\documentclass[reqno]{amsart}
\usepackage{hyperref}

\AtBeginDocument{{\noindent\small
\emph{Electronic Journal of Differential Equations},
Vol. 2009(2009), No. 96, pp. 1--10.\newline
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu}
\thanks{\copyright 2009 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2009/96\hfil Existence of solutions]
{Existence of solutions for an abstract second-order differential
equation  with nonlocal conditions}

\author[E. Hern\'andez\hfil EJDE-2009/96\hfilneg]
{Eduardo Hern\'andez} 

\address{Eduardo Hern\'andez \newline
Departamento de Matem\'atica, I.C.M.C. Universidade de S\~ao
Paulo, Caixa Postal 668, 13560-970, S\~ao Carlos SP, Brazil}
\email{lalohm@icmc.sc.usp.br}

\thanks{Submitted December 2, 2008. Published August 11, 2009.}
\subjclass[2000]{35R10, 47D09}
\keywords{Second order differential equations; cosine function
of operators; \hfill\break\indent abstract Cauchy problem}

\begin{abstract}
 We discuss the existence of mild solutions for abstract
 second-order differential equation with nonlocal conditions.
 Also we consider some application of our results.
\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{definition}[theorem]{Definition}
\newtheorem{remark}[theorem]{Remark}
\newtheorem{corollary}[theorem]{Corollary}

\section{Introduction}

In this  paper we study the existence of mild solutions for
the abstract second order differential system 
\begin{gather}
\frac{d^2}{dt^2} \big( x(t) - g(t,x(t))\big)
 = Ax(t) +  f(t,x(t) ), \quad   t \in I:=[0,a],  \label{2} \\
 x(0) = P(x_{0},x ),  \label{3} \\
 \frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0} = Q(y_{0},x ),  \label{4}
\end{gather}
where  $A$ is  the infinitesimal generator of
a strongly continuous cosine family of bounded linear operators
$(C(t))_{t\in \mathbb{R}}$ defined on a Banach space
 $(X,\|\cdot \|) $, $x_{0},y_{0}\in X$  and
$ f,g:I\times X\to X$, $P,Q:X\times C(I,X)\to X $
 are appropriate functions.

The study of initial-value problems with  nonlocal conditions
arises to deal specially with some situations in physics. For the
importance of nonlocal conditions in different fields we refer to
\cite{BY1,BY2} and the references contained therein.
There  exists a extensive literature treating the problem of
the existence of solutions for first and second order differential
equations with nonlocal conditions. Concerning first order
differential systems we cite   the pioneers Byszewski
 works  \cite{BY1,BY2} and   \cite{BY3,BY4} between some contributions.
In the case  of second  order differential equations with
nonlocal,   we mention    \cite{St1,St2,St3,St4}  for systems
described on  finite dimensional spaces and
\cite{HH1,H4,H1,H2,H3,NT1,NT2} for systems  defined on abstract
Banach spaces.

 To the best of our knowledge, the  existence  of solutions for
differential  systems with nonlocal conditions   described  in the
abstract  form  \eqref{2}-\eqref{4}  is a  untreated topic  in the
literature,  and this fact,   is the main motivation of the
present paper. We also  remark that the ideas, results and the
general   technical framework  introduced in this paper can be
used in the study of second order abstract  neutral differential
equations,  which  is  an   additional motivation.

First, we review  some basic concepts,  notation  and properties
needed to establish our results.  Throughout this paper,
$(X, \| \cdot\| )$ is a abstract Banach space and  $A$ is
the infinitesimal generator of a strongly continuous cosine family
 $(C(t))_{t\in \mathbb{R}}$ of bounded linear operators  on $X$.
We denote by   $(S(t))_{t\in \mathbb{R}}$ the associated sine
function   which is defined by $  S(t) x = \int_{0}^{t} C(s) x
ds$, for $(t,x) \in \mathbb{R}\times X$. In addition,      $N$ and
$\tilde{N}$ are  positive
 constants such that $\|C(t)\|\leq N$ and $\|S(t)\| \leq \tilde{N}$
for every $t\in I$.

