Abstract
By employing Clark’s theorem we prove the existence of infinitely many homoclinic solutions to the local and nonlocal discrete p-Laplacian equations on the integers. Our results extend and correct the reasoning of some recent findings expressed in the literature.
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1 Introduction and the Main Result
A wide class of difference equations represents the discrete counterpart of ordinary and partial differential equations and is usually studied in connection with numerical analysis (see, e.g., [1, 7, 8, 12, 17, 18, 21, 23] and references therein). The fractional Laplacian, understood as a positive power of the classical Laplacian, has been present in several areas of mathematics such as functional analysis, harmonic analysis, potential theory, fractional calculus, and probability [13, 25]. The fractional p-Laplacian on \( \mathbb {R} ^{N},p>1,\) is defined, for \(0<s<1\) and good enough functions U, as
where \(B(x,\varepsilon )\) is the ball centered at \(x\in \mathbb {R} ^{N}\) with radius \(\varepsilon \). Up to some normalization constant depending on N, p, and s, this definition is consistent with the one of the fractional Laplacian \(\left( -\Delta \right) ^{s}\) in the case \(p=2\) (see [15]). In [15], there is the generalization of this operator, i.e.
where the kernel \(K: \mathbb {R} ^{N}\smallsetminus \{0\}\rightarrow (0,+\infty )\) satisfies
- \((K_{1})\):
-
\(mK\in L^{1}(\mathbb {R}^{N}),\) where \(m(x)=\min \{\left| x\right| ^{p},1\}\),
- \((K_{2})\):
-
there exist \(\theta >0\) and \(s\in (0,1)\) such that \(K(x)\ge \theta \left| x\right| ^{-(N+ps)}\) for all \(x\in \mathbb {R}^{N}\smallsetminus \{0\}.\)
The main difficulties to overcome in numerical approaches are the nonlocality and singularity of these operators. The first approach to discretization of operator (1) with \(p=2\) was discussed in [4]. The authors defined the fractional powers of the discrete Laplacian \(\left( -\Delta \right) ^{s},\) \(0<s<1,\) where \(\left( -\Delta \right) (u(k))=-(u(k+1)-2u(k)+u(k-1))\) on \( \mathbb {Z},\) with the semigroup method as
where \(\Gamma \) denotes the Gamma function and \(e^{t\Delta }u(k)=w(t,k)\) is the solution to the semidiscrete heat equation
Theorem 1.1 in [4] shows that
for
where the discrete kernel \(K_{s}\) is given by
for any \(j\in \mathbb {Z} {\setminus } \{0\},\) and \(K_{s}(0)=0.\) This kernel satisfies
Moreover, if u is bounded then
We can generalize the operator given in (2) to a discrete fractional p-Laplacian in the following way: for \(0<s<1,\) \(p>1\) and good enough sequences \(u: \mathbb {Z} \rightarrow \mathbb {R} \) we put
where the discrete kernel \(K_{s,p}\) satisfies
and \(0<c_{s,p}\le C_{s,p}\) are constants. The class of operators \(\left( -\Delta \right) _{2}^{s}\) contains the fractional powers of the discrete Laplacian \(\left( -\Delta \right) ^{s}\) defined in [4]. Note that showing (4) requires using the explicit form of the kernel given in (3) (see the proof of Theorem 1.1 in [4]). However, the only constraint imposed on the kernel \(K_{s,p}\) is condition (6). The author does not know whether \(\lim _{s\rightarrow 1^{-}}\left( -\Delta \right) _{p}^{s}u=\left( -\Delta \right) _{p}u\) on \( \mathbb {Z},\) even for \(p=2\), where \(\left( -\Delta \right) _{p}u\) is a local discrete p-Laplacian, i.e.
for all \(k\in \mathbb {Z}.\)
With such discretization in hand, discrete counterparts of continuous problems were considered in [9, 10, 27, 28].
In the present paper we deal with the following fractional discrete p -Laplacian equations
Here \(s\in (0,1],p>1\) is a real number, \(V:{\mathbb {Z}}\rightarrow \mathbb {(} 0,+\infty )\), while \(f:{\mathbb {Z}}\times {\mathbb {R}}\rightarrow {\mathbb {R} }\) is a continuous function. For \(0<s<1,\) \(\left( -\Delta \right) _{p}^{s}\) is the nonlocal discrete p-Laplacian given by (5) and for \(s=1\), \(\left( -\Delta \right) _{p}^{1}\) is the local discrete p -Laplacian given by (7).
