈[,T]T, and there exista∈C(R+,R+),bσ ∈L(,T;R+)such that
F(t,x)≤a|x|b(t), ∇F(t,x)≤a|x|b(t)
for allx∈RN and-a.e.t∈[,T]
T, where∇F(t,x)denotes the gradient ofF(t,x) inx.
For the sake of convenience, in the sequel, we denote ={, , , . . . ,N},={, , , . . . ,p}.
WhenIij≡,i∈A,j∈BandA(t) is a zero matrix, (.) is the Hamiltonian system on
time scales
⎧ ⎨ ⎩
u(t) +∇F(σ(t),u(σ(t))) = , a.e.t∈[,T],
u() –u(T) =u() –u(T) = . (.)
In [], the authors study the Sobolev’s spaces on time scales and their properties. As ap-plications, they present a recent approach via variational methods and the critical point theory to obtain the existence of solutions for (.).
WhenIij(t)≡,i∈A, j∈BandA(t) is not a zero matrix, until now the variational
structure of (.) has not been studied.
Problem (.) covers the second-order Hamiltonian system with impulsive effects (when T=R)
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩ ¨
u(t) +A(t)u(t) +∇F(t,u(t)) = , a.e.t∈[,T];
u() –u(T) =u() –˙ u(T˙ ) = ,
u˙i(t
j) =u˙i(t+j) –u˙i(t–j) =Iij(ui(tj)), i∈,j∈,
(.)
as well as the second-order discrete Hamiltonian system (whenT=Z,T∈N,T≥)
⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
u(t+ ) – u(t+ ) +u(t) +A(t+ )u(t+ )
+∇F(t+ ,u(t+ )) = , t∈[,T– ]∩Z,
u() –u(T) = ,u(T) –u() =u(T+ ) –u(),
ui(t
j+ ) –ui(tj+ ) –ui(tj) +ui(tj– ) =Iij(ui(tj)), i∈,j∈.
In [], the authors establish some sufficient conditions on the existence of solutions of (.) by means of some critical point theorems whenA(t)≡. WhenT=R, until now, it is unknown whether problem (.) has a variational structure or not.
differential equations with or without delays occur in biology, medicine, mechanics, engi-neering, chaos theory and so on (see [–]).
For a second-order differential equationu=f(t,u,u), one usually considers impulses in the position uand the velocityu. However, in the motion of spacecraft, one has to consider instantaneous impulses depending on the position that result in jump discon-tinuities in velocity, but with no change in position (see []). The impulses only on the velocity occur also in impulsive mechanics (see []). An impulsive problem with impulses in the derivative only is considered in [].
The study of dynamical systems on time scales is now an active area of research. One of the reasons for this is the fact that the study on time scales unifies the study of both discrete and continuous processes, besides many others. The pioneering works in this direction are Refs. [–]. The theory of time scales was initiated by Stefan Hilger in his Ph.D. thesis in , providing a rich theory that unifies and extends discrete and continuous analy-sis [, ]. The time scales calculus has a tremendous potential for applications in some mathematical models of real processes and phenomena studied in physics, chemical tech-nology, population dynamics, biotechnology and economics, neural networks and social sciences (see []). For example, it can model insect populations that are continuous while in season (and may follow a difference scheme with variable step-size), die out in winter, while their eggs are incubating or dormant, and then hatch in a new season, giving rise to a nonoverlapping population.
There have been many approaches to study solutions of differential equations on time scales, such as the method of lower and upper solutions, fixed-point theory, coincidence degree theory and so on (see [, –]). In [], authors used the fixed point theorem of strict-set-contraction to study the existence of positive periodic solutions for functional differential equations with impulse effects on time scales. However, the study of the ex-istence and multiplicity of solutions for differential equations on time scales using the variational method has received considerably less attention (see, for example, [, ]). The variational method is, to the best of our knowledge, novel and it may open a new approach to deal with nonlinear problems, with some type of discontinuities such as impulses.
Motivated by the above, we research the existence of variational construction for prob-lem (.) in an appropriate space of functions and study the existence of solutions for (.) by some critical point theorems in this paper. All these results are new.
2 Preliminaries and statements
In this section, we present some fundamental definitions and results from the calculus on time scales and Sobolev’s spaces on time scales that will be required below. These are a generalization toRnof definitions and results found in [].
Definition .([, Definition .]) LetTbe a time scale. Fort∈T, the forward jump operatorσ:T→Tis defined by
σ(t) =inf{s∈T,s>t} for allt∈T,
while the backward jump operatorρ:T→Tis defined by
(supplemented byinf∅=supTandsup∅=infT, where∅denotes the empty set). A point t∈Tis called right-scattered, left-scattered, ifσ(t) >t,ρ(t) <thold, respectively. Points that are right-scattered and left-scattered at the same time are called isolated. Also, ift<
supTandσ(t) =t, thentis called right-dense, and ift>infTandρ(t) =t, thentis called left-dense. Points that are right-dense and left-dense at the same time are called dense. The setTκ which is derived from the time scaleTas follows. IfThas a left-scattered maximumm, thenTκ=T–{m}; otherwise,Tκ=T.
