In the present paper, with the combination of a compactness lemma and variational techniques, we establish a sufficient condition to guarantee the existence of two nontrivial homoclinic solutions for a nonperiodic fourth-order difference equation with a perturbation. Our result generalizes and improves some known results.
Citation: Yuhua Long. Existence of two homoclinic solutions for a nonperiodic difference equation with a perturbation[J]. AIMS Mathematics, 2021, 6(5): 4786-4802. doi: 10.3934/math.2021281
[1] | Yuhua Long, Sha Li . Results on homoclinic solutions of a partial difference equation involving the mean curvature operator. AIMS Mathematics, 2025, 10(3): 6429-6447. doi: 10.3934/math.2025293 |
[2] | Mohamed A. Barakat, Abd-Allah Hyder, Doaa Rizk . New fractional results for Langevin equations through extensive fractional operators. AIMS Mathematics, 2023, 8(3): 6119-6135. doi: 10.3934/math.2023309 |
[3] | Yuhua Long . Existence and nonexistence of positive solutions to a class of nonlocal discrete Kirchhoff type equations. AIMS Mathematics, 2023, 8(10): 24568-24589. doi: 10.3934/math.20231253 |
[4] | Xiaojie Guo, Zhiqing Han . Existence of solutions to a generalized quasilinear Schrödinger equation with concave-convex nonlinearities and potentials vanishing at infinity. AIMS Mathematics, 2023, 8(11): 27684-27711. doi: 10.3934/math.20231417 |
[5] | Lamya Almaghamsi, Aeshah Alghamdi, Abdeljabbar Ghanmi . Existence of solution for a Langevin equation involving the $ \psi $-Hilfer fractional derivative: A variational approach. AIMS Mathematics, 2025, 10(1): 534-550. doi: 10.3934/math.2025024 |
[6] | Song Wang, Xiao-Bao Shu, Linxin Shu . Existence of solutions to a class of damped random impulsive differential equations under Dirichlet boundary value conditions. AIMS Mathematics, 2022, 7(5): 7685-7705. doi: 10.3934/math.2022431 |
[7] | Wei Guo, Jinfu Yang, Jiafeng Zhang . Existence results of nontrivial solutions for a new $ p(x) $-biharmonic problem with weight function. AIMS Mathematics, 2022, 7(5): 8491-8509. doi: 10.3934/math.2022473 |
[8] | Zhilin Li, Guoping Chen, Weiwei Long, Xinyuan Pan . Variational approach to p-Laplacian fractional differential equations with instantaneous and non-instantaneous impulses. AIMS Mathematics, 2022, 7(9): 16986-17000. doi: 10.3934/math.2022933 |
[9] | Najla Alghamdi, Abdeljabbar Ghanmi . Multiple solutions for a singular fractional Kirchhoff problem with variable exponents. AIMS Mathematics, 2025, 10(1): 826-838. doi: 10.3934/math.2025039 |
[10] | H. Salah, M. Anis, C. Cesarano, S. S. Askar, A. M. Alshamrani, E. M. Elabbasy . Fourth-order differential equations with neutral delay: Investigation of monotonic and oscillatory features. AIMS Mathematics, 2024, 9(12): 34224-34247. doi: 10.3934/math.20241630 |
In the present paper, with the combination of a compactness lemma and variational techniques, we establish a sufficient condition to guarantee the existence of two nontrivial homoclinic solutions for a nonperiodic fourth-order difference equation with a perturbation. Our result generalizes and improves some known results.
It is well-known that homoclinic solutions play an important role in analyzing the chaos of dynamical systems. Hence, it is significative to deal with homoclinic solutions of dynamical systems. In the present paper, let Z and R be the set of integers and real numbers, respectively. For parameter λ>0, we investigate the existence of two nontrivial homoclinic solutions for the following nonperiodic fourth-order difference equation
Δ4u(t−2)+ωΔ2u(t−1)+a(t)u(t)=f(t,u(t))+λh(t)|u(t)|p−2u(t),t∈Z. | (1.1) |
Here ω is a given constant, 1≤p<2. f(t,u):Z×R→R is continuous in u and ∂F(t,u)∂u=f(t,u). a(t):Z→R and h(t):Z→R+. Let Δu(t)=u(t+1)−u(t) be the forward difference operator and define Δ0u(t)=u(t), Δiu(t)=Δ(Δi−1u(t)) for i≥1. As usual, we say that a solution u={u(t)} of (1.1) is homoclinic (to 0) if lim|t|→+∞u(t)=0. In addition, if u(t)≠0, then u is called a nontrivial homoclinic solution.
Difference equations possess theoretical background and practical significance. For example, [1] proposes a Dirichlet boundary value problem of difference equation to represent the amplitude of the motion of every particle in the string, [2] uses difference equations to study the impact of dispersal of a two-patch SIR disease model and [3] studies Wolbachia infection in mosquito population based on discrete models. Consequently, difference equations have attracted many researchers' attentions and rich results are obtained. To mention a few, [4,5,6] establish criteria for the existence and multiplicity of solutions, [7,8,9,10,11] focus on sign-changing solutions and [12,13,14,15,16,17,18] deal with homoclinic solutions or heteroclinic solutions.