  In this paper, $[D(A)]$ represents the domain of $A$
endowed with the graph  norm given by
$\| x\|_{A} = \| x\| + \| Ax \|$, $ x \in D(A)$, while $E$ stands
for the space  formed by the
vectors $x \in X$ for which  $C(\cdot)x$ is of class $C^{1}$ on
$\mathbb{R}$. We know from \cite{Ki},  that $E$ endowed with the
norm
\[
 \|x\|_{E} = \|x\|
+ \sup_{0 \leq t \leq a} \|A S(t) x\|, \quad x \in E,
\]
 is a Banach space. The operator  valued   function
 $ \mathcal{H}(t) =
\begin{bmatrix}
 C(t) & S(t) \\ A S(t) & C(t)
 \end{bmatrix}$
is a strongly continuous group of bounded linear operators  on the
space $E\times X$ generated by the operator
 $\mathcal{A}= \begin{bmatrix} 0 & I \\ A  & 0 \end{bmatrix}$
defined on $D(A) \times E$. It follows from this that $A S(t) : E
\to X$ is a bounded linear operator  and that $AS(t) x \to 0  $  as  
$ t \to 0$, for each $x \in E$. Furthermore, if $x :[0, \infty) \to X$
is  locally  integrable,  then $y(t) = \int_{0}^{t} S(t -s) x(s)ds$
defines an $E$-valued continuous function. This assertion is a
consequence of the fact that
\[
\int_{0}^{t} \mathcal{H}(t -s)  \begin{bmatrix} 0\\ x(s)
\end{bmatrix}
 ds =   \begin{bmatrix}
   \int_{0}^{t} S(t -s) x(s)\, ds, &
\int_{0}^{t} C(t -s) x(s)\, ds  \end{bmatrix}^{T}
\]
defines an $E \times X$-valued continuous function. In addition,
it follows from the definition of the norm in $E$ that a function
$u:I \to E$  is continuous  if, and only if, it is continuous with
respect to the norm in $X$ and the set of functions
$\{A S(t) u(\cdot): t\in [0,1]\}$ is an equicontinuous  subset
of $C(I,X)$.

The existence of solutions for the second-order abstract Cauchy
problem
\begin{gather}
\label{eq5} x''(t)  = Ax(t) + h(t),\quad t \in I,\\
\label{eq7}  x(0)   = w ,\quad x'(0) = z ,
\end{gather}
where $h:I \to X$ is an integrable function, is studied  in
\cite{TW2}. Similarly, the existence of solutions of semi-linear
second-order abstract Cauchy problems has been treated in
\cite{TW1}. We  mention here that the function $x( \cdot )$
given by
\begin{equation}
\label{eq8} x(t) = C(t) w + S(t) z + \int_0^t S(t - s)h(s)ds
,\quad t \in I,
\end{equation}
is called a mild solution of (\ref{eq5})-(\ref{eq7}). 
If $w \in E$, then  the function $x( \cdot )$ is of class $C^{1}$ on
$I$  and
\begin{equation}
x'(t) = AS(t) w + C(t) z + \int_{0}^{t} C(t - s)h(s) \,ds, \,\,t
\in I.
\end{equation}
For additional details on the  cosine function theory,
we  cite  \cite{Fa,TW1,TW2,vasilev}.


Let $(Z,\| \cdot\| _{Z})$ and   $(W,\| \cdot \|_{W})$ be Banach spaces.
In this paper,  the notation
$\mathcal{L}(Z,W)$ stands for the Banach space of bounded linear
operators  from $Z$ into $W$ endowed with the uniform  operator
norm $\| \cdot\|_{\mathcal{L}(Z,W)}$.   In addition,
$B_{r}(x,Z)$ represents  the closed ball
with center at $x$ and radius $r>0$ in $Z$.

This article has three sections. In the next section we discuss the
existence of mild solutions for the system {\rm\eqref{2}-\eqref{4}}.
In  Section 3, some applications are considered.

