\documentclass[reqno]{amsart}
\usepackage{hyperref}

\AtBeginDocument{{\noindent\small
\emph{Electronic Journal of Differential Equations},
Vol. 2011 (2011), No. 12, pp. 1--9.\newline
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu}
\thanks{\copyright 2011 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2011/12\hfil Existence of positive solutions]
{Existence of positive solutions for some
nonlinear elliptic systems on the half space}

\author[N. Zeddini\hfil EJDE-2011/12\hfilneg]
{Noureddine Zeddini}

\address{Noureddine Zeddini \newline
Department of Mathematics, College of Sciences and Arts\\
King Abdulaziz University,
P.O. Box 344. Rabigh 21911, Saudi Arabia.\newline
D\'epartement de Math\'ematiques,
Facult\'e des Sciences de Tunis,
Campus Universitaire, 2092 Tunis, Tunisia}
\email{noureddine.zeddini@ipein.rnu.tn}

\thanks{Submitted March 16, 2010. Published January 21, 2011.}
\subjclass[2000]{35J55, 35J60, 35J65}
\keywords{Green function; Kato class; elliptic systems;
 positive solutions}

\begin{abstract}
 We prove some existence of positive solutions to the semilinear
 elliptic system
 \begin{gather*}
 \Delta u =\lambda p(x)g(v)\\
 \Delta v =\mu q(x)f(u)
 \end{gather*}
 in the half space ${\mathbb{R}}^n_+$, $n\geq 2$,  subject to some
 Dirichlet conditions, where $\lambda$ and $\mu$ are nonnegative
 parameters. The functions $f, g$ are nonnegative continuous
 monotone on $(0,\infty)$ and the potentials  $p, q$ are nonnegative
 and satisfy some hypotheses related to the Kato class
 $K^\infty({\mathbb{R}}^n_+)$.
\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{corollary}[theorem]{Corollary}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{definition}[theorem]{Definition}

\section{Introduction}

The existence and nonexistence of solutions for semilinear elliptic
systems  have received much attention recently. Most of the studies
are about  existence and  nonexistence of positive radial solutions
\cite{CR1,LW1}.

In \cite{CR1}, the authors consider the system
\begin{equation} \label{S0}
\begin{gathered}
\Delta u = p ( x) g(v),\\
\Delta v = q (x) f(u)  \quad  x\in {\mathbb{R}}^n ,
\end{gathered}
\end{equation}
where $f, g$ are positive and nondecreasing functions on
$(0,\infty)$ and $p,q$ are nonnegative locally holder and radially
symmetric functions in ${\mathbb{R}}^n$, $n\geq 2$. They established
the existence of positive entire solutions for \eqref{S0} provided
that $\lim_{t\to \infty} g(cf(t))/t=0$
 for all $c>0$. Moreover,
they proved that if
$$
\int_0^{\infty}t p(t)\,dt=\int_0^{\infty}t q(t)\,dt=\infty ,
$$
then all positive entire radial solutions of \eqref{S0} blow-up at
infinity. However, if $p$ and $q$ satisfy the following condition
$$
\int_0^{\infty}t [p(t)+q(t)]\,dt<\infty ,
$$
then all positive entire radial solutions of \eqref{S0} are bounded.

In \cite{LW1}, the authors studied the system \eqref{S0}
when $f(u)=u^{\beta}$, $g(v)=v^{\alpha}$, $\alpha>0$, $\beta>0$ and
$p$, $q$ are nonnegative continuous and not necessarily radial. They
showed that entire positive bounded solutions exist if $p$ and $q$
satisfy at infinity the following decay condition
$$
p(x) + q(x) \leq C  |x|^{-(2+\delta)}
$$
for  some positive  constant $\delta$.

In \cite{GMTZ}, we were interested in the existence of positive
bounded solution for \eqref{S0} in some domains with compact
boundary in the case where $f$ and $g$ are monotone on $(0,\infty)$
and $p,q$ satisfy some hypotheses related to the Kato class
associated to these domains.
Our aim in this paper is to establish the existence of positive
bounded and unbounded continuous solutions for a domain
with non compact boundary which are parallel to those
established in \cite{GMTZ}.

