Multiplicity of solutions for the discrete boundary value problem involving the p-Laplacian

Abdelrachid El Amrouss (Mohammed I University, FSO, Oujda, Morocco)
Omar Hammouti (Department of Mathematical Sciences, Mohammed I University, FSO, Oujda, Morocco)

Arab Journal of Mathematical Sciences

ISSN: 1319-5166

Article publication date: 20 August 2021

Issue publication date: 30 January 2023

653

Abstract

Purpose

The purpose of this paper is the study of existence and multiplicity of solutions for a nonlinear discrete boundary value problems involving the p-laplacian.

Design/methodology/approach

The approach is based on variational methods and critical point theory.

Findings

Theorem 1.1. Theorem 1.2. Theorem 1.3. Theorem 1.4.

Originality/value

The paper is original and the authors think the results are new.

Keywords

Citation

El Amrouss, A. and Hammouti, O. (2023), "Multiplicity of solutions for the discrete boundary value problem involving the p-Laplacian", Arab Journal of Mathematical Sciences, Vol. 29 No. 1, pp. 73-82. https://doi.org/10.1108/AJMS-02-2021-0050

Publisher

:

Emerald Publishing Limited

Copyright © 2021, Abdelrachid El Amrouss and Omar Hammouti

License

Published in Arab Journal of Mathematical Sciences. Published by Emerald Publishing Limited. This article is published under the Creative Commons Attribution (CC BY 4.0) licence. Anyone may reproduce, distribute, translate and create derivative works of this article (for both commercial and non-commercial purposes), subject to full attribution to the original publication and authors. The full terms of this licence may be seen at http://creativecommons.org/licences/by/4.0/legalcode


1. Introduction

The main goal of the present paper is to establish the existence and multiplicity of nontrivial solutions for the following discrete nonlinear boundary value problems

(P)Δ(ϕp(Δu(t1)))=f(t,u(t)),t[1,N]Z,u(0)=u(N+1)=0,
where N ≥ 1 is an integer, [1,N]Z is the discrete interval 1,,N, Δ is the forward difference operator defined by Δu(t) = u(t + 1) − u(t), ϕp(s) = |s|p−2s, 1 < p <  and f:[1,N]Z×RR is a continuous function.

By a solution of (P), we mean a function u:[0,N+1]ZR satisfies both equations of (P).

If f(t, 0) = 0 for any t[1,N]Z, the constant function u = 0 is a trivial solution of problem (P). In this case, the key point is proving the existence of nontrivial solutions for (P). For this purpose, we need to introduce a condition that gives us information about the behaviors of the perturbed function f(t, x) or its primitive F(t, x) near infinity and near zero.

We may think of (P) as a discrete analogue of the following second-order p-Laplacian functional differential equation

ddtϕpdu(t)dt=f(t,u(t)),t[0,1],u(0)=u(1)=0.
Let λ1 > 0 be the first eigenvalue of the nonlinear eigenvalue problem (P0) corresponding to problem (P)
(P0)Δ(ϕp(Δu(t1)))=λϕp(u(t)),t[1,N]Z,u(0)=u(N+1)=0.
The value of λ1 is λ1=minuEN\{0}t=1N+1|Δu(t1)|pt=1N|u(t)|p, where EN defined in (2.1) (see [1]).

The discrete analogue of the Laplacian on Riemannian manifolds, the so-called discrete Laplacian, has been studied intensively for the past few decades (see [27]). But, most phenomena on many cases are not expressed by the discrete Laplacian, which is known to be linear because they have a nonlinear flow governed by these intrinsic characteristics. For this reason, a nonlinear operator, called the discrete p-Laplacian, which is a generalization of the discrete Laplacian has recently been studied by many researchers in various fields, for example, dynamical systems, molecular structures, internet webs, image processing and so on (for more details, see [812]). Especially, many researchers have paid attention to studying boundary value problems and spectral theories for the discrete p-Laplacian (see [1, 1319]).

As is well known, critical point theory and variational methods are powerful tools to investigate the existence of solutions of various problems.

In this paper, we shall study the existence and multiplicity of nontrivial solutions of (P), via variational methods and critical point theory.

For convenience, we introduce the following notations.