\section{Existence  Results} \label{results}

 In this section  we study the existence of mild solutions for
the system  \eqref{2}-\eqref{4}.
 From the theory of cosine functions of operators, we introduce
the  next definition.

\begin{definition}\label{def3} \rm
A  function $x \in C(I,X)$
is  a mild solution  of   \eqref{2}-\eqref{4} if $x(0)=P(x_{0},x)$  and
\begin{equation}
\begin{aligned}
x(t)&=C(t)  (P(x_{0},x)  -  g(0,P(x_{0},x) )   )
  +  S(t)  Q(y_{0},x ) +g(t, x(t)) \\
&\quad +  \int_0^t AS(t - s)g( s,x(s) )  d s
 + \int_0^t S(t - s)f(s,x(s) )  d s,\quad t\in I.
\end{aligned}\label{E1}
\end{equation}
\end{definition}

In the rest of this article, we assume the next hypotheses:
\begin{itemize}
\item[(H1)] There exists a Banach space $(Y,\| \cdot \|_{Y}  )$
continuously included in $X$ such  that $A S(t) \in
\mathcal{L}(Y,X) $  for all $t \in I$, and
$AS(\cdot)x \in C(I, X)$ for all  $x\in Y$. Let
$N_{Y}, \,\widetilde{N}_{1}$ be  constants such that
$\|x\| \leq N_{Y} \|x\|_{Y}$ for all $ x \in X$, and
$\|AS(t)\|_{\mathcal{L}(Y,X)} \leq \widetilde{N}_{1}$ for all
$t \in I$.

\item[(H2)] The cosine function $(C(t))_{t\in \mathbb{R}}$ is
such that the range  of $ (C(t) - I )$  is closed and
$ \dim \ker (C(t) - I) < \infty$  for all  $0 < t \leq a$.
\end{itemize}

We now  introduce some  assumptions for the functions  $f,g,P$ and $Q$.
\begin{itemize}
\item[(H3)] The function $f(\cdot,y)$ is strongly measurable for
every  $y\in X$, $f(t,\cdot)$ is continuous $a.e$  for
$t\in I$ and $ g \in C(I\times X, Y )$. There are positive constants
 $c_{1}, c_{2}$,  an integrable  function  $m_{f}  : I \to [ 0,\infty )$
and a  continuous nondecreasing function
$W_f :[0,\infty ) \to (0,\infty )$ such that
$ \| f(t, y ) \| \leq m_{f}(t) W_{f} ( \|  y\|) $   and
$\max\{\| g(t, y ) \|_{Y}, \| g(t, y ) \|\} \leq  c_{1} \| y
\|+c_{2}$ for all $ (t, y) \in I \times X$.

\item[(H4)] The function  $f(\cdot,  y) : I \to X$ strongly measurable
for every $ y \in X$, $ g \in C(I\times X, Y )$   and
 there are  positive numbers  $ L_{f}, L_{g}$ such that
\begin{gather*}
\| g(t, y_{1})- g(t, y_{2})\|_{Y}
 \leq   L_{g}\| y_{1}- y_{2} \|,  \quad y_{1},  y_{2} \in X ,\\
\| f(t, y_{1})- f(t, y_{2})\| \leq
L_{f}\| y_{1}- y_{2} \|, \quad y_{1},  y_{2} \in X .
\end{gather*}

\item[(H5)] The functions $P(x_{0},\cdot),Q(y_{0},\cdot): C(I,X) \to X  $
are continuous and there are positive constants $L_{P},L_{Q}$ such that
\begin{gather*}
  \|  P(x_{0},u)-P(x_{0},v)\| \leq L_{P}\|  u-v\|,\quad
 u,v\in C(I,X), \\
 \|  Q(y_{0},u)-Q(y_{0},v)\| \leq L_{Q}\|  u-v\|,\quad
 u,v\in C(I,X).
\end{gather*}

\item[(H6)] The functions $P(x_{0},\cdot),Q(y_{0},\cdot):  C(I,X) \to X  $
are continuous, locally  bounded and   $P$ is completely continuous.
Let  $N_{Q}^{r}=\sup\{\| Q(y_{0},u)\| :   u\in B_{r}(0,C(I,X)  \}$
and $N_{P}^{r} =\sup\{\| P(x_{0},u)\| :  u\in B_{r}(0,C(I,X) \}  $.
\end{itemize}

We consider important to make some observations about the above
conditions.

\begin{remark}\label{remark3}\rm
The  assumption   (H1) and the properties of  $g$ in condition
(H3),  are linked to the integrability of the function
$s\to AS(t-s)g(s, x(s)) $.  We observe that, except for trivial cases,
the operator function $s\to AS(s)$ is not integrable  over $[0,b]$
for $b>0$.  In fact, if we assume that $AS(\cdot ) \in L^{1}([0,b])$,
then from  the relation
$C(t)x - C(s)x = A \int_{s}^{t} S(\tau) x d\tau $, which is valid for
$s\leq t\leq b$ and   $x\in X$ (see \cite{TW1}), it follows that
\begin{equation}
C(t)x - x = A \int_{0}^{t} S(\tau) x \, d\tau =  \int_{0}^{t} A S(s) x
\,  ds, \label{E3}
\end{equation}
which implies that the  $C(\cdot)$ is uniformly continuous on
$[0,b]$ and, as consequence, that    $A$ is  a   bounded linear operator,  see     \cite{TW2} for details.

