In this paper, we consider the existence of infinitely many periodic solutions for some ordinary p(t)-Laplacian differential systems by minimax methods in critical point theory.
Citation: Chungen Liu, Yuyou Zhong. Infinitely many periodic solutions for ordinary p(t)-Laplacian differential systems[J]. Electronic Research Archive, 2022, 30(5): 1653-1667. doi: 10.3934/era.2022083
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In this paper, we consider the existence of infinitely many periodic solutions for some ordinary p(t)-Laplacian differential systems by minimax methods in critical point theory.
Consider periodic solution of the ordinary p(t)-Laplacian differential system
{ddt(|˙u(t)|p(t)−2˙u(t))+∇F(t,u(t))=0,u∈RN,u(0)−u(T)=˙u(0)−˙u(T)=0, | (1.1) |
where T>0, p(t)>1 is a T-periodic continuous function, F(t,x) is T-periodic in t for any x∈RN. Here we always assume that F(t,x) satisfies the following condition.
(A) F(t,x) is measurable in t for any x∈RN and continuously differentiable in x for a.e. t∈[0,T], and there exist two functions a∈C(R+;R+),b∈L1([0,T];R+) such that
|F(t,x)|≤a(|x|)b(t),|∇F(t,x)|≤a(|x|)b(t),∀x∈RNanda.e.t∈[0,T], |
where ∇F(t,x) denotes the gradient of F(t,x) in x.
In the sequel of this paper, we set p−:=min0≤t≤Tp(t), p+:=max0≤t≤Tp(t) and q−>1 such that 1p−+1q−=1.
We define the generalized Lebesgue space as
Lp(t)T=Lp(t)(ST;RN):={u∈L1(ST;RN):∫T0|u|p(t)dt<∞},ST=R/TZ |
with the norm
‖u‖Lp(t)=inf{λ>0:∫T0|uλ|p(t)dt≤1}. |
Lp(t)T is a kind of generalized Orlicz space. We also define the generalized Sobolev space by
W1,p(t)T=W1,p(t)(ST;RN):={u∈Lp(t)(ST;RN):˙u∈Lp(t)(ST;RN)} |
with the norm
‖u‖W1,p(t)T=‖u‖=‖u‖Lp(t)+‖˙u‖Lp(t). |
W1,p(t)T is a kind of generalized Orlicz-Sobolev space. In our case with the condition p(t)>1, the two spaces Lp(t)T and W1,p(t)T are both reflective Banach spaces with the norms defined above. It is known that there is a compact embedding W1,p(t)T↪C([0,T];RN). One can refer [1] for details.
The corresponding functional φ of (1.1) on W1,p(t)T is given by
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt,u∈W1,p(t)T. | (1.2) |
Wang and Yuan in [2] verified that the functional φ denoted in (1.2) is continuously differentiable, i.e., there holds
⟨φ′(u),v⟩=∫T0[(|˙u(t)|p(t)−2˙u(t),˙v(t))−(∇F(t,u(t)),v(t))]dt |
for any u,v∈W1,p(t)T. So the critical points of φ correspond to the solutions of problem (1.1). Then Zhang et al. in [3] proved that the functional φ defined in (1.2) is weakly lower semicontinuous on W1,p(t)T.
When p(t)=2, problem (1.1) reduces to the following Hamiltonian system
{¨u(t)+∇F(t,u(t))=0a.e.t∈[0,T],u(0)−u(T)=˙u(0)−˙u(T)=0, | (1.3) |
which has been extensively investigated in many literatures (see, e.g., [4,5,6,7,8] and the references therein). Particularly, under the following conditions:
(M1) there exists g∈L1([0,T];R+) such that |∇F(t,x)|≤g(t) for ∀x∈RN and a.e. t∈[0,T],
(M2) ∫T0F(t,x)dt→±∞ as |x|→+∞,
Mawhin and Willem in [6] established the existence of solutions for problem (1.3).