Recently, the existence and multiplicity of solutions to the problem of type (8) have been studied. For results on equations in \( \mathbb {Z} \) driven by the local discrete p-Laplacian we refer the reader to [6, 8, 11, 12, 21,22,23, 26]. In [8], the authors studied the existence of multiple homoclinic solutions (i.e. with \(\lim _{\left| k\right| \rightarrow \infty }u(k)=0\)) via critical point theory. In papers [6, 11, 12, 23], the authors imposing various conditions on nonlinearity considered the existence results of a sequence of infinitely many homoclinic orbits, by using the symmetric mountain pass theorem or fountain theorem or dual fountain theorem. Infinitely many solutions have also been obtained in [22] directly using the variational method, in [26] by applying Nehari manifold methods and in [21] by employ of the Ricceri’s theorem.
For results on problems (8) in \( \mathbb {Z} \) driven by the nonlocal discrete p-Laplacian we refer the reader to [9, 10, 27, 28]. In [27, 28], by using Ekeland’s variational principle, together with the mountain pass theorem, at least two homoclinic solutions were obtained. By using the Nehari manifold method, at least two homoclinic solutions to (8) were acquired in [9]. Finally, in [10], an infinite number of solutions have been obtained from different versions of Clark’s theorem.
In this paper, our goal is to apply the variational method and a variant of Clark’s theorem to find a sequence of homoclinic solutions for problem (8). To do this, we construct the appropriate space of solutions \(E_{s}\) ( \(s=1\) in the local case and \(0<s<1\) in the nonlocal case) and the energy functional \(J_{s}\) defined on it such that its critical points are solutions to our problem. By imposing appropriate conditions on the nonlinearity f, we obtain from Clark’s theorem a sequence of solutions in \(E_{s}\) with norms tending to zero. Let \(l^{r},1\le r\le \infty ,\) denote the sequence Lebesgue space with standard norm \(\left\| \cdot \right\| _{r}\). Since \(E_{s}\subset l^{p}\), we immediately get that the solutions are homoclinic.
A special case of our contributions reads as follows. We assume that potential V(k) and the nonlinearity f(k, t) satisfy the following conditions:
- (V):
-
\(V(k)\ge V_{0}>0\) for all \(k\in \mathbb {Z}\), \(V(k)\rightarrow +\infty \) as \(\left| k\right| \rightarrow +\infty ;\)
- \((f_{1})\):
-
there exists \(\varepsilon >0\ \)such that\(\ f(k,-t)=-f(k,t)\) for all \(k\in \mathbb {Z}\) and \(t\in \left( -\varepsilon ,\varepsilon \right) ;\)
- \((f_{2})\):
-
there exists a positive \(a\in l^{\frac{p}{p-1}}\) such that
$$\begin{aligned} \underset{t\rightarrow 0}{\lim \sup }~\frac{\left| f(k,t)\right| }{ a(k)+\left| t\right| ^{p-1}}<+\infty \end{aligned}$$(9)uniformly for all \(k\in \mathbb {Z}\);
- \((f_{3})\):
-
there exist \(1<\sigma <p\) and an infinitesubset \(Z_{0}\subset \mathbb {Z}\) such that
$$\begin{aligned} \underset{t\rightarrow 0}{\lim \inf }\frac{F(k,t)}{\left| t\right| ^{\sigma }}>0 \end{aligned}$$(10)for all \(k\in Z_{0}\);
where F(k, t) is the primitive function of f(k, t), that is \( F(k,t)=\int _{0}^{t}f(k,s)ds\) for every \(t\in \mathbb {R} \) and \(k\in \mathbb {Z} \).
Let us note that conditions \((f_{1})-(f_{3})\) control the behaviour of f only for a small t. Note also that since f(k, t) is odd in t, \( f(k,0)=0\) for all \(k\in \mathbb {Z}.\) As f is continuous and \(a(k)>0,\) we always have \(\lim _{t\rightarrow 0}\frac{\left| f(k,t)\right| }{a(k)+\left| t\right| ^{p-1}} =0.\) Hence the uniformity plays a key role in \((f_{2}).\) Finally, note that in (10) we do not assume uniformity in the limit. The simplest example for f satisfying \((f_{1})-(f_{3})\) is given by
where \(1<\sigma <p,\) \(\alpha >0\) and \(\{a(k)\}\in l^{1}\) is positive.
Now we state our main result.
Theorem 1
Let assumptions (V) and \((f_{1})-(f_{3})\) hold. Then problem ( 8) has infinitely many non-trivial homoclinic solutions with negative energy and with their norms tending to zero.