Consider (1.1), it has been put forward as a discrete mathematical model for the study of pattern formation in physics and mechanics and deeply studied. For example, [19,20] investigate sign-changing of a special case of (1.1) by the invariant sets of descending flow. As mention to homoclinic solutions, which play an important role in analyzing the chaos of dynamical systems, there are many publications such as [21] studies (1.1) in a special form with periodic assumption and [22,23] prove that some special kind of (1.1) admits one nontrivial homoclinic solution. To the best of our knowledge, as considering homoclinic solutions for fourth order difference equations similar to (1.1), in the most known results of the existence of one non-zero homoclinic solution usually depend on periodic conditions or on the multiplicity with assumption of odevity on nonlinear terms. Meanwhile, using a compactness lemma and variational techniques, we achieve two nontrivial homoclinic solutions for (1.1) not only with neither periodic conditions nor odd-even requirements on nonlinear terms, but also with a perturbation. In some sense that our result improves and extends some known results.
Let constants c0 be given in Lemma 2.2 and cs be the best constant for the embedding of a Hilbert space X, which is defined in Section 2, in Ls, 2≤s<+∞ and q(t):Z→R+ with maxt∈Z{q(t)}=q>c0c22. Write
μ∗=inf{‖u‖E:u∈E,+∞∑t=−∞q(t)u2(t)=1}. | (1.2) |
Remark 1.1. μ∗ defined as (1.2) is reasonable. We state the proof of it in Lemma 3.2.
With the above notations, now we establish our main result:
Theorem 1.1. Let h(t):Z→R+ with maxt∈Z{h(t)}=h>0. Assume a(t):Z→R and there exists a constant a1 such that ω≤2√a1 and
0<a1≤a(t)→+∞,as|t|→+∞. | (1.3) |
Further, for i≥1, suppose f(t,u):Z×R→R is continuous in u and the following assumptions hold:
(F1)f(t,u)≡0 for all u<0, t∈Z and there exists b(t):Z→R+ with maxt∈Z{b(t)}=b<c0c222 such that
limu→0+f(t,u)ui=b(t)∀t∈Z, |
and
f(t,u)ui≥b(t)∀u>0,t∈Z; |
(F2)
limu→+∞f(t,u)ui=q(t)∀t∈Z; |
(F3) there exist two constants θ>2 and c0c22(θ−2)4θ<d0<c0c22(θ−2)2θ, such that
F(t,u)−1θf(t,u)u≤d0u2,∀u>0,t∈Z. | (1.4) |
Then either (i)i=1 and μ∗<1 or (ii)i>1, there exists Λ0>0 such that (1.1) admits at least two distinct homoclinic solutions for every λ∈(0,Λ0).
Remark 1.2. The assumptions in Theorem 1.1 are feasible. For example, take b(t)=c0c224 for all t∈Z. It follows that 0<maxt∈Z{b(t)}=c0c224<c0c222. Let
f(t,u)={12πb(t)uiarctan(u+√6−√2√6+√2),ifu≥0,forallt∈Z;0,ifu<0,forallt∈Z; | (1.5) |
then
F(t,u)={12πb(t)∫u0xiarctan(x+√6−√2√6+√2)dx,ifu≥0,forallt∈Z;0,ifu<0,forallt∈Z. |
Consequently,
limu→0+f(t,u)ui=limu→0+12πb(t)arctan(u+√6−√2√6+√2)uiui=b(t)∀t∈Z, |
and
limu→+∞f(t,u)ui=limu→+∞12πb(t)arctan(u+√6−√2√6+√2)uiui=6b(t)=3c0c222:=q(t)>c0c22∀t∈Z, |
which means the assumptions (F1) and (F2) are satisfied.
Moreover, from the expression of F(t,u), for all t∈Z and u≥0, we have
F(t,u)=12πb(t)∫u0xiarctan(x+√6−√2√6+√2)dx=12πb(t)xi+1i+1arctan(x+√6−√2√6+√2)−12πb(t)1i+1∫u0xi+11+(x+√6−√2√6+√2)2dx. |
Obviously, xi+11+(x+√6−√2√6+√2)2>0 for x>0, which follows that ∫u0xi+11+(x+√6−√2√6+√2)2dx≥0. Then one can verify that condition (F3) is satisfied.
Remark 1.3. Our result improves and generalizes some known results. For example, similarly, [23] gives that there exists one homoclinic solution for the following difference equation
Δ2(φp(Δ2u(t−2)))−aΔ(φp(Δu(t−1)))+λV(t)φp(u(t))=f(t,u(t)). | (1.6) |
(1.1) can be regarded as a special case of (1.6) when p=2. Our result Theorem 1.1 points out that (1.1) has at least two nontrivial homoclinic solutions. Meanwhile, according to [23], (1.1) possesses one homoclinic solution. Therefore, our result improves the result in [23] in some sense.
The organization of the paper is as follows: After this introduction, we present some basic lemmas and establish the corresponding variational functional to (1.1) in Section 2. Section 3 provides the detailed proof of our main result.
In this section, we give some notations and basic lemmas to prepare for the proof of our main result Theorem 1.1.