Throughout this paper, we denote
$$
{\mathbb{R}}^n_+=\{x=(x_1,x_2,\dots ,x_n) \in {\mathbb{R}}^n :
x_n>0\},
$$
where $n \geq 2$.  By $\partial {\mathbb{R}}^n_+$ we denote the
boundary of ${\mathbb{R}}^n_+$,  by $B({\mathbb{R}}^n_+)$ the
set of Borel measurable functions in ${\mathbb{R}}^n_+$, and by
$C_0({\mathbb{R}}^n_+)$  the set of
continuous functions vanishing at
$\partial {\mathbb{R}}^n_+\cup \{\infty\}$.
We fix some nonnegative  constants $a, b, \alpha, \beta$
such that $a+\alpha>0$, $b+\beta>0$ and  two
nontrivial nonnegative bounded continuous functions $\varphi$ and
$\psi$ on $\partial {\mathbb{R}}^n_+$ and we will deal with the
existence of positive continuous bounded solutions (in the sense of
distributions) for the system
\begin{equation} \label{S}
\begin{gathered}
\Delta u = \lambda  p(x)  g(v),\quad \text{in }{\mathbb{R}}^n_+ \\
\Delta v = \mu  q(x)  f(u),\quad \text{in } {\mathbb{R}}^n_+  \\
u\big|_{{\partial {\mathbb{R}}^n_+}} = a \varphi ,\quad
\lim_{x_n\to \infty}\frac{u(x)}{x_n}=\alpha ,\\
v\big|_{{\partial {\mathbb{R}}^n_+}} = b \psi   , \quad
\lim_{x_n\to \infty}\frac{v(x)}{x_n}=\beta ,\\
\end{gathered}
\end{equation}
where $\lambda,  \mu$ are nonnegative constants,  the functions
$f, g : (0,\infty)\to [0,\infty)$ are continuous and the
functions $p$, $q$ are nonnegative in $B({\mathbb{R}}^n_+)$
satisfying  some hypotheses related to the Kato class
$K^\infty({\mathbb{R}}^n_+)$ introduced and studied in
\cite{BM+} for $n\geq 3$ and in \cite{BMM} for $n=2$. More
precisely, we will give two existence results for \eqref{S} as $f$
and $g$ are nondecreasing or nonincreasing. To this aim, we give in
the sequel some notations and we recall some properties of the Kato
class defined by means of the Green function $G(x,y)$ of the
Dirichlet Laplacian in ${\mathbb{R}}^n_+$.

\begin{definition}[\cite{BM+,BMM}] \label{def1.1} \rm
A Borel measurable function $s$ in ${\mathbb{R}}^n_+$ belongs to
the Kato class $K^\infty({\mathbb{R}}^n_+)$ if
\begin{gather*}
\lim_{\alpha\to 0}\sup_{x\in {\mathbb{R}}^n_+}\int_{
{\mathbb{R}}^n_+\cap B(x,\alpha)} \frac{y_n}{x_n} G(x,y) |s(y)| dy
= 0,\\
\lim_{M\to \infty}\sup_{x\in {\mathbb{R}}^n_+}\int_{{\mathbb{R}}^n_+
 \cap \{|y|\geq M\}}
\frac{y_n}{x_n} G(x,y) |s(y)| dy= 0.
\end{gather*}
\end{definition}

For any nonnegative function $f$ in $B({\mathbb{R}}^n_+)$, we
denote  the Green potential of $f$ defined on
${\mathbb{R}}^n_+$ by
$$
Vf(x):= \int_{{\mathbb{R}}^n_+} G(x,y) f(y)  dy
$$
and
$$
{\| f \|}:= \sup_{x\in {\mathbb{R}}^n_+}\int_{{\mathbb{R}}^n_+}\frac{
y_n}{x_n} G(x,y)f(y) dy.
$$
Next, we recall some properties of
$K^\infty({\mathbb{R}}^n_+)$.

\begin{proposition}\label{prop1.2}
Let $q$ be a nonnegative function in $K^\infty({\mathbb{R}}^n_+)$.
Then we have
\begin{itemize}
\item[(i)] ${\|q\|} < \infty$.
\item[(ii)] $V{q} \in C_0({\mathbb{R}}^n_+)$.
\end{itemize}
\end{proposition}