Our theorem improves the results in [10]. In [10] the set of conditions imposed on the nonlinearity is inconsistent and many arguments are fallacious in the proofs. To be more precise, in [10] problem (8) with \(0<s<1\) was investigated under the following set of hypotheses:
- \((\hat{V})\):
-
\(V(k)\ge V_{0}>0\) for all \(k\in \mathbb {Z} \) and there is \(r>0\) such that \(\lim _{\left| y\right| \rightarrow \infty }\mu (\{k\in \mathbb {Z}:V(k)\le b\}\cap U_{r}(y))=0\) for any \(b>0\), where \(U_{r}(y)\) is the neighbourhood in \( \mathbb {Z} \) centred at point y with radius r and \(\mu \) is the counting measure on \( \mathbb {Z} \).
- \((\hat{f}_{1})\):
-
\(\displaystyle f(k,t)\) is odd in t;
- \((\hat{f}_{2})\):
-
\(\displaystyle \lim \nolimits _{t\rightarrow 0}\frac{\left| f(k,t)\right| }{\left| t\right| ^{p-1}}=0\) uniformly for all \(k\in \mathbb {Z}\);
- \((\hat{f}_{3})\):
-
there exist \(\alpha >0\), \(1<\sigma <p\) and an infinite subset \(Z_{0}\subset \mathbb {Z}\) such that
$$\begin{aligned} F(k,t)\ge \alpha \left| t\right| ^{\sigma } \end{aligned}$$(12)for all \((k,t)\in Z_{0}\times \mathbb {R} \);
Observe that \((\hat{f}_{1}),(\hat{f}_{3})\) are global properties. Unfortunately, \((\hat{f}_{2})\) and \((\hat{f}_{3})\) are inconsistent. Indeed, from \((\hat{f}_{2})\) there exists \(\varepsilon >0\) such that we have \( \left| f(k,t)\right| \le \alpha p\left| t\right| ^{p-1}\) on \( \mathbb {Z} \times (-\varepsilon ,\varepsilon )\) and so \(F(k,t)\le \alpha \left| t\right| ^{p}\) on \( \mathbb {Z} \times (-\varepsilon ,\varepsilon ).\) Since \(1<\sigma <p,\) it is inconsistent with (12) for sufficiently small t. Moreover, the authors consider the nonlinearity in a special form \(f(k,t)=a(k)\left| t\right| ^{q-2}t+b(k)\left| t\right| ^{r-2}t,\) where \(1<q<p<r,\) with the assumption
- \((\hat{f}_{4})\):
-
there is \(a_{0}>0\) such that \(0<a_{0}\le a(k)\in l^{\frac{p}{p-q}}\) and \(0\le b(k)\in l^{\infty }.\)
However, there is no such \(\{a(k)\}.\) Let us list some false reasoning in [10]. The authors illegitimately use the norm \(\left\| \cdot \right\| _{\sigma }\) on \(l^{\sigma }\) for \(1<\sigma <p\) to elements from the solution space (pp. 11 and 12). Furthermore, the authors incorrectly show in proofs that the energy functional related to problem ( 8) is bounded from below (p. 9) and satisfies the (PS) condition (pp. 10 and 12). To be more precise in the case of the (PS) condition, there are incorrect estimates for \(1<p<2.\)
Let us note that our assumption \((f_{2})\) used for obtaining the required properties of energy functional is strictly weaker than those used in the literature. To the best of our knowledge, assumptions \((\hat{f}_{2})\) and
- \((\hat{f}_{5})\):
-
\(\sup _{\left| t\right| \le T}\left| f(\cdot ,t)\right| \in l^{1}\) for all \(T>0\)
have been used for this purpose so far. Our toy example (11) does not satisfy \((\hat{f}_{2})\) and \((\hat{f}_{5}).\)
Finally, let us make some remarks about the potential V. In the continuous setting, for problems considered on \( \mathbb {R} ^{N}\), we can find in the literature some assumptions on V(x), \(x\in \mathbb {R} ^{N},\) that guarantee compactness of the embedding of the solution space into the Lebesgue space (see [2, 3, 19]):
- \((V_{R})\):
-
\(V\in C(\mathbb {R}^{N},\mathbb {R}),\) \(V(x)\ge V_{0}>0\) for all \(x\in \mathbb {R}^{N}\) and \(V(x)\rightarrow +\infty \) as \(\left| x\right| \rightarrow +\infty .\)
- \((V_{BW})\):
-
\(V\in C( \mathbb {R} ^{N}, \mathbb {R} ),\) \(V(x)\ge V_{0}>0\) for all \(x\in \mathbb {R} ^{N}\) and for every \(M>0\)
$$\begin{aligned} \lambda (\{x\in \mathbb {R} ^{N}:V(x)\le M\})<+\infty , \end{aligned}$$where \(\lambda \) denotes Lebesgue measure in \( \mathbb {R} ^{N}.\)
- \((V_{BF})\):
-
\(V\in (L^{2}( \mathbb {R} ^{N}))_{\text {loc}}\) is positive and
$$\begin{aligned} \int _{S(x)}\frac{1}{V(y)}dy\rightarrow 0 \ \ \text {for}\left| x\right| \rightarrow +\infty , \end{aligned}$$where \(S(x)=\{y\in \mathbb {R} ^{N}:\left| y-x\right| <1\}\) is the unit sphere centred at x.