Denote u={u(t)}t∈Z=(⋯,u(−t),⋯,u(−1),u(0),u(1),⋯,u(t),⋯). Let the set of all two-sided sequences S={u={u(t)}:u(t)∈R,t∈Z}, then S is a vector space with au+bv={au(t)+bv(t)} for u,v∈S, a,b∈R. Define a subspace E of S as
E={u∈S:+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2]<+∞}. |
For any u,v∈E, define
<u,v>E=+∞∑t=−∞[Δ2u(t−1)⋅Δ2v(t−1)−ωΔu(t−1)⋅Δv(t−1)+a(t)u(t)⋅v(t)]. |
For later use, we define another Hilbert space (X,<u,v>X), where
X={u∈S:+∞∑t=−∞[|Δ2u(t−1)|2+|Δu(t−1)|2+|u(t)|2]<+∞} |
and, for any u,v∈X, the inner product is given by
<u,v>X=+∞∑t=−∞[Δ2u(t−1)⋅Δ2v(t−1)+Δu(t−1)⋅Δv(t−1)+u(t)⋅v(t)]. |
Then the corresponding norm is
‖u‖X=√<u,u>X=(+∞∑t=−∞[|Δ2u(t−1)|2+|Δu(t−1)|2+|u(t)|2])1/2,∀u,v∈X. |
In what follows, let
Ls={u∈S:‖u‖Ls=(+∞∑t=−∞|u(t)|s)1s<+∞} |
denote the space of functions whose s-th powers are summable on Z and
‖u‖L∞=supt∈Z|u(t)|<+∞. |
Thus the following embedding between Ls spaces holds,
Lq⊂Lp,‖u‖Lp≤‖u‖Lq,1≤q≤p≤∞. |
Now we start to consider the variational functional of (1.1). Define a functional J:E→R as
J(u)=12+∞∑t=−∞[Δ2u(t−1)⋅Δ2u(t−1)−ωΔu(t−1)⋅Δu(t−1)+a(t)u(t)⋅u(t)]−+∞∑t=−∞F(t,u(t))−λ+∞∑t=−∞h(t)|u(t)|p. | (2.1) |
Then the continuity of f indicates that J∈C1(E,R) and, for any u,v∈E, its derivative is expressed as
<J′(u),v>E=+∞∑t=−∞[Δ2u(t−1)⋅Δ2v(t−1)−ωΔu(t−1)⋅Δv(t−1)+a(t)u(t)⋅v(t)]−+∞∑t=−∞f(t,u(t))⋅v(t)−λ+∞∑t=−∞h(t)|u(t)|p−2u(t)⋅v(t), |
which means that u∈E is a critical point of J if and only if u is a homoclinic solution of (1.1).
Recall the definition of Cerami sequence and the variant version of the mountain pass theorem from critical point theory, which are helpful for us to seek critical points of (2.1).
Definition 2.1. Let J∈C1(E,R). A sequence {un}∈E is called a Cerami sequence ((C)c sequence for short) for J if J(un)→c for some c∈R and (1+‖un‖)J′(un)→0 as n→∞. If any (C)c sequence for J possesses a convergent subsequence, then J satisfies the (C)c condition.
Lemma 2.1. (Mountain pass theorem) ([24]) Let E be a real Banach space with its dual space E∗, and suppose that I∈C1(E,R) satisfies
max{I(0),I(e)}≤μ<η≤inf‖u‖=ρI(u), |
for some μ<η, ρ>0 and e∈E with ‖e‖>ρ. Let ˆc≥η be characterized by
ˆc=infγ∈Γmax0≤τ≤1I(γ(τ)), |
where Γ={γ∈C([0,1],E):γ(0)=0,γ(1)=e} is the set of continuous paths joining 0 and e, then there exists a sequence {un}⊂E such that
I(un)→ˆc≥ηand(1+‖un‖E∗)‖I′(un)‖E∗→0,asn→∞. |
Remark 2.1. Similar to [23], Lemma 2.1 allows us to find a (C)c sequence for J.
In the following, we establish some compactness conditions.
Lemma 2.2. Suppose a(t)≥a1>0 and ω<2√a1, then for any u∈E
+∞∑t=−∞[Δ2u(t−1)⋅Δ2u(t−1)−ωΔu(t−1)⋅Δu(t−1)+a(t)u(t)⋅u(t)]≥c0‖u‖2X | (2.2) |
is true for some constant c0>0.
Proof. Since ω<2√a1, we divide it into two cases.
Case 1. ω<0. Take c0=min{−ω,a1,1}, obviously,
+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2]≥c0+∞∑t=−∞[|Δ2u(t−1)|2+|Δu(t−1)|2+|u(t)|2] |
which implies that (2.2) is true.
Case 2. 0≤ω<2√a1. In this case, it is easy to get ω2<4a1, then there exists k∈(0,3) satisfying
3>k≥1−ω−2a1+√(ω+2a1−1)2+3(ω+1)2. |
Hence,
k2+2k(ω+2a1−1)−3(ω+1)2≥0. | (2.3) |
Consider
g(ξ):=ξ4+(1−3(ω+1)k)ξ2+(1+3(a1−1)k)∀ξ∈R. | (2.4) |
Denote
△:=(1−3(ω+1)k)2−4(1+3(a1−1)k), |
then (2.3) ensures
△≤0, |
which indicates that
g(ξ)≥0,∀ξ∈R. |
Therefore, for k∈(0,3), we have
(ω+1)ξ2−a1+1≤k3(1+ξ2+ξ4),∀ξ∈R. | (2.5) |
Analogous to [25], for any u(t)∈X, we take
u(t)=∑t∈Zeiζtˉu(ζ), |
then
Δu(t−1)=(1−eiζ)∑t∈Zeiζtˉu(ζ)andΔ2u(t−1)=(1−eiζ)2∑t∈Zeiζtˉu(ζ). |
Denote ξ=1−eiζ≜φ(ζ), then ζ=φ−1(ξ). Now we have
u(t)=∑t∈Zeiζtˉu(ζ)=∑t∈Zeiφ−1(ξ)tˉu(φ−1(ξ))≜ˆu(ξ) |
and
Δu(t−1)=ξˆu(ξ),Δ2u(t−1)=ξ2ˆu(ξ). |
Thanks to (2.5), there has
+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2]≥+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a1|u(t)|2]=+∞∑ξ=−∞(ξ4+ξ2+1−(ω+1)ξ2+a1−1)|ˆu(ξ)|2≥+∞∑ξ=−∞(ξ4+ξ2+1−k3(ξ4+ξ2+1))|ˆu(ξ)|2=(1−k3)+∞∑ξ=−∞(ξ4+ξ2+1)|ˆu(ξ)|2=(1−k3)‖u‖2X. | (2.6) |
Choose c0=√1−k3>0, then (2.6) leads to ‖u‖2E≥c0‖u‖2X, that is, (2.2) holds for 0≤ω<2√a1. Therefore, Lemma 2.2 is true and the proof is completed.
