\documentclass[reqno]{amsart}
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\AtBeginDocument{{\noindent\small
\emph{Electronic Journal of Differential Equations},
Vol. 2015 (2015), No. 232, pp. 1--16.\newline
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu}
\thanks{\copyright 2015 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2015/232\hfil 
 Non-smooth extension of a three critical points theorem]
{Non-smooth extension of a three critical points theorem by  Ricceri
 with an application to $p(x)$-Laplacian differential inclusions}

\author[Z. Yuan, L. Huang \hfil EJDE-2015/232\hfilneg]
{Ziqing Yuan, Lihong Huang}

\address{Ziqing Yuan (corresponding author)\newline
College of  Mathematics and Econometrics,
Hunan University, Changsha, Hunan 410082,  China}
\email{junjyuan@sina.com}

\address{Lihong Huang \newline
College of  Mathematics and Econometrics,
Hunan University, Changsha, Hunan 410082,  China}
\email{lhhuang@hnu.edu.cn}

\thanks{Submitted May 20, 2015. Published September 10, 2015.}
\subjclass[2010]{49J20, 35J85, 47J30}
\keywords{ Nonsmooth critical point theory; locally Lipschitz;
\hfill\break\indent differential inclusion; $p(x)$-Laplacian}

\begin{abstract}
 We extend a smooth Ricceri three critical-points theorem to a non-smooth case.
 Our approach is based on the non-smooth analysis. As an application,
 we obtain the existence of at least three critical points for a
 $p(x)$-Laplacian differential inclusion.
\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{remark}[theorem]{Remark}
\newtheorem{definition}[theorem]{Definition}
\allowdisplaybreaks

\section{Introduction}

 First, we give some definitions which will be used throughout this paper. 
If $X$ is a nonempty set and $I$, $\Psi$, $\Phi:X\to\mathbb{R}$ are three
given functions, for each $\mu>0$ and $r\in]\inf_X\Phi,\sup_X\Phi[$, we define
\begin{gather*}
h_1(\mu I+\Psi,\Phi, r)
=\inf_{u\in \Phi^{-1}(]-\infty, r[)}\frac{\mu I(u)+\Psi(u)
 -\inf_{u\in \Phi^{-1}(]-\infty, r])}(\mu I+\Psi)}{r-\Phi(u)},\\
h_2(\mu I+\Psi,\Phi, r)
=\sup_{u\in \Phi^{-1}(]r,+\infty[)}  \frac{\mu I(u)+\Psi(u)
 -\inf_{u\in \Phi^{-1}(]-\infty, r])}(\mu I+\Psi)}{r-\Phi(u)}.
\end{gather*}
When $\Psi+\Phi$ is bounded below, for each $r\in ]\inf_X\Phi,\sup_X\Phi[$ such that
$$
\inf_{u\in\Phi^{-1}(]-\infty,r])}I(u)<\inf_{u\in\Phi^{-1}(r)}I(u).
$$
We define
$$
h_3(I,\Psi,\Phi, r)
=\inf\Big\{\frac{\Psi(u)-\gamma+r}{\eta_r-I(u)}:u\in X,\Phi(u)<r,I(u)<\eta_r\Big\},
$$
where
\[
\gamma=\inf_{u\in X}(\Psi(u)+\Phi(u)),\quad 
\eta_r=\inf_{u\in\Phi^{-1}(r)}I(u).
\]

In the past years, many authors have studied three critical points theorems.  
We refer to \cite{a3} for $C^2$ functions, to \cite{s1} 
for application in quasilinear elliptic system, and to \cite{r1} for $C^1$ functions. 
Recently,  Ricceri \cite{r4}  established the following three critical points theorem.

\begin{theorem} \label{thmA}
Let $X$ be a reflexive real Banach space. $I:X\to \mathbb{R}$ a sequentially
weakly lower semicontinuous $C^1$ function bounded on each bounded subset of 
$X$ and whose derivative admits a continuous inverse on $X^*$. 
$\Psi,\Phi:X\to \mathbb{R}$ are two $C^1$ functions with compact derivative.
Moreover, assume that there exists $r\in]\inf_X\Phi,\sup_X\Phi[$ such that
$$
h_1(I+\Psi,\Phi,r)<h_2(I+\Psi,\Phi,r)
$$
and that, for each $\lambda\in]h_1(I+\Psi,\Phi,r),h_2(I+\Psi,\Phi,r)[$, 
the function $I+\Psi+\lambda\Phi$ is coercive.

Then, for each compact interval 
$[a,b]\subset]h_1(I+\Psi,\Phi,r),h_2(I+\Psi,\Phi,r)[$, there exists 
$\rho>0$ with the following property: for every $\lambda\in[a,b]$ and every 
$C^1$ function $\Gamma:X\to\mathbb{R}$ with compact derivative, there exists
$\delta>0$ such that, for each $\nu\in [0,\delta]$, the equation
$$
I'(u)+\Psi'(u)+\lambda\Phi'(u)+\nu\Gamma'(u)=0
$$
has at least three solutions whose norms are less than $\rho$.
\end{theorem}

As pointed out in \cite{r4}, a natural framework where the above result 
applies successfully is given by quasilinear equations in bounded domains. 
This situation occurs, for example, when $X=W^{1,p}_0(\Omega)$ and
\begin{gather*}
I(u)=\frac{1}{p}\int_\Omega|\nabla u|^p{\rm d}x,\quad
\Psi(u)=\int_\Omega\int_0^uf(x,t){\rm d}t{\rm d}x, \\
\Phi(u)=\int_\Omega\int_0^ug(x,t){\rm d}t{\rm d}x,\quad
\Gamma(u)=\int_\Omega\int_0^uh(x,t){\rm d}t{\rm d}x, \quad\forall u\in X,
\end{gather*}
$f,g,h:\Omega\times\mathbb{R}\to\mathbb{R}$ being three continuous functions
 with subcritical growth.

However, because of the $C^1$ assumption on $\Psi,\Phi$ and $\Gamma$, 
several other problems that one meets in important concrete setting cannot be 
treated through  Theorem \ref{thmA}. For instance, let us mention both variational 
inequalities and elliptic equations with discontinuous nonlinearities. 
In fact, $\Psi,\Phi$ and $\Gamma$ usually  are locally Lipschitz at most. 
So the question of providing a non-smooth  version of the above results
 which applies also to these meaning situations spontaneously arises.
 Our interest in the present paper is to extend Theorem \ref{thmA} into a non-smooth version
by adopting the framework of Motreanu-Panagiotopoulos \cite{m1}.

Recently, smooth  critical points have been extended to nonsmooth cases by 
several authors via  different methods. We should mention that 
Krist\'aly et al \cite{k2} extended a Ricceri's multiplicity theorem for
the existence of three critical points of  nonsmooth functionals. 
Arcoya and Carmona \cite{a2} dealt with the Pucci-Serrin type critical point 
theorem in \cite{p1} to the nondifferentiable type.
Li and Shen \cite{l1} proved a Pucci-Serrin type three critical points
for continuous functionals. These results based on various conditions. 
All these results enrich the theory of nonsmooth analysis. 
We think that our abstract results in this direction presented here can be 
used to  study  a large number of differential equations with nonsmooth potentials.
Furthermore, we improve the results in \cite{k2} by omitting the
restrictions on the nonsmooth potentials, see Remark \ref{rmk3.1} below.

The rest of the article is organized as follows. 
Section 2 contains the necessary preliminaries. 
Section 3 contains the proofs our main results. 
Section 4 provides  an application to a $p(x)$-Laplacian  differential inclusion.

\section{Preliminaries}

Basic notation:
\begin{itemize}

\item $|\cdot|_{p(x)}$ is the usual $L^{p(x)}(\Omega)$-norm.

\item $\rightharpoonup$ means weak convergence, and $\to$ strong convergence.

\item $C$ denotes all the embedding constants (the exact value may be 
different from line to line).