F=lim|x|infmint[1,N]ZpF(t,x)|x|p,F=lim|x|supmaxt[1,N]ZpF(t,x)|x|p,F0=limx0infmint[1,N]ZpF(t,x)|x|p

And we make the following conditions:

  • (H1) there exists η with η < λ1 such that F  ≤ η, where

(1.1)λ1=minuEN\{0}t=1N+1|Δu(t1)|pt=1N|u(t)|p;
  • (H2) there exists δ with δ > λN such that Fδ, where

(1.2)λN=maxuEN\{0}t=1N+1|Δu(t1)|pt=1N|u(t)|p;
  • (H3) F0 > λN;

  • (H4) limx0F(t,x)|x|p=0, t[1,N]Z;

  • (H5) f(t, x) is odd in x, i.e. f(t, −x) = −f(t, x) for (t,x)[1,N]Z×R.

The main results in this paper are the following theorems:

Theorem 1.1.

λN (defined in (1.2)) is the last eigenvalue of the nonlinear eigenvalue problem (P0).

Theorem 1.2.

Assume that (H1) and (H3) hold, then problem (P) has at least one nontrivial solution.

Theorem 1.3.

Assume that (H2) and (H4) hold, then problem (P) has at least two nontrivial solutions.

Theorem 1.4.

Assume that (H1), (H3) and (H5) hold, then problem (P) has at least 2N nontrivial solutions.

The rest of this paper is organized as follows. Section 2 contains some preliminary lemmas. The main results will be proved in Sections 3 and 4.

2. Preliminary lemmas

In the present paper, we define a vector space EN by

(2.1)EN={u:[0,N+1]ZRu(0)=u(N+1)=0},
and for any u ∈ EN, define u=t=1N|u(t)|p1/p.

Equipped with ‖ ‖, EN is an N dimensional Banach space. In fact, EN is isomorphic to RN.

Let u ∈ EN, we consider the functional as follows:

(2.2)Φ(u)=1pt=1N+1|Δu(t1)|pt=1NF(t,u(t)).

It is easy to see that ΦC1(EN,R) and its derivative Φ′(u) at u ∈ EN is given by

Φ(u).v=t=1N+1|Δu(t1)|p2Δu(t1)Δv(t1)t=1Nf(t,u(t))v(t),vEN.

By the summation by parts formula and the fact that v(0) = v(N + 1) = 0, it follows that

t=1N+1|Δu(t1)|p2Δu(t1)Δv(t1)=|Δu(N)|p2Δu(N)Δv(N)+t=1N|Δu(t1)|p2Δu(t1)Δv(t1)=|Δu(N)|p2Δu(N)v(N)+|Δu(t1)|p2Δu(t1)v(t1)1N+1t=1NΔ(|Δu(t1)|p2Δu(t1))v(t)=|Δu(N)|p2Δu(N)v(N)+|Δu(N)|p2Δu(N)v(N)|Δu(0)|p2Δu(0)v(0)t=1NΔ(|Δu(t1)|p2Δu(t1))v(t)=t=1NΔ(|Δu(t1)|p2Δu(t1))v(t).

Therefore, Φ′ can be written as

Φ(u).v=t=1NΔ(|Δu(t1)|p2Δu(t1))f(t,u(t))v(t),vEN.

Thus, finding solutions of (P) is equivalent to finding critical point of the functional Φ.

Definition 2.1.

Let E be a real Banach space and ΦC1(E,R). Recall that Φ is said to satisfy the Palais Smale (PS) condition if every sequence (un) ⊂ E, such that Φ(un) is bounded and Φ′(un) → 0 as n, has a convergent subsequence. Here, the sequence (un) is called a PS sequence.

Let Bρ denote the open ball in E about 0 of radius ρ and let ∂Bρ denote its boundary.

Lemma 2.1.

(Mountain pass lemma [20]) Let E be a real Banach space and ΦC1(E,R) satisfy the (PS) condition. If Φ(0) = 0 and

  • σ1) there exist constants ρ, α > 0 such that Φ|Bρα,

  • σ2) there exist e ∈ E\Bρ such that Φ(e) ≤ 0.

Then Φ possesses a critical value c ≥ a given by c=infgΓmaxs0,1Φ(g(s)),

where

Γ={gC(0,1,E)/g(0)=0,g(1)=e}.
Lemma 2.2.

(see [21] ) Let E be a real Banach space and ΦC1(E,R) be even, bounded from below, and satisfy the (PS) condition. Suppose that Φ(0) = 0 and there is a set Ω ⊂ E such that Ω is homeomorphic to Sn−1 by an odd map and supuΩΦ(u)<0, where Sn−1 is the n − 1 dimensional unit sphere. Then, Φ has at least n disjoint pairs of nontrivial critical points.

3. Eigenvalue problem

We consider the nonlinear eigenvalue problem (P0) corresponding to problem (P):

(P0)Δ(ϕp(Δu(t1)))=λϕp(u(t)),t[1,N]Z,u(0)=u(N+1)=0,
Definition 3.1.