Whena,b∈T,a<b, we denote the intervals [a,b]T, [a,b)Tand (a,b]TinTby
[a,b]T= [a,b]∩T, [a,b)T= [a,b)∩T, (a,b]T= (a,b]∩T,
respectively. Note that [a,b]κ
T= [a,b]Tifbis left-dense and [a,b]κT= a,b)T= [a,ρ(b)]Tifb is left-scattered. We denote [a,b]κ
T = ([a,b]κT)κ, therefore [a,b]κ
T = [a,b]Tifbis left-dense and [a,b]κ
T = [a,ρ(b)]κTifbis left-scattered.
Definition .([, Definition .]) Assume thatf :T→Ris a function and lett∈Tκ.
Then we definef(t) to be the number (provided it exists) with the property that given any> , there is a neighborhoodUoft(i.e.,U= (t–δ,t+δ)∩Tfor someδ> ) such that
fσ(t)–f(s)–f(t)σ(t) –s≤σ(t) –s for alls∈U.
We callf(t) the delta (or Hilger) derivative off att. The functionf is delta (or Hilger) differentiable onTκprovidedf(t) exists for allt∈Tκ. The functionf:Tκ→Ris then called the delta derivative off onTκ.
Definition .([, Definition .]) Assume thatf:T→RN is a function,
f(t) =f(t),f(t), . . . ,fN(t),
and lett∈Tκ. Then we definef(t) = (f
(t),f(t), . . . ,fN(t)) (provided it exists). We callf(t) the delta (or Hilger) derivative off att. The functionf is delta (or Hilger) differ-entiable providedf(t) exists for allt∈Tκ. The functionf:Tκ→RN is then called the
delta derivative off onTκ.
Definition . ([, Definition .]) For a functionf :T→R, we will talk about the second derivativef providedf is differentiable onTκ= (Tκ)κ with derivativef= (f):Tκ→R.
Definition .([, Definition .]) For a function f :T→RN, we will talk about the second derivativef providedf is differentiable onTκ= (Tκ)κ with derivativef= (f):Tκ→RN.
Definition . ([, Definition .]) Assume that f : T → RN is a function, f(t) =
(f(t),f(t), . . . ,fN(t)) and let A be a-measurable subset ofT.f is integrable onA if
and only iffi(i= , , . . . ,N) are integrable onA, and
Af(t)t= (
Af(t)t,
Af(t)t,
. . . ,AfN(t)t).
Definition .([, Definition .]) LetB⊂T.Bis called a-null set ifμ(B) = . Say that a propertyPholds-almost everywhere (-a.e.) onB, or for-almost all (-a.a.) t∈Bif there is a-null setE⊂Bsuch thatPholds for allt∈B\E.
Forp∈R,p≥, we set the space
Lp
[,T)T,RN=
u: [,T)T→RN:
[,T)T
f(t)pt< +∞
with the norm
fLp
=
[,T)T
f(t)pt
p
.
We have the following theorem.
Theorem .([, Theorem .]) Let p∈Rbe such that p≥.Then the space Lp( [,T)T, RN) is a Banach space together with the norm ·
Lp. Moreover, L( [a,b)T,RN) is a Hilbert space together with the inner product given for every(f,g)∈Lp( [a,b)T,RN)× Lp( a,b)T,RN)by
f,gL
=
[a,b)T
f(t),g(t)t,
where(·,·)denotes the inner product inRN.
Definition . ([, Definition .]) A function f : [a,b]T → RN,f(t) = (f(t),f(t), . . . ,fN(t)). We say thatf is absolutely continuous on [a,b]
T (i.e.,f ∈AC([a,b]T,RN)) if for every > , there existsδ> such that if{[ak,bk)T}nk= is a finite pairwise disjoint family of subintervals of [a,b]Tsatisfyingnk=(bk–ak) <δ, then
n
k=|f(bk) –f(ak)|<.
Now, we recall the Sobolev spaceW,,pT([,T]T,RN) on [,T]Tdefined in []. For the sake of convenience, in the sequel we letuσ(t) =u(σ(t)).
Definition .([, Definition .]) Letp∈Rbe such thatp> andu: [,T]T→RN. We say thatu∈W,p,T([,T]T,RN) if and only ifu∈Lp( [,T)T,RN) and there existsg: [,T]κT→RN suchg∈Lp( [,T)T,RN) and
[,T)T
u(t),φ(t)t= –
[,T)T
g(t),φσ(t)t, ∀φ∈CT,rd[,T]T,RN. (.)
Forp∈R,p> , we denote
V,,pT
[,T]T,RN=x∈AC[,T]T,RN:x∈Lp
It follows from Remark . in [] that
V,p
[,T]T,RN
⊂W,p
[,T]T,RN
is true for every p∈Rwithp> . These two sets are, as a class of functions, equiva-lent. It is the characterization of functions inW,p,T([,T]T,RN) in terms of functions in V,,pT([,T]T,RN) too. That is the following theorem.
Theorem .([, Theorem .]) Suppose that u∈W,p,T([,T]T,RN)for some p∈Rwith p> ,and that(.)holds for g∈Lp( [,T)T,RN).Then there exists a unique function x∈V,p,T([,T]T,RN)such that the equalities
x=u, x=g -a.e. on [,T)T (.)
are satisfied and
[,T)T
g(t)t= . (.)