With the help of Lemma 2.2, we obtain that <u,u>E is positive for all nonzero u∈E and E is a Hilbert space. Here and hereafter, we write
‖u‖2E=+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2]. |
Now we state the main compactness lemma and present its proof in detail.
Lemma 2.3. Let (1.3) hold and ω<2√a1. Then, for 2≤s≤+∞, E is compactly embedded in Ls.
Proof. First, we prove Lemma 2.3 holds for s=2.
Define
α(A)=inf|t|>Aa(t),A∈[0,+∞). |
From (1.3), α(A) increases and α(A)→+∞ as |t|→+∞.
Let K be a bounded subset of E. It follows that, if u∈K, there exists a constant M>0 such that ‖u‖E≤M. Thanks to (2.2), we have
‖u‖2X≤1c0‖u‖2E≤M2c0and‖u‖2L2≤M2c0,∀u∈K. |
Hence, we have
+∞∑t=−∞a(t)|u(t)|2=+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2−|Δ2u(t−1)|2+ω|Δu(t−1)|2]≤+∞∑t=−∞[|Δ2u(t−1)|2−ω|Δu(t−1)|2+a(t)|u(t)|2+|ω||Δu(t−1)|2]≤M2+|ω|+∞∑t=−∞|Δu(t−1)|2≤M2+4|ω|+∞∑t=−∞|u(t)|2≤M2+|ω|⋅4M2c0. |
Write ˆb≜M2+|ω|⋅4M2c0. For any ϵ>0, take A0 large enough such that
4ˆbα(A0)<ϵ22. | (2.7) |
Since K⊂E is bounded by M, there are u1,u2,⋯,um∈K such that for any u∈K, there exists some ul (1≤l≤m) satisfying
A0∑t=−A0|u(t)−ul(t)|≤ϵ√2 | (2.8) |
Combining (2.7) with (2.8), it yields
+∞∑t=−∞|u(t)−ul(t)|2=∑|t|≤A0|u(t)−ul(t)|2+∑|t|>A0|u(t)−ul(t)|2 | (2.9) |
≤ϵ22+∑|t|>A0a(t)α(A0)|u(t)−ul(t)|2<ϵ22+4ˆbα(A0)<ϵ2 |
which implies ‖u−ul‖L2→0.
Next we verify that our claim is true for s=+∞. Notice that for any n∈N, T∈Z, 2≤k∈N and u∈E, thanks to the Newton-Lebnitz formula of indefinite summation and step by step summation [26], we have
t−1∑s=T[(s−T)n+1(t−T)nΔu(s)]=(t−T)u(t)−t−1∑s=T[u(s+1)Δ(s−T)n+1(t−T)n] |
and
T+k−1∑s=t[(T+k−s)n+1(T+k−t)nΔu(s)]=(T+k−t)u(t)−T+k−1∑s=t[u(s+1)Δ(T+k−s)n+1(T+k−t)n]. |
Hence, for all T≤t≤T+k−1, we have
ku(t)=t−1∑s=T[(s−T)n+1(t−T)nΔu(s)+u(s+1)Δ(s−T)n+1(t−T)n]+T+k−1∑s=t[(T+k−s)n+1(T+k−t)nΔu(s)+u(s+1)Δ(T+k−s)n+1(T+k−t)n]. |
On the other hand, owing to aθ+bθ≤(a+b)θ holds for a,b≥0 and θ≥1, it follows
t−1∑s=T|(s−T)n+1(t−T)nΔu(s)|+T+k−1∑s=t|(T+k−s)n+1(T+k−t)nΔu(s)|≤1(t−T)n(t−1∑s=T|(s−T)n+1|2)1/2⋅(t−1∑s=T|Δu(s)|2)1/2+1(T+k−t)n(T+k−1∑s=t|(T+k−s)n+1|2)1/2⋅(T+k−1∑s=t|Δu(s)|2)1/2=1√2n+3(t−T)3/2(t−1∑s=T|Δu(s)|2)1/2+1√2n+3(T+k−t)3/2(T+k−1∑s=t|Δu(s)|2)1/2≤1√2n+3[(t−T)3/2+(T+k−t)3/2](T+k−1∑s=T|Δu(s)|2)1/2≤k3/2√2n+3(T+k−1∑s=T|Δu(s)|2)1/2. | (2.10) |
In view of √a+√b√2≤√a+b (a,b≥0), similar to (2.10), we have
t−1∑s=T|u(s+1)Δ(s−T)n+1(t−T)n|+T+k−1∑s=t|u(s+1)Δ(T+k−s)n+1(T+k−t)n|≤√2k(n+1)√2n+1(T+k−1∑s=T|u(s+1)|2)1/2. | (2.11) |
Therefore, for all T≤t≤T+k−1 and 2≤k∈N, with the aid of (2.10) and (2.11), we have
|u(t)|≤√k√2n+3(T+k−1∑s=T|Δu(s)|2)1/2+√2√k⋅n+1√2n+1(T+k−1∑s=T|u(s+1)|2)1/2, | (2.12) |
which implies that
|u(t)−v(t)|≤√k√2n+3(∑|s|≥A|Δ(u(s)−v(s))|2)1/2+√2(n+1)√k(2n+1)(∑|s|≥A|u(s+1)−v(s+1)|2)1/2≤√k√2n+3[(+∞∑s=−∞|Δu(s)|2)1/2+(+∞∑s=−∞|Δv(s)|2)1/2]+√2(n+1)√k(2n+1)(∑|s|>Aa(s)|u(s+1)−v(s+1)|2α(A))1/2=4M√k√2n+3+√2(n+1)√k(2n+1)⋅2√ˆb√α(A) |