The proof of the above propositions is found in \cite{BM+,BMM}.

\begin{theorem}[3G-Theorem] \label{thm3G}
 There exists a constant $C_0 > 0$ such that
for all $x, y$ and $ z$ in ${\mathbb{R}}^n_+$, we have
$$
\frac{G(x,z)G(y,z)}{G(x,y)} \leq C_0
\Big(\frac{z_n}{x_n}G(x,z) + \frac{z_n}{y_n}G(x,z)\Big).
$$
\end{theorem}

The proof of the above Theorem is found in  \cite{BM+,BMM}.

\begin{proposition}\label{prop1.3}
Let $q$ be a nonnegative function in $K^\infty({\mathbb{R}}^n_+)$.
Then we have
\begin{itemize}
\item[(i)] $\alpha_q:=\sup_{x,y \in {\mathbb{R}}^n_+}
\int_{{\mathbb{R}}^n_+} \frac{G(x,z)G(z,y)}{G(x,y)}q(z)dz<\infty$.

\item[(ii)] For any nonnegative superharmonic function $v$ in
${\mathbb{R}}^n_+$ and all $x\in {\mathbb{R}}^n_+$, we have
\[
\int_{{\mathbb{R}}^n_+}G(x,y) v(y) q(y)\,dy \leq \alpha_q v(x).
\]
\item[(iii)] Let $h_0$ be a positive harmonic function in
${\mathbb{R}}^n_+$ which
is continuous and bounded in $\overline{{\mathbb{R}}^n_+}$. Then
the family of functions
$$
\Big\{\int_{{\mathbb{R}}^n_+}G(.,y)h_0(y)p(y)\,dy: |p|\leq q\Big\}
$$
is relatively compact in $C_0({\mathbb{R}}^n_+)$.
\end{itemize}
\end{proposition}

\begin{proof}
(i) From  the 3G-Theorem, we have
$\alpha_{q} \leq 2C_0{\|q\|}$. Which implies by Proposition
\ref{prop1.2}  that $\alpha_{q}<\infty$.

(ii) Let $v$ be a nonnegative superharmonic function in
${\mathbb{R}}^n_+$. Then by \cite[theorem 2.1]{PS1}, there
exists a sequence $(f_k)_{k\in \mathbb{N}}$ of nonnegative
measurable functions in ${\mathbb{R}}^n_+$ such that the sequence
$(v_k)_k$ defined on ${\mathbb{R}}^n_+$ by
$$
v_k(y) := \int_{{\mathbb{R}}^n_+}G(y,z)f_k(z)dz
$$
increases to $v$. Since for each $x\in {\mathbb{R}}^n_+$, we have
\[
\int_{{\mathbb{R}}^n_+}G(x,y) v_k(y) q(y)\,dy \leq
\alpha_q v_k(x),
\]
the result follows from the monotone convergence theorem.

(iii) This assertion was proved in \cite{BMZ,BMM}.
\end{proof}

For any nonnegative bounded continuous function $\varphi$  on
$\partial {\mathbb{R}}^n_+$, we denote by $H \varphi$ the unique
bounded harmonic function $u$ in ${\mathbb{R}}^n_+$ with boundary
value $\varphi$. As long of this work, we denote  by $\theta$ the
harmonic function defined on ${\mathbb{R}}^n_+$
by $\theta(x)=x_n$.

Let $v$ and $\omega$ be two positive functions on a set $S$. We
denote $v\sim \omega$, if there exists a constant $C>0$ such that
$$
\frac{1}{C} v(x)\leq \omega(x)\leq C v(x), \quad \forall x \in S.
$$
In this paper, by  $C$ we denote a positive generic
constant whose value  may vary from line to line.

\section{First existence result}

In this section we will give a first existence result for the system
\eqref{S} in the case where $f$ and $g$ are nondecreasing. We
assume the following hypotheses:
\begin{itemize}
\item[(H1)] The functions $f,g : [0,\infty)\to [0,\infty)$ are
nondecreasing and continuous.

