\documentclass[reqno]{amsart}
\usepackage{hyperref}

\AtBeginDocument{{\noindent\small
\emph{Electronic Journal of Differential Equations},
Vol. 2014 (2014), No. 38, pp. 1--13.\newline
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu}
\thanks{\copyright 2014 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2014/38\hfil Multiple positive solutions]
{Multiple positive solutions for singular multi-point
boundary-value problems with a positive parameter}

\author[C.-G. Kim, E. K. Lee \hfil EJDE-2014/38\hfilneg]
{Chan-Gyun Kim, Eun Kyoung Lee }  % in alphabetical order

\address{Chan-Gyun Kim \newline
Department of Mathematics,
College of William and Mary, Williamsburg, Virginia 23187-8795, USA}
\email{cgkim75@gmail.com}

\address{Eun Kyoung Lee (corresponding author)\newline
Department of Mathematics and Education,
Pusan National University, Busan 609-735, Korea}
\email{eunkyoung165@gmail.com}

\thanks{Submitted July 3, 2013. Published February 5, 2014.}
\subjclass[2000]{34B10, 34B16}
\keywords{Singular problem; multi-point boundary value problems;
\hfill\break\indent  positive solution; $p$-Laplacian; multiplicity}

\begin{abstract}
 In this article we study the existence, nonexistence,
 and multiplicity of positive solutions for a singular multi-point
 boundary value problem with positive parameter. We use the fixed point
 index theory on a cone and a well-known theorem for the existence
 of a global continuum of solutions to establish our results.

\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{example}[theorem]{Example}
\newtheorem{remark}[theorem]{Remark}
\allowdisplaybreaks

\section{Introduction}

Consider the  singular multi-point boundary-value problem
\begin{gather} \label{ePl} 
(\varphi_{p}(u'(t)))'+\lambda f(t,u(t))=0,\quad t \in (0,1), \\
\label{eBC} 
u(0)= \sum_{i=1}^{m-2} a_i u(\xi_i),\quad u(1)=\sum_{i=1}^{m-2} b_i u(\xi_i),
\end{gather}
where $\varphi_{p}(s)=|s|^{p-2}s,~p>1,~\lambda$ a nonnegative real
 parameter, $\xi_i \in (0,1)$ with $0<\xi_1<\xi_2 < \dots
 < \xi_{m-2}<1$, $a_i,b_i \in [0,1)$ with
$0 \le \sum_{i=1}^{m-2} a_i<1$, $0 \le \sum_{i=1}^{m-2} b_i<1$, and
$f \in C((0,1) \times [0,\infty),(0,\infty))$.
Here, $f(t,u)$ may be singular at $t=0$ and/or $1$ and satisfies
the following conditions:
\begin{itemize}
\item[(F1)] for all $M>0$, there exists $h_M \in \mathcal{A}$
such that $f(t,u) \le h_M(t)$, for all $u \in [0,M]$ and all $t \in (0,1)$,
where
$$
\mathcal{A}=\{h :\int_{0}^{1/2}
\varphi_{p}^{-1} \Big( \int_{s}^{1/2} h(\tau) d \tau
\Big) ds + \int_{1/2}^{1} \varphi_{p}^{-1} \Big(
\int_{1/2}^{s} h(\tau) d \tau \Big) ds < \infty\}:
$$

\item[(F2)]  there exists $[\alpha,\beta] \subset (0,1)$ such that
$\lim_{u \to \infty}f(t,u)/u^{p-1}=\infty$ uniformly in $[\alpha,\beta]$.
\end{itemize}

By a positive solution of problem
\eqref{ePl}-\eqref{eBC}, we mean a function $u \in C[0,1] \cap C^1(0,1)$
with $\varphi_p(u') \in C^1(0,1)$ that satisfies \eqref{ePl}-\eqref{eBC} and
$u>0$ in $(0,1)$. Here $\|\cdot\|$ denotes the usual maximum norm in $C[0,1]$.

Motivated by the work of Bitsadze \cite{Bitsadze84,Bitsadze85},
the study of multi-point boundary value problem for linear second-order
ordinary differential equations was initially done by
Il'in and Moiseev \cite{Il'in1,Il'in2}.
Gupta \cite{Gupta92} studied three-point boundary value problems for
nonlinear ordinary differential equations. Since then, many researchers
have studied nonlinear second-order multi-point boundary value problems
 under various conditions on the nonlinear term. We refer the reader
to \cite{Bai,Feng,Hu,Infante,Kim09A,Liu03,Ma05,Sun,wang,Wong08,Xu04}
and references therein.


Problem \eqref{ePl}-\eqref{eBC} is a singular boundary value problem since
 $f$ is allowed to have singularity at $t=0$ and/or $1$.
Singular problems have been extensively studied in the literature.
For the case of two-point boundary value problems, the results were
proved in \cite{agarwal:eop02,Choi,Dal,Ha,Kim09,Lee5,Wong93,Xu,Yang}
and for multi-point boundary value problems, the results were proved
in \cite{Feng,Hu,Kim09A,Liu03,Sun,Xu04}. However, there are few results
for multi-point boundary value problems having nonlinear term which
does not satisfy $L^1$-Carath\'eodory condition. Recently, in semi-linear
 case, Sun et al. \cite{Sun} studied the following singular three-point
boundary-value problem
\begin{equation}\label{0.1}
\begin{gathered}
y''+\mu a(t)g_1(t,y)=0,\quad t\in(0,1)\\
y(0)-\beta y'(0)=0, \quad y(1)=\alpha y(\eta),
\end{gathered}
\end{equation}
where $\mu>0$ is a parameter, $\beta>0$, $0<\eta<1$, $0<\alpha\eta<1$,
$(1-\alpha\eta)+\beta(1-\alpha)>0$, $a \in C((0,1),(0,\infty))$
satisfies $0<\int_0^1(\beta+s)(1-s)a(s)ds<\infty$, and
$g_1 \in C([0,1]\times(0,\infty),(0,\infty))$ may be singular at $y=0$.
Without any monotone or growth conditions imposed on the nonlinearity
$g_1$, using fixed point index theorem, they obtained not only the
existence results of positive solutions to the problem \eqref{0.1},
 but also the explicit interval about positive parameter $\mu$.
Kim \cite{Kim09A}, in $p$-Laplacian case, presented some sufficient
conditions for one or multiple positive solutions to the problem
\eqref{ePl}-\eqref{eBC}, where $f(t,u)=h(t)g_2(t,u)$,
$h \in \mathcal{A}, g_2 \in C([0,1]\times [0,\infty),[0,\infty))$.

To the authors' knowledge, in the case of $p$-Laplacian, there is
no result about the global structure of positive solutions for
parameter $\lambda \in (0,\infty)$ to multi-point boundary-value
problems with the nonlinear term admitting stronger singularity
than $L^1(0,1)$ at $t=0$ and/or $1$. The following is the main
result in this paper.

\begin{theorem}\label{Thm1.2}
Assume that {\rm (F1)} and {\rm (F2)} hold. Assume in addition
that $f(t,u)=h(t)g(t,u)$, where $h \in \mathcal{A}$ and
$g \in C((0,1) \times [0,\infty),(0,\infty))$ satisfies
\begin{itemize}
\item[(A1)] for all $N>0$ and all $\epsilon>0$, there exists
$\delta=\delta(N,\epsilon)>0$ such that if $u,v \in [0,N]$
and $|u-v|<\delta$, then $|g(t,u)-g(t,v)|<\epsilon$, for all $t \in (0,1)$,

\item[(A2)] $\inf\{g(t,u)~|~t \in (0,1),~u \in [0,\infty)\}>0$.
\end{itemize}
Then there exists $\lambda^*>0$ such that problem \eqref{ePl}-\eqref{eBC}
 has at least two positive solutions for $\lambda \in (0,\lambda^*)$, at
least one positive solution for $\lambda=\lambda^*$ and no positive
solution for $\lambda > \lambda^*$.
\end{theorem}

The above result is an extension of previous works for two-point
boundary-value problems by Choi \cite{Choi}, Wong \cite{Wong93},
 Dalmasso \cite{Dal}, Ha and Lee \cite{Ha}, Lee \cite{Lee5},
Xu and Ma \cite{Xu}, and Kim \cite{Kim09}.