By identifyingu∈W,,pT([,T]T,RN) with its absolutely continuous representativex∈
V,,pT([,T]T,RN) for which (.) holds, the setW,p,T([,T]T,RN) can be endowed with
the structure of a Banach space. That is the following theorem.
Theorem .([, Theorem .]) Assume p∈Rand p> .The set W,p,T([,T]T,RN)is
a Banach space together with the norm defined as
uW,p
,T=
[,T)T
uσ(t)pt+
[,T)T
u(t)pt
p
∀u∈W,p,T
[,T]T,RN. (.)
Moreover,the set H,T=W
,
,T([,T]T,RN)is a Hilbert space together with the inner
prod-uct
u,vH
,T=
[,T)T
uσ(t),vσ(t)t+
[,T)T
u(t),v(t)t ∀u,v∈H,T.
The Banach spaceW,p,T([,T]T,RN) has some important properties.
Theorem .([, Theorem .]) There exists C> such that the inequality
u∞≤CuH,T (.)
holds for all u∈H
,T,whereu∞=maxt∈[,T]T|u(t)|. Moreover,if[,T)Tu(t)t= ,then
u∞≤CuL
Theorem .([, Theorem .]) If the sequence{uk}k∈N⊂W,p,T([,T]T,RN)converges
weakly to u in W,,pT([,T]T,RN),then{uk}k∈Nconverges strongly in C([,T]T,RN)to u.
Theorem .([, Theorem .]) Let L: [,T]T×RN ×RN →R, (t,x,y)→L(t,x,y) be-measurable in t for each(x,y)∈RN ×RN and continuously differentiable in(x,y) for-almost every t∈[,T]T. If there exist a∈C(R+,R+),b∈L([,T]T,R+)and c∈ Lq([,T]T,R+) ( <q< +∞)such that for-almost t∈[,T]Tand every(x,y)∈RN×RN, one has
L(t,x,y)≤a|x|b(t) +|y|p,
Lx(t,x,y)≤a
|x|b(t) +|y|p, (.)
Ly(t,x,y)≤a
|x|c(t) +|y|p–,
wherep+q= ,then the functional:W,p,T([,T]T,RN)→Rdefined as
(u) =
[,T)T
Lσ(t),uσ(t),u(t)t
is continuously differentiable on W,p,T([,T]T,RN)and
(u),v=
[,T)T Lx
σ(t),uσ(t),u(t),vσ(t)
+Ly
σ(t),uσ(t),u(t),v(t)t. (.)
3 Variational setting
In this section, we recall some basic facts which will be used in the proofs of our main results. In order to apply the critical point theory, we make a variational structure. From this variational structure, we can reduce the problem of finding solutions of (.) to the one of seeking the critical points of a corresponding functional.
If u ∈H
,T, by identifying u ∈H,T with its absolutely continuous representative
x∈ V,,T([,T]T,RN) for which (.) holds, then u is absolutely continuous and u˙ ∈ L( [,T)
T;RN). In this case,u(t+) –u(t–) = may not hold for somet∈(,T)T. This leads to impulsive effects.
Takev∈H
,Tand multiply the two sides of the equality
u(t) +Aσ(t)uσ(t)+∇Fσ(t),uσ(t)=
byvσ and integrate on [,T)
T, then we have
[,T)T
u(t) +Aσ(t)uσ(t)+∇Fσ(t),uσ(t)vσ(t)t= . (.)
Moreover, combiningu() –u(T) = , one has
[,T)T
u(t),vσ(t)t
=
p
j=
[tj,tj+)T
=
p
j=
utj–+,vtj–+–ut+j,vtj+–
[tj,tj+)
u(t),v(t)t
= p j= N i=
uitj–+vitj–+–uit+jvitj+–
[tj,tj+)
u(t),v(t)t
=u(T)v(T) –u()v() –
p j= N i= Iij
ui(tj)
vi(tj) –
[,T)T
u(t),v(t)t
= – p j= N i= Iij
ui(tj)
vi(tj) –
[,T)T
u(t),v(t)t.
Combining (.), we have
[,T)T
u(t),v(t)t+
p j= N i= Iij
ui(tj)
vi(tj)
–
[,T)T
Aσ(t)uσ(t),vσ(t)t–
[,T)T
∇Fσ(t),uσ(t),vσ(t)t= .
Considering the above, we introduce the following concept solution for problem (.).
Definition . We say that a functionu∈H
,Tis a weak solution of problem (.) if the
identity
[,T)T
u(t),v(t)t+
p j= N i= Iij
ui(tj)
vi(tj)
=
[,T)T
Aσ(t)uσ(t),vσ(t)t+
[,T)T
∇Fσ(t),uσ(t),vσ(t)t
holds for anyv∈H,T.
Consider the functionalϕ:H
,T→Rdefined by
ϕ(u) =
[,T)T
u(t)t+
p j= N i=
ui(t j)
Iij(t) dt
–
[,T)T
Aσ(t)uσ(t),uσ(t)t+J(u)
=ψ(u) +φ(u), (.)
where
J(u) = –
[,T)T
Fσ(t),uσ(t)t,
ψ(u) =
[,T)T
u(t)t–
[,T)T
and
φ(u) =
p
j=
N
i=
ui(tj)
Iij(t) dt.