\item[(H2)] The functions $p,q$ are nonnegative in ${\mathbb{R}}^n_+$
such that  for each positive constant $c$,  the functions
$x\mapsto p(x) g(c (x_n+1))$ and $x\mapsto q(x) f(c(x_n+1))$
belong to $K^\infty({\mathbb{R}}^n_+)$.

\item[(H3)]
$$
\lambda_0:=\inf_{x\in {\mathbb{R}}^n_+} \frac{
\alpha \theta(x) + a H\varphi(x)}{V \big(p  g (\beta \theta
 + bH\psi)\big)(x)}> 0, \quad
\mu_0 :=\inf_{x\in {\mathbb{R}}^n_+}\frac{\beta \theta(x)
 + bH\psi(x)}{V \big(q f (\alpha \theta + a H\varphi)\big)(x)}>0.
$$
\end{itemize}

Next, we give our first existence result.

\begin{theorem}\label{thm1}
Assume {\rm (H1)--(H3)}.
Then  for each $\lambda \in [0,\lambda_0)$ and each
$\mu \in [0,\mu_0)$,  problem \eqref{S} has a positive continuous
solution $(u,v)$ such that
\begin{gather*}
( 1- \frac{\lambda}{\lambda_0})[ \alpha \theta  + a H\varphi ]\leq u
\leq \alpha \theta + a H\varphi, \\
( 1-\frac{\mu}{\mu_0})[\beta \theta + b H\psi] \leq v \leq
\beta \theta + b H\psi.
\end{gather*}
\end{theorem}

For the next Corollary, (H2) and (H3) are replaced by
the following hypotheses:
\begin{itemize}
\item[(H2')] The functions $p,q$ are nonnegative in
$K^\infty({\mathbb{R}}^n_+)$;

\item[(H3')]  $\lambda_0':=\inf_{x\in {\mathbb{R}}^n_+} \frac{
H\varphi(x)}{V (p  g ( H\psi))(x)}> 0 $ and
$\mu_0' :=\inf_{x\in {\mathbb{R}}^n_+}\frac{H\psi(x)}{V
(q  f (H\varphi))(x)}>\nolinebreak0$\,.
\end{itemize}

\begin{corollary} \label{coro2.3}
Assume  {\rm (H1), (H2'), (H3')}. Then for each
$\lambda \in [0,\lambda_0')$ and each $\mu \in [0,\mu_0')$,
 problem \eqref{S} has a positive bounded continuous solution
$(u,v)$ such that
\begin{gather*}
( 1- \frac{\lambda}{\lambda_0'}) H\varphi \leq u \leq  H\varphi, \\
( 1- \frac{\mu}{\mu_0'}) H\psi \leq v \leq  H\psi.
\end{gather*}
\end{corollary}

Before proving Theorem \ref{thm1}, we give an
example where the hypotheses (H2) and (H3) are satisfied.

\subsection*{Example}
Let $f,g$ be two continuous functions such that there exists
$\eta>0$ satisfying $0\leq f(t)\leq \eta (t+1)$ and
$0\leq g(t)\leq \eta (t+1)$ for all $t>0$. Let
$\psi$ be a nontrivial nonnegative
bounded continuous function in $\partial {\mathbb{R}}^n_+$. Let
$\alpha=1$, $a=0$, $\beta=0$, $b=1$ and  $p,q$ be two nonnegative
measurable function in ${\mathbb{R}}^n_+$ such that
\begin{gather*}
0\leq p(y)\leq \frac{C}{y_n^{\sigma}(1+|y|)^{\gamma-\sigma}}\quad
 \text{ with }  \sigma <1<3<\gamma,\\
0\leq q(y)\leq \frac{C}{y_n^r(1+|y|)^{s-r}} \quad \text{with }
r<1,\; n+2<s.
\end{gather*}
For this choice of $\gamma, \sigma$ and using
\cite[Proposition 5]{BM+} we deduce that for each $c>0$, the
functions $y \to p(y)g(c(y_n+1))$;
$y \to q(y)f(c(y_n+1))$ and
$y \to p_0(y)=\frac{p(y)}{y_n}$ are in
$K^\infty({\mathbb{R}}^n_+)$. This implies that (H2)
is satisfied. Moreover, using Proposition \ref{prop1.3} we obtain
\[
\frac{ \theta(x)}{ V(p g(H\psi))(x)}
\geq C \frac{\theta(x)}{{\|g(H\psi)\|}_\infty V(p_0 \theta)(x)}
\geq C\frac{\theta(x)}{\alpha_{p_0} \theta(x)}.
\]
Therefore, $\lambda_0>0$.