The rest of this article is organized as follows.
In Section 2, the operator for problem \eqref{ePl}-\eqref{eBC} is introduced,
and well-known facts such as Picone-type identity and Global continuation
theorem are presented. In Section 3, the proofs of our results
(Theorem \ref{thm3.4} and Theorem \ref{Thm1.2}) and examples for
 nonlinear term to illustrate our results are given.


\section{Preliminaries}

First we introduce the operator corresponding to problem \eqref{ePl}-\eqref{eBC}.
 Throughout this section we assume that (F1) holds. Set
$$
\mathcal{K}=\{u \in C[0,1] : u\text{i s a nonnegative concave function on
$[0,1]$, $u$ satisfies \eqref{eBC}}\}.
$$
Then $\mathcal{K}$ is an ordered cone in $C[0,1]$.
For $(\lambda,u) \in [0,\infty) \times \mathcal{K}$, we define
$x_{\lambda,u} : [0,1] \to \mathbb{R}$ as
$x_{\lambda,u}(t)=x_{\lambda,u}^1(t)-x_{\lambda,u}^2(t)$, where
\begin{equation*}
x_{\lambda,u}^1(t)=A^{-1}{\sum_{i=1}^{m-2}a_i}
\int_0^{\xi_i}\varphi_p^{-1}\Big[\int_s^t \lambda f(\tau,u(\tau))d\tau\Big]ds
+\int_0^t\varphi_p^{-1}\Big[\int_s^t \lambda f(\tau,u(\tau))d\tau\Big]ds
\end{equation*}
and
\begin{equation*}
x_{\lambda,u}^2(t)=B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
\Big[\int_t^s \lambda f(\tau,u(\tau))d\tau\Big]ds
+\int_t^1\varphi_p^{-1}\Big[\int_t^s \lambda f(\tau,u(\tau))d\tau\Big]ds.
\end{equation*}
Here
$$
A=1-\sum_{i=1}^{m-2}a_i, \quad
B=1-\sum_{i=1}^{m-2}b_i.
$$
For $\lambda>0$, $\lim_{t \to 0^+}x_{\lambda,u}(t)<0$ and
$\lim_{t \to 1^-}x_{\lambda,u}(t)>0$. Indeed we can rewrite
$x_{\lambda,u}^1(t)$ as
\begin{align*}
&x_{\lambda,u}^1(t) \\
&=A^{-1}\Big(-{\sum_{i=1}^{m-2}a_i}
\int_t^{\xi_i}\varphi_p^{-1}\Big[\int_t^s \lambda f(\tau,u(\tau))d\tau\Big]ds
+\int_0^t\varphi_p^{-1}\Big[\int_s^t \lambda f(\tau,u(\tau))d\tau\Big]ds\Big).
\end{align*}
By (F1), there exists $h_2 \in \mathcal{A}$ such that
$$
0 \le \int_0^t\varphi_p^{-1}\Big[\int_s^t \lambda f(\tau,u(\tau))d\tau\Big]ds
\le \int_0^t\varphi_p^{-1}\Big[\int_s^t h_2(\tau)d\tau\Big]ds,
$$
and
$$
\lim_{t \to 0^+} \int_0^t\varphi_p^{-1}
\Big[\int_s^t \lambda f(\tau,u(\tau))d\tau\Big]ds=0.
$$
Clearly $\lim_{t \to 0^+}x_{\lambda,u}^2(t)>0$, and thus
$\lim_{t \to 0^+}x_{\lambda,u}(t)<0$. In a similar manner we can show
$\lim_{t \to 1^-}x_{\lambda,u}(t)>0$. Since $x_{\lambda,u}$ is continuous
and strictly increasing in $(0,1)$, there exists a unique zero
 $A_{\lambda,u} \in (0,1)$ such that $x_{\lambda,u}(A_{\lambda,u})=0$.
For $\lambda=0$, we may take $A_{0,u}=0$ since $x_{0,u}\equiv 0$.
Then, for $(\lambda,u)\in [0,\infty) \times \mathcal{K}$,
\begin{align*}
&A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \Big[\int_s^{A_{\lambda,u}} \lambda f(\tau,u(\tau))d\tau\Big]ds
 +\int_0^{A_{\lambda,u}}\varphi_p^{-1}
 \Big[\int_s^{A_{\lambda,u}} \lambda f(\tau,u(\tau))d\tau\Big]ds\\
&=B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
 \Big[\int_{A_{\lambda,u}}^s \lambda f(\tau,u(\tau))d\tau\Big]ds
 +\int_{A_{\lambda,u}}^1\varphi_p^{-1}
\Big[\int_{A_{\lambda,u}}^s \lambda f(\tau,u(\tau))d\tau\Big]ds.
\end{align*}
Define $H:[0,\infty)\times \mathcal{K} \to C[0,1]$
as
\begin{equation*}
H(\lambda,u)(t)=
\begin{cases}
A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \big[\int_s^{A_{\lambda,u}} \lambda f(\tau,u(\tau))d\tau\big]ds\\
+\int_0^t\varphi_p^{-1}
 \big[\int_s^{A_{\lambda,u}} \lambda f(\tau,u(\tau))d\tau\big]ds,
 &0 \le t \le A_{\lambda,u},\\[4pt]
B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
 \big[\int_{A_{\lambda,u}}^s \lambda f(\tau,u(\tau))d\tau\big]ds\\
 +\int_{A_{\lambda,u}}^1\varphi_p^{-1}
 \big[\int_{A_{\lambda,u}}^s \lambda f(\tau,u(\tau))d\tau\big]ds,
 &A_{\lambda,u} \le t \le 1.
\end{cases}
\end{equation*}
In view of the definition of $A_{\lambda,u}$, $H(\lambda,u)$ is well-defined,
$\|H(\lambda,u)\|$ $=H(\lambda,u)(A_{\lambda,u})$, and
$H(\lambda,u) \in \mathcal{K}$ for all
$(\lambda,u) \in [0,\infty)\times \mathcal{K}$
(see, e.g., \cite[Lemma 2.2]{Feng}).