λR is called eigenvalue of (P0) if there exists u ∈ EN \{0} such that:

t=1N+1ϕp(Δu(t1))Δv(t1)=λt=1Nϕp(u(t))v(t),vEN.

Proposition 3.1.

(see [22]) Let E be a real Banach space, G,JC1(E,R) and a set of constraints

S = {u ∈ EG(u) = 0}. Suppose that for any u ∈ S, G′(u) ≠ 0 and there exists u0 ∈ S such that J(u0)=infuSJ(u). Then there is λR such that J′(u0) = λG′(u0).

Proof of Theorem 1.1.

Put J(u)=t=1N+1|Δu(t1)|p,G(u)=t=1N|u(t)|p1, and

S={uENG(u)=0}={uENu=1}.

It is easy to see that G′(u) ≠ 0 for any u ∈ S.

If the set S is compact and J is continuous on S, then there exists uN ∈ S such that

J(uN)=maxuSJ(u)=λ.
Thus,
J(uN)=minuS(J(u))=λ.

Clearly λ′ > 0. From the Proposition 3.1, there exists λN such that

J(uN)=λNG(uN).
Which means that
(3.1)Δ(ϕp(ΔuN(t1)))=λNϕp(uN(t)),t[1,N]Z.

Multiplying (3.1) by uN in the sense of inner product, we obtain

t=1N+1|ΔuN(t1)|p=λNt=1N|uN(t)|p,
i.e.
J(uN)=λNuNp=λN.

Therefore, λ′ = λN is an eigenvalue of the problem (P0).

Thus, we have

λN=maxuSt=1N+1|Δu(t1)|p=maxuEN\{0}t=1N+1|Δu(t1)u|p=maxuEN\{0}t=1N+1|Δu(t1)|pt=1N|u(t)|p.

If λ is an eigenvalue of the problem (P0), then there exists u ∈ EN \{0} such that:

t=1N+1ϕp(Δu(t1))Δv(t1)=λt=1Nϕp(u(t))v(t),vEN.
In particular for v = u, we get λ=t=1N+1|Δu(t1)|pt=1N|u(t)|p.

So, we deduce that λ1 ≤ λ ≤ λN.

Then, λN is the last eigenvalue of the problem (P0).

The proof of Theorem 1.1 is completed. □

4. Proofs of the main results

Proof of Theorem 1.2.

Since Fη, there exists R1 > 0 such that

pF(t,x)|x|pη+εfor(t,|x|)[1,N]Z×R1,+,
where 0 < ɛ < λ1 − η, i.e.
(4.1) F(t,x)1p(η+ε)|x|pfor(t,|x|)[1,N]Z×R1,+.

Then, by (4.1) and the continuity of xF(t, x), there exists c1 > 0 such that

(4.2)F(t,x)1pη+ε|x|p+c1,(t,x)[1,N]Z×R.

According to (1.1), we have

(4.3)t=1N+1|Δu(t1)|pλ1up.

Using (4.2) and (4.3), we obtain

Φ(u)1pλ1up1p(η+ε)t=1N|u(t)|pc1N1pλ1(η+ε)upc1N.

Since ɛ < λ1 − η, then Φ(u) → as ‖u‖ → . Thus, Φ is coercive and bounded from below, hence there is a minimum point of Φ at some u0 ∈ EN i.e. Φ(u0)=infuENΦ(u), which is a critical point of Φ and in turn is a solution of problem (P).

From (H3), there exists ρ1 > 0 such that

pF(t,x)|x|pF0ε,for(t,|x|)[1,N]Z×0,ρ1,
where 0 < ɛ < F0 − λN, i.e.
(4.4)F(t,x)1p(F0ε)|x|pfor(t,|x|)[1,N]Z×0,ρ1.
Put
(4.5)Ω={uENu=ρ1}.

For any u ∈ Ω,

|u(t)|u=ρ1,t[1,N]Z.

From (1.2), we get

(4.6)t=1N+1|Δu(t1)|pλNup.

Combining the preceding inequality and (4.4), we have

Φ(u)1pλNup1p(F0ε)up=1pλN(F0ε)ρ1p<0.

Thus, we obtain

(4.7)supuΩΦ(u)<0.

Hence,

Φ(u0)=infuENΦ(u)infuΩΦ(u)supuΩΦ(u)<0.

So problem (P) has at least one nontrivial solution.

The proof of Theorem 1.2 is completed. □

Proof of Theorem 1.3.

From the condition (H4), for ε=λ12p there exists ρ2 > 0 such that:

(4.8) |F(t,x)|λ12p|x|pfor(t,|x|)[1,N]Z×0,ρ2.