When N=1, T=2π, Habets, Manasevich and Zanolin in [4] established the existence of two sequences of different periodic solutions for problem (1.3) when the potential F(t,x) satisfies the following oscillating conditions:
lim supa→±∞∫2π0F(t,a)dt=+∞,lim infb→±∞∫2π0F(t,b)dt=−∞. |
When the nonlinearity ∇F(t,x) is sublinear, i.e., there exist f,g∈L1([0,T];R+) and α∈[0,1) such that
|∇F(t,x)|≤f(t)|x|α+g(t),∀x∈RNanda.e.t∈[0,T], |
and F(t,x) satisfies oscillating conditions, i.e., there holds
lim supr→+∞infx∈RN,|x|=r|x|−2α∫T0F(t,x)dt=+∞,lim infR→+∞supx∈RN,|x|=R|x|−2α∫T0F(t,x)dt=−∞, |
Zhang and Tang in [8] obtained the existence of two sequences of different periodic solutions for problem (1.3).
When p(t)=p is a constant for general p>1, problem (1.1) reduces to the following ordinary p-Laplacian problem
{ddt(|˙u(t)|p−2˙u(t))+∇F(t,u(t))=0,a.e.t∈[0,T],u(0)−u(T)=˙u(0)−˙u(T)=0. | (1.4) |
In recent years, the existence results for problem (1.4) was considered via the variational methods (see, e.g., [9,10,11] and references therein). Specially, L¨u, O'Regan and Agarwal in [10] generalized the results of [4] to the p-Laplacian problem (1.4) and established the existence of two sequences of different periodic solutions for problem (1.4). Li, Agarwal and Tang in [9] also established the existence of two sequences of different periodic solutions for problem (1.4) for the case with the potential F(t,x) possessing the mixed nonlinearity, that is, F(t,x)=F1(t,x)+F2(t,x) with F1(t,x) being (λ,μ)-subconvex in x, i.e., function F1(t,⋅):RN→R satisfies
F1(t,λ(x+y))≤μ(F1(t,x)+F1(t,y)) | (1.5) |
for some λ,μ>0 and each x,y∈RN (see [7] for details) and ∇F2(t,x) being p-sublinear, namely, there exist f,g∈L1([0,T];R+) and α∈[0,p−1) such that
|∇F2(t,x)|≤f(t)|x|α+g(t),∀x∈RNanda.e.t∈[0,T]. |
Then they also considered the other case with the nonlinearity ∇F(t,x) being p-linear, i.e., there exist f,g∈L1([0,T];R+) such that
|∇F(t,x)|≤f(t)|x|p−1+g(t),∀x∈RNanda.e.t∈[0,T]. |
Many scholars are interested in the nonlinear problems including the p(t)-Laplacian problem, this kind of problems can be used to model the dynamical phenomena arising from the field of elastic mechanics. One can refer [12,13] and the references therein for more application of the p(t)-Laplacian problem to various practical issues. The p(t)-Laplacian problem has more complicated nonlinearity than that of the p-Laplacian problem, for example, the second order differential operator is not homogeneous, this may causes some troubles such as some classical theories and methods, for instance, the Sobolev spaces theory are not applicable.
In recent years, the study of variational problems and elliptic partial differential equations with nonstandard growth conditions has been an interesting topic (see, e.g., [13,14] and references therein). In 2001, Fan et al. in [14,15] established some basic theory of space Lp(x)(Ω) and Wk,p(x)(Ω). In 2003, Fan et al. in [1] first studied the ordinary p(t)-Laplacian problem (1.1). Subsequently, Wang and Ruan in [2] established the existence and multiplicity of periodic solutions for the ordinary p(t)-Laplacian problem (1.1) under the generalized Ambrosetti-Rabinowitz conditions. Recently, many scholars considered the existence of periodic solutions of the ordinary p(t)-Laplacian problem (1.1). Some existence theorems of the ordinary p(t)-Laplacian problem (1.1) are established by using the least action principle and minimax methods in critical point theory (see, e.g., [1,3,16] and the references therein).