\begin{lemma}\label{Lem3.1}
Problem \eqref{ePl}-\eqref{eBC} has a positive solution $u$ if and only
if $H(\lambda,\cdot)$ has a fixed point $u$ in $\mathcal{K}$ for $\lambda>0$.
\end{lemma}

\begin{proof}
We assume that $u$ is a positive solution of problem \eqref{ePl}-\eqref{eBC}.
If $\lambda=0$, $u\equiv0$ by the facts that $0\le\sum_{i=1}^{m-2}a_i<1$
and $0\le\sum_{i=1}^{m-2}b_i<1$. Thus $\lambda>0$. Since $u'$ is
 strictly decreasing in $(0,1)$, $u \in \mathcal K$. From the fact that
$u$ satisfies $(BC)$, $\max\{u(0),u(1)\}<u(\xi_j)$ for some
$1\le j \le m-2$, and there exists a unique $A_u \in (0,1)$
such that $u'(A_u)=0$. Integrating $(P_\lambda)$ from $s$ to $A_u$, we have
\begin{equation}\label{3.1}
u'(s)=\varphi_p^{-1}\Big[\lambda \int_s^{A_u}f(\tau,u(\tau))d\tau\Big].
\end{equation}
Again integrating \eqref{3.1} from $0$ to $t$, we have
$$
u(t)=u(0)+\int_0^t\varphi_p^{-1}
 \Big[\int_s^{A_{u}} \lambda f(\tau,u(\tau))d\tau\Big]ds,\quad t \in [0,1).
$$
Then $u(\xi_i)=u(0)+\int_0^{\xi_i}\varphi_p^{-1}
\big[\int_s^{A_{u}} \lambda f(\tau,u(\tau))d\tau\big]ds$
and
\begin{align*}
u(0)&=\sum_{i=1}^{m-2}a_i u(\xi_i)\\
&=\sum_{i=1}^{m-2}a_i u(0)+\sum_{i=1}^{m-2}a_i\int_0^{\xi_i}\varphi_p^{-1}
\Big[\int_s^{A_{u}} \lambda f(\tau,u(\tau))d\tau\Big]ds.
\end{align*}
Thus
$$
u(0)=A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
\Big[\int_s^{A_{u}} \lambda f(\tau,u(\tau))d\tau\Big]ds.
$$
Similarly, integrating \eqref{3.1} from $t$ to $1$,
$$
u(t)=u(1)+\int_t^1\varphi_p^{-1}
\Big[\int_{A_{u}}^s \lambda f(\tau,u(\tau))d\tau\Big]ds,~t \in (0,1]
$$
and
$$
u(1)=B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
\Big[\int_{A_{u}}^s \lambda f(\tau,u(\tau))d\tau\Big]ds.
$$
Then, by the definition of $A_{\lambda,u}$, $A_u=A_{\lambda,u}$
and consequently $H(\lambda,u)\equiv u$.

Conversely, if we assume that there exists $u \in \mathcal{K}$ such that
$H(\lambda,u)=u$ for $\lambda>0$, then one can easily see that $u$
is a positive solution of problem \eqref{ePl}-\eqref{eBC}.
\end{proof}

\begin{lemma}\label{Lem3.2}
Let $M>0$ be given and let $\{(\lambda_n,u_n)\}$ be a sequence in
$[0,\infty)\times \mathcal{K}$ with $|\lambda_n|+\|u_n\| \le M$.
If $A_{\lambda_n,u_n} \to 0$ (or 1) as $n \to \infty$, then
$\lambda_n \to 0$ and $\|H(\lambda_n,u_n)\| \to 0$ as $n \to \infty$.
\end{lemma}

\begin{proof}
We only prove the case $A_{\lambda_n,u_n} \to 0$ as $n \to \infty$
since the other case can be showed in a similar manner.
By the definition of $A_{\lambda,u}$, we can easily know
$\lambda_n \to 0$ as $n \to \infty$. By (F1), there exists
$h_M \in \mathcal{A}$ such that $f(t,u) \le h_M(t)$, $t \in (0,1)$, $u \in [0,M]$.
 For sufficiently large $n$, we have $A_{\lambda_n,u_n}<\xi_1$,
\begin{align*}
0 \le H(\lambda_n,u_n)(0)
&= A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \Big[\int_s^{A_{\lambda_n,u_n}} \lambda_n f(\tau,u_n(\tau))d\tau\Big]ds\\
&\le \lambda_n A^{-1}\int_0^{\xi_{m-2}}\varphi_p^{-1}
 \Big[\int_s^{\xi_{m-2}}  h_M(\tau)d\tau\Big]ds,
\end{align*}
and
\begin{align*}
\|H(\lambda_n,u_n)\|=H(\lambda_n,u_n)(0)
+\lambda_n \int_0^{A_{\lambda_n,u_n}}\varphi_p^{-1}
\Big[\int_s^{A_{\lambda_n,u_n}} h_M(\tau)d\tau\Big]ds.
\end{align*}
Thus $\|H(\lambda_n,u_n)\| \to 0$ as $n \to \infty$ since
$h_M \in \mathcal{A}$ and $\lambda_n \to 0$ as $n \to \infty$.
\end{proof}

\begin{lemma}\label{Lem3.3}
$H:[0,\infty)\times \mathcal{K} \to \mathcal{K}$ is completely continuous.
\end{lemma}

\begin{proof}
 By Lemma \ref{Lem3.2}, Ascoli-Arzel\`{a} theorem, and Lebesgue dominated
convergence theorem, one can easily show the completely continuity of $H$
(e.g., see \cite{agarwal:eop02,Kim09A}). Thus we omit the proof here.
\end{proof}

Next we introduce the generalized Picone identity due to
 Jaros and Kusano (\cite{kusano:pis09}). Let us consider
the following operators:
\begin{gather*}
l_{p}[y] \equiv (\varphi_{p}(y'))' + q(t) \varphi_{p}(y), \\
L_{p}[z] \equiv (\varphi_{p}(z'))' + Q(t) \varphi_{p}(z).
\end{gather*}

\begin{theorem}[{\cite[p~382]{kusano:pis00}}] \label{Thm2.1}
Let $q(t)$ and $Q(t)$ be measurable functions on an interval $I$.
If $y$ and $z$ are any functions such that $y, z, \varphi_{p}(y')$,
$\varphi_{p}(z')$ are differentiable a.e. on $I$ and $z(t) \neq 0$ for
$t \in I$, then the following holds
\begin{equation} \label{2.1}
\begin{aligned}
&\frac{d}{dt} \Big\{ \frac {|y|^{p} \varphi_{p}(z')}
{\varphi_{p}(z)} - y \varphi_{p}(y') \Big\}\\
& = (q - Q) |y|^{p}  - \big[ |y'|^{p} + (p-1) | \frac{yz'}{z}|^{p}
             - p\varphi_{p}(y) y' \varphi_{p} \big( \frac{z'}{z} \big) \big]
- y l_{p}[y] + \frac{|y|^{p}}{\varphi_{p}(z)} L_{p}[z].
\end{aligned}
\end{equation}
\end{theorem}

\begin{remark}\label{Rem2.2} \rm
By Young's inequality, we have
$$
|y'|^{p} + (p-1) | \frac{yz'}{z}|^{p}
             - p\varphi_{p}(y)y' \varphi_{p} \big( \frac{z'}{z} \big) \geq 0,
$$
and the equality holds if and only if $y'=y z'/z$ in $(a,b)$.
\end{remark}

Finally we recall a well-known theorem for the existence of a global
continuum of solutions by Leray and Schauder \cite{MR1509338}.

\begin{theorem}[{\cite[Corollary 14.12]{zeidler:nfa85}}] \label{Thm2.5}
 Let $X$ be a Banach space with $X \neq \{0\}$ and let $\mathcal{K}$
 be an ordered cone in $X$. Consider
\begin{equation}\label{2.1b}
x=H(\mu,x),
\end{equation}
where $\mu \in [0,\infty)$ and $x \in \mathcal{K}$. If
$H:[0,\infty)\times \mathcal{K} \to \mathcal{K}$ is completely
continuous and $H(0,x)=0$ for all $x \in \mathcal{K}$. Then
the solution component $\mathcal{C}$ of
\eqref{2.1} in $[0,\infty)\times \mathcal{K}$ which contains $(0,0)$ is unbounded.
\end{theorem}