holds for any u,v∈K, A>0 and all |t|>A. For any ϵ>0, take first n large enough such that
4M√k√2n+3<ϵ2. |
Notice that 2≤k∈N, then, for any ϵ>0, choose A0 large enough such that
√2(n+1)√k(2n+1)⋅2√ˆb√α(A0)<ϵ2. |
Therefore, we can draw a conclusion that
max|t|>A0|u(t)−v(t)|<ϵ,∀u,v∈K. | (2.13) |
By the same method of (2.8), it follows that
max|t|≤A0|u(t)−ul(t)|<ϵ. | (2.14) |
Combing (2.13) with (2.14), we obtain
‖u−ul‖L∞<ϵ. | (2.15) |
Finally, we accomplish the proof of Lemma 2.3 by verifying it is correct for 2<s<+∞. Given an arbitrary u∈E, there has
+∞∑t=−∞|u(t)|s=+∞∑t=−∞(|u(t)|s−2⋅|u(t)|2)≤maxt∈N|u(t)|s−2⋅+∞∑t=−∞|u(t)|2=‖u‖s−2L∞⋅‖u‖2L2, | (2.16) |
which implies that K is precompact in Ls. Combing (2.9), (2.15) and (2.16), we complete the proof of Lemma 2.3 immediately.
In this section, we intend to prove the main result at length. Now we are in the position to state the following several lemmas which guarantee that the functional J, defined by (2.1), has the mountain pass geometry at first.
Lemma 3.1. Let a(t) and ω satisfy the assumptions in Theorem 1.1 and the conditions (F1) and (F2) hold. Then there exist Λ0>0 and constants ρ,η>0 such that
J(u)|‖u‖E=ρ≥η>0 |
for every λ∈(0,Λ0).
Proof. For every ϵ>0, notice that the condition (F1) implies that there exists a constant δ>0 such that f(t,s)≤(b+ϵ)si≤(b+ϵ)s holds for 0<s<δ. From (F2), lims→∞f(t,s)si=q(t) leads to lims→∞f(t,s)si+1=0, which implies that there exists a constant M>0 big sufficiently such that f(t,s)si+1≤ϵ, that is, f(t,s)≤ϵsi+1 with s>M. Further, since f(t,s) is continuous, it is not difficult to choose a constant C such that f(t,s)si+1≤C for δ≤s≤M. Therefore,
f(t,s)≤(b+ϵ)s+ϵsi+1+Csi+1,∀s∈R, | (3.1) |
which indicates that there exist Cϵ>0 and r≥i+2 such that
F(t,s)≤b+ϵ2s2+Cϵr|s|r,∀s∈R. | (3.2) |
For 2≤r<+∞, let cr be the best constants for the embedded of X in Lr. With the aid of Lemma 2.2, we get
‖u‖rE≥cr20‖u‖rX≥cr20crr‖u‖rLr, |
that is,
‖u‖rLr≤1cr20crr‖u‖rE. |
Together with (3.1), for all u∈E, one can obtain
+∞∑t=−∞F(t,u(t))≤b+ϵ2+∞∑t=−∞|u(t)|2+Cϵr+∞∑t=−∞|u(t)|r=b+ϵ2‖u‖2L2+Cϵr‖u‖rLr≤b+ϵ2c0c22‖u‖2E+Cϵrcr20crr‖u‖rE. |
Therefore,
J(u)=12‖u‖2E−+∞∑t=−∞F(t,u(t))−λ+∞∑t=−∞h(t)|u(t)|p≥12‖u‖2E−b+ϵ2c0c22‖u‖2E−Cϵrcr20crr‖u‖rE−λc−p20c−pph‖u‖pE=‖u‖pE[12(1−b+ϵc0c22)‖u‖2−pE−Cϵrcr20crr‖u‖r−pE−λc−p20c−pph]. | (3.3) |
By the last equation in (3.3), select ϵ=c0c222−b>0 and denote t=‖u‖E≥0, we define
g(t)=14t2−p−Cϵrcr20crrtr−p. |
Since r>2 and 1≤p<2, it is easy to find that g(t) will get its maximum value at t=(rcr20crr(2−p)4Cϵ(r−p))1r−2≜ρ>0. Hence
maxt≥0g(t)=g(ρ)=r−24(r−p)((2−p)rcr20crr4(r−p)Cϵ)2−pr−2≜M>0. |
Combing with (3.3), it yields that there exists Λ0=Mcp20cpph>0 such that we can find a constant η>0 which satisfies J(u)|‖u‖E=ρ≥η for every λ∈(0,Λ0).