In this paper, motivated by the results of [4,5,8,9,10], we first aim to consider the ordinary p(t)-Laplacian problem (1.1) with a mixed nonlinearity, that is, F(t,x)=F1(t,x)+F2(t,x) with F1(t,x) being (λ,μ)-subconvex and ∇F2(t,x) being p−-sublinear. Then we consider the other case with the nonlinearity ∇F(t,x) being p−-linear. Following the idea of paper [8,9], we obtain the existence of two sequences of different periodic solutions for problem (1.1). The main results of this paper are stated as follows.
Theorem 1.1 Assume that F(t,x)=F1(t,x)+F2(t,x) where F1(t,x) and F2(t,x) satisfy condition (A) and the following conditions.
(H1) F1(t,⋅) is (λ,μ)-subconvex defined in (1.5) with λ>12 and 1≤2μ<(2λ)p− for a.e. t∈[0,T], and there exist α∈[0,p−−1),f,g∈L1([0,T];R+) such that
|∇F2(t,x)|≤f(t)|x|α+g(t),for∀x∈RNanda.e.t∈[0,T]. |
(H2) There exists a positive sequence {Rn} with limn→+∞Rn=+∞, such that
limn→+∞infx∈RN,|x|=Rn∫T0F(t,x)dt=+∞ |
and there exists a positive sequence {rm} with limm→+∞rm=+∞, such that
limm→+∞supx∈RN,|x|=rm1rq−αm(μ∫T0F1(t,xλ)dt+∫T0F2(t,x)dt)=−∞. |
Then problem (1.1) possesses two sequences of solutions {u±n} with φ(u±n)→±∞ as n→+∞.
Remark 1.2 Theorem 1.1 above generalizes Theorem 1.1 of [10], Theorem 1.1 of [8], Theorem 1 of [5] and Theorem 1.1 of [9]. There are functions F(t,x) satisfying the conditions in Theorem 1.1 but not satisfying the conditions in [5,8,9,10]. For example, for p(t)=4+cosωt with ω=2πT, we take
F1(t,x)=5+sin|x|6,F2(t,x)=|x|7/4sin(ln(|x|2+1))+(e(t),x), |
where e∈L1([0,T];RN) and ∫T0e(t)dt=0. Then F(t,x)=F1(t,x)+F2(t,x) is such a function.
Theorem 1.3 Assume that F(t,x) satisfies condition (A) and the following conditions.
(H3) There exist f,g∈L1([0,T];R+) with ‖f‖L1<α(p) such that
|∇F(t,x)|≤f(t)|x|p−−1+g(t),∀x∈RNanda.e.t∈[0,T], |
where α(p) is a positive constant depending on the function p(t), and so on the constants p±.
(H4) There exists a positive sequence {Rn} with limn→+∞Rn=+∞, such that
limn→+∞infx∈RN,|x|=Rn∫T0F(t,x)dt=+∞ |
and there exists a positive sequence {rm} with limm→+∞rm=+∞, such that
limm→+∞supx∈RN,|x|=rm1rp−m∫T0F(t,x)dt<−β(p), |
where β(p) is a positive constant depending on the function p(t), and so on the constants p±. Then problem (1.1) possesses two sequences of solutions {u±n} such that φ(u±n)→±∞ as n→+∞.
Remark 1.4 In the process of the proof of Theorem 1.3, the constants α(p) and β(p) will be defined clearly (see (3.20) and (3.26)). Theorem 1.3 above generalizes Theorem 1.3 of [9] since here the range of the function p(t) is wider than theirs. There exist functions satisfying the conditions of Theorem 1.3. For example, for p(t)=54+18cosωt, one can take
F(t,x)=1T|x|178sin(716ln(|x|2+1)). |
Then F(t,x) satisfies the conditions of Theorem 1.3 with p−=98,p+=118,q−=9,θp−=1,f(t)=3T.