\section{Main results}

Since $H(0,u)=0$ and $H(\lambda,0) \neq 0$ if $\lambda \neq 0$,
by Lemma \ref{Lem3.3}, Theorem \ref{Thm2.5}, we obtain the
following proposition.

\begin{proposition}\label{Pro4.1}
Assume that (F1) holds. Then there exists an unbounded continuum
$\mathcal{C}$ emanating from $(0,0)$ in the closure of the set of
positive solutions of problem \eqref{ePl}-\eqref{eBC} in $[0,\infty) \times
\mathcal{K}$.
\end{proposition}

To see the shape of $\mathcal{C}$, we need lemmas regarding
$\lambda$-direction block and {\it a priori} estimate. Using the
generalized Picone identity (Theorem \ref{Thm2.1}) and the
properties of the $p$-sine function
\cite{delpino:hdl89,zhang:nns00}, we obtain the following two lemmas.

\begin{lemma}\label{Lem4.2}
Assume that {\rm (F1)} and {\rm (F2)} hold.
Then there exists $\bar \lambda >0 $ such that if
problem \eqref{ePl}-\eqref{eBC} has a positive solution $u_\lambda$,
then $\lambda \leq \bar \lambda$.
\end{lemma}

\begin{proof}
 Let $u_\lambda$ be a positive solution of
problem \eqref{ePl}-\eqref{eBC}. Since $f(t,u)>0$ for all
$(t,u) \in (0,1)\times [0,\infty)$, by (F2), there exists
$C_1> 0$ such that
\begin{equation}\label{4.1}
f(t,u)> C_1 \varphi_p(u)\quad \text{for } u \in [0,\infty),\; t \in [\alpha,\beta].
\end{equation}
It is easy to check that
$w(t) = S_{q}\left(\pi_{q}(t-\alpha)/(\beta-\alpha)\right)$,
where $S_q$ is the $q$-sine function and
$\frac{1}{p} + \frac{1}{q} = 1$, is a solution of
\begin{gather*}
(\varphi_{p}(w'(t)))' + \big(\frac{\pi_{q}}{\beta-\alpha}\big)^{p}
 \varphi_{p}(w(t)) = 0,\quad t \in(\alpha,\beta),\\
w(\alpha)=w(\beta)=0.
\end{gather*}
Taking $y = w$, $z = u_\lambda$,
$q(t)=\left(\pi_{q}/(\beta-\alpha)\right)^{p}$ and
$Q(t)=\lambda f(t,u_\lambda)/\varphi_p(u_\lambda)$
in \eqref{2.1} and integrating \eqref{2.1} from $\alpha$ to $\beta$,
by Remark \ref{Rem2.2},
$$
 \int_{\alpha}^{\beta} \Big(\big(\frac{\pi_{q}}{\beta-\alpha}\big)^{p}
- \lambda \frac{f(t,u_\lambda)}{\varphi_p(u_\lambda)} \Big)  |w|^{p}
dt \ge 0.
$$
It follows from \eqref{4.1} that
$$
\Big(\big(\frac{\pi_{q}}{\beta-\alpha}\big)^{p}
- \lambda C_1 \Big)\int_{\alpha}^{\beta} |w|^{p} dt \ge 0,
$$
and thus the proof is complete.
\end{proof}

\begin{lemma}\label{Lem4.3}
Assume that {\rm (F1)} and {\rm (F2)} hold, and let $J=[D,E]$
be a compact subset of
$(0,\infty)$. Then there exists $M_J >0$ such that if $u$ is a
positive solution of problem \eqref{ePl}-\eqref{eBC} with
$\lambda \in J$, then $\|u\| \leq M_J$.
\end{lemma}

\begin{proof}
Suppose on the contrary that there exists a
sequence $\{u_{n}\}$ of positive solutions of problem
\eqref{ePl}-\eqref{eBC} with $\lambda_n$ instead of $\lambda$, and
$\{\lambda_{n}\} \subset J = [D,E]$ and
$\|u_{n}\| \to \infty$ as $n \to \infty$.
It follows from the concavity of $u_{n}$ for all $n$ that
\begin{equation}\label{4.3}
u_{n}(t) \ge \min\{\alpha,1-\beta\} \|u_{n}\|, \quad
 t \in (\alpha,\beta).
\end{equation}
Take $C = 2 D^{-1}\left(\pi_{q}/(\beta-\alpha)\right)^{p}> 0$.
 By (F2), there exists $K > 0$ such that $f(t,u) > C\varphi_{p}(u)$,
for $t \in (\alpha,\beta)$, $u > K$. From the
assumption, we get  $\|u_{N}\| > (\min\{\alpha,1-\beta\})^{-1} K$,
for sufficiently large $N$.
Therefore, by \eqref{4.3}, we have
$$
f(t,u_{N}(t)) > C \varphi_{p}(u_{N}(t)), \quad t \in (\alpha,\beta).
$$
As in the proof of Lemma \ref{Lem4.2}, if we take
$y(t) = S_{q}\left(\pi_{q}(t-\alpha)/(\beta-\alpha)\right)$ and
$z=u_N$, by Theorem \ref{Thm2.1} and Remark \ref{Rem2.2},
$$
C  \le D^{-1}\big(\frac{\pi_{q}}{\beta-\alpha}\big)^{p}.
$$
This contradicts the choice of $C$, and thus the proof is
complete.
\end{proof}

Setting $\lambda^*=\sup \{\mu>0$: for all $\lambda \in (0,\mu)$, there
exists at least two positive solutions of problem \eqref{ePl}-\eqref{eBC}, then
$\lambda^*>0$ is well-defined. Indeed by Proposition \ref{Pro4.1},
$\mathcal{C}$ emanates from $(0, 0)$, and problem \eqref{ePl}-\eqref{eBC}
has a small solution near $(0, 0)$ for $\lambda \in (0,s)$ with small $s>0$.
On the other hand, for any $M > 0$, define
$\mathcal{C}_M = \{(\lambda,u) \in \mathcal{C} :  \|u\| \ge M\}$
and the projection of $\mathcal{C}_M$ to the $\lambda$-axis as $\Lambda_M$.
Then, by Lemma \ref{Lem4.2} and Lemma \ref{Lem4.3}, for large $M$,
 $\Lambda_M=(0,a_M]$, where $a_M>0$ and it is decreasing in $M$.
This implies that, for any interval $(0,s)$ with
small $s>0$, problem \eqref{ePl}-\eqref{eBC} also has a large solution
for $\lambda \in (0,s)$. Thus $\lambda^*>0$ is well-defined. Moreover it follows from an easy compactness argument that problem \eqref{ePl}-\eqref{eBC} has at least two positive solution
for $\lambda \in (0,\lambda^*)$ and at least one
positive solution for $\lambda=\lambda^*$.