The condition \((V_{R}),\) i.e. the coerciveness of V, is strictly weaker than \((V_{BW}),\) and \((V_{BW})\) is strictly weaker than \((V_{BF})\) (see [Proposition 3.1 and Remark 3.2][20]).
It is easy to observe that if we create the discrete counterparts of conditions \((V_{R}),(V_{BW})\) and \((V_{BF}),\) they will all be equivalent. In particular, (V) and \((\hat{V})\) are equivalent. We also note that conditions (V) and \((\hat{V})\) guarantee compactness of the embedding of the suitable solution space into \(l^{p}\) (see [Lemma 2.3] [9] and [Lemma 2.3][10]).
Our main tool is a variant of Clark’s theorem from [14]. Here we state it for the reader’s convenience. For \(J\in C^{1}(E, \mathbb {R} ),\) where E is a Banach space, we say J satisfies the Palais-Smale (write by (PS), for short) condition if any sequence \(\{u^{(n)}\}\subset E\) for which \(J(u^{(n)})\) is bounded and \(J^{\prime }(u^{(n)})\rightarrow 0\) has a convergent subsequence.
Theorem 2
Let E be a Banach space, \(J\in C^{1}(E, \mathbb {R} )\). Assume J satisfies the (PS) condition, is even and bounded from below, and \(J(0)=0\). If for any \(m\in \mathbb {N} \), there exists a m-dimensional subspace \(E_{m}\) of E and \(\varrho _{m}>0 \) such that \(\sup _{E_{m}\cap S_{\varrho _{m}}}J<0\), where \(S_{\varrho }=\{u\in E:\left\| u\right\| =\varrho \}\), then there exists a sequence of critical points \(\{u^{(m)}\}\) satisfying \(J(u^{(m)})<0\) for all m and \(\left\| u^{(m)}\right\| \rightarrow 0\) as \(m\rightarrow \infty \).
2 Proof of the Main Result
To use Clark’s theorem, we need to construct an appropriate solution space and define an energy functional on it such that its critical points are solutions to our problem. The conditions imposed on the nonlinearity f control its behavior only in the neighbourhood of the point \(t=0\). As will be seen below, this is enough to obtain most of the needed properties of the energy functional, such as its continuous differentiability and the weak-strong continuity of it and its derivative. On the other hand, in order to obtain boundedness from below of the energy functional, we need the appropriate behavior of the nonlinearity f on \( \mathbb {Z} \times \mathbb {R} \). Therefore, we will use the truncation method.
By \((f_{1})\) and \((f_{2})\) we can find \(\varepsilon >0\) and \(\alpha >0\) such that
and
for all \(k\in \mathbb {Z} \) and \(t\in (-2\varepsilon ,2\varepsilon ).\)
Choose \(g\in C_{0}^{\infty }( \mathbb {R}, \mathbb {R} )\) such that \(g(-t)=g(t),\) \(0\le g(t)\le 1\) for all \(t\in \mathbb {R},\) \(g(t)=1\) for \(\left| t\right| \le \varepsilon \) and \(g(t)=0\) for \(\left| t\right| \ge 2\varepsilon .\) Let
for all \(k\in \mathbb {Z},\) \(t\in \mathbb {R}.\) Then \(\tilde{f}\) satisfies (13) and (14) for all \(k\in \mathbb {Z},\) \(t\in \mathbb {R}.\) Let \(\tilde{F}(k,t)=\int _{0}^{t}\tilde{f}(k,s)ds\) for every \(t\in \mathbb {R} \) and \(k\in \mathbb {Z}.\) It is important for us to note that there is \(M>0\) such that
Indeed, it is easy to see that for all \(k\in \mathbb {Z} \) we have \(\left| \tilde{f}(k,t)\right| \le \alpha \left( \left\| a\right\| _{\infty }+(2\varepsilon )^{p-1}\right) \) if \( \left| t\right| <2\varepsilon \) and \(\tilde{f}(k,t)=0\) if \( \left| t\right| \ge 2\varepsilon .\) Hence (15) holds.
We consider the auxiliary problem
Clearly, if u is a solution of problem (16) with \(\left\| u\right\| _{\infty }<\varepsilon ,\) then u is a solution of problem ( 8). So, if we find a sequence of non-trivial solutions of (16) with \(\left\| \cdot \right\| _{\infty }\)-norms tending to zero, we obtain infinite many non-trivial solutions of (8).