\item $(X,\|\cdot\|)$  denotes a (real)
 Banach space and $(X^{*},\|\cdot\|_{*})$ its topological dual.
\end{itemize}

\begin{definition} \label{def2.1} \rm
 A function $I: X\to  \mathbb{R}$ is locally Lipschitz if for every $u\in X$ 
there exist  a neighborhood $U$ of $u$ and $L>0$ such that for every 
$\nu,\eta \in U$,
\[
|I (\nu)-I(\eta)|\leq L\|\nu-\eta\|.
\]
\end{definition}

\begin{definition} \label{def2.2} \rm
 Let $I:X\to \mathbb{R}$ be a locally Lipschitz function, $u,\nu\in X$. The
generalized derivative of $I$ in $u$ along the direction $\nu$ is
\[
I^{0}(u; \nu)=\limsup_{\eta\to u, \tau\to
0^{+}} \frac{I(\eta+\tau\nu)-I(\eta)}{\tau}.
\]
\end{definition}

It is easy to see that the function $\nu\mapsto I^{0}(u;\nu)$ is sublinear,
continuous and so is the support function of a nonempty, convex and
 $w^{*}$-compact set $\partial I (u)\subset X^{*}$, defined by
\[
\partial I (u)=\{u^{*}\in X^{*}:\langle u^{*},\nu \rangle_{X}\leq I^{0}(u; \nu)
\text{ for all }v\in X\}.
\]
If $I\in C^{1}(X)$, then
$\partial I(u)=\{I'(u)\}$.
Clearly, these definitions extend those of the G\^{a}teaux
directional derivative and gradient.

A point $u\in X$ is a critical point of $I$, if $0\in \partial I(u)$. 
It is easy to see that, if $u\in X$ is a local
minimum of $I$, then $0\in\partial I(u)$. For more details we
refer the reader to Clarke \cite{c1}.

\begin{definition} \label{def2.3} \rm
 The locally Lipschitz function $\varphi:X\to\mathbb{R}$ satisfies the 
non-smooth $(PS)_c$, if for every sequence $\{u_n\}$ in $X$ such that
\begin{itemize}
\item[(i)] $\varphi(u_n)\to c$ as $n\to\infty$;

\item[(ii)] there exists a sequence $\{\varepsilon_n\}$ in $]0,+\infty[$ with 
$\varepsilon_n\to 0$ such that
$$
\varphi^\circ(u_n;y-u_n)+\varepsilon_n\|y-u_n\|\geq 0 \quad
\text{for all }y\in X, n\in\mathbb{N},
$$
\end{itemize}
admits a convergent subsequence.
\end{definition}

\begin{definition} \label{def2.4} \rm
If $X$ is a topological space, a function $\varphi:X\to\mathbb{R}$ is said 
to be sequentially inf-compact if, for each $r\in\mathbb{R}$, the set 
$\varphi^{-1}(]-\infty,r])$ is sequentially compact.
\end{definition}

\begin{definition} \label{def2.5} \rm
 A mapping $A:X\to X^*$ is of type $(S_+)$ if for every sequence $\{u_n\}$ such 
that $u_n\rightharpoonup u\in X$ and
$$
\limsup\langle A(u_n),u_n-u\rangle\leq 0,
$$
one has $u_n\to u$.
\end{definition}

In the following, we state some properties of the spaces $L^{p(x)}(\Omega)$ and 
$W^{1,p(x)}(\Omega)$ which we call generalized Lebesgue-Sobolev spaces.
Set
$$
C_+(\bar\Omega)=\{h~|~h(x)\in C(\Omega), h(x)>1, \text{ for any }x\in\bar\Omega\}.
$$
For $h(x)\in C_+(\bar\Omega)$, we write
$$
h^-=\inf_{x\in\Omega}h(x),\quad h^+=\sup_{x\in\Omega}h(x).
$$
We define, for $p(x)\in C_+(\bar\Omega)$
$$
L^{p(x)}(\Omega)=\Big\{u:u \text{ is a measurable real-valued function},
\int_\Omega |u(x)|^{p(x)}{\rm d}x<\infty\Big\}
$$
with the norm on $L^{p(x)}(\Omega)$ by
$$
|u|_{p(x)}=\inf\Big\{\lambda>0
:\int_\Omega\big|\frac{u(x)}{\lambda}\big|^{p(x)}{\rm d}x \leq 1\Big\},
$$
then $(L^{p(x)}(\Omega),|\cdot|_{p(x)})$ is a Banach space. 
We call it a generalized Lebesgue space.

The generalized Lebesgue-Sobolev space $W^{1,p(x)}(\Omega)$ is defined by
$$
W^{1,p(x)}(\Omega)=\{u\in L^{p(x)}(\Omega):|\nabla u|\in L^{p(x)}(\Omega)\}
$$
equipped with the norm
$$
\|u\|=|u|_{p(x)}+|\nabla u|_{p(x)}.
$$
We denote $W_0^{1,p(x)}(\Omega)$ as the closure of $C^\infty_0(\Omega)$ in 
$W^{1,p(x)}(\Omega)$.
Then $W^{1,p(x)}(\Omega)$ and  $W_0^{1,p(x)}(\Omega)$ are separable reflexive 
Banach spaces (see \cite{e1,f1,f4,f5,k1}).

\begin{proposition}[\cite{f1,f3}] \label{prop2.1} \rm
 (i) If $q(x)\in C_+(\bar\Omega)$ and $q(x)< p^*(x), \forall x\in\bar\Omega$,
then the embedding from $W^{1,p(x)}(\Omega)$ to $L^{q(x)}$ is compact and 
it is also continuous for $q(x)\leq p^*(x)$, where
$$
p^{*}(x)=\begin{cases}  
\frac{Np(x)}{N-p(x)} &\text{if } p(x)<N,\\
 +\infty &\text{if } p(x)\geq N,
\end{cases}
$$

(ii) If $p_1(x), p_2(x)\in C_+(\bar\Omega)$, and 
$p_1(x)\leq p_2(x)$ for all $x\in\bar\Omega$, then 
$L^{p_2(x)}(\Omega)\hookrightarrow L^{p_1(x)}(\Omega)$, and the embedding 
is continuous.
\end{proposition}

\begin{proposition}[\cite{f3}] \label{prop2.2}
Set $\rho(u)=\int_\Omega|u(x)|^{p(x)}{\rm d}x$.
For $u,u_k\in L^{p(x)}(\Omega)$, we have
\begin{itemize}
\item[(i)] For $u\neq 0$, $|u|_{p(x)}=\lambda \Leftrightarrow
\rho(\frac{u}{\lambda})=1$;

\item[(ii)]  $|u|_{p(x)}<1 (=1, >1)\Leftrightarrow \rho (u)<1 (=1, >1)$;

\item[(iii)] If $|u|_{p(x)}>1$, then $|u|_{p(x)}^{p^-}
\leq \rho (u)\leq |u|_{p(x)}^{p^+}$;

\item[(iv)] If $|u|_{p(x)}<1$, then $|u|_{p(x)}^{p^+}
\leq \rho (u)\leq |u|_{p(x)}^{p^-}$;

\item[(v)] $\lim_{k\to \infty}|u_k|_{p(x)}=0\Leftrightarrow
\lim_{k\to \infty} \rho(u_k)=0$;

\item[(vi)] $|u_k|_{p(x)}\to\infty\Leftrightarrow
\rho(u_k)\to\infty$.
\end{itemize}
\end{proposition}

\begin{proposition}[\cite{f3}] \label{prop2.3}
 (i) The space $L^{p(x)}(\Omega)$ is a separable,
uniform Banach space, and its conjugate space is $L^{p'(x)}(\Omega)$, 
where $1/p(x)+1/p'(x)=1$.
For any $u\in L^{p(x)}(\Omega)$ and $v\in L^{p'(x)}(\Omega)$ we have
$$
\big| \int_\Omega uv{\rm d}x\big|
\leq \Big(\frac{1}{p^-}+\frac{1}{(p')^-}\Big)|u|_{L^{p(x)}(\Omega)}|v|_{L^{p'(x)}
(\Omega)}
\leq 2|u|_{L^{p(x)}(\Omega)}|v|_{L^{p'(x)}(\Omega)}.
$$

(ii) There is a constant $C>0$, such that
$$
|u|_{p(x)}\leq C|\nabla u|_{p(x)} \quad \forall u\in W_0^{1,p(x)}(\Omega).
$$
By (ii) of Proposition \ref{prop2.3}, we know that $|\nabla u|_{p(x)}$ and $\|u\|$ 
are equivalent norms on $W_0^{1,p(x)}(\Omega)$.
\end{proposition}


\begin{proposition}[\cite{c1}] \label{prop2.4}
 Let $h:X\to\mathbb{R}$ be locally Lipschitz function. Then
\begin{itemize}
\item[(i)] $(-h)^\circ (u;z)=h^\circ (u;-z)$ for all $u, z\in X$;