The following is the first result in this work.

\begin{theorem}\label{thm3.4}
Assume that {\rm (F1)} and {\rm (F2)} hold.  Then there exists
$\lambda_* \ge \lambda^*>0$ such that problem \eqref{ePl}-\eqref{eBC}
has at least two positive solutions for $\lambda \in (0,\lambda^*)$,
 at least one positive solution for $\lambda \in [\lambda^*,\lambda_*]$,
and no positive solution for $\lambda>\lambda_*$.
\end{theorem}

\begin{proof}
Define $\lambda_*=\sup\{ \lambda:$ problem \eqref{ePl}-\eqref{eBC} has at
least one positive solution$\}$. Then by Lemma \ref{Lem4.2},
 $\lambda^* \leq \lambda_*<\infty$. We only consider the case
$\lambda^* < \lambda_*$, since the proof is done for the case
$\lambda^* = \lambda_*$.
 For $\lambda\in [\lambda^*, \lambda_*)$, there exists
$\hat \lambda \in [ \lambda,  \lambda_{*})$ such that
\eqref{ePl}-\eqref{eBC} with $\hat{\lambda}$ instead of $\lambda$,
has a positive solution, say $\hat u$.
Consider the  modified problem
\begin{equation} \label{eMl} %\tag*{$(M_{\lambda})$}
\begin{gathered}
(\varphi_{p}(u'(t)))' + \lambda \bar f(t,u(t))=0, \quad t \in (0,1),  \\
u(0)= {\sum_{i=1}^{m-2} a_i} u(\xi_i),\quad
u(1)={\sum_{i=1}^{m-2} b_i} u(\xi_i),
\end{gathered}
\end{equation}
where $\bar f(t,u)=f(t,\gamma(t,u))$ and
 $\gamma : (0,1) \times \mathbb{R} \to \mathbb{R}$ is defined as
\begin{equation*}
\gamma(t,u) =\begin{cases}
\hat u(t) , & \text{if } u > \hat u(t) ,\\
u, & \text{if }0 \le u \le \hat u(t) ,\\
0, & \text{if }u < 0.
\end{cases}
\end{equation*}
Then all solutions $u$ of \eqref{eMl} are concave and non-trivial.
Define $T_\lambda : C[0,1] \to C[0,1]$ as
\begin{equation*}
T_{\lambda}(u)(t) = \begin{cases}
A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \big[\int_s^{\hat{A}} \lambda \bar f(\tau,u(\tau))d\tau\big]ds\\
+\int_0^t\varphi_p^{-1}
 \big[\int_s^{\hat{A}} \lambda \bar f(\tau,u(\tau))d\tau\big]ds,
 &0 \le t \le \hat{A}\\[4pt]
B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
\big[\int_{\hat{A}}^s \lambda \bar f(\tau,u(\tau))d\tau\big]ds\\
 +\int_{\hat{A}}^1\varphi_p^{-1}
 \big[\int_{\hat{A}}^s \lambda \bar f(\tau,u(\tau))d\tau\big]ds,
 &\hat{A} \le t \le 1.\end{cases}
\end{equation*}
where $\hat{A}$ satisfies
\begin{align*}
&A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \Big[\int_s^{\hat{A}} \lambda \bar f(\tau,u(\tau))d\tau\Big]ds
 +\int_0^{\hat{A}}\varphi_p^{-1}
 \Big[\int_s^{\hat{A}} \lambda \bar f(\tau,u(\tau))d\tau\Big]ds\\
&=B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
 \Big[\int_{\hat{A}}^s \lambda \bar f(\tau,u(\tau))d\tau\Big]ds
 +\int_{\hat{A}}^1\varphi_p^{-1}
 \Big[\int_{\hat{A}}^s \lambda \bar f(\tau,u(\tau))d\tau\Big]ds.
\end{align*}
It is easy to check that $T_{\lambda}$ is completely
continuous on $C[0,1]$, and $u$ is a solution of \eqref{eMl}
 if and only if $u=T_\lambda u$. It follows from the definition of
$\gamma$ and the continuity of $f$ that there exists $R_{1} > 0$
such that $\|T_\lambda u\| < R_{1}$ for all $u \in C[0,1]$.
Then by Schauder fixed point theorem, there exists $u_\lambda \in C[0,1]$
such that $T_\lambda u_\lambda = u_\lambda$, and $u_\lambda$ is a
positive solution of $(M_{\lambda})$.

We first claim that $u_\lambda(0) \leq \hat u(0)$. If the
claim is not true, $u_\lambda(0) > \hat u(0)$.
Put $x(t)=u_\lambda(t)-\hat u(t)$. Then
$$
0< x(0)=u_\lambda(0)-\hat u(0)={\sum_{i=1}^{m-2} a_i}x(\xi_i)
\le {\sum_{i=1}^{m-2} a_i} x(\xi_j)<x(\xi_j),
$$
where $x(\xi_j)=\max\{x(\xi_i)|1\le i \le m-2\}$.
Similarly, $x(1) < x(\xi_j)$. Thus, there exists $\sigma \in (0,1)$ and
 $a \in [0, \sigma)$ such that $x(\sigma)=\max_{t\in[0,1]}x(t)>0$,
$x'(\sigma)=0$, $x(a)=0$, and $x(t)>0$ for $t\in (a,\sigma]$.
Since $\lambda <\hat \lambda$, for $t\in (a,\sigma]$,
$(\varphi_p(u_\lambda'(t)))'>(\varphi_p(\hat u'(t)))'$ and integrating
this from $t$ to $\sigma$, $u_\lambda'(t)<\hat u'(t)$.
Again integrating from $a$ to $\sigma$, we have
$x(\sigma)=u_\lambda(\sigma)-\hat u(\sigma)<u_\lambda(a)-\hat u(a)=x(a)$.
This is a contradiction. Thus the claim is proved. Similarly,
we have $u_\lambda(1) \leq \hat u(1)$. Next we show that
$u_\lambda(t) \le \hat u(t)$ for $t \in (0,1)$. If it is not true,
it follows from $u_\lambda(0) \le \hat u(0)$ and $u_\lambda(1) \le \hat u(1)$
that there exists an interval $[t_{1},t_{2}]\subset [0,1]$ such that
$u_\lambda(t_{1}) = \hat u(t_{1})$,
$ u_\lambda(t_{2}) = \hat u(t_{2})$ and $u_\lambda(t)> \hat u(t)$
for all $t \in (t_{1},t_{2})$. Then
\begin{equation}\label{1}
(\varphi_p(u_\lambda'(t)))'>(\varphi_p(\hat u'(t)))', \quad t\in (t_{1},t_{2})
\end{equation}
and we can choose an interval $[b,c] \subset [t_{1},t_{2}]$
such that $u_\lambda'(b)> \hat u'(b)$ and
$ u_\lambda'(c) <\hat u'(c) $. Using \eqref{1},
we can get the contradiction
\begin{align*}
0 & >
 [\varphi_{p}(u_\lambda'(c) ) - \varphi_{p}(u_\lambda'(b) ) ]
 -[\varphi_{p}(\hat u'(c) ) - \varphi_{p}(\hat u'(b) ) ] \\
  & =  \int_{b}^{c} \big\{ [\varphi_{p}(u_\lambda'(t) ) ]'
        - [\varphi_{p}(\hat u'(t) ) ]' \big\} dt  > 0.
\end{align*}
Therefore, by the definition of $\gamma$, $u_\lambda$ turns out a
positive solution of problem \eqref{ePl}-\eqref{eBC}.
Furthermore, by Lemma \ref{Lem4.3} and
the complete continuity of $H$, we can show that problem
\eqref{ePl}-\eqref{eBC}, with $\lambda_*$ instead of $\lambda$, has a
positive solution $u_*$, and thus the proof is complete.
\end{proof}

Now we consider $f(t,u)=h(t)g(t,u)$ and let $u_*$ be
a positive solution of problem \eqref{ePl}-\eqref{eBC}, with
$\lambda_*$ instead of $\lambda$.