For the convenience of readers, we first introduce two important properties of the variable exponent Lebesgue-Sobolev spaces Lp(t) and W1,p(t)T.
We define
˜W1,p(t)T={u∈W1,p(t)T:∫T0u(s)ds=0}. |
For u∈W1,p(t)T, let
ˉu=1T∫T0u(s)ds, |
then ˜u(t)=u(t)−ˉu∈˜W1,p(t)T. So we get
W1,p(t)T=RN⊕˜W1,p(t)T. |
Lemma 2.1 [16] For all u∈˜W1,p(t)T, there exist constants C′0, C0 such that
‖u‖∞≤C′0‖˙u‖Lp(t),‖u‖∞≤2C0[(∫T0|˙u(t)|p(t)dt)1p−+T1p−], |
where C′0, C0>0.
Lemma 2.2 [1] Let u=ˉu+˜u∈W1,p(t)T with ˉu∈RN and ˜u∈˜W1,p(t)T, then the norm ‖˙˜u‖Lp(t) is an equivalent norm on ˜W1,p(t)T and |ˉu|+‖˙u‖Lp(t) is an equivalent norm on W1,p(t)T. Therefore, for u∈W1,p(t)T,
‖u‖→+∞⇒|ˉu|+∫T0|˙u(t)|p(t)dt→+∞. |
Next we give two important properties of minimax methods as follows.
Lemma 2.3[6] Let K be a compact metric space, X a Banach space and K0⊂K is a closed subset, χ∈C(K0;X). We define a complete metric space M as
M={γ∈C(K;X):γ(s)=χ(s),∀s∈K0} |
with the usual norm and metric. Let φ∈C1(X;R) and
c=infγ∈Mmaxs∈Kφ(γ(s)),c1=maxχ(K0)φ. |
If c>c1, then for each ε>0 and each γ∈M such that
maxs∈Kφ(γ(s))≤c+ε, |
there exists v∈X such that
c−ε≤φ(v)≤maxs∈Kφ(γ(s)),dist(v,γ(K))≤ε1/2,|φ′(v)|≤ε1/2. |
Corollary 2.4[6] Under the conditions of Lemma 2.3, for each sequence (γk) in M such that
maxKφ(γk)→c, |
there exists a sequence (vk) in X such that
φ(vk)→c,dist(vk,γk(K))→0,|φ′(vk)|→0ask→+∞. |
Proof of Theorem 1.1. The proof is divided into four steps.
Step 1. We demonstrate that φ(u)→+∞ as ‖u‖→∞ for u∈˜W1,p(t)T.
Let β=log2λ(2μ), then one gets 0≤β<p−. For |x|>1, there exists a positive integer n such that
n−1<log2λ|x|≤n. |
Therefore one has |x|β>(2λ)(n−1)β=(2μ)n−1 and |x|≤(2λ)n. Combining the conditions (A) and (H1), one obtains
F1(t,x)≤2μF1(t,x2λ)≤⋯≤(2μ)nF1(t,x(2λ)n)≤2μ|x|βa0b(t) |
for any |x|>1 and a.e. t∈[0,T], where a0=max0≤s≤1a(s). Therefore one gets
F1(t,x)≤(2μ|x|β+1)a0b(t) | (3.1) |
for any |x|>1 and a.e. t∈[0,T]. In the sequel, we denote by C a suitable positive constant which may take different value in various estimations.
Combining Lemma 2.1, (H1) and (3.1), for the functional φ defined in (1.2), we obtain
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−∫T0F1(t,u(t))dt−∫T0F2(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−∫T0(2μ|u(t)|β+1)a0b(t)dt−1α+1∫T0f(t)|u(t)|α+1dt−∫T0g(t)|u(t)|dt≥1p+∫T0|˙u(t)|p(t)dt−2μa0‖u‖β∞∫T0b(t)dt−∫T0a0b(t)dt−‖u‖α+1∞‖f‖L1α+1−‖u‖∞‖g‖L1≥1p+∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)βp−−C(∫T0|˙u(t)|p(t)dt)α+1p−−C(∫T0|˙u(t)|p(t)dt)1p−−C | (3.2) |
for any u∈˜W1,p(t)T. From Lemma 2.2, estimate (3.2) implies that
φ(u)→+∞as‖u‖→+∞foru∈˜W1,p(t)T. |
Step 2. We verify that for the positive sequence {rm} defined in (H2), there holds
limm→+∞infu∈Wrmφ(u)=+∞, | (3.3) |
where Wrm={u∈RN||u|=rm}⊕˜W1,p(t)T.