\item[(ii)] $h^\circ(u;z)=\max\{\langle u^*,z\rangle_X:u^*\in \partial h(u)\}
\leq L\|z\|$ with $L$ as in Definition \ref{def2.1}, for all $u, z\in X$;

\item[(iii)] Let $j:X\to\mathbb{R}$ be a continuously differentiable function
Then $\partial j(u)=\{j'(u)\}$, $j^\circ (u;z)$ coincides with 
$\langle j'(u),z\rangle_X$
and $(h+j)^\circ(u;z)=h^\circ(u;z)+\langle j'(u),z\rangle_X$ for all $u, z\in X$;

\item[(iv)] (Lebourg's mean value theorem) Let $u$ and $v$ be two points in $X$. 
Then, there exists a
point $\omega$ in the open segment between $u$ and $v$, and a 
$u^*_\omega\in \partial h(\omega)$ such that
    $$
    h(u)-h(v)=\langle u^*_\omega,u-v\rangle_X;
    $$

\item[(v)] Let $Y$ be a Banach space and $j:Y\to X$ a continuously differentiable 
function. Then $h\circ j$ is locally Lipschitz and
  $$
  \partial (h\circ j)(u)\subseteq \partial h(j(y))\circ j'(y)\text{ for all }y\in Y;
  $$

\item[(vi)] If $h_1, h_2:X\to\mathbb{R}$ are locally Lipschitz, then
$$
\partial (h_1+h_2)(u)\subseteq \partial h_1(u)+\partial h_2(u);
$$

\item[(vii)] $\partial h(u)$ is convex and weakly$^*$ compact and the set-valued 
mapping $\partial h:X\to 2^{X^*}$ is weakly$^*$ u.s.c.;

\item[(viii)] $\partial(\lambda h)(u)=\lambda\partial h(u)$ for every 
$\lambda\in\mathbb{R}$.
\end{itemize}
\end{proposition}

\begin{lemma} \label{lem2.1}
 Let $\varphi:X\to\mathbb{R}$ be a locally Lipschitz function with compact gradient. 
Then, $\varphi$ is sequentially weakly continuous.
\end{lemma}

\begin{proof}
 Our assumptions imply  that the set-valued mapping $\partial\varphi:X\to\mathbb{R}$ 
sends bounded sets into relatively compact sets. We proceed by contradiction. 
Suppose that $\{u_n\}$ is a sequence in $X$ such that $u_n\rightharpoonup u\in X$, 
and $\{\varphi(u_n)\}$ does not converge to $\{\varphi(u)\}$. 
Then, passing to a subsequence, there exists some $\epsilon>0$ such that
\begin{equation}\label{e2.1a}
|\varphi(u_n)-\varphi(u)|\geq\epsilon
\end{equation}
for all $n\in\mathbb{N}$.
Since the  sequence $\{u_n\}$ is bounded, there exists $M>0$ such that 
$\|u_n-u\|\leq M$ for all $n\in\mathbb{N}$. By Proposition \ref{prop2.4} (iv) 
there exist some $\omega_n$ between  $u$ and $u_n$, and  
$\omega_n^*\in\partial\varphi(\omega_n)$ such that
$$
\varphi(u_n)-\varphi(u)=\langle \omega^*_n, u_n-u\rangle.
$$
Note that $\{\omega_n\}$ is bounded as well. Up to a subsequence, we may 
assume that $\omega^*_n\to \omega^*\in X^*$. So, for $n$ large enough we have
$$
\|\omega_n^*-\omega^*\|<\frac{\varepsilon}{2M}, \quad 
|\langle \omega^*,u_n-u\rangle|<\frac{\epsilon}{2},
$$
which means
$$
|\varphi(u_n)-\varphi(u)|\leq \|\omega^*_n-\omega^*\|_*\|u_n-u\|
+|\langle \omega^*,u_n-u\rangle|<\epsilon,
$$
contradicting \eqref{e2.1a}.
\end{proof}

For the convenience of the reader, we recall two results which are crucial in our 
further investigations. The first result is due to Ricceri \cite{r3} which ensures 
the existence of two local minima for a parametric function defined on a Banach space. 
Note that no smoothness assumption is required on the function.
 We denote by $\overline{(A)}_w$ the closure of $A$ in the weak topology.


\begin{theorem} \label{thm2.1}
 Let $X$ be a reflexive Banach space, and $J, H: X\to\mathbb{R}$ two sequentially 
weakly lower semi-continuous functions, with $J$ continuous. Assume that there 
is $\sigma>\inf_X J$ such that the set $\overline{(J^{-1}(]-\infty,\sigma[))}_w$ 
is bounded and disconnected in the weak topology. Then, there exists $\theta>0$ 
such that, for each $\nu\in[0,\theta]$, the function $J+\nu H$ has at least two 
local minima lying in  $J^{-1}(]-\infty,\sigma[)$.
\end{theorem}

The second main tool in our argument is the zero-altitude mountain pass theorem 
for locally Lipschitz functions, due to Motreanu-Varga \cite{m2}.


\begin{theorem} \label{thm2.2}
 Let $\varphi:X\to\mathbb{R}$ be a locally Lipschitz function satisfying 
$(PS)_c$ for all $c\in\mathbb{R}$. If there exist $u_1, u_2\in X, u_1\neq u_2$ 
and $r\in(0,\|u_2-u_1\|)$ such that
$$
\inf\{\varphi(u):\|u-u_1\|=r\}\geq \max\{\varphi(u_1),\varphi(u_2)\},
$$
and we denote $\Gamma$ the family of continuous paths $\gamma:[0,1]\to X$ 
joining $u_1$ and $u_2$, then
$$
c=\inf_{\gamma\in\Gamma}\max_{s\in[0,1]}\varphi(\gamma(s))
\geq\max\{\varphi(u_1),\varphi(u_2)\}
$$
is a critical value for $E$ and $K_c\setminus\{u_1,u_2\}\neq\emptyset$.
\end{theorem}

\section{The main results}

This section is devoted to the statement  and proof of our main results.

\begin{theorem} \label{thm3.1}
 Let $(X,\|\cdot\|)$ be a reflexive Banach space, $I\in C^1(X,\mathbb{R})$ a 
sequentially weakly lower semicontinuous function, bounded on any bounded subset of $X$,
such that $I'$ is of type $(S)_+$. $\Psi,\Phi:X\to\mathbb{R}$ are two 
locally Lipschitz functions with compact gradient. Moreover, assume that 
there exists $r\in]\inf_X\Phi,\sup_X\Phi[$ such that
$$
h_1(I+\Psi,\Phi, r)<h_2(I+\Psi,\Phi, r)
$$
and that for each $\lambda\in]h_1(I+\Psi,\Phi, r),h_2(I+\Psi,\Phi, r)[$, 
the function  $I+\Psi+\lambda\Phi$ is coercive.