If \(0<s<1,\) for the solution space, we take
equipped with the norm
If \(s=1,\) for the solution space, we take
equipped with the norm
Then \(E_{s}\) is a reflexive Banach space which compactly embeds into \(l^{r}\) for all \(p\le r\le \infty \) (see [10] for \(0<s<1\) and [6, 8] for \(s=1\)). Moreover, \(\left\| u\right\| _{\infty }\le V_{0}^{-1/p}\left\| u\right\| \) for all \(u\in E_{s}.\)
Define functionals \(J_{s},I_{s},K:E_{s}\rightarrow \mathbb {R} \) as
for \(u\in E_{s},0<s\le 1\). By [Lemma 2.5] [9], \(I_{s}\in C^{1}(E_{s}, \mathbb {R} ),0<s<1,\) with
for all \(u,v\in E_{s}.\) By [8][Proposition 5], \(I_{1}\in C^{1}(E_{1}, \mathbb {R} )\) with
for all \(u,v\in E_{1}.\)
Now, we will prove the needed properties of the functional K. First, we will recall the Vitali Theorem for sequence spaces (see [Proposition 3.128][5]).
Theorem 3
Let \(\{w^{(n)}\}_{n\in \mathbb {N} }\subset l^{1}\) be a sequence such that \(w_{k}^{(n)}\rightarrow w_{k}\) for all \(k\in \mathbb {Z}.\) Then the following assertions are equivalent:
-
(a)
\(w^{(n)}\rightarrow w\) in \(l^{1}.\)
-
(b)
The family \(\{\left| w^{(n)}\right| :n\in \mathbb {N} \}\) is uniformly summable, that is, for every \(\varepsilon >0,\) we can find \(h\in \mathbb {N} \) such that
$$\begin{aligned} \sup _{n\in \mathbb {N} }\sum _{\left| k\right| \ge h}\left| w_{k}^{(n)}\right| <\varepsilon . \end{aligned}$$
In our case, the function \(\tilde{f}\) satisfies condition (14) globally, i.e. on \( \mathbb {Z} \times \mathbb {R}.\) In order to obtain the needed properties of the functional K, it is enough to control \(\tilde{f}\) in a neighbour of \(t=0.\) Therefore, we formulate and prove the result with a weaker assumption. Here we follow [24].
Lemma 4
Assume (V) and let \(f\in C( \mathbb {Z} \times \mathbb {R}, \mathbb {R} )\) satisfy the following condition: there exist \(\varepsilon ,C>0\) and a positive \(a\in l^{p^{\prime }},\) \(p^{\prime }=\frac{p}{p-1},\) such that
for all \(k\in \mathbb {Z} \) and \(\left| t\right| <\varepsilon .\) Then the functional \( K:E_{s}\rightarrow \mathbb {R},\) \(K(u)=\sum _{k\in \mathbb {Z} }F(k,u(k)),\) where \(F(k,t)=\int _{0}^{t}f(k,s)ds\) for every \(t\in \mathbb {R} \) and \(k\in \mathbb {Z},\) has the following properties:
-
(a)
K is sequentially weakly-strongly continuous, that is, if \( u^{(n)}\rightharpoonup u\), then \(K(u^{(n)})\rightarrow K(u)\).
-
(b)
K is of class \(C^{1}\) with
$$\begin{aligned} \left\langle K^{\prime }(u),v\right\rangle =\sum _{k\in \mathbb {Z} }f(k,u(k))v(k) \end{aligned}$$(18)for all \(u,v\in E_{s}.\)
-
(c)
\(K^{\prime }\) is sequentially weakly-strongly continuous, i.e., if \(u^{(n)}\rightharpoonup u\), then \(K^{\prime }(u^{(n)})\rightarrow K^{\prime }(u)\) in \(E_{s}^{*}.\)
Proof
By (17), there exists \(C_{1}>0\) such that
For any \(u\in E_{s}\) there exists \(h\in \mathbb {N} \) such that \(\left| u(k)\right| <\varepsilon \) for all \(\left| k\right| \ge h\) and so, using (19) and Hölder’s inequality, we deduce that \(F(\cdot ,u(\cdot ))\) is summable and K(u) is well defined.