 On the other hand taking into
account this choice of $q$, we deduce from
\cite[Proposition 8]{BM+} that
$$
V(q(1+\theta))(x)\leq C\frac{x_n}{(1+|x|)^n}.
$$
This together with  $H\psi(x)\geq C\frac{x_n}{(1+|x|)^n}$
imply that
\[
\frac{ H\psi(x)}{ V(q f(\theta))(x)}\geq  \frac{H\psi(x)}{\eta
V(q (1+\theta))(x)}  \geq  C>0.
\]
Consequently $\mu_0>0$.

\begin{proof}[Proof of Theorem \ref{thm1}]
 Let $\lambda \in [0,\lambda_0)$ and
$\mu \in [0,\mu_0)$, then for each $x\in {\mathbb{R}}^n_+$ we have
\begin{gather*}
\lambda_0  V(p g (\beta \theta + b H\psi)) (x) \leq
\alpha \theta(x) + a H\varphi(x),\\
\mu _0 V(q f (\alpha \theta + a H\varphi)) (x) \leq
 \beta \theta(x) + b H\psi(x).
\end{gather*}
We define the sequences $(u_k)_{k\geq 0}$ and $(v_k)_{k\geq 0}$ by
\begin{gather*}
v_0 = \beta \theta + b H\psi, \\
u_k= \alpha \theta + a H\varphi - \lambda V ( p  g(v_k)), \\
v_{k+1} = \beta \theta + b H\psi-\mu V ( q f (u_k)).
\end{gather*}
 We intend to prove that for all $k\in\mathbb{N}$,
\begin{gather*}
0 < ( 1-
\frac{\lambda}{\lambda_0})(\alpha \theta + a H\varphi)
\leq u_k \leq u_{k+1}\leq
\alpha \theta + a H\varphi,\\
0 < (1- \frac{\mu}{\mu_0})(\beta \theta + b H\psi)
\leq v_{k+1}\leq
v_k \leq \beta \theta + b H\psi.
\end{gather*}
 For all integer $k$, we have
\begin{align*}
u_k &\geq \alpha \theta + a H\varphi - \lambda V ( p
g(\beta \theta + b H\psi)) \\
&\geq \alpha \theta + a H\varphi-\frac{\lambda}{\lambda_0}
(\alpha \theta + a H\varphi) \\
&\geq (1-\frac{\lambda}{\lambda_0})(\alpha \theta
+ a H\varphi)>0.
\end{align*}
and
\begin{align*}
v_k &\geq  \beta \theta + b H\psi - \mu V ( q f(\alpha \theta
+ aH\varphi)) \\
&\geq \beta \theta + b H\psi-\frac{\mu}{\mu_0}
(\beta \theta + b H\psi)\\
&\geq (1-\frac{\mu}{\mu_0})(\beta \theta + b H\psi)>0.
\end{align*}
On the other hand, we have $v_1-v_0=-\mu V(q f(u_0))\leq0$ and
$ u_1-u_0=\lambda V(p(g(v_0)-g(v_1))\geq0$.
Since $u_1\leq \alpha \theta + a H\varphi$, we have
$$
u_0\leq u_1\leq \alpha \theta + a H\varphi ,\quad
v_1\leq v_0\leq \beta \theta + b H\psi.
$$
By induction, assume that
$u_k\leq u_{k+1}\leq \alpha \theta + a H\varphi$ and
$v_{k+1}\leq v_k$. Then, we have
\begin{gather*}
v_{k+2}-v_{k+1}= \mu V(q(f(u_k)-f(u_{k+1})))\leq0,\\
u_{k+2}-u_{k+1}= \lambda V(p(g(v_{k+1})-g(v_{k+2})))\geq0.
\end{gather*}
Since $v_{k+1}>0$, we have,
$$
u_{k+1}\leq u_{k+2}\leq \alpha \theta + a H\varphi,\quad
v_{k+2}\leq v_{k+1}\leq \beta \theta + b H\psi.
$$
Therefore, the sequences $(u_k)_{k\geq 0}$ and $(v_k)_{k\geq 0}$
converge to two functions $u$ and $v$ (respectively)
satisfying
\begin{gather*}
0 < ( 1-\frac{\lambda}{\lambda_0})(\alpha \theta + a H\varphi)
\leq u \leq \alpha \theta + a H\varphi,\\
0 < (1- \frac{\mu}{\mu_0})(\beta \theta + b H\psi)
\leq v \leq \beta \theta + b H\psi.
\end{gather*}
 We prove now that $(u, v)$ is a solution for the system
\eqref{S}. Since $(u_k)_k$ and $(v_k)_k$ are monotone and $f, g$
are nondecreasing, then the sequences $(f(u_k))_k$ and $(g(v_k))_k$
are monotone. Hence it follows from hypothesis (H2),
Proposition \ref{prop1.2} and Lebesgue's theorem that $(u,v)$
satisfies
\begin{equation} \label{eq2.1}
\begin{gathered}
u=\alpha  \theta +a H\varphi -\lambda V(p g(v)),\\
v= \beta  \theta +b H\psi -\mu V(q f(u)).
\end{gathered}
\end{equation}
So  $(u,v)$ is a positive continuous solution of \eqref{S}.
\end{proof}