Then, for each compact interval 
$[a,b]\subset ]h_1(I+\Psi,\Phi, r),h_2(I+\Psi,\Phi, r)[$, there exists 
$\rho>0$ with the following property: for every $\lambda\in[a,b]$ and every 
locally Lipschitz function $H:X\to\mathbb{R}$ with compact gradient, there 
exists $\delta>0$ such that, for each $\nu\in[0,\delta],$  the function 
$I(u)+\Psi(u)+\lambda \Phi(u)+\nu H(u)$ has at least three critical points 
whose norms are less than $\rho$.
\end{theorem}

\begin{remark} \label{rmk3.1} \rm
In \cite{k2}, Krist\'aly et al. proved a non-smooth three critical points
theorem (see \cite[Theorem 2.1]{k2}).  While in our paper we improved
\cite[Theorem 2.1]{k2}. Since the inequality $h_1(I,\Phi,r)<h_2(I,\Phi,r)$
 is equivalent to
$$
\sup_{\lambda\in\Lambda}\inf_{u\in X}[I(u)+\lambda(\Phi(u)-r)]
<\inf_{u\in X}\sup_{\lambda\in\Lambda}[I(u)+\lambda(\Phi(u)-r)].
$$
\end{remark}

\begin{proof}[Proof of Theorem \ref{thm3.1}]
 Although  the proof is similar as that in \cite{r4}, our proof is based on the
non-smooth  analysis and we will see that it is more complicated to prove the 
third critical point. The difficulty  is caused by the lack of differentiability 
of the potential function $F$.   From Lemma \ref{lem2.1}, we know that a locally Lipschitz 
function with compact gradient is sequentially weakly continuous, and so in 
particular, it is bounded on each bounded subset of $X$, due to the reflexivity 
of $X$. Set $\lambda\in ]h_1(I+\Psi,\Phi, r),h_2(I+\Psi,\Phi, r)[$. 
Note that the function $I+\Psi+\lambda\Phi$ is sequentially weakly lower 
semicontinuous and coercive, and the set $\Phi^{-1}(]-\infty,r])$ is sequentially 
weakly closed, the set, denoted by $N_1$, of all global minima of the restriction 
of $I+\Psi+\lambda\Phi$ to $\Phi^{-1}(]-\infty,r])$ is nonempty. 
Fix $\tilde u\in N_1$. We assert that $\Phi(\tilde u)<r$. Proceeding by 
contradiction, assume that $\Phi(\tilde u)=r$. Since $\lambda>h_1(I+\Psi,\Phi, r)$, 
there exists $u_1\in\Phi(]-\infty,r[)$ such that
$$
\frac{I(u_1)+\Psi(u_1)-\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)}{r-\Phi(u_1)}<\lambda.
$$
Thus
$$
I(u_1)+\Psi(u_1)-\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)<\lambda(r-\Phi(u_1))
$$
and so
$$
I(u_1)+\Psi(u_1)+\lambda \Phi(u_1)<\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)+\lambda r
=I(\tilde u)+\Psi(\tilde u)+\lambda\Phi(\tilde u),
$$
which contradicts the fact $\tilde u\in N_1$. Likewise, recall  that the set 
$\Phi^{-1}([r,+\infty[)$ is sequentially weakly closed, the set of all global 
minima, denoted by $N_2$, of the restriction of $I+\Psi+\lambda\Phi$ to 
$\Phi^{-1}([r,+\infty[)$ is nonempty. Set $\hat u\in N_2$. We claim that 
$\Phi(\hat u)>r$. Proceeding by contradiction, suppose that $\Phi(\hat u)=r$. 
Since $\lambda<h_2(I+\Psi,\Phi,r)$, there exists $u_2\in\Phi^{-1}(]r,+\infty[)$ 
such that
$$
\frac{I(u_2)+\Psi(u_2)-\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)}{r-\Phi(u_2)}>\lambda.
$$
Hence
$$
I(u_2)+\Psi(u_2)-\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)<\lambda(r-\Phi(u_2))
$$
and so
$$
I(u_2)+\Psi(u_2)+\lambda\Phi(u_2)
<\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi)+\lambda r
\leq I(\hat u)+\Psi(\hat u)+\lambda\Phi(\hat u),
$$
which contradicts the fact $\hat u\in N_2$. Now, set
$$
a_\lambda=\max\Big\{\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi+\lambda\Phi),
\inf_{\Phi^{-1}([r,+\infty[)}(I+\Psi+\lambda\Phi)\Big\}.
$$
If $a_\lambda=\inf_{\Phi^{-1}(]-\infty,r])}(I+\Psi+\lambda\Phi)$, then we obtain
$$
(I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])
=N_1\cup((I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])\cap
\Phi^{-1}([r,+\infty[)).
$$
While, if $a_\lambda=\inf_{\Phi^{-1}([r,+\infty[)}(I+\Psi+\lambda\Phi)$, we derive
$$
(I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])
=N_2\cup((I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])\cap
\Phi^{-1}(]-\infty,r])).
$$
From the Eberlein-Smulian theorem, the set 
$(I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])$ is weakly compact being 
sequentially weakly compact. Furthermore, for what seen above, the same 
set turns out to be the union of two nonempty, weakly closed and disjoint sets. 
So it is disconnected in the weak topology. Now, set any compact interval 
$[a,b]\subset ]h_1(I+\Psi,\Phi, r),h_2(I+\Psi,\Phi, r)[$. 
It is obvious that the function $\lambda\to a_\lambda$ is upper semicontinuous 
in $]h_1(I+\Psi,\Phi, r),h_2(I+\Psi,\Phi, r)[$. Consequently
$$
\sigma=\sup_{\lambda\in[a,b]}a_\lambda<+\infty.
$$
We obtain
\begin{align*}
&\cup_{\lambda\in[a,b]}(I+\Psi+\lambda\Phi)^{-1}(]-\infty,\sigma+1]) \\
&=(I+\Psi+a\Phi)^{-1}
(]-\infty,\sigma+1])\cup(I+\Psi+b\Phi)^{-1}(]-\infty,\sigma+1]).
\end{align*}
Obviously, the right-hand side set is bounded and so there exists some 
$\eta>0$ such that
$$
\cup_{\lambda\in[a,b]}(I+\Psi+\lambda\Phi)^{-1}(]-\infty,\sigma+1])\subseteq B_\eta,
$$
where $B_\eta=\{u\in X:\|u\|<\eta\}$. Now, put
$$
\tilde c=\sup_{B_\eta}(I+\Psi)+\max\{|a|,|b|\}\sup_{B_\eta}|\Phi|
$$
and fix $\rho>\eta$ such that
\begin{equation}\label{e3.1a}
\cup_{\lambda\in[a,b]}(I+\Psi+\lambda\Phi)^{-1}(]-\infty,\tilde c+2])
\subseteq B_\rho.
\end{equation}
Set $H:X\to\mathbb{R}$ be a locally Lipschitz function with compact gradient. 
We choose a bounded function $g\in C^1(\mathbb{R},\mathbb{R})$, 
$g(t)\in[-M,M], g'(t)\in[0,1]$, $M>\sup_{B_\rho}|H|$ and $g(t)=t$ for all 
$t\in[-\sup_{B_\rho}|H|,\sup_{B_\rho}|H|]$. Let
$$
\tilde H(u)=g(H(u))\quad\text{for all }u\in X.
$$
Clearly $\tilde H:X\to\mathbb{R}$ is a locally Lipschitz function and 
$\tilde H(u)=H(u)$ for all $u\in B_\rho$. From the chain rule, we obtain
$$
\partial \tilde H(u)\subseteq g'(H(u))\partial H(u)
$$
for all $u\in X$.