\begin{lemma}\label{Lem4.4}
Assume that {\rm (F1)} and {\rm (F2)} hold.
Assume in addition that $g$ satisfies the conditions {\rm (A1)}
and {\rm (A2)}. Then, for all $\lambda \in (0,\lambda_*)$,
there exists $\delta_\lambda >0$ such that
$\alpha_\lambda(t)=u_*(t)+\delta_\lambda$ satisfies
\begin{equation}\label{4.4}
(\varphi_p(\alpha_\lambda'(t)))' + \lambda h(t)g(t,\alpha_\lambda(t)) <0, \quad
 t \in (0,1).
\end{equation}
\end{lemma}

\begin{proof} Let $\lambda$ be fixed in $(0,\lambda_*)$.
Put
$$
\epsilon=\frac{1}{2} [\lambda_*/\lambda-1]\inf_{t\in(0,1)} g(t,u_*(t))>0.
$$
By (A1), there exists $\delta_\lambda>0$ such that if $u,v \in [0,\|u_*\|+1]$
and $|u-v|<\delta_\lambda$, then $|g(t,u)-g(t,v)|<\epsilon,~t \in (0,1)$.
Put $\alpha_\lambda(t)=u_*(t)+\delta_\lambda$. Then
\begin{align*}
 (\varphi_p(\alpha_\lambda'(t)))'+ \lambda f(t,\alpha_\lambda(t))
&= (\varphi_p(u_*'(t)))'+ \lambda f(t,u_*(t)+\delta_\lambda)\\
&= h(t)[-\lambda_*g(t,u_*(t))+ \lambda g(t,u_*(t)+\delta_\lambda)].
\end{align*}
From this, if $\alpha_\lambda$ does not satisfy \eqref{4.4}, there exists
$t_0\in(0,1)$ such that
$$
-\lambda_*g(t_0,u_*(t_0))+ \lambda g(t_0,u_*(t_0)+\delta_\lambda)\ge 0,
$$
and then
$$
g(t_0,u_*(t_0)+\delta_\lambda) \geq
\frac{\lambda_*}{\lambda}g(t_0,u_*(t_0)).
$$
By the choice of $\delta_\lambda$,
$$
\epsilon \geq \big(\frac{\lambda_*}{\lambda}-1\big)g(t_0,u_*(t_0)),
$$
which contradicts the choice of $\epsilon$. This completes the proof.
\end{proof}

\begin{proof}[Proof of Theorem \ref{Thm1.2}]
Suppose on the contrary that $\lambda^* < \lambda_*$.
Let $\lambda$ be fixed with $\lambda^* \le \lambda < \lambda_*$.
Then by showing that \eqref{ePl}-\eqref{eBC} has at least two positive
solutions for $\lambda \in [\lambda^*,\lambda_*)$, we get a contradiction
to the definition of $\lambda^*$, which completes the proof.
By Lemma \ref{Lem4.4}, there exists $\delta_\lambda>0$ such that
$\alpha_\lambda(t)=u_*(t)+ \delta_\lambda$ satisfies \eqref{4.4}.
Consider the modified problem
\begin{equation}\label{ebarMl} %\tag{$\ol M_\lambda$}
\begin{gathered}
(\varphi_p(u'(t)))'+\lambda h(t)g(t,\gamma_1(t,u(t)))=0,\\
u(0)={\sum_{i=1}^{m-2} a_i}u(\xi_i),\quad
u(1)={\sum_{i=1}^{m-2} b_i} u(\xi_i),
\end{gathered}
\end{equation}
where $\gamma_1 : (0,1) \times \mathbb{R} \to [0,\infty)$
is defined as
$$
\gamma_1 (t,u)= \begin{cases}
\alpha_\lambda(t),& \text{if }  u>\alpha_\lambda(t),\\
u, & \text{if }  0 \leq u \leq \alpha_\lambda(t),\\
0, &\text{if }  u<0.
\end{cases}
$$
Let $u$ be a positive solution of \eqref{ebarMl}. Set
$$
\Omega=\{u\in C[0,1] |~-1<u(t)<\alpha_\lambda(t), \quad t \in [0,1]\}.
$$
Then $\Omega$ is bounded and open in $C[0,1]$. We claim that if
$u$ is a positive solution of \eqref{ebarMl}, then
$u \in \Omega \cap \mathcal{K}$. Indeed, by the similar argument as
in the proof of Theorem \ref{thm3.4},
 $0 \le u(t) \le \alpha_\lambda(t)$, $t \in [0,1]$ and
\begin{align*}
u(0)
&={\sum_{i=1}^{m-2} a_i}u(\xi_i)
 \leq {\sum_{i=1}^{m-2} a_i}\alpha_\lambda(\xi_i)\\
&= {\sum_{i=1}^{m-2} a_i}(u_* (\xi_i)+ \delta_\lambda)
< {\sum_{i=1}^{m-2} a_i}u_* (\xi_i)+ \delta_\lambda \\
&= u_* (0)+ \delta_\lambda = \alpha_\lambda (0).
\end{align*}
Similarly, $\alpha_\lambda(1)>u(1)$. If the claim is not true, then there
exists $[t_0,t_1] \subset (0,1)$ with $t_0 \le t_1$ such that
$0<u(t)=\alpha_\lambda(t)$, $t \in [t_0,t_1]$ and
$0<u(t)<\alpha_\lambda(t)$, $t \in (t_0-\delta_1, t_1+\delta_1) \setminus
[t_0,t_1]$ for some $\delta_1>0$. Since $\alpha_\lambda$ satisfies \eqref{4.4},
$$
\max_{t \in [t_0-\delta_1,t_1+\delta_1]}
\{(\varphi_p(\alpha_\lambda'(t)))'+ \lambda
h(t)g(t,\alpha_\lambda(t))\}=-\epsilon_1<0.
$$
 By  condition (A1), there exists $\delta_2>0$ such that
if $|u-v|< \delta_2$ and $u,v \in [0, \|\alpha_\lambda\|]$, then
$$
|g(t,u)-g(t,v)|< \epsilon_2,
$$
where $\epsilon_2=\epsilon_1[2\lambda
 \max_{t \in [t_0-\delta_1,t_1+\delta_1]}h(t)]^{-1} >0$,
and then there exists an interval
$[a,b] \subset (t_0-\delta_1, t_1 +\delta_1)$ such that
$$
(u-\alpha_\lambda)'(a)>0, ~(u-\alpha_\lambda)'(b)<0
$$
and
$$-\delta_2 < \gamma(t,u(t))-\alpha_\lambda(t)
=u(t)-\alpha_\lambda(t) \leq 0, \quad t \in [a,b].
$$
Consequently,
\begin{gather*}
\varphi_p(u'(a))-\varphi_p(\alpha_\lambda'(a))>0,\quad
\varphi_p(u'(b))-\varphi_p(\alpha_\lambda'(b))<0,\\
g(t,\gamma(t,u(t))) < g(t,\alpha_\lambda(t))+ \epsilon_2,\quad t \in [a,b].
\end{gather*}
Then, by the choice of $\epsilon_2$,
\begin{align*}
0 & >  \varphi_{p}(u'(b)) - \varphi_{p}(\alpha_\lambda'(b))
     - \varphi_{p}(u'(a)) + \varphi_{p}(\alpha_\lambda'(a)), \\
  & =  \left[\varphi_{p}(u'(b)) - \varphi_{p}(u'(a)) \right] -
     \left[\varphi_{p}(\alpha_\lambda'(b)) - \varphi_{p}(\alpha_\lambda'(a)) \right] \\
  & =  \int_{a}^{b} \left\{ (\varphi_{p}(u'(t)))'
        - (\varphi_{p}(\alpha_\lambda'(t)))' \right \} dt \\
  & =  \int_{a}^{b} \left\{-\lambda h(t) g(t,\gamma(t,u(t)))
        -(\varphi_{p}(\alpha_\lambda'(t)))' \right \} dt \\
  & > \int_{a}^{b} \left\{-\lambda h(t) [g(t,\alpha_\lambda(t))+
  \epsilon_2]
        -(\varphi_{p}(\alpha_\lambda'(t)))' \right \} dt\\
  &> \int_{a}^{b} \left(-\lambda h(t)\epsilon_2
  -\left[(\varphi_p(\alpha_\lambda'(t)))'+ \lambda
h(t)g(t,\alpha_\lambda(t))\right]\right)dt\\
&\ge \int_{a}^{b}(-\lambda \epsilon_2 h(t) +\epsilon_1 )dt \ge 0.
  \end{align*}
This is a contradiction. Thus the claim is proved. Define
\begin{equation*}
Mu(t)= \begin{cases}
A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \big[\int_s^{A_{u}} \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\big]ds\\
 +\int_0^t\varphi_p^{-1}
 \big[\int_s^{A_{u}} \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\big]ds,
& 0\le t \le A_{u},\\[4pt]
B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
 \big[\int_{A_{u}}^s \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\big]ds\\
 +\int_{A_{u}}^1\varphi_p^{-1}
\big[\int_{A_{u}}^s \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\big]ds,
& A_{u} \le t \le 1,
\end{cases}
\end{equation*}
where $A_u$ is defined as
\begin{align*}
& A^{-1}{\sum_{i=1}^{m-2}a_i}\int_0^{\xi_i}\varphi_p^{-1}
 \Big[\int_s^{A_{u}} \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\Big]ds\\
&\quad +\int_0^{A_{u}}\varphi_p^{-1}
 \Big[\int_s^{A_{u}} \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\Big]ds\\
&=B^{-1}{\sum_{i=1}^{m-2}b_i}\int_{\xi_i}^1\varphi_p^{-1}
 \Big[\int_{A_{u}}^s \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\Big]ds\\
&\quad +\int_{A_{u}}^1\varphi_p^{-1}
 \Big[\int_{A_{u}}^s \lambda f(\tau,\gamma_1(\tau, u(\tau)))d\tau\Big]ds.
\end{align*}
Then $M:\mathcal{K} \to \mathcal{K}$ is completely continuous, and
$u$ is a positive solution of \eqref{ebarMl} if and only if $u=Mu$ on
$\mathcal{K}$. By simple calculation, there exists $R_1>0$ such that
$\|Mu\|<R_1$ for all $u \in \mathcal{K}$ and $\Omega \subset B_{R_1}$.
Applying \cite[Lemma 2.3.1]{guo:npa98} with $O=B_{R_1}$,
$$
i(M,B_{R_1}\cap \mathcal{K},\mathcal{K})=1.
$$
By the above claim and excision property,
$$
i(M,\Omega \cap \mathcal{K},\mathcal{K})
=i(M,{B_{R_1}}\cap \mathcal{K}, \mathcal{K})=1.
$$
Since problem \eqref{ePl}-\eqref{eBC} is equivalent to problem \eqref{ebarMl}
on $\Omega \cap \mathcal{K}$, we conclude \eqref{ePl}-\eqref{eBC}
has a positive solution in $\Omega \cap \mathcal{K}$. Assume
$H(\lambda,\cdot)$ has no fixed point in
$\partial \Omega \cap \mathcal{K}$, since otherwise the proof is done.
Then, $i(H(\lambda,\cdot), \Omega \cap \mathcal{K},\mathcal{K})$
is well-defined, and
\begin{equation}\label{4.5}
i(H(\lambda,\cdot), \Omega \cap \mathcal{K},\mathcal{K})
=i(M, \Omega\cap \mathcal{K}, \mathcal{K})=1
\end{equation}
since $Mu=H(\lambda,u)$  for $u \in \Omega \cap \mathcal{K}$.
By Lemma \ref{Lem4.2}, \eqref{ePl}-\eqref{eBC} with $\lambda_{N_0}$
instead of $\lambda$
 has no solution in $\mathcal{K}$ for
$\lambda_{N_0}>\overline{\lambda}$. Thus, for any open subset $\mathcal{O}$ in $ X$,
$$
i(H(\lambda_{N_0},\cdot) , \mathcal{O}\cap \mathcal{K},\mathcal{K})=0.
 $$
By {\it a priori} estimate (Lemma
\ref{Lem4.3}) with $I=[\lambda,\lambda_{N_0}]$, there exists
$R_2(>R_1)$ such that  all possible positive solutions $u$ of
\eqref{ePl}-\eqref{eBC} with $\mu$ instead of $\lambda$ for
$\mu \in[\lambda,\lambda_{N_0}]$, satisfy $\|u\|<R_2$.