(a) Assume that \(u^{(n)}\rightharpoonup u\) in E. Since \(E_{s}\) compactly embeds into \(l^{p}\), up to a subsequence, \(\{\left| u^{(n)}\right| ^{p}\}\) converges in \(l^{1}.\) Thus
is uniformly summable by Theorem 3. In particular, there exists \( h_{1}\in \mathbb {N} \) such that \(\left| u^{(n)}(k)\right| ,\left| u(k)\right| <\varepsilon \) for all \(\left| k\right| >h_{1}\) and \(n\in \mathbb {N}.\) Now, from (19) and Young’s inequality, there exists \(C_{2}>0,\) such that
for all \(\left| k\right| >h_{1}\) and \(n\in \mathbb {N} \). Hence \(\left\{ F(\cdot ,u^{(n)})-F(\cdot ,u):n\in \mathbb {N} \right\} \) is uniformly summable. As F is continuous, we have
by Theorem 3. This shows \(K(u^{(n)})\rightarrow K(u).\)
(b) To see formula (18) take \(u,v\in E_{s}\). For any \(k\in \mathbb {Z} \) and \(0<\left| t\right| <1\) there exists \(\lambda _{k,t}\in [0,1]\) such that
by the Mean Value Theorem. We claim that
Suppose, by contradiction, that there exist \(\delta >0\) and a null sequence \(\{t_{n}\}_{n\in \mathbb {N} }\subset [-1,1]\) such that
Since \(u,v\in l^{p},\) there is \(h_{2}\in \mathbb {N} \) such that \(\left| u(k)\right| +\left| v(k)\right| <\varepsilon \) for all \(\left| k\right| >h_{2}\). By (17) and Young’s inequality, we have for all \(\left| t\right| <1,\) \(\lambda \in [0,1],\) \(k\in \mathbb {Z} \) and some constant \(C_{3}>0\)
Since \(a^{p^{\prime }},\left| u\right| ^{p},\left| v\right| ^{p}\in l^{1},\) the family \(\left\{ \{f(k,u(k)+\lambda _{k,t_{n}}t_{n}v(k))\}_{k\in \mathbb {Z} }:n\in \mathbb {N} \right\} \subset l^{1}\) is uniformly summable. This and the continuity of f give us
by Theorem 3, which contradicts (20). Hence K is Gateaux differentiable and formula (18) holds. Clearly, after proving (c) we will have continuous Frechet differentiability of K.
(c) Assume that \(u^{(n)}\rightharpoonup u\) in E. We have
Set
We assert that \(\alpha =0\). Suppose, by contradiction, that \(\alpha >0\). Hence, there exists a sequence \(\{v^{(n)}\}\subset E\) with \(\left\| v^{(n)}\right\| =1\) such that
for sufficiently large n. Since \(E_{s}\) compactly embeds into \(l^{p}\), up to subsequences, \(\{\left| u^{(n)}\right| ^{p}\}\) and \(\{\left| v^{(n)}\right| ^{p}\}\) converge in \(l^{1}.\) Thus
is uniformly summable by Theorem 3. In particular, there exists \(h_{3}\in \mathbb {N} \) such that \(\left| u^{(n)}(k)\right| ,\left| u(k)\right| <\varepsilon \) for all \(\left| k\right| >h_{3}\) and \(n\in \mathbb {N}.\) From (17) and Young’s inequality, we have
for some constant \(C_{4}>0\) and all \(\left| k\right| >h_{3},n\in \mathbb {N}.\) Hence
is uniformly summable. Since f is continuous,
by Vitali Theorem. This contradicts (21) if \(\alpha >0\). Hence, \( \left\| K^{\prime }(u^{(n)})-K^{\prime }(u)\right\| _{E_{s}^{*}}\rightarrow 0\) as \(n\rightarrow +\infty \). \(\square \)
All the above establish \(J_{s}\in C^{1}(E_{s}, \mathbb {R} )\) with
if \(0<s<1\) and
if \(s=1\), for all \(u,v\in E_{s}.\) For every \(k\in \mathbb {Z},\) taking in the above formulas \(v=e_{k}=\{\delta _{kj}\}_{j\in \mathbb {Z} },\) where \(\delta _{kj}\) is the Kronecker delta, we conclude that every critical point of \(J_{s}\) is a homoclinic solution of problem (16).
Now, we show that \(J_{s}\) satisfies all assumptions in Theorem 2. Clearly, \(J_{s}\) is even and \(J_{s}(0)=0.\)
Claim 5
\(J_{s}\) is bounded from below.
First, we observe that there exists a constant \(C>0\) such that
for all \(u\in E_{s}\). Indeed, applying (13)-(15) gives
for all \(k\in \mathbb {Z},t\in \mathbb {R}.\) Moreover, by (V), there exists \(h\in \mathbb {N} \) such that
for all \(\left| k\right| \ge h.\) Hence
, all the above and Young’s inequality give us
for all \(u\in E_{s}\), where \(C=2hM+\frac{\alpha }{p^{\prime }}\left\| a\right\| _{p^{\prime }}\). Therefore,
for all \(u\in E_{s}.\) Hence, \(J_{s}\) is bounded from below. This proves Claim 5.
Claim 6
\(J_{s}\) satisfies the (PS) condition.