Lemma . The functionalϕis continuously differentiable on H ,Tand
ϕ(u),v=
[,T)T
u(t),v(t)t+
p
j=
N
i= Iij
ui(tj)
vi(tj)
–
[,T)T
Aσ(t)uσ(t),vσ(t)–∇Fσ(t),uσ(t),vσ(t)t. (.)
Proof Set L(t,x,y) = |y|
–
(A(t)x,x) –F(t,x) for all x,y∈R
N andt∈[,T]
T. Then L(t,x,y) satisfies all assumptions of Theorem .. Hence, by Theorem ., we know that the functionalψ is continuously differentiable onH,Tand
ψ(u),v=
[,T)T
u(t),v(t)–Aσ(t)uσ(t),vσ(t)–∇Fσ(t),uσ(t),vσ(t)t
for allu,v∈H ,T.
On the other hand, by the continuity ofIij,i∈,j∈, one has thatφ∈C(H,T,R) and
φ(u),v=
p
j=
N
i= Iij
ui(tj)
vi(tj)
for allu,v∈H,T. Thus,ϕis continuously differentiable onH,Tand (.) holds.
By Definition . and Lemma ., the weak solutions of problem (.) correspond to the critical points ofϕ.
Moreover, we need more preliminaries. For anyu∈H,T, let
q(u) =
[,T)T
uσ(t)–Aσ(t)uσ(t),uσ(t)t.
We see that
q(u) = u
–
[,T)T
Aσ(t) +IN×N
uσ(t),uσ(t)t
=
(I–K)u,u,
whereK:H,T→H,Tis the bounded self-adjoint linear operator defined, using the Riesz
representation theorem, by
Ku,v=
[,T)T
Aσ(t) +IN×N
IN×NandIdenote anN×Nidentity matrix and an identity operator, respectively. By (.), ϕ(u) can be rewritten as
ϕ(u) =q(u) +φ(u) +J(u)
=
(I–K)u,u+φ(u) +J(u). (.)
The compact imbedding ofH,TintoC([,T]T,RN) implies thatKis compact. By classical
spectral theory, we can decomposeH,Tinto the orthogonal sum of invariant subspaces
forI–K
H,T=H–⊕H⊕H+,
whereH=ker(I–K) andH–,H+are such that, for someδ> ,
q(u)≤–δu ifu∈H–, (.)
q(u)≥δu ifu∈H+. (.)
Remark . K has only finitely many eigenvaluesλiwithλi> sinceKis compact on
HT. HenceH– is finite dimensional. Notice thatI–Kis a compact perturbation of the self-adjoint operatorI. By a well-known theorem, we know that is not in the essential spectrum ofI–K. Hence,His a finite dimensional space too.
To prove our main results, we need the following definitions and theorems.
Definition .([,P]) LetXbe a real Banach space andI∈C(X,R).Iis said to be satisfying (PS) condition onXif any sequence{xn} ⊆Xfor whichI(xn) is bounded and
I(xn)→ asn→ ∞, possesses a convergent subsequence inX.
Firstly, we state the local linking theorem.
LetXbe a real Banach space with a direct decompositionX=X⊕X. Consider two sequences of a subspace
X⊂X⊂ · · · ⊂X, X⊂X⊂ · · · ⊂X
such that
dimXn< +∞, dimXn< +∞, n∈N
and
X=
n∈N X
n, X=
n∈N X
n.
For every multi-indexα= (α,α)∈N, we denote byXα the spaceXα⊕Xα. We say
α≤β⇔α≤β,α≤β. A sequence (αn)⊂Nis admissible if, for everyα∈N, there is
Definition .([, Definition .]) LetI∈C(X,R). The functionalIsatisfies the (C)* condition if every sequence (uαn) such thatαnis admissible and
uαn∈Xαn,supI(uαn)<∞,
+uαn
I(uαn)→
contains a subsequence which converges to a critical point ofI.
Theorem .[, Theorem .] Suppose that I∈C(X,R)satisfies the following assump-tions:
(I) X={}andIhas a local linking atwith respect to(X,X);that is,for someM> ,
I(u)≥, u∈X,u ≤M,
I(u)≤, u∈X,u ≤M.
(I) Isatisfies(C)*condition.
(I) Imaps bounded sets into bounded sets.
(I) For everyn∈N,I(u)→–∞asu → ∞,u∈X
n⊕X.
Then I has at least two critical points.
Remark . SinceI∈C(X,R), by the condition (I) of Theorem ., is the critical point ofI. Thus, under the conditions of Theorem .,Ihas at least one nontrivial critical point.
Secondly, we state another three critical point theorems.
Theorem .([, Theorem .]) Let E be a Hilbert space with E=E⊕Eand E=E⊥. Suppose I∈C(E,R),satisfies(PS)condition,and
(I) I(u) = Lu,u+b(u),whereLu=LPu+LPu andLκ:Eκ →Eκ is bounded and self-adjoint,κ= , ,
(I) bis compact,and
(I) there exist a subspaceE⊂Eand setsS⊂E,Q⊂Eand constantsα>ωsuch that
(i) S⊂EandI|S≥α, (ii) Qis bounded andI|∂Q≤ω,
(iii) Sand∂Qlink.