\section{Second existence result}

Let $\varphi$ and $\psi$ be two nontrivial nonnegative bounded
continuous functions on $\partial {\mathbb{R}}^n_+$ and
$\alpha, \beta\geq0$. We fix $\phi$ a nontrivial nonnegative
bounded continuous function
on $\partial {\mathbb{R}}^n_+$ and we put $h_0=H\phi$.

In this section,  we aim at proving the existence of positive
continuous solutions  for the system
\begin{equation} \label{e4}
\begin{gathered}
\Delta u =  p(x)  g(v),\quad \text{in } {\mathbb{R}}^n_+ \\
\Delta v =  q(x)  f(u),\quad \text{in } {\mathbb{R}}^n_+  \\
u\big|_{{\partial {\mathbb{R}}^n_+ }} =  \varphi , \quad
\lim_{x_n\to \infty}\frac{u(x)}{x_n}=\alpha ,\\
v\big|_{{\partial {\mathbb{R}}^n_+}} = \psi , \quad
\lim_{x_n\to \infty}\frac{v(x)}{x_n}= \beta ,
\end{gathered}
\end{equation}
where $f$ and $g$ are continuous and nonincreasing. We assume
the following hypotheses:
\begin{itemize}
\item[(H4)] The functions $f,g : (0,\infty)\to [0,\infty)$ are
non-increasing and continuous;

\item[(H5)] the functions
$\widetilde{p} :=p \frac{f(h_0)}{h_0}$ and
$\widetilde{q} :=q  \frac{g(h_0)}{h_0}$ belong
to the Kato class $K^{\infty}({\mathbb{R}}^n_+)$.
\end{itemize}

Our second existence result is the following.

\begin{theorem} \label{thm3.1}
Under assumptions {\rm (H4)} and {\rm (H5)},
there exists a constant $c>1 $ such that if $\varphi \geq c \phi$
and $\psi \geq c \phi$ on $\partial {\mathbb{R}}^n_+$, then
problem \eqref{e4} has a positive continuous solution $(u,v)$
satisfying for each $x\in {\mathbb{R}}^n_+$,
\begin{gather*}
\alpha x_n+h_0(x)\leq u(x) \leq \alpha x_n+H\varphi(x),\\
\beta x_n+h_0(x)\leq v(x) \leq \beta x_n+H\psi(x).
\end{gather*}
\end{theorem}
We note that this result generalizes those of Athreya \cite{Ath}
and Bachar, M\^aagli and Zribi \cite{BMZ} stated for semilinear
elliptic equations.