Now we show that $\partial \tilde H(u):X\to 2^{X^*}$ is a compact set-valued mapping.
 Let $\{u_n\}$ be a bounded sequence in $X$ and $u^*_n\in\partial \tilde H(u_n)$ 
for every $n\in\mathbb{N}$. Then there exists a sequence $\{w^*_n\}$ in $X^*$ 
such that for all $n\in\mathbb{N}$ we have $w^*_n\in\partial H(u_n)$ and
$$
u^*_n=g'(H(u_n))w^*_n.
$$
Note that $\partial H(u)$ is compact. Passing to a subsequence, we have 
$w^*_n\to w^*\in X^*$ and $g'(H(u_n))\to d\in[0,1]$ (from Bolzano-Weirstrass theorem).
 Hence $u^*_n\to dw^*$. Fix $\lambda\in [a,b]$. Recall that there exists
 $c_\lambda\in]a_\lambda,a_\lambda+1[$ such that the set 
$\overline{((I+\Psi+\lambda\Phi)^{-1}(]-\infty,c_\lambda[)_\omega}$ 
is disconnected in the weak topology. Indeed, otherwise for any decreasing 
sequence $\{a_n\}$ in $]a_\lambda,a_\lambda+1[$ with 
$\lim_{n\to\infty}a_n=a_\lambda$, from Lemma \ref{lem2.1} we have  that the function 
$I+\Psi+\lambda \Phi$ is weakly lower semicontinuous. Then, we obtain
$$
(I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_\lambda])=\cap_{n\in\mathbb{N}}
\overline{((I+\Psi+\lambda\Phi)^{-1}(]-\infty,a_n[))_\omega}
$$
and so the set on the left-hand side would be connected in the weak topology, 
contrary to what seen  above. Hence, we can use Theorem \ref{thm2.1}
 to obtain $\theta>0$ 
such that for each $\nu\in[0,\theta]$ the function $I+\Psi+\lambda\Phi+\nu\tilde H$ 
has at least two local minima, denoted by $u_1, u_2$, lying in $B_\eta$. 
Further, put
$$
\delta=\min\big\{\theta,\frac{1}{M}\big\}
$$
and choose $\nu\in[0,\delta]$, we will prove that the function
$$
\phi=I+\Psi+\lambda\Phi+\nu\tilde H
$$
possesses at least three critical points lying in $B_\rho$. 
With this aim in mind, we show that $\phi$ satisfies the non-smooth $(PS)_c$. 
Let $\{u_n\}$ be a sequence in $X, \forall y\in X$, such that
\begin{gather}\label{e3.1}
\phi(u_n)\to c, \\
\label{e3.2}
\phi^\circ(u_n)(u_n;y-u_n)+\varepsilon_n\|y-u_n\|\geq 0
\end{gather}
with $\varepsilon_n\to 0$ and $n\to\infty.$ Observe that $\tilde H$ is bounded, 
i.e.,
\begin{equation}\label{e3.2a}
\sup_{u\in X}|\tilde H(u)|\leq M.
\end{equation}
Note that $I+\Psi+\lambda\Phi$ is coercive. It follows  that $\phi$ 
is also coercive from \eqref{e3.2a}. Then $\{u_n\}$ is a bounded sequence.
Passing to a subsequence, we have $u_n\rightharpoonup u\in X$.
 Put $R>0$ such that 
$$
\|u_n-u\|\leq R
$$
for all $n\in\mathbb{N}$. Chose
 sequences $\{\xi^1_n\}$, $\{\xi^2_n\}$, $\{\xi^3_n\}$ in $X^*$ such that 
$\xi^1_n\in\partial\Psi(x,u_n)$, $\xi^2_n\in\partial\Phi(x,u_n)$, 
$\xi^3_n\in\partial\tilde H(x,u_n)$ and
\begin{gather*}
\Psi^\circ(u_n;u-u_n)=\langle\xi^1_n,u-u_n\rangle,\quad
\Phi^\circ(u_n;u-u_n)=\langle\xi^2_n,u -u_n\rangle,\\
\tilde H^\circ(u_n;u-u_n)=\langle\xi^3_n,u-u_n\rangle.
\end{gather*}
From the compactness of $\partial\Psi$, $\partial\Phi$ and $\partial\tilde H$, 
up to a subsequence, we have $\xi^1_n\to\xi^1\in X^*$,  
$\xi^2_n\to\xi^2\in X^*$ and $\xi^3_n\to\xi^3\in X^*$. 
By \eqref{e3.2}, we obtain
\begin{equation}\label{e3.3}
\begin{aligned}
&\langle I'(u_n),u-u_n\rangle +\Psi^\circ(u_n,u-u_n)
 +\lambda\Phi^\circ(u_n,u-u_n)\\
&+\nu\tilde H^\circ(u_n,u-u_n)+\varepsilon_n\|u-u_n\|\geq 0.
\end{aligned}
\end{equation}
Fix $\varepsilon >0$. From what was stated above, we have
$$\aligned
&\|\xi^1_n-\xi^1\|_*<\frac{\varepsilon}{5R}, ~~\|\xi^2_n-\xi^2\|_*<\frac{\varepsilon}{5\lambda R}, ~~
\|\xi^3_n-\xi^3\|_*<\frac{\varepsilon}{5\nu R}\\
&\varepsilon_n<\frac{\varepsilon}{5R}, ~~\langle\xi^1+\lambda\xi^2+\nu\xi^3,u-u_n\rangle
<\frac{\varepsilon}{5R}
\endaligned$$
for $n\in\mathbb{N}$ big enough.
Then, by virtue of \eqref{e3.3} we can obtain
$$
\langle I'(u_n),u_n-u\rangle<\varepsilon
$$
for $n$ large enough. This means that
$$
\limsup_n\langle I'(u_n),u_n-u\rangle\leq 0.
$$
Recall that $I'$ is of type $(S)_+$. So $u_n\to u$ in $X$;
 i.e., $\phi$ satisfies the non-smooth $(PS)_c$. 
Since $u_1, u_2$ are local minima  of $\phi$ we  apply Theorem \ref{thm2.2} 
to obtain 
$$
c_{\lambda,\nu}=\inf_{\gamma\in\Gamma}\max_{s\in[0,1]}\phi(\gamma(s))
\geq\max\{\phi(u_1),\phi(u_2)\}
$$
is a critical value of $\phi$, where $\Gamma$ is the family of continuous 
paths $\gamma:[0,1]\to X$ combining $u_1$ and $u_2$. Hence, there exists
 $u_3\in X$ such that
$$
c_{\lambda,\nu}=\phi(u_3)\quad\text{and}\quad 0\in\partial\phi(u_3).
$$
If we consider the path $\gamma\in\Gamma$, given by 
$\gamma(s)=u_1+s(u_2-u_1)\subset B_\eta$, then  we have
\begin{align*}
c_{\lambda,\nu}
&\leq\sup_{s\in[0,1]}(I(\gamma(s))+\Psi(\gamma(s))
 +\lambda\Phi(\gamma(s))+\nu\tilde H(\gamma(s)))\\
&\leq\sup_{B_\eta}(I+\Psi)+\max\{|a|,|b|\}\sup_{B_\eta}|\Phi|
 +\delta \sup_{u\in X}|\tilde H|\\
&\leq\tilde c+1.
\end{align*} 
Consequently, we derive
$$
I(u_3)+\Psi(u_3)+\lambda\Phi(u_3)\leq\tilde c+2.
$$
From \eqref{e3.1a} we have $u_3\in B_\rho$. Therefore,
$u_i$ $(i=1,2,3)$ are critical points for $\phi$, all belong to the ball $B_\rho$. 
It remains to prove that these elements are critical points not only for $\phi$, 
but also for $E=I(u)+\Psi(u)+\lambda\Phi(u)+\nu H(u)$ (removing the truncation). 
For every $u_i\in X$, there exists $\xi^3_i\in\partial H(u_i)$ such that
$$
H^\circ(u_i;u-u_i)=\langle g'(H(u_i))\xi_i^3,u-u_i\rangle
=\langle \xi_i^3,u-u_i\rangle
$$
(since $|g(u_i)|\leq \sup_{B_\rho}|H|$ and $g'(H(u_i))=1$). So
\begin{align*}
0
&\leq\langle I'(u_i),u-u_i\rangle+\Psi^\circ(u_i,u-u_i)
 +\lambda\Phi^\circ(u_i,u-u_i)+\nu\tilde H^\circ (u_i,u-u_i)\\
&=\langle I'(u_i),u-u_i\rangle+\Psi^\circ(u_i,u-u_i)
 +\lambda\Phi^\circ(u_i,u-u_i)+\nu\langle \xi_i^3,u-u_i\rangle\\
&\leq\langle I'(u_i),u-u_i\rangle+\Psi^\circ(u_i,u-u_i)
 +\lambda\Phi^\circ(u_i,u-u_i)+\nu H^\circ (u_i,u-u_i).
\end{align*}
This completes the proof.
\end{proof}