On the another hand, if   (H1) and  (H3) hold, then from
Bochner's criterion for integrable functions   and the estimate
$$
\| AS(t-s) g(s, x(s))\|   \leq  \widetilde{N}_{1} (c_{1} \| x(s) \|
+c_{2}) ,
$$
we infer  that  the function  $s \mapsto AS(t-s)g(s, x(s))$ is
integrable on   $[0, t)$, for  all  $t\in I$.
\end{remark}

\begin{remark}\label{remark1}\rm
If assumption (H1) holds, then $Y $ is
continuously included in $E$. To prove this claim,  we note that
for $x\in Y$
\[
C(t)x - x = A \int_{0}^{t} S(\tau) x  d\tau =  \int_{0}^{t} A S(s) x\, ds,
\]
 which implies that $C(\cdot) x$ is of class $C^{1}$  and
$Y \subseteq E$.  Moreover, since
\[
\|x\|_{E} = \|x\| + \sup_{0 \leq t \leq a} \|A S(t)x\| \leq (N_{Y}
+ \widetilde{N}_{1}) \|x\|_{Y}
\]
when $a \geq 1$, we obtain  that the inclusion
$\iota : Y \to  E$ is continuous in this case. A similar argument
using the properties of the sine function  shows that $\iota : Y \to   E$ is also continuous for $0 < a < 1$.
To complete this remark, we  note  that   $[D(A)]$ and $E$
satisfy (H1).
\end{remark}

Our main result is  proved using a point fixed criterion for condensing
operators.  The assumption (H2)  will be  useful to this objective.

\begin{lemma}\label{lema1} \rm
 Let condition  (H2) be holds.  If $B \subseteq Y$ is  bounded in $X$
and the set  $\{ AS(t) x: t\in  I,  x \in B \}$ is relatively compact
 in $X$, then $B$ is relatively compact  in $X$.
\end{lemma}

 \begin{proof}   Let  $x \in B$. From  (\ref{E3})
and the  mean value theorem for the
Bochner integral (see \cite[Lemma 2.1.3]{Ma}) it follows that
$C(t) x - x   \in  t \, \overline{c(\{ AS(s) x : s\in [0,t] \})}$,
where $c(\cdot)$ denotes the convex hull of a set. Now, the assertion
is a consequence of the fact that
$\overline{c(\{ AS(s)y: s\in [0,t] , y \in B \})}$  is compact and
the properties of the operators $C(t) - I$.
 \end{proof}

We now establish  our first existence  result.

\begin{theorem}\label{theo1}
Let  assumptions {\rm (H1)-(H3), (H6)}
hold, and assume that the following two conditions hold
\begin{itemize}
\item[(a)] For every $t\in I$ and all   $r>0$, the set
$$
U_{r}^{t}=\{S(t)[f(s, y )+P(x_{0},u)]:  s\in I,
 y\in B_{r}(0,X), u\in B_{r}(0,C(I,X) \}
$$
is relatively compact in $X$.

\item[(b)] For each $r > 0$ and all $t\in I$, the
sets $ V_{1}^{ r} =\{A S(s)g(s, y ):   s\in I, \; y\in B_{r}(0,X)\}$
 and $ V_{2}^{ r}=\{S(t) Q(y_{0},u): u\in B_{r}(0,C(I,X))\}$
are  relatively compact in $X$,  and the set of functions
$\{ t\mapsto  g(\cdot,u(\cdot)) : u\in B_{r}(0,C(I,X))\}$ is
 equicontinuous on  $I$.
\end{itemize}
If
\begin{equation} \label{des2}
\limsup_{r\to \infty}\big[\frac{N  N_{P}^{r} +  \tilde{N} N_{Q}^{r}
+ W_{f}(r)\tilde{N}a }{r}\big]
+  c_{1}\Big(1+N+\int_{0}^{a}\| AS(t)\|_{\mathcal{L}(Y,X)}dt\Big) <1,
\end{equation}
then there exists a mild solution  of \eqref{2}-\eqref{4}.
\end{theorem}