\begin{proof}[Proof of Theorem \ref{thm1}]
Let $c=1+\alpha_{\widetilde{p}} + \alpha_{\widetilde{q}}$, where
$\alpha_{\widetilde{p}} $ and $\alpha_{\widetilde{q}}$ are the
constants defined in Proposition \ref{prop1.3} associated to the
functions ${\widetilde{p}}$ and ${\widetilde{q}}$ given in
hypothesis (H5). Let us consider two nonnegative
continuous functions $\varphi$ and $\psi$ on $\partial
{\mathbb{R}}^n_+$ such that $\varphi \geq c \phi$ and $\psi \geq
c \phi$. It follows from the maximum principle that for each
$x\in {{\mathbb{R}}^n_+}$,  we have
\[
H\varphi(x)\geq c h_0(x),\quad  H\psi(x)\geq c h_0(x).
\]
Let $\alpha\geq 0$, $\beta\geq 0$ and $\Lambda$ be the non-empty
closed convex set given by
$$
\Lambda = \{w \in C_b({\mathbb{R}}^n_+) : h_0 \leq w \leq H\varphi \} ,
$$
where $C_b({\mathbb{R}}^n_+)$ denotes the set of continuous
bounded functions in ${\mathbb{R}}^n_+$.

We define the operator $T$ on $\Lambda$ by
$$
T(w) = H\varphi - V(p f[\beta \theta + H\psi
- V(q g(w + \alpha \theta))]).
$$
And we  prove that $T$ has a fixed point.  Let $w\in\Lambda$.
Since $w+ \alpha \theta \geq h_0$, then we deduce from hypotheses
(H4) that
$$
V(q g(w + \alpha \theta))\leq V(q g(h_0)).
$$
Then
\begin{align*}
\beta \theta + H\psi - V(q g(w + \alpha \theta))
&\geq \beta \theta + H\psi - V(\widetilde{q}h_0) \\
&\geq  \beta \theta + H\psi - \alpha_{\widetilde{q}} h_0\\
&\geq \beta \theta + ch_0 - \alpha_{\widetilde{q}} h_0\\
&= \beta \theta + (1+\alpha_{\widetilde{p}}) h_0 \\
&\geq  h_0 > 0.
\end{align*}
Hence,
$V(p f(\beta \theta + H\psi - V(q g(w + \alpha \theta))))
\leq V(p f(h_0)) =  V(\widetilde{p}h_0)$.
Using Proposition \ref{prop1.3} we
deduce that the family of functions
$$
\big\{V(p f(\beta \theta + H\psi - V(q g(w + \alpha \theta)))):
w \in \Lambda\big\}
$$
is relatively compact in $C_0({\mathbb{R}}^n_+)$. Since
$H\varphi \in C_b({\mathbb{R}}^n_+)$, we deduce that the set
$T\Lambda$ is relatively compact in
$C_b({\mathbb{R}}^n_+)$.

Next, we shall prove that $T$ maps $\Lambda$ into itself. Since
$\beta \theta + H\psi - V(q g(w + \alpha \theta)) \geq h_0 > 0$,
we have for all $w \in \Lambda$, $Tw(x) \leq H\varphi(x)$,
for all $x \in {\mathbb{R}}^n_+$. Moreover,
$$
V(p f(\beta \theta  + H\psi - V(q g(w + \alpha \theta))))\leq
V(p f(h_0))=V({\widetilde{p}} h_0)\leq
\alpha_{\widetilde{p}} h_0.
$$
 Then, we obtain
$Tw(x) \geq H\varphi - \alpha_{\widetilde{q}} h_0 \geq h_0$,
which proves that $T(\Lambda) \subset \Lambda$.