Let us recall \cite[Theorem 2]{r4}, where $h_1=0$ and $h_2>0$.

\begin{theorem} \label{thm3.2}
Let $X$ be a topological space and $I, \Psi, \Phi:X\to\mathbb{R}$ 
be three sequentially lower semicontinuous functions, with $I$ also 
sequentially inf-compact, satisfying the following conditions:
\begin{itemize}
\item[(i)] $\inf_{u\in X}(\mu I(u)+\Psi(u))=-\infty$ for all $\mu>0$;

\item[(ii)]  $\inf_{u\in X}(\Psi(u)+\Phi(u))>-\infty$;

\item[(iii)] there exists $r\in ]\inf_X\Phi,\sup_X\Phi[$ such that
$$
\inf_{u\in\Phi^{-1}(]-\infty,r])}I(u)<\inf_{u\in \Phi^{-1}(r)}I(u).
$$
\end{itemize}

Under such hypotheses, for each $\mu>\max\{0,h_3(I,\Psi,\Phi,r)\}$, one has
$$
h_1(\mu I+\Psi,\Phi,r)=0, \quad 
h_2(\mu I+\Psi,\Phi,r)>0.
$$
\end{theorem}

Based on Theorems \ref{thm3.1} and \ref{thm3.2}, we have the following result.

\begin{theorem} \label{thm3.3}
 Let $(X,\|\cdot\|)$ be a reflexive Banach space, $I\in C^1(X,\mathbb{R})$ 
a sequentially weakly lower semicontinuous function, bounded on any bounded 
subset of $X$,  such that $I'$ is of type $(S)_+$. 
$\Psi$ and $\Phi:X\to\mathbb{R}$ are two locally Lipschitz functions with 
compact gradient. Assume also that the function $\Psi+\lambda\Phi$ is 
bounded below for all $\lambda>0$ and that
\begin{equation}\label{e3.4}
\liminf_{\|u\|\to +\infty}\frac{\Psi(u)}{I(u)}=-\infty.
\end{equation}
Then, for each $r>\sup_N\Phi$, where $N$ is the set of all global minima of $I$, 
for each $\mu>\max\{0,h_3(I,\Psi,\Phi,r)\}$ and each compact interval 
$[a,b]\subset]0, h_2(\mu I+\Psi,\Phi,r)[$, there exists a number $\rho>0$ 
with the following property: for every $\lambda\in[a,b]$ and every locally 
Lipschitz function $H:X\to\mathbb{R}$ with compact gradient, there exists 
$\delta>0$ such that, for each $\nu\in [0,\delta]$, the function 
$\mu I(u)+\Psi(u)+\lambda \Phi(u)+\nu H(u)$ has at least three critical points 
in $X$ whose norms are less than $\rho$.
\end{theorem}

\begin{proof} 
It is obvious that \eqref{e3.4} is equivalent to the fact that the function
$\mu I+\Psi$ is unbounded below for all $\mu>0$. Likewise it is obvious 
that $\sup_X\Phi=+\infty$. Clearly, our hypotheses mean that $N$ is non-empty 
and bounded. As a consequence, $\Phi$ is bounded in $N$. Set $r>\sup_N\Phi$. 
Note  that $\Phi^{-1}(r)$ is non-empty and sequentially weakly closed. 
Then there exists $\bar u\in \Phi^{-1}(r)$ such that
$$
I(\bar{u})=\inf_{u\in\Phi^{-1}(r)}I(u).
$$
The choice of $r$ means that $\bar u\not\in N$. So we deduce that
$$
\inf_{u\in\Phi^{-1}(]-\infty,r])}I(u)<\inf_{u\in\Phi^{-1}(r)}I(u).
$$
If we endow $X$ with the weak topology, all the hypotheses of Theorem \ref{thm3.2} 
are satisfied, and the conclusion can be deduced  from Theorem \ref{thm3.1}.
\end{proof}

\section{Application}

In this section, we will apply Theorem \ref{thm3.3} to obtain the existence and 
multiplicity of solutions for the following $p(x)-$Laplacian differential 
inclusion.
\begin{equation}\label{e4.1}
 \begin{gathered}
-\operatorname{div}(|\nabla u|^{p(x)-2}\nabla u)
+|u|^{p(x)-2}u\in\epsilon\partial F(x,u)-\lambda
\partial G(x,u)+\nu \partial K(x,u)\\
\text{for a. a. } x\in\Omega,\\
u|_{\partial\Omega}=0,
\end{gathered}
\end{equation}
where $\Omega$ is a bounded set in $\mathbb{R}^N$, $p(x)>1$, 
$p(x)\in C(\bar\Omega)$, 
$\partial F(x,\cdot)(\partial G(x,\cdot), \partial K(x,\cdot))$ 
is the Clarke sub-differential of $F(x,\cdot)(G(x,\cdot), K(x,\cdot))$.

Let $X=W^{1,p(x)}_0(\Omega)$, and define 
$I(u),\Psi(u),\Phi(u),H(u):X\mapsto \mathbb{R}$ by
\begin{gather*}
I(u)=\int_\Omega \frac{1}{p(x)}|\nabla u|^{p(x)}{\rm d}x
 +\int_\Omega \frac{1}{p(x)}|u|^{p(x)}{\rm d}x, \quad
\Psi(u)=-\mathscr{F}(u),\\ 
\mathscr{F}(u)=\int_\Omega F(x,u){\rm d}x, \quad
\Phi(u)=\int_\Omega G(x,u){\rm d}x, \quad
H(u)=\int_\Omega K(x,u){\rm d}x
\end{gather*}
for all $u\in X$. For each $r\in]\inf_X\Phi,\sup_X\Phi[$, set
$$
h_3^*(I,\Psi,\Phi,r)
=\inf\Big\{\frac{\Psi(u)-\hat\gamma+r}{\hat\eta_r-I(u)}:
u\in X,\Phi(u)<r,I(u)<\hat\eta_r\Big\},
$$
where
$$
\hat\gamma=\int_\Omega \inf_{u\in\mathbb{R}}(G(x,u)-F(x,u)){\rm d}x, \quad
\hat\eta_r=\inf_{u\in\Phi^{-1}(r)}I(u).
$$
For each $\epsilon\in\big]0,\frac{1}{\max\{0,h_3^*(I,\Psi,\Phi,r)\}}\big[$, let
$$
h_2^*(I+\Psi,\Phi,r)=\sup_{u\in\Phi^{-1}(]r,+\infty[)}\frac{I(u)
+\epsilon \Psi(u)-\inf_{\Phi^{-1}(]-\infty,r])}(I+\epsilon \Psi)}{r-\Phi(u)}.
$$
To discuss problem  \eqref{e4.1}, we need the following hypotheses:
\begin{itemize}
\item[(F1)] for all $u\in\mathbb{R}$, $\Omega\ni x\mapsto F(x,u)$ is measurable;

\item[(F2)] for a.a. $x\in\Omega$, $\mathbb{R}\ni u\mapsto F(x,u)$ 
is locally Lipschitz;

\item[(F3)] $|\xi^1|\leq k_1(1+|u|^{q_1(x)-1})$ for a.a. $x\in\Omega$ 
and every $u\in\mathbb{R}$, $\xi^1\in\partial F(x,u)$ $(k_1>0, p(x)<q_1(x)<p^*(x))$;

\item[(F4)]
$$
\lim_{|u|\to+\infty}\frac{\inf_{x\in\Omega}F(x,u)}{u^{p^+}}=+\infty~{\rm and}~
\lim_{|u|\to+\infty}\frac{\sup_{x\in\Omega}F(x,u)}{|u|^{\alpha^-}}<+\infty,
$$
where $p^+<\alpha^-\leq\alpha^+<p^*(x)$;

\item[(G1)] for all $u\in\mathbb{R}$, $\Omega\ni x\mapsto G(x,u)$ is measurable;

\item[(G2)] for a.a.  $x\in\Omega$, $\mathbb{R}\ni u\mapsto G(x,u)$ is locally Lipschitz;

\item[(G3)] $|\xi^2|\leq k_2(1+|u|^{q_2(x)-1})$ for a.a. $x\in\Omega$ and every $u\in\mathbb{R}$, $\xi^2\in\partial G(x,u)$ $(k_2>0, p(x)<q_2(x)<p^*(x))$;

\item[(G4)]
$$
\lim_{|u|\to+\infty}\frac{\inf_{x\in\Omega}G(x,u)}{|u|^{\alpha^+}}=+\infty,
$$
where $p^+<\alpha^-\leq\alpha^+<p^*(x)$;

\item[(K1)] for all $u\in\mathbb{R}$, $\Omega\ni x\mapsto K(x,u)$ is measurable;

\item[(K2)] for a.a.  $x\in\Omega$, $\mathbb{R}\ni u\mapsto K(x,u)$ 
is locally Lipschitz;

\item[(K3)] $|\xi^3|\leq k_3(1+|u|^{q_3(x)-1})$ for a.a. $x\in\Omega$ 
and every $u\in\mathbb{R}$, $\xi^3\in\partial K(x,u)$ $(k_3>0, p(x)<q_3(x)<p^*(x))$.