Lemma 3.2. Let ρ and Λ0 be defined in Lemma 3.1. Suppose that the conditions (F1) and (F2) hold, then for every λ∈(0,Λ0) there exists e∈E with ‖e‖E>ρ such that J(e)<0 holds for either i=1 and μ∗<1 or i>1.
Proof. We give the proof in two cases.
Case Ⅰ. If i=1 and μ∗<1, we first declare μ∗, defined as (1.2), is reasonable. Let u∈E satisfy +∞∑t=−∞q(t)u2(t)=1. Then
1=+∞∑t=−∞q(t)u2(t)≤q+∞∑t=−∞u2(t)=q⋅‖u‖2L2, |
which means that ‖u‖2L2≥1q. In view of Lemma 2.2, we get
‖u‖2E≥c0‖u‖2X≥c0c22‖u‖2L2≥c0c22q>0. |
Thus μ∗≥c0c22q>0. Aim to get μ∗ is attainable, let {un}∈E be a minimizing sequence of (1.2), then {un} is bounded and satisfies +∞∑t=−∞q(t)u2n(t)=1. Choose a subsequence of {un}, without loss of generality, still denoted by {un}. In view of Lemma 2.3, there exists ϕ1∈E such that un⇀ϕ1 weakly in E and un→ϕ1 strongly in L2. Hence
+∞∑t=−∞q(t)u2n(t)→+∞∑t=−∞q(t)ϕ21(t)asn→∞,and+∞∑t=−∞q(t)ϕ21(t)=1. |
Therefore,
μ∗≤+∞∑t=−∞[(Δ2ϕ1(t−1))2−ω(Δϕ1(t−1))2+a(t)ϕ21(t)]≤limn→∞inf+∞∑t=−∞[(Δ2un(t−1))2−ω(Δun(t−1))2+a(t)u2n(t)]=μ∗, |
which indicates that μ∗=+∞∑t=−∞[(Δ2ϕ1(t−1))2−ω(Δϕ1(t−1))2+a(t)ϕ21(t)]=‖ϕ1‖2E.
Since μ∗<1, it is not difficult to choose 0≤φ∈E with +∞∑t=−∞q(t)φ2(t)=1 such that ‖φ‖E<1. Using the given condition (F2), we have
lims→+∞J(sφ)s2=12‖φ‖2E−lims→+∞+∞∑t=−∞F(t,sφ(t))s2−lims→+∞λs2+∞∑t=−∞h(t)|sφ(t)|p≤12‖φ‖2E−lims→+∞+∞∑t=−∞F(t,sφ(t))s2=12‖φ‖2E−+∞∑t=−∞lims→+∞f(t,sφ(t))⋅φ(t)2s=12‖φ‖2E−+∞∑t=−∞lims→+∞f(t,sφ(t))⋅φ(t)2sφ(t)⋅φ(t)=12‖φ‖2E−12+∞∑t=−∞q(t)φ2(t)=12(‖φ‖2E−1)<0, |
which tells us that J(sφ)→−∞ as s→+∞. Then there exists e∈E with ‖e‖E>ρ such that J(e)<0.
Case Ⅱ. If i>1, in view of q(t):Z→R+, we find there exists ψ∈E such that
+∞∑t=−∞q(t)ψi+1(t)>0. |
In the same manner as Case Ⅰ, we have
lims→+∞J(sψ)si+1=lims→+∞12‖sψ‖2E−+∞∑t=−∞F(t,sψ(t))−λ+∞∑t=−∞h(t)|sψ(t)|psi+1≤lims→+∞‖ψ‖2E2si−1−lims→+∞+∞∑t=−∞F(t,sψ(t))si+1=lims→+∞‖ψ‖2E2si−1−1i+1+∞∑t=−∞q(t)ψi+1(t)≤−1i+1+∞∑t=−∞q(t)ψi+1(t)<0. |
Therefore, there exists e∈E with ‖e‖E>ρ such that J(e)<0. The proof is completed.
Notice Lemma 3.1 and Lemma 3.2 show that J meets all conditions in Lemma 2.1, hence J possesses a (C)c sequence {un}⊂E for the mountain pass level β which is defined by
β=infγ∈Γmax0≤t≤1J(γ(t)) |
and Γ={γ∈C([0,1],E)|γ(0)=0,γ(1)=e}.
In the following, we set out to look for homoclinic solutions for (1.1). Denote Bρ={u∈E:‖u‖E<ρ}, where ρ is given by Lemma 3.1. We first seek for a critical point of J by showing J attains a local minimum for small λ.
Lemma 3.3. Let ρ and Λ0 be defined in Lemma 3.1. Assume a(t), ω and h(t) satisfy Theorem 1.1 and (F1) hold. Then, for λ∈(0,Λ0), (1.1) possesses a homoclinic solution u0∈E such that
J(u0)=inf{J(u)|u∈ˉBρ}<0. |
Proof. Since h(t):Z→R+, it is convenient to select ζ∈E such that +∞∑t=−∞h(t)|ζ(t)|p>0. For κ>0 small enough, (F1) induces F(t,κζ(t))>0 is correct for all t∈Z. Then for 1≤p<2, one has
J(κζ)=12‖κζ‖2E−+∞∑t=−∞F(t,κζ(t))−λ+∞∑t=−∞h(t)|κζ(t)|p=κ22‖ζ‖2E−+∞∑t=−∞F(t,κζ(t))−λκp+∞∑t=−∞h(t)|ζ(t)|p≤κ22‖ζ‖2E−λκp+∞∑t=−∞h(t)|ζ(t)|p<0 |
Write m≜inf{J(u):u∈¯Bρ}, then m<0. Thus there exists a minimizing sequence {un}⊂E such that J(un)→m and J′(un)→0 as n→∞. Therefore, Lemma 2.3 ensures that J admits a critical point u0∈E which satisfies J′(u0)=0 and J(u0)=m<0.