By Lemma 2.1, (H1) and Young inequality, we obtain
|∫T0(F2(t,u(t))−F2(t,ˉu))dt|=|∫T0∫10(∇F2(t,ˉu+s˜u(t)),˜u(t))dsdt|≤∫T0∫10f(t)|ˉu+s˜u(t)|α|˜u(t)|dsdt+∫T0∫10g(t)|˜u(t)|dsdt≤2p−−1(|ˉu|α+‖˜u‖α∞)‖˜u‖∞∫T0f(t)dt+‖˜u‖∞∫T0g(t)dt=((p−2p+)1/p−‖˜u‖∞2C0)((p−2p+)−1/p−2p−C0∫T0f(t)dt)|ˉu|α+2p−−1‖˜u‖α+1∞∫T0f(t)dt+‖˜u‖∞∫T0g(t)dt≤12p+∫T0|˙u(t)|p(t)dt+C|ˉu|q−α+C(∫T0|˙u(t)|p(t)dt)α+1p−+C(∫T0|˙u(t)|p(t)dt)1p−+C | (3.4) |
for any u∈W1,p(t)T, where C0 is the constant defined in Lemma 2.1.
Hence from (H1), (3.1) and (3.4), for the functional φ defined in (1.2), we have
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−∫T0F1(t,u(t))dt−∫T0F2(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−μ∫T0F1(t,ˉuλ)dt−μ∫T0F1(t,˜u(t)λ)dt−∫T0(F2(t,u(t))−F2(t,ˉu))dt−∫T0F2(t,ˉu)dt≥12p+∫T0|˙u(t)|p(t)dt−μ∫T0F1(t,ˉuλ)dt−μ(2μλ−β‖˜u‖β∞+1)∫T0a0b(t)dt−C|ˉu|q−α−∫T0F2(t,ˉu)dt−C(∫T0|˙u(t)|p(t)dt)α+1p−−C(∫T0|˙u(t)|p(t)dt)1p−−C≥12p+∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)α+1p−−C(∫T0|˙u(t)|p(t)dt)1p−−C(∫T0|˙u(t)|p(t)dt)βp−−|ˉu|q−α(1|ˉu|q−α(μ∫T0F1(t,ˉuλ)dt+∫T0F2(t,ˉu)dt+C))−C. | (3.5) |
One can check that
B=inf˜u∈˜W1,p(t)T(12p+∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)α+1p−−C(∫T0|˙u(t)|p(t)dt)1p−−C(∫T0|˙u(t)|p(t)dt)βp−)>−∞ |
and
infu∈Wrmφ(u)≥B−C−supˉu∈RN,|ˉu|=rm|rm|q−α(1|rm|q−α(μ∫T0F1(t,ˉuλ)dt+∫T0F2(t,ˉu)dt)). |
Thus the above inequality and (H2) imply (3.3).
Step 3. Prove (ⅰ) of Theorem 1.1. For the positive sequence {Rn} defined in the condition (H2), we define
Γn={γ∈C(BRn;W1,p(t)T)|γ|∂BRn=id|∂BRn} |
and
cn=infγ∈Γnmaxx∈BRnφ(γ(x)), | (3.6) |
where
Bδ={x∈RN||x|≤δ}. |
One can verify that γ(BRn)∩˜W1,p(t)T≠∅ (for more details see [10]).