\begin{proof} Let   $\Gamma:C(I,X) \to  C(I,X) $  be the map
defined by
\begin{align*}
\Gamma u (t)&=  C(t)( P(x_{0},u) -  g(0, u(0))   ) +  S(t)Q(y_{0},u)
 +   g(t,u(t) ) \\
&\quad +\int_{0}^{t} AS(t-s) g(s, u(s) ) ds
 + \int_{0}^{t} S(t -s) f(s, u(s) ) ds,\quad t \in I,
\end{align*}
and consider the decomposition  $\Gamma=\Gamma_{1}+\Gamma_{2}$ where
\begin{gather*}
\Gamma_{1}u (t) =   C(t)(  P(x_{0},u) -  g(0, u(0))   )
 +  S(t) Q(y_{0},u)    +   g(t,u(t)), \quad  t\in I,  \\
\Gamma_{1}u (t) = \int_{0}^{t} AS(t-s) g(s, u(s) ) ds
 + \int_{0}^{t} S(t -s) f(s, u(s) ) ds, \quad  t\in I.
\end{gather*}
 From  Remark \ref{remark3} and the properties of the functions
$f,g,P,Q$, it is easy to see that
 $ \Gamma_{i} u\in C(I,X)$ for $i=1,2$.

Now, we  prove that $\Gamma$ is  completely continuous.
Let  $(u^n)_{n\in\mathbb{N}}$ be  a sequence in $C(I,X)$
and $u\in C(I,X) $ such that $u^n\to u$.  Let
$(u^{n_{j}} )_{j\in\mathbb{N}}$  be a sub-sequence of
$(u^n)_{n\in\mathbb{N}}$.  From the condition \textbf{(b)}
and Lemma \ref{lema1},  it is easy to see that the set of functions
$\{  g(\cdot,u^{n_{j}}(\cdot)): j\in \mathbb{N}\}$ is relatively
compact in $C(I,X)$. Then,  there exists a    sub-sequence
$(u^{n_{j_{p}}} )_{p\in\mathbb{N}}$   of
$(u^{n_{j}} )_{j\in\mathbb{N}}$  such that
$ g(s,u^{n_{j_{p}}}(s))\to g(s,u(s))  $    uniformly for
$s\in I$ as $p\to \infty$, from which  we obtain that
$\Gamma_{1} u^{n_{j_{p}}}\to  \Gamma_{1}  u $ in $C(I,X)$
as $p\to \infty$.  Moreover, an standard application of the
 Lebesgue dominated convergence Theorem permit to prove that
$\Gamma_{2} (u^{n_{j_{p}}})\to \Gamma_{2} u$ in
 $C(I,X)$ as $p\to \infty$ which implies that
$\Gamma (u^{n_{j_{p}}})\to \Gamma u$ in  $C(I,X)$ as $p\to \infty$.
Since the  $(u^{n_{j}} )_{j\in\mathbb{N}}$ is an arbitrary
subsequence of $(u^{n})_{n\in\mathbb{N}}$, we can  conclude
that $\Gamma u^{n}\to \Gamma u$ in  $C(I,X)$. Thus,  $\Gamma$
is continuous.