In view of Lemma 3.3, it is necessary for us to show that there exists another ˉu∈E such that J′(ˉu)=0 and ˉu≠u0 to accomplish the proof of Theorem 1.1.
Proof of Theorem 1.1. We complete the proof in two steps.
Step 1. The (C)c sequence {un}∈E of J, defined by
J(un)→β>0and(1+‖un‖E)‖J′(un)‖E∗→0,asn→∞, |
is bounded. Let n be large enough. By the condition (F3) and Lemma 3.1, it follows that
β+1≥J(un)−1θ<J′(un),un>=(12−1θ)‖un‖2E−+∞∑t=−∞[F(t,un(t))−1θf(t,un(t))un(t)]−λ(1−1θ)+∞∑t=−∞h(t)|un(t)|p≥θ−22θ‖un‖2E−d0+∞∑t=−∞u2n(t)−λ(1−1θ)h+∞∑t=−∞|un(t)|p≥θ−22θ‖un‖2E−d0‖un‖2L2−λ(1−1θ)h‖un‖pLp≥θ−22θ‖un‖2E−d0c0c22‖un‖2E−λ(1−1θ)hc−p20c−pp‖un‖pE=(θ−22θ−d0c0c22)‖un‖2E−λ(1−1θ)hc−p20c−pp‖un‖pE<(θ−22θ−c0c22(θ−2)4θc0c22)‖un‖2E−λ(1−1θ)hc−p20c−pp‖un‖pE=θ−24θ‖un‖2E−λ(1−1θ)hc−p20c−pp‖un‖pE. | (3.4) |
Obviously, for θ>2 and p<2, (3.4) implies ‖un‖E is bounded for all λ∈(0,Λ0).
Step 2. Now it is time for us to verify that J has another critical point ˉu which satisfies J′(ˉu)=0 and J(ˉu)=β>0. Since the (C)c sequence {un}⊂E of J is bounded, from Lemma 2.3, there exists ˉu∈E satisfying, up to a subsequence,
un⇀ˉuweakly inE,un→ˉustrongly inL2. |
Together with the Hölder inequality, it follows that
+∞∑t=−∞[f(t,un(t))−f(t,ˉu(t))](un(t)−ˉu(t))→0,asn→∞, |
and
+∞∑t=−∞[h(t)(|un(t)|p−2un(t)−|ˉu(t)|p−2ˉu(t))](un(t)−ˉu(t))→0,asn→∞. |
On the other hand, the definition of J(u) indicates that
‖un−ˉu‖2E=<J′(un)−J′(ˉu),un−ˉu>E−+∞∑t=−∞[f(t,un(t))−f(t,ˉu(t))](un(t)−ˉu(t))−λ+∞∑t=−∞[h(t)(|un(t)|p−2un(t)−|ˉu(t)|p−2ˉu(t))](un(t)−ˉu(t)). |
Hence un→ˉu strongly in E. Moreover, J(ˉu)=β>0 and ˉu is another homoclinic solution of (1.1). Consequently, u0 and ˉu are two distinct homoclinic solutions of (1.1). And the proof of Theorem 1.1 is finished.
The author sincerely thanks the handling editor and the anonymous referees for their valuable comments and suggestions.
All authors declare no conflicts of interest in this paper.
[1] | R. P. Agarwal, Difference equations and inequalities: Theory, methods and applications, Marcel Dekker, 1992. |
[2] |
Y. H. Long, L. Wang, Global dynamics of a delayed two-patch discrete SIR disease model, Commu. Nonlinear Sci., 83 (2020), 105117. doi: 10.1016/j.cnsns.2019.105117
![]() |
[3] |
Y. T. Shi, J. S. Yu, Wolbachia infection enhancing and decaying domains in mosquito population based on discrete models, J. Biol. Dynam., 14 (2020), 679–695. doi: 10.1080/17513758.2020.1805035
![]() |
[4] |
F. M. Atici, G. S. Guseinov, Positive periodic solutions for nonlinear difference equations with periodic coefficients, J. Math. Anal. Appl., 232 (1999), 166–182. doi: 10.1006/jmaa.1998.6257
![]() |
[5] |
Z. M. Guo, J. S. Yu, The existence of periodic and subharmonic solutions of sub-quadratic second order difference equations, J. Lond. Math. Soc., 68 (2003), 419–430. doi: 10.1112/S0024610703004563
![]() |
[6] |
J. Hendersona, R. Luca, Existence of positive solutions for a system of semipositone coupled discrete boundary value problems, J. Differ. Equ. Appl., 25 (2019), 516–541. doi: 10.1080/10236198.2019.1585831
![]() |
[7] |
T. S. He, Y. W. Zhou, Y. T. Xu, C. Y. Chen, Sign-changing solutions for discrete second-order periodic boundary value problems, B. Malays. Math. Sci. So., 38 (2015), 181–195. doi: 10.1007/s40840-014-0012-1
![]() |
[8] |
Y. H. Long, B. L. Zeng, Multiple and sign-changing solutions for discrete Robin boundary value problem with parameter dependence, Open Math., 15 (2017), 1549–1557. doi: 10.1515/math-2017-0129
![]() |
[9] |
Y. H. Long, J. L. Chen, Existence of multiple solutions to second-order discrete Neumann boundary value problems, Appl. Math. Lett., 83 (2018), 7–14. doi: 10.1016/j.aml.2018.03.006
![]() |
[10] |
Y. H. Long, S. H. Wang, Multiple solutions for nonlinear functional difference equations by the invariant sets of descending flow, J. Differ. Equ. Appl., 25 (2019), 1768–1789. doi: 10.1080/10236198.2019.1694014