Let \(\{u^{(n)}\}\) be a sequence in \(E_{s}\) such that \(\{J_{s}(u^{(n)})\}\) is bounded and \(J_{s}^{\prime }(u^{(n)})\rightarrow 0.\) By (23), \(\{u^{(n)}\}\) is bounded. Then, passing to a subsequence if necessary, it can be assumed that there exists \(u\in E_{s}\) such that \( u^{(n)}\rightharpoonup u\) weakly in \(E_{s}\) and \(u^{(n)}\rightarrow u\) strongly in \(l^{p}.\) All this and Lemma 4 give us
and so
Now, if \(s=1,\) we argue as in [12][Lemma 3.4] and we obtain \( u^{(n)}\rightarrow u\) in \(E_{1}.\) If \(0<s<1,\)we argue similarly. Let \( \varphi _{p}(t)=\left| t\right| ^{p-2}t,t\in \mathbb {R}.\) Recall the following inequalities (see [16][p. 25])
for all \(s,t\in \mathbb {R},\) where \(c_{1}(p),c_{2}(p)>0\) are constants.
If \(p\ge 2,\) then
Hence \(u^{(n)}\rightarrow u\) in \(E_{s},\) by (24).
If \(1<p<2\), then, by Hölder’s inequality, we obtain
and similarly,
Thus, using (25)-(27), we have
and so \(u^{(n)}\rightarrow u\) in \(E_{s},\) by (24). This proves Claim 6.
Claim 7
For any \(m\in \mathbb {N} \), there exists a m-dimensional subspace \(E_{m}\) of \(E_{s}\) and \(\varrho _{m}>0\) such that \(\sup _{E_{m}\cap S_{\varrho _{m}}}J_{s}<0.\)
Let \(Z_{0}=\{k_{i}:i\in \mathbb {N} \}\subset \mathbb {Z} \) be the set with the properties listed in \((f_{3})\). Define \( e^{(i)}:=e_{k_{i}},\) that is \(e^{(i)}=\{e^{(i)}(k)\}_{k\in \mathbb {Z} },i\in \mathbb {N},\) with
Define \(E_{m}:=\)span\(\{e^{(i)}:i=1,...,m\},\) \(m\in \mathbb {N}.\) Clearly, \(E_{m}\subset E_{s}\) and \(\dim E_{m}=m.\) Now, fix \(m\in \mathbb {N} \) and write \(Z_{m}:=\{k_{1},...,k_{m}\}\subset Z_{0}.\) Since \(Z_{m}\) is a finite set, there exist \(C_{m}>0\) and \(0<\varepsilon _{m}<\varepsilon \) such that
for all \(k\in Z_{m}\) and \(\left| t\right| <\varepsilon _{m},\) by \( (f_{3})\) and the fact that \(\tilde{F}=F\) on \( \mathbb {Z} \times (-\varepsilon ,\varepsilon ).\) Since all norms are equivalent on the finite dimensional space \(E_{m}\), we have
for all \(u\in E_{m}\) with \(\left\| u\right\| _{\infty }<\varepsilon _{m}.\) From this and \(1<\sigma <p,\) we conclude that there exists \( 0<\varrho _{m}<\varepsilon _{m}\) such that \(\sup _{E_{m}\cap S_{\varrho _{m}}}J_{s}<0.\) This proves Claim 7.
We have verified all the conditions of Theorem 2. Consequently, problem (16) has a sequence \(\{u^{(m)}\}\) of non-trivial solutions with \(\left\| u^{(m)}\right\| \rightarrow 0\) as \(m\rightarrow \infty \). Since also \(\left\| u^{(m)}\right\| _{\infty }\rightarrow 0\) as \( m\rightarrow \infty ,\) there exists \(m_{0}\) such that for every \(m\ge m_{0},\) \(u^{(m)}\) is the solution of problem (8). This proves Theorem 1.