Then I possesses a critical value c≥α.
Theorem .([, Theorem .]) Let E be a Banach space.Let I∈C(E,R)be an even
functional which satisfies the(PS)condition and I() = .If E=V⊕W,where V is finite dimensional,and I satisfies
(I) there are constantsρ,α> such thatI|∂Bρ∩W≥α,whereBρ={x∈E:x<ρ},
(I) for each finite dimensional subspaceE⊂E,there is an R=R(E)such thatI≤on
E\BR(E),
In order to state another critical point theorem, we need the following notions. LetXand Y be Banach spaces withXbeing separable and reflexive, and setE=X⊕Y. LetS⊂X* be a dense subset. For eachs∈S, there is a semi-norm onEdefined by
ps:E→R, ps(u) =s(x)+y foru=x+y∈X⊕Y.
We denote byTSthe topology onEinduced by a semi-norm family{ps}, and letwandw* denote the weak-topology and weak*-topology, respectively.
For a functional∈C(E,R), we write
a={u∈E:(u)≥a}. Recall that is said
to be weak sequentially continuous if, for anyuku inE, one haslimk→∞(uk)v→ (u)vfor eachv∈E,i.e.,: (E,w)→(E*,w*) is sequentially continuous. Forc∈R, we say thatsatisfies the (C)ccondition if any sequence{uk} ⊂Esuch that(uk)→cand
( +uk)(uk)→ ask→ ∞contains a convergent subsequence.
Suppose that
() for anyc∈R,cisTS-closed, and: (c,TS)→(E*,w*)is continuous; () there existsρ> such thatκ:=inf(∂Bρ∩Y) > , where
Bρ=
u∈E:u<ρ;
() there exist a finite dimensional subspaceY⊂Y andR>ρsuch thatc¯:=sup(E) <
∞andsup(E\S) <inf(Bρ∩Y), where
E:=X⊕Y, and S=
u∈E:u ≤R
.
Theorem .([]) Assume thatis even and()-()are satisfied.Thenhas at least m=dimYpairs of critical points with critical values less than or equal toc provided¯
satisfies the(C)ccondition for all c∈[κ,¯c].
Remark . In our applications, we take S=X* so thatTS is the product topology on E=X⊕Ygiven by the weak topology onXand the strong topology onY.
4 Main results
Lemma . φis compact on H ,T.
Proof Let{uk} ⊂H,T be any bounded sequence. SinceH,T is a Hilbert space, we can
assume thatuku. Theorem . implies thatuk–u∞→. By (.), we have
φ(uk) –φ(u)
= sup
v∈H
,T,v≤
φ(uk) –φ(u),v
= sup
v∈H,T,v≤
p
j=
N
i= Iij
uik(tj)
–Iij
ui(tj)
vi(tj)
≤ v∞ sup
v∈H,T,v≤ p
j=
N
i=
Iij
uik(tj)
–Iij
≤Cv sup v∈H,T,v≤
p
j=
N
i=
Iij
uik(tj)
–Iij
ui(tj)
=C sup
v∈H
,T,v≤
p
j=
N
i=
Iij
uik(tj)
–Iij
ui(tj).
The continuity ofIijand this imply thatφ(uk)→φ(u) inH,T. The proof is complete.
First of all, we give two existence results.
Theorem . Suppose that(A)and the following conditions are satisfied.
(F) lim|x|→∞F|(xt|,x)= +∞uniformly for-a.e.t∈[,T]T,
(F) lim|x|→F|(xt|,x)= uniformly for-a.e.t∈[,T]T, (F) there existλ> andβ>λ– such that
lim sup
|x|→∞ F(t,x)
|x|λ <∞ uniformly for-a.e.t∈[,T]T
and
lim inf
|x|→∞
(∇F(t,x),x) – F(t,x)
|x|β > uniformly for-a.e.t∈[,T]T,
(F) there existsr> such that
F(t,x)≥, ∀|x| ≤r,and-a.e.t∈[,T]T,
(F) there existaij,bij> andξij∈[, )such that
Iij(t)≤aij+bij|t|ξij for everyt∈R,i∈,j∈,
(F) tIij(s) ds≤for everyt∈R,i∈,j∈,
(F) there existsζij> such that
t
Iij(s) ds–Iij(t)t≥ for alli∈,j∈and|t| ≥ζij,
and
lim t→
Iij(t)
t = for alli∈,j∈.
Then problem(.)has at least two weak solutions.The one is a nontrivial weak solution, the other is a trivial weak solution.
Proof By Lemma .,ϕ∈C(X,R). SetX=H
,T,X=H+with (en)n≥being its Hilbertian basis,X=H–⊕Hand define
Then we have
X⊂X⊂ · · · ⊂X, X⊂X⊂ · · · ⊂X, X=
n∈N X
n, X=
n∈N X
n
and
dimXn< +∞, dimXn< +∞, n∈N.