 From  \eqref{des2},  there exists a positive number
$r$ such that $\Gamma (B_{r}(0,C(I,X)))\subset B_{r}(0,C(I,X)) $.
In fact, let  $r>0$ be such that
\begin{equation}
\frac{1}{r}\big[ N   N_{P}^{r}  + \tilde{N}     N_{Q}^{r}
+ W_{f}(r)\tilde{N}a\big]
+ (c_{1}+\frac{c_{2}}{r})(1+N+\int_{0}^{a}\| AS(t)\|_{\mathcal{L}(Y,X)}dt)
<1. \label{des3}
\end{equation}
Then,  for $t\in [0,a]$ and  $u\in B_{r}(0,C([0,a],X))$   we see that
\begin{align*}
 \| \Gamma u (t)\|
&\leq    N(     N_{P}^{r} + c_{1}r+c_{2})  +
  \tilde{N}      N_{Q}^{r} +  c_{1}r +c_{2}   \\
&\quad +  \int_{0}^{t}\| AS(t-s)\|_{\mathcal{L}(Y,X)} \|  g(s,u(s)) \| ds
  +\widetilde{N}   \int_{0}^{t}m_{f}(s)  W( \| u(s)\|) ds  \\
&\leq    \big[  N    N_{P}^{r}   + \tilde{N}    N_{Q}^{r}
 + W_{f}(r)\tilde{N}\int_{0}^{a}m_{f}(s)ds \big] \\
&\quad +  (c_{1}r+ c_{2} )(1+N+\int_{0}^{a}\|
  AS(t)\|_{\mathcal{L}(Y,X)}dt),
\end{align*}
which  from (\ref{des3}) implies that $\Gamma u \in B_{r}(0,C(I,X))$.
Thus,  $\Gamma (B_{r}(0,C(I,X)))\subset B_{r}(0,C(I,X)) $.

 From  Lemma \ref{lema1},  the assumptions  (H6) and  (b),
 it is easy to see that     $\Gamma_{1}  $    is completely continuous.
Moreover, from   \cite[Lemma 3.1]{HH3}  we infer that  $\Gamma _{2}$
is also  completely continuous, which complete the proof  that
$\Gamma $ is completely continuous.  Now, from  the
Schauder's point fixed Theorem we obtain a mild solution
for \eqref{2}-\eqref{4}.
\end{proof}


\begin{proposition}\label{prop1}
Assume that  the assumptions in Theorem  \ref{theo1} be hold.
If  $x(\cdot)$  is  a mild solution of   \eqref{2}-\eqref{4},
$ P(x_{0},x)\in Y$   and $\frac{d}{dt}C(t)g(0,x(0))\big|_{t=0}=0  $,
then    $\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0} =Q(y_{0},x)$. 
\end{proposition}

 \begin{proof}  At first, we note that from the inequality
\[
\|\frac{1}{t} \int_{0}^{t} S(t - s) f(s, x(s)) \, ds\| \leq N
\int_{0}^{t} \|f(s, x(s))\| \, ds
\]
it follows  that $ \frac{1}{t} \int_{0}^{t} S(t - s) f(s, x(s)) ds\to 0 $
as $t\to 0$.
  In addition, for $\delta >
0$, we can write
\begin{equation}
\begin{aligned}
 \int_{0}^{t} A S(t - s) g(s, x(s))  ds
& =  (I -\frac{1}{\delta} S(\delta)) \int_{0}^{t} A S(t - s)
  g(s, x(s))\, ds   \\
&\quad +  \frac{1}{\delta} \int_{0}^{t}  S(t - s) A S(\delta) g(s,
x(s)) \, ds.
\end{aligned}\label{E2}
\end{equation}
Let $r > 0 $ be such that $\|x(s)\|  \leq r$ for every
$s\in I$. Since $A S(t - s) g(s, x(s)) \in V_{1}^{r}$, it follows from
the mean value theorem for the Bochner integral \cite[Lemma 2.1.3]{Ma}
 that $
\int_{0}^{t} A S(t - s) g(s, x(s)) ds \in t \overline{c(V_{1}^{r} )}$,
so that
\[
(I - \frac{1}{\delta} S(\delta)) \frac{1}{t} \int_{0}^{t} A S(t -
s)
 g(s, x(s)) \, ds \in  (I - \frac{1}{\delta} S(\delta))
\overline{c(V_{1}^{r} )}.
\]
In view of the fact that $(I - \frac{1}{\delta} S(\delta))x \to 0$,
as $\delta \to 0$, for each $x \in X$ and $\overline{c(V_{1}^{r} )}$ is
a compact, we can affirm that
$(I - \frac{1}{\delta} S(\delta))x \to 0$, as $\delta \to 0$, uniformly
for $x \in \overline{c(V_{1}^{r} )}$, which implies that the first
term of the right hand side of (\ref{E2})  converge to zero as
$\delta\to 0$.  Moreover,  if   $c_{\delta}>0$ is  such that
$ \|A S(\delta) g(s, x(s))\| \leq c_{\delta}$ for all  $s\in I$, then
\[
\big\| \frac{1}{\delta} \int_{0}^{t}  S(t - s) A S(\delta) g(s, x(s))
\, ds\big\|
\leq \frac{ N}{\delta}  \int_{0}^{t}(t - s) c_{\delta} \,
ds \leq   \frac{N c_{\delta}}{2 \delta} t^2.
\]
 From  the above remarks, we infer that
$ \frac{1}{t} \int_{0}^{t} A S(t - s) g(s, x(s)) ds \to 0$, as
$ t \to 0^{+}$.
Finally, by using that
$ P(x_{0},x)\in Y$ and $\frac{d}{dt}C(t)g(0,x(0))\big|_{t=0}=0  $,
we obtain
\begin{align*}
&\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0} \\
&= \lim_{t \to 0^{+}} \frac{1}{t}\big( C(t) P(x_{0},x )-
P(x_{0},x) \big)  -\frac{1}{t}[C(t)g(0,x(0))-g(0,x(0))] \\
&\quad +    \frac{S(t)}{t} Q(y_{0},x )
 +  \lim_{t \to 0^{+}} \frac{1}{t} \int_{0}^{t} A S(t - s)
g(s, x(s))ds  \\
&\quad  +  \lim_{t \to 0^{+}} \frac{1}{t} \int_{0}^{t}  S(t - s)
f(s, x(s)) \, ds  \\
&= \lim_{t \to 0^{+}} \frac{1}{t}\int_{0}^{t} AS(s) P(x_{0},x) ds
+  \frac{S(t)}{t} Q(y_{0},x)  =Q(y_{0},x),
\end{align*}
which completes the proof.
\end{proof}