Let u ∈ EN with ‖u‖ ≤ ρ2, then |u(t)|ρ2,t[1,N]Z.

Thus, we have

Φ(u)λ1pupλ12pupλ12pup.

Take α=λ12pρ2p>0. Therefore,

(4.9)Φ(u)α>0,uBρ2.

At the same time, we have also proved that there exist constants α > 0 and ρ2 > 0 such that Φ|Bρ2α. That is to say, Φ satisfies the condition σ1 of the mountain pass lemma.

For our setting, clear Φ(0) = 0. In order to exploit the mountain pass lemma in critical point theory, we need to verify all other conditions of the mountain pass lemma.

According to the condition (H2), there exists R2 > 0 such that

pF(t,x)|x|pδεfor(t,|x|)[1,N]Z×R2,+,
where 0 < ɛ < δ − λN, i.e.
(4.10)F(t,x)1p(δε)|x|pfor(t,|x|)[1,N]Z×R1,+.

Then, by (4.10) and the continuity of xF(t, x), there exists c2 > 0 such that

(4.11)F(t,x)1p(δε)|x|pc2,(t,x)[1,N]Z×R.

Now, using again (4.6) and (4.11), it follows that,

Φ(u)λNpup1p(δε)up+c2N
1pλN(δε)up+c2N.

Consequently, since ɛ < δ − λN, we have

(4.12)Φ(u),asu.

Thus, we can choose u¯ large enough to ensure that Φ(u¯)<0, that is, there exists e=u¯E\Bρ2 such that Φ(e) < 0.

From (4.12), Φ is anti-coercive, hence for any PS sequence (un) is bounded. In view of the fact that the dimension of EN is finite, we see that Φ satisfies the (PS) condition.

By the mountain pass lemma, Φ possesses a critical value cα=λ12pρ2p>0,

where c=infgΓmaxs0,1Φ(g(s)) and Γ={gC(0,1,E)g(0)=0,g(1)=u¯}.

Let u1 ∈ EN be a critical point associated to the critical value c of Φ, i.e. Φ(u1) = c.

Hence, u1 is a nontrivial solution of problem (P).

Since Φ is anti-coercive and bounded from above, there is a maximum point of Φ at some u2 ∈ EN,

i.e. Φ(u2)=supuENΦ(u).

Using the preceding equality and (4.9), we obtain

Φ(u2)=supuENΦ(u)supuBρ2Φ(u)>0.

Hence u2 is a nontrivial solution of problem (P).

If u1u2, then we have two nontrivial solutions: u1 and u2.

Otherwise, suppose u1 = u2, then infgΓmaxs0,1Φ(g(s))=supuENΦ(u).

Therefore, we have Φ(u1)maxs0,1Φ(g(s))Φ(u2),gΓ.

Since u1 = u2, we deduce that Φ(u1)=maxs0,1Φ(g(s)),gΓ.

The continuity of Φ(g(s)) with respect to s, Φ(0) = 0 and Φ(u¯)<0 implies that there exists s10,1 such that Φ(u1) = Φ(g(s1)). Choose g2, g3 ∈ Γ such that

{g2(s)s0,1}{g3(s)s0,1}=,
then there exists s2,s30,1 such that
Φ(g2(s2))=Φ(g3(s3))=Φ(u1)=maxs0,1Φ(g(s)).

Thus, we get two different critical points of Φ on EN denoted by v2 = g2(s2), v3 = g3(s3) that are nontrivial solutions of problem (P).

The proof is completed. □

Proof of Theorem 1.4.

Let Φ be defined by (2.2). Then, it is clear that Φ(0) = 0 and Φ is even by (H5).

From the proof of Theorem 1.2, Φ is bounded from below, coercive and any PS sequence (un) is bounded. In view of the fact that the dimension of EN is finite, we see that Φ satisfies the (PS) condition.

Let SN−1 be the unit sphere in RN and define T: Ω → SN−1 by

T(u)=1ρ1u,
where Ω (defined in (4.5)).

Then, T is an odd homeomorphism between Ω and SN−1, and supuΩΦ(u)<0 (see (4.7)).

Hence, all the conditions of Lemma 2.2 are satisfied, so Φ has at least 2N nontrivial critical points, which are nontrivial solutions of problem (P).

This completes the proof of Theorem 1.4.□

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Acknowledgements

The authors are grateful to the anonymous referee for carefully reading and giving valuable comments and suggestions to improve the earlier version of the paper.

Corresponding author

Omar Hammouti can be contacted at: omar.hammouti.83@gmail.com

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