We divide our proof into four parts in order to show Theorem .. Firstly, we show thatϕsatisfies the (C)*condition.
Let{uαn}be a sequence inH,Tsuch thatαnis admissible and
uαn∈Xαn,supϕ(uαn)< +∞,
+uαn
ϕ(uαn)→,
then there exists a constantC> such that
ϕ(uαn)≤C,
+uαn
ϕ(uαn)≤C (.)
for all largen. On the other hand, by (F), there are constantsC> andρ> such that
F(t,x)≤C|x|λ (.)
for all|x| ≥ρand-a.e.t∈[,T]T. By (A) one has
F(t,x)≤ max s∈[,ρ]
a(s)b(t) (.)
for all|x| ≤ρand-a.e.t∈[,T]T. It follows from (.) and (.) that
F(t,x)≤ max s∈[,ρ]
a(s)b(t) +C|x|λ (.)
for allx∈RN and-a.e.t∈[,T]T. Sincedlm∈L∞([,T]) for alll,m= , , . . . ,N, there
exists a constantC≥ such that
[,T)
T
Aσ(t)uσ(t),uσ(t)t≤C
[,T)T
uσ(t)t, ∀u∈H,T. (.)
From (F) and (.), we have that
φ(u)≤
p
j=
N
i=
|ui(tj)|
aij+bij|t|ξij
dt
≤apNu∞+b
p
j=
N
i=
uξ∞ij+
≤apNCu+bC
p
j=
N
i=
for allu∈H
,T, wherea=maxi∈,j∈{aij},b=maxi∈,j∈{bij}. Combining (.), (.), (.) and Hölder’s inequality, we have
uαn
=ϕ(u
αn) –φ(uαn) +
[,T)T
uσ αn(t)
t
+
[,T)T
Aσ(t)uσαn(t),u
σ αn(t)
t–J(uαn)
≤C+apNCuαn+bC
p j= N i=
uαn
ξij++C
[,T)T
uσαn(t)
t
+C
[,T)T
uσαn(t)
λ
t+ max s∈[,ρ]
a(s)
[,T)T bσ(t)t
≤C+apNCuαn+bC
p j= N i=
uαn
ξij+
+CTλ–λ
[,T)T
uσαn(t)
λ t λ +C
[,T)T
uσαn(t)
λ
t+C (.)
for all largen, whereC=maxs∈[,ρ]a(s)
[,T)Tb
σ(t)t. On the other hand, by (F), there
existC> andρ> such that
∇F(t,x),x– F(t,x)≥C|x|β (.)
for all|x| ≥ρand-a.e.t∈[,T]T. By (A),
∇F(t,x),x– F(t,x)≤Cb(t) (.)
for all|x| ≤ρand-a.e.t∈[,T]T, whereC= ( +ρ)maxs∈[,ρ]a(s). Combining (.) and (.), one has
∇F(t,x),x– F(t,x)≥C|x|β–Cρβ–Cb(t) (.)
for allx∈RN and-a.e.t∈[,T]
T. According to (F), there existsC> such that
t
Iij(s) ds–Iij(t)t≥–C for alli∈,j∈andt∈R. (.)
Thus, by (.), (.) and (.), we obtain
C≥ϕ(uαn) –
ϕ(uαn),uαn
= φ(uαn) –
φ(uαn),uαn
+
[,T)T
∇Fσ(t),uσαn(t)
,uσαn(t)
– Fσ(t),uσαn(t)
t = p j= N i=
uiαn(tj)
Iij(t) dt–Iij
uiαn(tj)
uiαn(tj)
+
[,T)T
∇Fσ(t),uσαn(t)
,uσαn(t)
– Fσ(t),uσαn(t)
t
≥–pNC+C
[,T)T
uσαn
β
t–CρβT–C
[,T)T
bσ(t)t (.)
for all largen. From (.),[,T)T|uσ αn|
βtis bounded. Ifβ>λ, by Hölder’s inequality, we
have
[,T)T
uσαn(t)
λ
t≤Tβ–βλ
[,T)T
uσαn(t)
β
t
λ β
. (.)
Sinceξij∈[, ) for alli∈,j∈, by (.) and (.),{uαn}is bounded inH,T. Ifβ≤λ,
by (.), we obtain
[,T)T
uσαn(t)
λ
t=
[,T)T
uσαn(t)
β uσαn(t)
λ–β
t
≤ uαn
λ–β ∞
[,T)T
uσαn(t)
β
t
≤Cλ–βuαn
λ–β
[,T)T
uσαn(t)
β
t. (.)
Sinceξij∈[, ),λ–β< , by (.) and (.),{uαn}is also bounded inH,T. Hence,{uαn}
is also bounded inH
,T. Going if necessary to a subsequence, we can assume thatuαnu
inH,T. From Theorem ., we haveuαn–u∞→ and
[,T)T|u σ αn(t) –u
σ(t)|t→.
Since
[,T)T
uαn(t) –u
(t)t
=ϕ(uαn) –ϕ(u),uαn–u
+
[,T)T
Aσ(t)uσαn(t) –u
σ(t),
uσαn(t) –u
σ(t) t – p j= N i= Iij
uiαn(tj)
–Iij
ui(tj)
uiαn(tj) –ui(tj)
+
[,T)T
∇Fσ(t),uσ αn(t)
–∇Fσ(t),uσ(t),uσ αn(t) –u
σ(t)t.