Now, we prove the continuity of the operator $T$ in $\Lambda$
in the supremum norm.
Let $(w_k)_{k\in\mathbb{N}}$ be a sequence in $\Lambda$ which
converges uniformly to a function $w$ in $\Lambda$. Then, for each
$x\in {\mathbb{R}}^n_+$, we have
 $$
|Tw_k(x)-Tw(x)| \leq V[p|f(\beta \theta + H\psi - V(q g(w_k
+ \alpha \theta)))
  - f(\beta \theta + H\psi - V(q g(w + \alpha \theta)))|].
$$
On the other hand we have
\begin{align*}
&p |f(\beta \theta + H\psi - V(q g(w_k + \alpha \theta)))
 - f(\beta \theta + H\psi  - V(q g(w + \alpha \theta)))| \\
& \leq p [f(\beta \theta + H\psi - V(q g(w_k + \alpha \theta)))
+ f(\beta \theta + H\psi  - V(q g(w + \alpha \theta)))] \\
& \leq 2p f(\beta \theta + H\psi - V(q g(h_0))) \\
& \leq 2p f(\beta \theta + H\psi - \alpha_{\widetilde{q}}h_0) \\
& \leq 2p f(h_0) \\
& \leq 2{\|h_0\|}_{\infty} \widetilde{p}.
\end{align*}
Since $\widetilde{p} $  belongs to
$K^{\infty}({\mathbb{R}}^n_+)$, $V\widetilde{p} $ is bounded, we
conclude by the dominated convergence theorem that for all
$x \in {\mathbb{R}}^n_+$,
$$
Tw_k(x)\to Tw(x) \quad\text{as }  k\to +\infty .
$$
Consequently, as $T(\Lambda)$ is relatively compact in
$C_b({\mathbb{R}}^n_+)$, we deduce that the pointwise convergence
implies the uniform convergence, namely,
$$
{\| Tw_k - Tw\|}_{\infty} \to 0  as  k \to +\infty.
$$
Therefore, $T$ is a continuous mapping from $\Lambda$ into itself.
So, since $T(\Lambda)$ is relatively compact in
$C_b({\mathbb{R}}^n_+)$, it follows
that $T$ is compact mapping on $\Lambda$.
Finally, the Schauder  fixed-point theorem implies the existence of
a function  $w\in \Lambda$ such that $w=Tw$.
For $x \in {\mathbb{R}}^n_+$, put
$$
u(x)=  \alpha \theta(x)+w(x),\quad
v(x)= \beta  \theta(x) + H\psi(x)-V(qg(u)),.
$$
Then $(u,v)$ is a positive continuous solution of \eqref{e4}.
\end{proof}

\subsection*{Example}
Let $\delta>0$,  $\gamma>0$, $\lambda<2<\mu$ and $r<2<s$.
Let  $p$, $q$ be two nonnegative functions such that
\begin{gather*}
p(x)\leq \frac{C}{(1+|x|)^{n(1+\delta)+\mu-\lambda}
x_n^{\lambda-1-\delta}}, \quad
q(x)\leq \frac{C}{(1+|x|)^{n(1+\gamma)+ s-r} x_n^{r-1-\gamma}} .
\end{gather*}
Let $\varphi$, $\psi$ and $\phi$ be three  nontrivial nonnegative
bounded continuous functions on $\partial {\mathbb{R}}^n_+$. Then,
for each $\alpha \geq 0$, $\beta \geq 0$, there exist a constant
$c > 1$ such that if $\varphi \geq c  \phi$ and
$\psi \geq c \phi$, the problem
\begin{gather*}
\Delta u =  p(x)  v^{-\gamma},\quad \text{in } {\mathbb{R}}^n_+ \\
\Delta v =  q(x)  u^{-\delta},\quad \text{in }  {\mathbb{R}}^n_+\\
u\big|_{{\partial {\mathbb{R}}^n_+ }} = \varphi , \quad
\lim_{x_n\to \infty}\frac{u(x)}{x_n}=\alpha ,\\
v\big|_{{\partial {\mathbb{R}}^n_+}} = \psi , \quad
\lim_{x_n\to \infty}\frac{v(x)}{x_n}= \beta ,
\end{gather*}
has a positive continuous solution $(u,v)$ satisfying
for each $x \in {\mathbb{R}}^n_+$,
\begin{gather*}
\alpha x_n+H\phi(x)\leq u(x) \leq \alpha x_n + H\varphi(x),\\
\beta x_n +H\phi(x)\leq v(x) \leq \beta x_n+H\psi(x).
\end{gather*}

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