Define $h:[0,1]\times(\overline{B}_{R_2} \cap \mathcal{K}) \to \mathcal{K}$ as
$$
h(\tau,u)=H(\tau \lambda_{N_0}+(1-\tau)\lambda,u).
$$
Then $h$ is completely continuous on $[0,1]\times \mathcal{K}$,
and it satisfies that
$h(\tau,u) \neq u$ for all $(\tau,u) \in [0,1] \times (\partial
B_{R_2} \cap \mathcal{K})$. By the property of homotopy invariance,
$$
i(H(\lambda,\cdot),B_{R_2}\cap \mathcal{K},\mathcal{K})
=i(H(\lambda_{N_0},\cdot),B_{R_2}\cap \mathcal{K},\mathcal{K})=0.
$$
By \eqref{4.5} and the additivity property,
$$
i(H(\lambda,\cdot),(B_{R_2}\setminus \overline{\Omega})\cap \mathcal{K},\mathcal{K})=-1.
$$
Thus problem \eqref{ePl}-\eqref{eBC} has another positive solution in $(B_{R_2}
\backslash \overline{\Omega})\cap \mathcal{K}$. This completes the proof.
\end{proof}

Finally, we give the examples for the nonlinear term to illustrate our results.

\begin{example} \rm
(1) Put $f_1(t,u)=[t(1-t)]^{-p+1/(u+1)}exp(u)$.
Then, it is easily verified that $f_1$ satisfies the assumptions of
Theorem \ref{thm3.4}.

(2) Put $f_2(t,u)=(1-t)^{-\alpha_1}g(t,u)$, where
 $g(t,u)=c_1t^{-\beta_1}+c_2 (u^q+1)$. Then $f_2$
satisfies the assumptions of Theorem \ref{Thm1.2} if
 $\alpha_1,\beta_1 <p$, $c_1 \ge 0$, $c_2>0$, and $q>p-1$.
\end{example}

\subsection*{Acknowledgments}
Chan-Gyun Kim was supported by National Research Foundation of
Korea Grant funded by the Korean Government
(Ministry of Education, Science and Technology, NRF-2011-357-C00006)
Eun Kyoung Lee was supported by a 2-Year Research Grant of Pusan
National University.

This work was done when the first author visited College ofWilliam and Mary. He would like to thank Department of Mathematics, 
College of William and Mary for warm hospitality, and thank ProfessorJunping Shi for constant encouragement and helpful discussions.


\begin{thebibliography}{00}

\bibitem{agarwal:eop02}
R.P. Agarwal, H. L\"u, D. O'Regan;
\newblock Eigenvalues and the one-dimensional $p$-{L}aplacian,
\newblock \emph{J. Math. Anal. Appl.}, \textbf{266} (2002) 383-400.

\bibitem{Bai}
C. Bai, J. Fang;
\newblock Existence of multiple positive solutions for nonlinear $m$-point boundary value problems,
\newblock \emph{J. Math. Anal. Appl.}, \textbf{281} (2003) 76-85.