This implies[,T)T|u αn(t) –u
(t)|t→, and henceu
αn–u →. Therefore,uαn→u
inH
,T. Henceϕsatisfies the (C)*condition.
Secondly, we show thatϕmaps bounded sets into bounded sets. It follows from (.), (.), (.) and (.) that
ϕ(u)=
[,T)T
u(t)t+
p j= N i=
ui(tj)
Iij(t) dt
–
[,T)T
Aσ(t)uσ(t),uσ(t)t+J(u)
≤
[,T)T
u(t)t+C
[,T)T
+bC
p
j=
N
i=
uξij+
+C
[,T)T
uσ(t)λt+ max s∈[,ρ]
a(s)
[,T)T bσ(t)t
≤
Cu
+apNCu+bC
p
j=
N
i=
uξij++CTuλ
∞+C
≤
Cu
+apNC
u+bC
p
j=
N
i=
uξij++C
TCλuλ+C
for allu∈H
,T. Thus,ϕmaps bounded sets into bounded sets.
Thirdly, we claim thatϕhas a local linking at with respect to (X,X). Applying (F), for=δ, there existsρ> such that
F(t,x)≤|x| (.)
for all|x| ≤ρand-a.e.t∈[,T]T. By (F), for=pNCδ , there existsρ> such that
Iij(t)≤|t|, |t| ≤ρ,i∈,j∈. (.)
Letρ=min{ρ,ρ}. Foru∈Xwithu ≤rρC, by (.), (.), (.), (.) and (.), we have
ϕ(u) =q(u) +
p
j=
N
i=
ui(tj)
Iij(t) dt–
[,T)T
Fσ(t),uσ(t)t
≥δu–
p
j=
N
i=
|ui(tj)|
Iij(t)dt–
[,T)T
uσ(t)t
≥δu–
p
j=
N
i=
|ui(tj)|
|t|dt–
[,T)T
uσ(t)t
≥δu–
p
j=
N
i=
u∞–
[,T)T
uσ(t)t
≥δu–pNCu–u
≥δu–δ u
–δ u
= δ u
.
This implies that
ϕ(u)≥, ∀u∈Xwithu ≤r.
On the other hand, it follows from (F) that
for allu∈H
,T. Letu=u–+u∈X satisfyu ≤r Cr. Using (F), (.), (.), (.) and (.), we obtain
ϕ(u) =q(u) +φ(u) –
[,T)T
Fσ(t),uσ(t)t
≤–δu––
[,T)T
Fσ(t),uσ(t)t
≤–δu–.
This implies that
ϕ(u)≤, ∀u∈Xwithu ≤r.
LetM=min{r,r}. Thenϕsatisfies the condition (I) of Theorem .. Finally, we claim that for everyn∈N,
ϕ(u)→–∞ asu → ∞,u∈Xn⊕X.
For givenn∈N, sinceX
n⊕Xis a finite dimensional space, there existsC> such that
u ≤CuL, ∀u∈Xn⊕X. (.)
By (F), there existsρ> such that
F(t,x)≥C(C+δ)|x| (.)
for all|x| ≥ρand-a.e.t∈[,T]T. From (A), we get
F(t,x)≤ max s∈[,ρ]
a(s)b(t) (.)
for all|x| ≤ρand-a.e.t∈[,T]T. Equations (.) and (.) imply that
F(t,x)≥C(C+δ)|x|–C– max
s∈[,ρ]
a(s)b(t) (.)
for allx∈RN and-a.e.t∈[,T]T, whereC=C(C+δ)ρ. Using (.), (.), (.), (.), (.) and (.), we have, foru=u++u+u–∈X
n⊕X=Xn⊕H⊕H–,
ϕ(u) =
[,T)T
u(t)t+
p
j=
N
i=
ui(t j)
Iij(t) dt
–
[,T)T
Aσ(t)uσ(t),uσ(t)t–
[,T)T
Fσ(t),uσ(t)t
≤–δu–+
[,T)T
u+(t)t
–
[,T)T
Aσ(t)u+σ(t),u+σ(t)t–
[,T)T
≤–δu–+
[,T)T
u+(t)t+C
[,T)T
u+σ(t)t
–
[,T)T
Fσ(t),uσ(t)t
≤–δu–+C u
+–C
(C+δ)u σ
L+CT+ max
s∈[,ρ] a(s)
[,T)T bσ(t)t
≤–δu–+Cu+– (C+δ)u+CT+C
= –δu–+Cu+
– (C+δ)u++u+u–
+CT+C
≤–δu–+Cu+
– (C+δ)u+
–δu+u–+CT+C
≤–δu–+Cu+
– (C+δ)u+
–δu+CT+C
= –δu+CT+C,
whereC=maxs∈[,ρ]a(s)
[,T)Tb
σ(t)t. Hence, for everyn∈N,ϕ(u)→–∞asu →
∞andX
n⊕X.
Thus, by Theorem ., problem (.) has at least one nontrivial weak solution. The proof
is complete.