![]() |
[11] |
Y. H. Long, Existence of multiple and sign-changing solutions for a second-order nonlinear functional difference equation with periodic coefficients, J. Differ. Equ. Appl., 26 (2020), 966–986. doi: 10.1080/10236198.2020.1804557
![]() |
[12] | M. J. Ma, Z. M. Guo, Homoclinic orbits for second order self-adjoint difference equations, J. Math. Anal. Appl., 232 (2006), 513–521. |
[13] | Y. H. Long, Homoclinic orbits for a class of noncoercive discrete hamiltonian systems, J. Appl. Math., 2012 (2012), 1–21. |
[14] |
Z. Zhou, D. F. Ma, Multiplicity results of breathers for the discrete nonlinear Schrödinger equations with unbounded potentials, Sci. China Math., 58 (2015), 781–790. doi: 10.1007/s11425-014-4883-2
![]() |
[15] |
Y. H. Long, Y. B. Zhang, H. P. Shi, Homoclinic solutions of 2nth-order difference equations containing both advance and retardation, Open Math., 14 (2016), 520–530. doi: 10.1515/math-2016-0046
![]() |
[16] | L. Erbe, B. G. Jia, Q. Q. Zhang, Homoclinic solutions of discrete nonlinear systems via variational method, J. Appl. Anal. Compt., 9 (2019), 271–294. |
[17] |
Q. Q. Zhang, Homoclinic orbits for discrete Hamiltonian systems with local super-quadratic conditions, Commun. Pur. Appl. Anal., 18 (2019), 425–434. doi: 10.3934/cpaa.2019021
![]() |
[18] |
J. H. Kuang, Z. M. Guo, Heteroclinic solutions for a class of p-Laplacian difference equations with a parameter, Appl. Math. Lett., 100 (2020), 106034. doi: 10.1016/j.aml.2019.106034
![]() |
[19] |
Y. H. Long, S. H. Wang, J. L. Chen, Multiple solutions of fourth-order difference equations with different boundary conditions, Bound. Value Probl., 2019 (2019), 1–25. doi: 10.1186/s13661-018-1115-7
![]() |
[20] |
S. H. Wang, Y. H. Long, Multiple solutions of fourth-order functional difference equation with periodic boundary conditions, Appl. Math. Lett., 104 (2020), 106292. doi: 10.1016/j.aml.2020.106292
![]() |
[21] |
G. H. Lin, Z. Zhou, Homoclinic solutions of discrete ϕ-Laplacian equations with mixed nonlinearities, Commun. Pur. Appl. Anal., 17 (2018), 1723–1747. doi: 10.3934/cpaa.2018082
![]() |
[22] |
H. Fang, D. P. Zhao, Existence of nontrivial homoclinic orbits for fourth-order difference equations, Appl. Math. Compt., 214 (2009), 163–170. doi: 10.1016/j.amc.2009.03.061
![]() |
[23] | N. Dimitrov, S. Tersian, Existence of homoclinic solutions for a nonlinear fourth order p-Laplacian difference equation, Discrete Cont. Dyn. B, 25 (2020), 555–567. |
[24] | I. Ekeland, Convexity methods in Hamiltonian mechanics, Springer-Verlag Berlin Heidelberg, 1990. |
[25] |
S. Tersian, J. Chaparova, Periodic and homoclinic solutions of extended Fisher-Kolmogorov equations, J. Math. Anal. Appl., 260 (2001), 490–506. doi: 10.1006/jmaa.2001.7470
![]() |
[26] | Y. C. Zhou, H. Cao, Y. N. Cao, Difference equations and their applications, Beijing, Science Press, 2014. |
1. | Huan Zhang, Yin Zhou, Yuhua Long, Results on multiple nontrivial solutions to partial difference equations, 2022, 8, 2473-6988, 5413, 10.3934/math.2023272 | |
2. | Yuhua Long, Multiple results on nontrivial solutions of discrete Kirchhoff type problems, 2023, 69, 1598-5865, 1, 10.1007/s12190-022-01731-0 | |
3. | Yuhua Long, Dan Li, Multiple nontrivial periodic solutions to a second-order partial difference equation, 2023, 31, 2688-1594, 1596, 10.3934/era.2023082 | |
4. | Yuhua Long, Huan Zhang, Existence and multiplicity of nontrivial solutions to discrete elliptic Dirichlet problems, 2022, 30, 2688-1594, 2681, 10.3934/era.2022137 | |
5. | Yuhua Long, Qinqin Zhang, SIGN-CHANGING SOLUTIONS OF A DISCRETE FOURTH-ORDER LIDSTONE PROBLEM WITH THREE PARAMETERS, 2022, 12, 2156-907X, 1118, 10.11948/20220148 | |
6. | Yuhua Long, Nontrivial solutions of discrete Kirchhoff-type problems via Morse theory, 2022, 11, 2191-950X, 1352, 10.1515/anona-2022-0251 |