\end{itemize}


\begin{definition} \label{def4.1} \rm
We say that $u\in X$ is a solution of  problem  \eqref{e4.1} if there exist
$\xi^1\in\partial F(x,u)$, $\xi^2\in\partial G(x,u)$ and 
$\xi^3\in\partial K(x,u)$ for a.a. $x\in\Omega$ such that for all $v\in X$ we have
\begin{align*}
&\int_\Omega|\nabla u|^{p(x)-2}\nabla u\cdot\nabla v{\rm d}x
 +\int_\Omega| u|^{p(x)-2}u\cdot  v{\rm d}x\\
&-\epsilon\int_\Omega \xi^1 v{\rm d}x
 +\lambda \int_\Omega \xi^2 v{\rm d}x
 -\nu \int_\Omega\xi^3 v{\rm d}x=0.
\end{align*}
\end{definition}

The proof of the following lemma can be found in \cite{f1,f3}.

\begin{lemma} \label{lem4.1}
$I\in C^1(X,\mathbb{R})$ and its gradient, defined for every $u,v\in X$ by
$$
\langle I'(u),v\rangle=\int_\Omega(|\nabla u|^{p(x)-2}
\nabla u\cdot\nabla v+|u|^{p(x)-2} u\cdot v){\rm d}x,
$$
is of type $(S)_+$.
\end{lemma}

The next lemma displays some properties of $\mathscr{F}(u)$.

\begin{lemma} \label{lem4.2}
 If hypotheses {\rm (F1)--(F3)} hold, then $\mathscr{F}:X\to \mathbb{R}$ 
is a locally Lipschitz function with compact gradient.
\end{lemma}

\begin{proof} 
We firstly  prove that $\mathscr{F}$ is locally Lipschitz. 
Let $u,v\in X$. Apply the Lebourg's mean value theorem, Proposition \ref{prop2.1} 
and the Holder inequality to obtain
\begin{align*}
&|\mathscr{F}(u)-\mathscr{F}(v)|\\
&\leq \int_\Omega|F(x,u(x))-F(x,v(x))|{\rm d}x\\
&\leq \int_\Omega k_1(1+|u(x)|^{q_1(x)-1}+1+|v(x)|^{q_1(x)-1})|u(x)-v(x)|{\rm d}x\\
&\leq k_1C|u-v|_{p(x)}
 +k_1(|u|^{q_1^--1}_{q_1(x)}+|u|^{q_1^+-1}_{q_1(x)}+|v|^{q_1^--1}_{q_1(x)}
 +|v|^{q_1^+-1}_{q_1(x)})|u-v|_{q_1(x)}\\
&\leq k_1 C\|u-v\|+k_1C(\|u\|^{q_1^--1}+\|u\|^{q_1^+-1}+\|v\|^{q_1^--1}
 +\|v\|^{q_1^+-1})\|u-v\|.
\end{align*}
From the above computation, it is obvious that $\mathscr{F}$ is locally Lipschitz.

Now, we prove that $\partial \mathscr{F}$ is compact. 
Choosing $u\in X$, $u^*\in\partial\mathscr{F}(u)$, we obtain for every $v\in X$
\begin{equation}\label{e4.2a}
\langle u^*,v\rangle\leq\mathscr{F}^\circ(u;v)
\end{equation}
and $\mathscr{F}^\circ(u;\cdot):L^r(\Omega)\to\mathbb{R}$ is a subadditive 
function (see Proposition \ref{prop2.4}). Furthermore, $u^*\in X^*$ is continuous 
also with respect to the topology induced on $X$ by the norm $|\cdot|_r$. 
Indeed, setting $L>0$ a Lipschitz constant for $\mathscr{F}$ in a neighborhood 
of $u$, for all $z\in X$  from Proposition \ref{prop2.4} (ii) we obtain
$$
\langle u^*,z\rangle\leq L|z|_r, ~~~~\langle u^*,-z\rangle\leq L|-z|_r.
$$
So
$$
\langle u^*,z\rangle\leq L|z|_r.
$$
Hence, from the Hahn-Banach Theorem, $u^*$ can be extended to an element 
of the dual $L^r(\Omega)$ (complying with \eqref{e4.2a}) for every
$v\in L^r(\Omega)$, this means that we can represent $u^*$ as an element of 
$L^{r'}(\Omega)$ and write for every $v\in L^r(\Omega)$
\begin{equation}\label{e4.2b}
\langle u^*,v\rangle=\int_\Omega u^*(x)v(x){\rm d}x.
\end{equation}
Set $\{u_n\}$ be a sequence in $X$ such that $\|u_n\|\leq M$ for all 
$n\in\mathbb{N}$ $(M>0)$ and take $u^*_{F_n}\in \partial\mathscr{F}(u_n)$ for all  
$n\in\mathbb{N}$. From  $(F_3)$ and \eqref{e4.2b}  we have
\begin{align*}
\langle u^*_{F_n},v\rangle
&=\int_\Omega u^*_{F_n}v(x){\rm d}x\leq \int_\Omega |u^*_{F_n}||v(x)|{\rm d}x\\
&\leq \int_\Omega k_1(1+|u_n(x)|^{q_1(x)-1})|v(x)|{\rm d}x\\
&\leq k_1 C(1+\|u_n\|^{q_1^+-1}+\|u_n\|^{q^-_1-1})\|v\|\\
&\leq k_1C(1+M^{q_1^+-1}+M^{q^-_1-1})\|v\|
\end{align*}
for all  $n\in\mathbb{N}$, $u\in X$.
Hence
$$
\|u^*_{F_n}\|_{X^*}\leq k_1C(1+M^{q_1^+-1}+M^{q^-_1-1}),
$$
i.e., the sequence $\{u^*_{F_n}\}$ is bounded. 
So, passing to a subsequence, we have $u^*_{F_n}\rightharpoonup u^*_{F}\in X^*$. 
We will prove that $\{u^*_{F_n}\}\subset X^*$ has a strong convergence. 
We proceed by contradiction. Assume that there exists some $\varepsilon>0$ 
such that
$$
\|u^*_{F_n}-u^*_{F}\|_{X^*}>\varepsilon
$$
for all $n\in\mathbb{N}$
and hence for all $n\in\mathbb{N}$ there is a $v_n\in B(0,1)$ such that
\begin{equation}\label{e4.3}
\langle u^*_{F_n}-u^*_{F},v_n\rangle>\varepsilon.
\end{equation}
Noting that $\{v_n\}$ is a bounded sequence and passing to a subsequence, one has
$$
v_n\rightharpoonup v\in X, \quad |v_n-v|_{p(x)}\to 0,\quad
|v_n-v|_{q_1(x)}\to 0.
$$
So, for $n$ big enough, we have
\begin{gather*}
|\langle u^*_{F_n}-u^*_{F},v\rangle|<\frac{\varepsilon}{4}, \quad
|\langle  u^*_{F},v_n-v\rangle|<\frac{\varepsilon}{4},\\
|v_n-v|_{p(x)}<\frac{\varepsilon}{4k_1C}, \quad
|v_n-v|_{q_1(x)}<\frac{\varepsilon}{4k_1C(M^{q^+-1}+M^{q^--1})}.
\end{gather*}
Then
\begin{align*}
\langle u^*_{F_n}-u^*_{F},v_n\rangle
&=\langle u^*_{F_n}-u^*_{F},v\rangle+\langle u^*_{F_n},v_n-v\rangle
 -\langle u^*_{F},v_n-v\rangle\\
&\leq\frac{\varepsilon}{2}+\int_\Omega |u^*_{F_n}||v_n(x)-v(x)|{\rm d}x\\
&\leq \frac{\varepsilon}{2}+k_1\int_\Omega (1+|u_n|^{q_1(x)-1})|v_n(x)-v(x)|{\rm d}x\\
&\leq \frac{\varepsilon}{2}+k_1C|v_n-v|_{p(x)}+k_1 (|u_n|^{q_1^+-1}_{q_1(x)}
 +|u_n|^{q_1^--1}_{q_1(x)})|v_n-v|_{q_1(x)}\\
&\leq \frac{\varepsilon}{2}+k_1C|v_n-v|_{p(x)}+k_1 C (M^{q_1^+-1}
 +M^{q_1^--1})|v_n-v|_{q_1(x)}
\leq \varepsilon,
\end{align*}
which contradicts to \eqref{e4.3}.
\end{proof}

Analogously, we can obtain the following properties of the functions 
$\Phi(u)$ and $H(u)$.