From Step 1, we know that φ is coercive on ˜W1,p(t)T. Since W1,p(t)T is a reflective Banach space, hence there is a constant M such that
maxx∈BRnφ(γ(x))≥infu∈˜W1,p(t)Tφ(u)=M. | (3.7) |
Combining (3.6) and (3.7), one obtains that cn≥M.
As in (3.3), we can easily verify that
limn→+∞supu∈RN,|u|=Rnφ(u)=−∞. | (3.8) |
From (3.8), for large enough n, we obtain
cn>supu∈RN,|u|=Rnφ(u). |
Now in Lemma 2.3 and Corollary 2.4, we take the compact set K=BRn and K0=∂BRn, then for any sequence {γk}⊂Γn such that
maxx∈BRnφ(γk(x))→cn, | (3.9) |
there exists a sequence {vk}⊂W1,p(t)T satisfying
φ(vk)→cn,dist(vk,γk(BRn))→0,|φ′(vk)|→0,ask→∞. | (3.10) |
Combining (3.6), (3.9) and (3.10), for k large enough, we have
cn≤maxx∈BRnφ(γk(x))≤cn+1 | (3.11) |
Define π:W1,p(t)T→RN as
π(u)=1T∫T0u(t)dt,foru∈W1,p(t)T. |
For fixed n, we obtain
|π(γk(BRn))|≤Kn. |
for some positive constant Kn, here |S|:=supx∈S‖x‖ for a set S⊂RN.
We now take ωk∈γk(BRn) such that
‖vk−ωk‖≤1. | (3.12) |
We write ωk=ˉωk+˜ωk with ˉωk∈RN and ˜ωk∈˜W1,p(t)T. So there holds |ˉωk|≤Kn, which implies that
μ∫T0F1(t,ˉωkλ)dt+∫T0F2(t,ˉωk)dt |
is bounded. Combining (H1), (3.1), (3.4), (3.11) and Lemma 2.1, we obtain
cn+1≥φ(ωk)=∫T0|˙ωk(t)|p(t)p(t)dt−∫T0F(t,ωk(t))dt≥1p+∫T0|˙ωk(t)|p(t)dt−∫T0F1(t,ωk(t))dt−∫T0F2(t,ωk(t))dt≥1p+∫T0|˙ωk(t)|p(t)dt−μ∫T0F1(t,ˉωkλ)dt−μ∫T0F1(t,˜ωk(t)λ)dt−∫T0(F2(t,ωk(t))−F2(t,ˉωk))dt−∫T0F2(t,ˉωk)dt≥12p+∫T0|˙ωk(t)|p(t)dt−μ∫T0F1(t,ˉωkλ)dt−μ(2μλ−β‖˜ωk‖β∞+1)∫T0a0b(t)dt−C−∫T0F2(t,ˉωk)dt−C|ˉωk|q−α−C(∫T0|˙ωk(t)|p(t)dt)α+1p−−C(∫T0|˙ωk(t)|p(t)dt)1p−≥12p+∫T0|˙ωk(t)|p(t)dt−C(∫T0|˙ωk(t)|p(t)dt)α+1p−−C(∫T0|˙ωk(t)|p(t)dt)1p−−C(∫T0|˙ωk(t)|p(t)dt)βp−−C. | (3.13) |
Therefore one can check that {˜ωk} and {ωk} is bounded from Lemma 2.2 and (3.13). By (3.12), we obtain that {vk} is bounded. By a standard argument, one can easy to verify that {vk} possesses a convergent subsequence. It is still denoted by {vk}. One can refer [2] for more details about the proof of (PS) condition.
Let
u+n=limk→+∞vk. |
Then from (3.10), we obtain
φ(u+n)=limk→+∞φ(vk)=cn,φ′(u+n)=limk→+∞φ′(vk)=0. |
This means u+n is a solution of problem (1.1) with φ(u+n)=cn.