References
Balanov, Z., Garcia-Azpeitia, C., Krawcewicz, W.: On variational and topological methods in nonlinear difference equations. Commun. Pure. Appl. Anal. 17, 2813–2844 (2018)
Bartsch, T., Wang, Z.Q.: Existence and multiplicity results for some superlinear elliptic problems on \( R^{N}\). Comm. Partial Differ. Equ. 20(910), 1725–1741 (1995)
Benci, V., Fortunato, D.: Discreteness conditions of the spectrum of Schrödinger operators. J. Math. Anal. Appl. 64, 695–700 (1978)
Ciaurri, O., Roncal, L., Stinga, P.R., Torrea, J.L., Varona, J.L.: Nonlocal discrete diffusion equations and the fractional discrete Laplacian, regularity and applications. Adv. Math. 330, 688–738 (2018)
Gasiński, L., Papageorgiou, N.: Exercises in analysis. Part 1. Problem Books in Mathematics. Springer, Cham, x+1037 pp (2014)
Graef, J.R., Kong, L., Wang, M.: Existence of homoclinic solutions for second order difference equations with p-Laplacian. Dyn. Syst. Differ. Equ. Appl. Special 2015, 533–539 (2015)
Iannizzotto, A., Rădulescu, V.: Positive homoclinic solutions for the discrete \(p\)-Laplacian with a coercive weight function. Differ. Integral Equ. 27(1–2), 35–44 (2014)
Iannizzotto, A., Tersian, S.: Multiple homoclinic solutions for the discrete \(p\)-Laplacian via critical point theory. J. Math. Anal. Appl. 43(1), 173–182 (2013)
Ju, X., Die, H., Xiang, M.: The nehari manifold method for discrete fractional \(p\)-Laplacian equations. Adv. Differ. Equ. 559, 1–21 (2020)
Ju, C., Zhang, B.: On fractional discrete \(p\)-Laplacian equations via Clark’s theorem. Appl. Math. Comput. 434, 127443 (2022)
Kim, J.-M., Yang, S.-O.: Multiple homoclinic orbits for a class of the discrete p-Laplacian with unbounded potentials. Math. Methods Appl. Sci. 44(1), 1103–1117 (2021)
Kong, L.: Homoclinic solutions for a second order difference equation with \(p\)-Laplacian. Appl. Math. Comput. 247, 1113–21 (2014)
Landkof, N.S.: Foundations of Modern Potential Theory (Translated from the Russian by A.P. Doohovskoy), Die Grundlehren der mathematischen Wissenschaften, vol. 180, Springer-Verlag, New York, (1972)
Liu, Z., Wang, Z.Q.: On clark’s theorem and its applications to partially sublinear problems. Ann. Inst. H. Poincaré Anal. Non Linéaire 32, 1015–1037 (2015)
Molica Bisci, G., Radulescu, V., Servadei, R.: Variational methods for nonlocal fractional problems, vol. 162, p. xvi+383. Cambridge University Press, Cambridge (2016)
Motreanu, D., Motreanu, V.V., Papageorgiou, N.: Topological and variational methods with applications to nonlinear boundary value problems, p. xii+459. Springer, New York (2014)
Nastasi, A., Tersian, S., Vetro, C.: Homoclinic solutions of nonlinear laplacian difference equations without ambrosetti-rabinowitz condition. Acta Math. Sci. Ser. B (Engl. Ed.) 41(3), 712–718 (2021)
Pankov, A.: Gap solitons in periodic discrete nonlinear Schrö dinger equations. Nonlinearity 19, 27–40 (2006)
Rabinowitz, P.H.: On a class of nonlinear Schrödinger equations. Z. Angew. Math. Phys. 43(2), 270–291 (1992)
Salvatore, A.: Multiple solutions for perturbed elliptic equations in unbounded domains. Adv. Nonlinear Stud. 3(1), 1–23 (2003)
Stegliński, R.: On sequences of large homoclinic solutions for a difference equations on the integers. Adv. Differ. Equ. 38, 11 (2016)
Stegliński, R.: On sequences of large homoclinic solutions for a difference equations on the integers involving oscillatory nonlinearities. Electron. J. Qual. Theory Differ. Equ. 35, 1–11 (2016)
Stegliński, R.: On homoclinic solutions for a second order difference equation with \(p\)-Laplacian. Discrete Contin. Dyn. Syst. Ser. B 23(1), 487–492 (2018)
Stegliński, R.: Infinitely many solutions for double phase problem with unbounded potential in \( R^{N}\). Nonlinear Anal. 214(112580), 20 (2022)
Stein, E.M.: Singular integrals and differentiability properties of functions. Princeton Univ. Press, Princeton, NY (1970)
Sun, G., Mai, A.: Infinitely many homoclinic solutions for second order nonlinear difference equations with p-Laplacian. Sci. World J. 2014(276372), 6 (2014)
Wu, Y., Tahar, B., Rafik, G., Rahmoune, A., Yang, L.: The existence and multiplicity of homoclinic solutions for a fractional discrete \(p\)-Laplacian equation. Mathematics 10, 1–16 (2022)
Xiang, M., Zhang, B.: Homoclinic solutions for fractional discrete Laplacian equations. Nonlinear Anal. 198, 111886 (2020)
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Stegliński, R. On Local and Nonlocal Discrete p-Laplacian Equations via Clark’s Theorem. Qual. Theory Dyn. Syst. 22, 73 (2023). https://doi.org/10.1007/s12346-023-00767-2
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DOI: https://doi.org/10.1007/s12346-023-00767-2