\bibitem{Bitsadze84}
A.V. Bitsadze;
\newblock On the theory of nonlocal boundary value problems,
\newblock \emph{Soviet Math. Dokl.}, \textbf{30} (1984) 8-10.

\bibitem{Bitsadze85}
A.V. Bitsadze;
\newblock On a class of conditionally solvable nonlocal boundary value problems for harmonic functions,
\newblock \emph{Soviet Math. Dokl.}, \textbf{31} (1985) 91-94.

\bibitem{Choi}
Y.S. Choi;
\newblock A singular boundary value problem arising from near-ignition analysis of flame structure,
\newblock\emph{Differential Integral Equations}, \textbf{4} (1991) 891-895.

\bibitem{Dal}
R. Dalmasso;
\newblock Positive solutions of singular boundary value problems,
\newblock\emph{Nonlinear Anal.}, \textbf{27} (1996) 645-652.

\bibitem{delpino:hdl89}
M. del Pino, M. Elgueta, R. Man\'asevich;
\newblock A homotopic deformation along $p$ of a Leray-Schauder degree result and
existence for $(|u'|^{p-2}u')' + f(t,u) = 0, u(0)=u(T)=0, p > 1$,
\newblock \emph{J. of Differential Equations}, \textbf{80} (1989) 1-13.


\bibitem{Feng}
H. Feng, W. Ge, M. Jiang;
\newblock Multiple positive solutions for $m$-point boundary-value problems with a one-dimensional $p$-Laplacian,
\newblock \emph{Nonlinear Anal.}, \textbf{68} (2008) 2269-2279.

\bibitem{Hu}
M. Garc\'{i}a-Huidobro, R. Man\'{a}sevich, P. Yan, M. Zhang;
\newblock A $p$-Laplacian problem with a multi-point boundary condition,
\newblock \emph{Nonlinear Anal.}, \textbf{59} (2004) 319-333.

\bibitem{guo:npa98}
D. Guo, V. Lakshmikantham;
\newblock``Nonlinear Problems in Abstract Cones,"
\newblock Academic Press, 1988, New York.

\bibitem{Gupta92}
C. P. Gupta;
\newblock Solvability of a three-point nonlinear boundary value problem for a second order ordinary differential equation,
\newblock \emph{J. Math. Anal. Appl.}, \textbf{168} (1992) 540-551.

\bibitem{Ha}
K. S. Ha, Y. H. Lee;
\newblock Existence of multiple positive solutions of singular
boundary value problems,
\newblock\emph{Nonlinear Anal.}, \textbf{28} (1997) 1429-1438.

\bibitem{Il'in1}
V. A. Il'in, E. I. Moiseev;
\newblock A nonlocal boundary value problem of the first kind for a Sturm-Liouville operator in its differential and finite difference aspects,
\newblock \emph{Differential Equations}, \textbf{23} (1987) 803-810.

\bibitem{Il'in2}
V. A. Il'in, E. I. Moiseev;
\newblock A nonlocal boundary value problem of the second kind for a Sturm-Liouville operator,
\newblock \emph{Differential Equations}, \textbf{23} (1987) 979-987.

\bibitem{Infante}
G. Infante, M. Zima;
\newblock Positive solutions of multi-point boundary value problems at resonance,
\newblock \emph{Nonlinear Anal.}, \textbf{69} (2008) 2458-2465.

\bibitem{kusano:pis09}
J. Jaro$\rm{\check{s}}$, T. Kusano,
\newblock A Picone type identity for second order half-linear differential equations,
\newblock \emph{Acta Math. Univ. Comenian.}, \textbf{68} (1999) 117-121.

\bibitem{MR1509338}
J. Leray, J. Schauder;
\newblock Topologie et \'equations fonctionnelles,
\newblock \emph{Ann. Sci. \'Ecole Norm. Sup.}, \textbf{51} (1934) 45-78.


\bibitem{Kim09}
C. G. Kim;
\newblock Existence of positive solutions for singular boundary value problems involving the one-dimensional $p$-Laplacian,
\newblock \emph{Nonlinear Anal.}, \textbf{70} (2009) 4259-4267.

\bibitem{Kim09A}
C. G. Kim;
\newblock Existence of positive solutions for multi-point boundary value problem with strong singularity,
\newblock \emph{Acta Appl. Math.}, \textbf{112} (2010) 79-90.

\bibitem{kusano:pis00}
T. Kusano, J. Jaro$\rm{\check{s}}$, N. Yoshida,
\newblock A Picone-type identity and Sturmian comparison and oscillation theorems
         for a class of half-linear partial differential equations of second order,
\newblock \emph{Nonlinear Anal.}, \textbf{40} (2000) 381-395.

\bibitem{Lee5}
Y. H. Lee;
\newblock A multiplicity result of positive solutions for the generalized
gelfand type singular boundary value problems,
\newblock \emph{Nonlinear Anal.}, \textbf{30} (1997) 3829-3835.

\bibitem{Liu03}
Y. Liu, W. Ge;
\newblock Multiple positive solutions to a three-point boundary value problem with $p$-{L}aplacian,
\newblock \emph{J. Math. Anal. Appl.}, \textbf{277} (2003) 293-302.

\bibitem{Ma05}
R. Ma, B. Thompson,
\newblock Global behavior of positive solutions of nonlinear three-point boundary value problems,
\newblock \emph{Nonlinear Anal.}, \textbf{60} (2005) 685-701.

\bibitem{Sun}
Y. Sun, L. Liu, J. Zhang, R.P. Agarwal;
\newblock Positive solutions of singular three-point boundary value problems for second-order differential equations,
\newblock \emph{J. Comput. Appl. Math.}, \textbf{230} (2009) 738-750.

\bibitem{wang}
Y. Wang, W. Ge;
\newblock Existence of multiple positive solutions for multipoint boundary value problems with a one-dimensional $p$-Laplacian,
\newblock \emph{Nonlinear Anal.}, \textbf{67} (2007) 476-485.

\bibitem{Wong93}
F.H. Wong,
\newblock Existence of positive solutions of singular boundary value problems,
\newblock\emph{Nonlinear Anal.}, \textbf{21} (1993) 397-406.

\bibitem{Wong08}
F. H. Wong, T. G. Chen, S. P. Wang;
\newblock Existence of positive solutions for various boundary value problems,
\newblock \emph{Comput. Math. Appl.}, \textbf{56} (2008) 953-958.

\bibitem{Xu04}
X. Xu;
\newblock Positive solutions for singular $m$-point boundary value problems with positive parameter,
\newblock \emph{J. Math. Anal. Appl.}, \textbf{291} (2004) 352-367.

\bibitem{Xu}
X. Xu, J. Ma;
\newblock A note on singular nonlinear boundary value problems,
\newblock\emph{J. Math. Anal. Appl.}, \textbf{293} (2004) 108-124.

\bibitem{Yang}
X. Yang;
\newblock Positive solutions for nonlinear singular boundary value problems,
\newblock\emph{Appl. Math. Comput.}, \textbf{130} (2002) 225-234.

\bibitem{zeidler:nfa85}
E. Zeidler;
\newblock ``Nonlinear Functional Analysis and its Applications I,"
\newblock Springer-Verlag, 1985, New York.

\bibitem{zhang:nns00}
M. Zhang;
\newblock Nonuniform nonresonance of semilinear differential equations,
\newblock \emph{J. of Differential Equations}, \textbf{166} (2000) 33-50.

\end{thebibliography}

\end{document}