For all γ∈Γn, by definition, there holds γ(BRn)∩Wrm≠∅. Then we get
maxx∈BRnφ(γ(x))≥infu∈Wrmφ(u). | (3.14) |
Now combining (3.3), (3.6) and (3.14), we obtain
limn→+∞cn=+∞. |
Hence there exists a sequence of periodic solutions {u+n} which are minimax-type critical points of the functional φ and φ(u+n)→+∞ as n→+∞. So (ⅰ) of Theorem 1.1 is proved.
Step 4. Prove (ⅱ) of Theorem 1.1. For the sequence {rn} defined in condition (H2) and as the same from (3.3), we define Pn as
Pn={u∈W1,p(t)T|u=ˉu+˜u,ˉu∈RN,|ˉu|≤rn,˜u∈˜W1,p(t)T}. |
For u∈Pn, it is easy to see that
μ∫T0F1(t,ˉuλ)dt+∫T0F2(t,ˉu)dt |
is bounded.
Combining (H1), (3.1) and (3.4), for u∈Pn, by the same process as in (3.13), we get
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt≥12p+∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)α+1p−−C(∫T0|˙u(t)|p(t)dt)1p−−C(∫T0|˙u(t)|p(t)dt)βp−−C. | (3.15) |
Thus the functional φ is bounded below in Pn.
Set
ρn=infu∈Pnφ(u) | (3.16) |
and let {uk} be a sequence on Pn such that
φ(uk)→ρnask→∞. |
We write
uk=ˉuk+˜uk,ˉuk∈RN,|ˉuk|≤rn,˜uk∈˜W1,p(t)T. |
From (3.15) and (3.16), it is easy to see that {uk} is bounded sequence in W1,p(t)T. Then {uk} possesses a subsequence, which is still denoted by {uk} such that
uk⇀u−ninW1,p(t)T. |
As Pn is a closed convex subset of W1,p(t)T, one has u−n∈Pn.
Since the functional φ is weakly lower semicontinuous, we obtain
ρn=limk→∞φ(uk)≥φ(u−n). |
Therefore we get
ρn=φ(u−n). | (3.17) |
From (3.3), for large n, we get that u−n∉{ˉu+˜u,ˉu∈RN,|ˉu|=rn}, and hence u−n∈IntPn={u∈W1,p(t)T|u=ˉu+˜u,|ˉu|<rn}. Thus combining (3.16) and (3.17), one obtains
φ′(u−n)=0 |
and u−n is a solution of problem (1.1).
Since rn→+∞ as n→+∞, we can choose the sequence {Rn} in the condition (H2) and as the same in (3.8) satisfying 0<Rn<rn. By (3.16), we obtain
φ(u−n)≤supx∈RN,|x|=Rnφ(x). | (3.18) |
From (3.8) and (3.18), we have
φ(u−n)→−∞asn→∞. |
So (ⅱ) of Theorem 1.1 is true. The proof of Theorem 1.1 is complete.
Proof of Theorem 1.3. The proof is divided into two steps.
Step 1. We show that φ(u)→+∞ as ‖u‖→∞ for u∈˜W1,p(t)T.
Combining Lemma 2.1 and (H3), we obtain
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−1p−∫T0f(t)|u(t)|p−dt−∫T0g(t)|u(t)|dt≥1p+∫T0|˙u(t)|p(t)dt−‖f‖L1p−‖u‖p−∞−‖u‖∞‖g‖L1≥(1p+−(2C0)p−p−‖f‖L1)∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)1p−−C, | (3.19) |
for any u∈˜W1,p(t)T, where C0 is the positive constant defined in Lemma 2.1. We now define the constant α(p) in Theorem 1.3 as
α(p)=p−2p+θp−(2C0)p−, | (3.20) |
where θp− is a positive constant defined by θp−=1 for p−∈(1,2], and θp−=2p–2 for p−>2. Now if ‖f‖L1<α(p), in view of Lemma 2.2, the estimate (3.19) implies that
φ(u)→+∞as‖u‖→+∞foru∈˜W1,p(t)T. |
Step 2. We verify that for the positive sequence {rm} defined in condition (H4), there holds
limm→+∞infu∈Wrmφ(u)=+∞, | (3.21) |
where Wrm={u∈RN||u|=rm}⊕˜W1,p(t)T.