Example . LetT=R,T =π
, N= , t= π
. Consider the second-order Hamiltonian system with impulsive effects
⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩ ¨
u(t) +A(t)u(t) +∇F(t,x) = , a.e.t∈[,π ];
u() –u(π) =u() –˙ u(˙ π) = ,
u(t) =˙ u(t˙ +
) –u(t˙ –) =I(u(t)),
(.)
whereA(t) = ,
F(t,x) =
⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
|x|, |x| ≥,
–√x– √
–√,
√
<x< ,
, |x| ≤√,
√–x+
√
√–, –≤x< –
√
for allx∈Randt∈[,π ], I(t) = ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩
, t≥,
–(t– ), ≤t< ,
t– , <t< ,
–t, |t| ≤,
t+ , – <t< –,
–(t+ ), – <t≤–,
then all conditions of Theorem . hold. According to Theorem ., problem (.) has at least one nontrivial weak solution. In fact,
u(t) =
⎧ ⎨ ⎩
√cost, t∈[,π];
√sint, t∈[π ,
π ]
is the solution of problem (.).
Theorem . Assume that(A), (F), (F), (F)and the following conditions are satisfied.
(F) lim sup|x|→F|(t,x)
x| ≤uniformly for-a.e.t∈[,T]T,
(F) there exist constantsμ> andr≥such that(∇F(t,x),x)≥μF(t,x) > for allt∈ [,T]Tand|x| ≥r,
(F) F(t,x)≥for allx∈RN and-a.e.t∈[,T]
T.
Then problem(.)has at least one nontrivial weak solution.
Proof SetE=H+,E=H–⊕HandE=H,T. ThenEis a real Hilbert space,E=E⊕E, E=E⊥ anddim(E) < +∞.
Firstly, we prove thatϕsatisfies the (PS) condition. Indeed, let{uk} ⊂H,Tbe a sequence
such that|ϕ(uk)| ≤Candϕ(uk)→ ask→ ∞. As the proof of Theorem ., it suffices
to show that{uk}is bounded inH
,T. By (F) there exist positive constantsC,Csuch
that
F(t,x)≥C|x|μ–C, ∀t∈[,T]
T,∀x∈Rn (.)
(see []). By (F), (.) and (.), we have
C+uk
≥ϕ(uk) –
ϕ(uk),uk
= φ(uk) –
φ(uk),uk
+
[,T)T
∇Fσ(t),uσk(t),ukσ(t)– Fσ(t),uσk(t)t
=
p
j=
N
i=
uik(tj)
Iij(t) dt–Iij
uik(tj)
uik(tj)
+
[,T)T
∇Fσ(t),uσ
k(t)
,uσ
k(t)
– Fσ(t),uσ
k(t)
t
= –pNC+
[,T)T
∇Fσ(t),uσ
k(t)
,uσ
k(t)
– Fσ(t),uσ
k(t)
t
= –pNC+ (μ– )
[,T)T
Fσ(t),uσk(t)t
+
[,T)T
∇Fσ(t),uσk(t),uσk(t)–μFσ(t),uσk(t)t
≥–pNC+ (μ– )
[,T)T
+
[,T)T
∇Fσ(t),uσk(t),uσk(t)–μFσ(t),uσk(t)t
≥–pNC+ (μ– )C
[,T)T
|uσk|(t)μt– (μ– )CT–C (.)
for largek, whereC= (r+μ)maxs∈[,r]a(s)
[,T)Tb
σ(t)t. Equation (.) implies that
there existsC> such that
[,T)T
uσk(t)μt≤C +uk. (.)
Combining (.), (.), (.) and (.), we obtain
μc+uk
≥μϕ(uk) –
ϕ(uk),uk
=
μ
– [,T)T
uk(t)–Aσ(t)uσk(t),uσk(t)t
+
[,T)T
∇Fσ(t),uσ
k(t)
,uσ
k(t)
–μFσ(t),uσ
k(t)
t+μφ(uk) –
φ(uk),uk
=
μ
– [,T)T
uk(t)–Aσ(t)uσk(t),ukσ(t)t+ (μ– )φ(uk) + φ(uk)
+
[,T)T
∇Fσ(t),uσ
k(t)
,uσ
k(t)
–μFσ(t),uσ
k(t)
t–φ(uk),uk ≥ μ – uk–
μ – – μ – C [,T)T
uσ
k(t)
t–C–pNC
– (μ– )apNCuk– (μ– )bC
p j= N i=
ukξij+
≥
μ
–
uk–
μ – – μ – C
Tμμ–
[,T)T
uσ k(t) μ t μ
–C–pNC– (μ– )apNCuk– (μ– )bC
p j= N i=
ukξij+
≥
μ
–
uk–
μ – – μ – C
Tμμ– C
+ukμ
–C–pNC– (μ– )apNCuk– (μ– )bC
p j= N i=
ukξij+ (.)
for largek. Sinceμ> ,ξij∈[, ), by (.),{uk}is bounded inH,T.
For any small=δ, by (F) we know that there is aρ> such that
F(t,x)≤|x|, for|x|<ρ-a.e.t∈[,T]T. (.)
By (F), for=pNCδ , there existsρ> such that