\begin{lemma} \label{lem4.3}
If {\rm (G1)--(G3), (K1)--(K3)} hold, then $\Phi(u)$, $H(u):X\to\mathbb{R}$ 
are locally Lipschitz functions with compact gradient.
\end{lemma}

Now we state our main results.

\begin{theorem} \label{thm4.1}
 If {\rm (F1)--(F4), (G1)--(G4), (K1)--(K3)} hold, then for all $r>0$, 
$\epsilon\in\big]0,\frac{1}{\max\{0,h^*_3(I,\Psi,\Phi,r)\}}\big[$ and all 
compact interval $[a,b]\subset ]0,h^*_2(I+\Psi,\Phi,r)[$, there exist numbers 
$\rho>0$ and $\delta>0$  such that for all $\lambda\in[a,b]$ and all 
$\nu\in[0,\delta]$, problem \eqref{e4.1} has at least three weak solutions
whose norms in $X$ are less than $\rho$.
\end{theorem}

Contrary to  most of the known results, we do not make any hypothesis on 
the behavior of the involved nonlinearities at the origin in Theorem \ref{thm4.1}. 
So our results are more interesting.

\begin{proof}[Proof of Theorem \ref{thm4.1}]
We  use Theorem \ref{thm3.3} in this proof. We observe that $X$ is a reflexive Banach space, 
$I\in C^1(X,\mathbb{R})$ is continuous and convex, and hence weakly 
lower semicontinuous and obviously bounded on any bounded subset of $X$. 
From Lemma \ref{lem4.1}, $I'$ is of type $(S_+)$. Furthermore,  it follows from 
Lemmas \ref{lem4.2} and \ref{lem4.3} that $\Phi, \Psi$ and $H$ are locally Lipschitz 
functions with compact gradient. So we only need to prove that the function 
$\Psi+\lambda\Phi$ is bounded below for all $\lambda>0$ and  
$\liminf_{\|u\|\to +\infty}\frac{\Psi(u)}{I(u)}=-\infty$. 
We firstly prove that $\Psi+\lambda\Phi$ is bounded below for all $\lambda>0$. 
By  (F3) and (F4) there exists a constant $c_1>0$ such that
\begin{equation}\label{e4.4}
F(x,u)\leq c_1(1+|u|^{\alpha(x)})
\end{equation}
for a.a. $x\in\Omega$. Moreover, from (G3) and (G4), we also have that for 
all $c_2>0$ there exists a constant $c_3>0$ such that
\begin{equation}\label{e4.5}
G(x,u)\geq c_2|u|^{\alpha(x)}-c_3
\end{equation}
for a.a. $x\in\Omega$. From \eqref{e4.4} and \eqref{e4.5}, noting that
$\lambda>0$ and  choosing $c_2>\frac{c_1}{\lambda}$ we obtain that
\begin{align*}
\Psi+\lambda\Phi
&=\int_\Omega[\lambda G(x,u)-F(x,u)]{\rm d}x\\
&\geq\int_\Omega[\lambda(c_2|u|^{\alpha(x)}-c_3)-c_1(1+|u|^{\alpha(x)})]{\rm d}x\\
&=\int_\Omega[(\lambda c_2-c_1)|u|^{\alpha(x)}-\lambda c_3-c_1]{\rm d}x
\to+\infty\quad\text{as }|u|\to+\infty,
\end{align*}
which means that $\Psi+\lambda\Phi$ is bounded below.

Next, we prove that
\begin{equation}\label{e4.5a}
\liminf_{\|u\|\to +\infty}\frac{\Psi(u)}{I(u)}=-\infty.
\end{equation}
From \cite{a1} we can find a $\beta>0$ and a function $\theta(x)\in X$,
positive in $\Omega$, such that
$$
\int_\Omega(|\nabla u|^{p(x)}+| u|^{p(x)}){\rm d}x
=\beta \int_\Omega|\theta(x)|^{p(x)}{\rm d}x.
$$
To obtain \eqref{e4.5a}, it is sufficient to show that
\begin{equation}\label{e4.6}
\lim_{k\to +\infty}\frac{\mathscr{F}(k\theta)}{I(k\theta)}=+\infty.
\end{equation}
For this purpose, let us fix two numbers $M_1, M_2$ with $0<2M_1<M_2$. 
From (F4), there exists a large constant $m_1>0$. When $|u|>m_1$ we have
$$
F(x,u)\geq M_2c_3u^{p^+}
$$
for a.a. $x\in\Omega$,
where $c_3=\frac{\beta\max\{|\theta|^{p^+}_{p(x)},|
\theta|^{p^-}_{p(x)}\}}{|\theta|^{p^+}_{p^+}}$. For each $k\in\mathbb{N}$, put
$$
\Omega_k=\big\{x\in\Omega:\theta(x)\geq\frac{m_1}{k}\big\}.
$$
It is obvious that the sequence $\{\int_{\Omega_k}|\theta(x)|^{p^+}{\rm d}x\}$ 
is non-decreasing and converges to $\int_{\Omega}|\theta(x)|^{p^+}{\rm d}x$. 
Set $\hat k\in\mathbb{N}$ such  that
$$
\int_{\Omega_{\hat k}}|\theta(x)|^{p^+}{\rm d}x
>\frac{2M_1}{M_2}\int_{\Omega}|\theta(x)|^{p^+}{\rm d}x.
$$
From (F1)--(F3), there is a constant $c_4>0$ such that
$$
\sup_{\Omega\times[0,m_1]}|F(x,u)|<c_4.
$$
For all $k\in\mathbb{N}$ satisfying
$$
k>\max\Big\{\hat k,\Big(\frac{|\Omega|\sup_{\Omega\times[0,m_1]}|F(x,u)|}
{M_1\min\{|\theta(x)|^{p^+}_{p(x)},|\theta(x)|^{p^-}_{p(x)}\}}
\Big)^{\frac{1}{p^+}}\Big\},
$$
we obtain
\begin{align*}
&\lim_{k\to +\infty}\frac{\mathscr{F}(k\theta)}{I(k\theta)}\\
&=\lim_{k\to +\infty}\frac{\int_{\Omega_{ k}}F(x,k\theta(x)){\rm d}x
 +\int_{\Omega\setminus\Omega_{ k}}F(x,k\theta(x)){\rm d}x}{I(k\theta)}\\
&\geq \lim_{k\to +\infty}\frac{k^{p^+}M_2c_3
 \int_{\Omega_{ k}}|\theta(x)|^{p^+} {\rm d}x
 +\int_{\Omega\setminus\Omega_{ k}}F(x,k\theta(x)){\rm d}x}{k^{p^+}
 \beta \int_{\Omega}|\theta(x)|^{p(x)}{\rm d}x}\\
&\geq\frac{2M_1c_3\int_{\Omega}|\theta(x)|^{p^+}{\rm d}x}
 {\beta\max\{|\theta(x)|^{p^+}_{p(x)},|\theta(x)|^{p^-}_{p(x)}\}}
 +\lim_{k\to +\infty}\frac{\int_{\Omega\setminus\Omega_{ k}}
 F(x,k\theta(x)){\rm d}x}{k^{p^+}\beta \int_{\Omega}|\theta(x)|^{p(x)}{\rm d}x}\\
&\geq \frac{2M_1c_3|\theta(x)|^{p^+}_{p^+}}{\beta\max\{|\theta(x)|^{p^+}_{p(x)},
 |\theta(x)|^{p^-}_{p(x)}\}}-\lim_{k\to +\infty}
 \frac{|\Omega|\sup_{\Omega\times[0,m_1]} |F(x,k\theta(x))|}{k^{p^+}
 \beta \min\{|\theta(x)|^{p^+}_{p(x)},|\theta(x)|^{p^-}_{p(x)}\}}\\
&\geq 2M_1-M_1=M_1\to+\infty~~(\rm as~M_1\to+\infty).
\end{align*}
Hence,  the proof is complete.
\end{proof}

\subsection*{Acknowledgments}
This research was supported by the National Natural Science
 Foundation of China (11371127).
We want to thanks Professor Ricceri for his valuable guidance. 
The authors would like to thank the  editor and the reviewer for their
 valuable comments and constructive suggestions, which help  to improve 
the presentation of this article.

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\end{document}