For u∈W1,p(t)T with u=ˉu+˜u where |ˉu|=rm and ˜u∈˜W1,p(t)T. Here we recall that rm is defined in condition (H4), namely we have
limm→+∞supx∈RN,|x|=rm1|rm|p−∫T0F(t,x)dt<−β(p). | (3.22) |
Combining (H3), we obtain
|∫T0(F(t,u(t))−F(t,ˉu))dt|=|∫T0∫10(∇F(t,ˉu+s˜u(t)),˜u(t))dsdt|≤∫T0∫10f(t)|ˉu+s˜u(t)|p−−1|˜u(t)|dsdt+∫T0∫10g(t)|˜u(t)|dsdt≤θp−(|ˉu|p−−1‖˜u‖∞+1p−‖˜u‖p−∞)‖f‖L1+‖˜u‖∞‖g‖L1≤2θp−p−‖f‖L1‖˜u‖p−∞+α(p)θp−q−|ˉu|p−+C‖˜u‖∞, | (3.23) |
for any u∈W1,p(t)T, where 1p−+1q−=1. Where in (3.23), in the second estimate, we have used the inequality (a+b)c≤ac+bc for a,b≥0, c∈(0,1], (a+b)c≤2c−1(ac+bc) for a,b≥0, c∈(1,+∞), and in the last estimate, we have used the Young inequality ab≤ap−p−+bq−q−, a,b≥0. In the Lemma 2.1 of [11], we know that for a fixed ρ>1 and any ε>0, there is a number B(ε)>0 such that
(a+b)ρ≤(1+ε)aρ+B(ε)bρ,∀a,b>0. |
Now we take ε>0 such that α(p)≥(1+ε)‖f‖L1+ε, and ρ=p−, from Lemma 2.1, there holds
‖f‖L1‖˜u‖p−∞≤(α(p)−ε)(2C0)p−∫T0|˙˜u|p(t)dt+C. |
Thus we get
|∫T0(F(t,u(t))−F(t,ˉu))dt|≤2θp−(2C0)p−(α(p)−ε)p−∫T0|˙˜u|p(t)dt+θp−α(p)q−|ˉu|p−+C(∫T0|˙˜u|p(t)dt)1p−+C. | (3.24) |
Therefore, from (H3) and (3.24), we have
φ(u)=∫T0|˙u(t)|p(t)p(t)dt−∫T0F(t,u(t))dt≥1p+∫T0|˙u(t)|p(t)dt−∫T0(F(t,u(t))−F(t,ˉu))dt−∫T0F(t,ˉu)dt≥(1p+−2θp−(2C0)p−(α(p)−ε)p−)∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)1p−−|ˉu|p−(1|ˉu|p−∫T0F(t,ˉu)dt+θp−α(p)q−)−C | (3.25) |
for all u∈W1,p(t)T. From (3.20), we can check that
1p+−2θp−(2C0)p−(α(p)−ε)p−>0. |
Hence we obtain
D=inf˜u∈˜W1,p(t)T(1p+−2θp−(2C0)p−(α(p)−ε)p−)∫T0|˙u(t)|p(t)dt−C(∫T0|˙u(t)|p(t)dt)1p−)>−∞. |
Now define the constant β(p) in Theorem 1.3 as
β(p)=p−2p+q−(2C0)p−. | (3.26) |
Therefore combining the above expression and (3.22), we obtain (3.21).
The remainder is similar to that as in the proof of Theorem 1.1, we omit the detail here.
The first author is Partially supported by the NSF of China (11790271, 12171108), Guangdong Basic and Applied basic Research Foundation(2020A1515011019), Innovation and Development Project of Guangzhou University.
All authors declare no conflicts of interest in this paper.
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