The following result is a  consequence of Theorem \ref{theo1}
and Proposition \ref{prop1}.

\begin{corollary} \label{C1}
Let conditions  {\rm (H1)-(H3), (H6)}  hold with
$m_{f} \in L^{\infty}(I)$.  Assume  $S(t)$ is
compact, for  all  $t \geq 0$  and
\begin{itemize}
\item[(b*)] For $r > 0$, the
set  $ V_{1}^{ r} =\{A S(s)g(s, y ):   s\in I, \;   y\in
B_{r}(0,X)\}$ is   relatively compact in $X$,  and the set of
functions $\{g(\cdot,u(\cdot))  : u\in B_{r}(0,C(I,X))\}$ is
 equicontinuous on  $I$.
\end{itemize}
 If    \eqref{des2} is valid,  then  there exists a mild
solution of  $x(\cdot)$  of \eqref{2}-\eqref{4}. Moreover,
if   $ P(x_{0},x)\in Y$   and $\frac{d}{dt}C(t)g(0,x(0))\big|_{t=0}=0 $
then  $\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0}  =   Q(y_{0},x)$.
\end{corollary}

The proof of the next result is an standard application of the
contraction mapping principle. We  omit it.

\begin{theorem}\label{theo3}
Let {\rm (H1), (H4),  (H5)} hold. If
 $$
\big[ L_{g} (N_{Y} + a \widetilde{N}_{1}) + a L_{f} \tilde{N}
 + NL_{P}+  \tilde{N}L_{Q}\big]  < 1,
$$
then there exists a unique  mild solution  $x(\cdot)$ of
\eqref{2}-\eqref{4}.   Moreover,  $ P(x_{0},x)\in Y$ and
$\frac{d}{dt}C(t)g(0,x(0))\big|_{t=0}=0 $ then
$\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0}  =   Q(y_{0},x)$.
\end{theorem}

\section{ Applications}\label{example}

In this section, we consider some applications of our abstract results.
At first,  we  discuss briefly   the  particular  case  in which $X$
is finite   dimensional.
 In this  case, the operator $A$  is a matrix of order $n \times n$ which
generates the uniformly continuous cosine function
$C(t)=\cosh{(t A^{1/2})}=\sum_{n=1}^{\infty}\frac{t^{2n}}{(2n)! }A^{n}$,
with associated  sine function
$S(t)=A^{-\frac{1}{2}}\sinh{(t A^{1/2})}
 =\sum_{n=1}^{\infty}\frac{t^{2n+2}}{(2n+1)!}A^{n}$
(here,  the expressions  $\cosh{(t A^{1/2})}$ and
$\sinh{(t A ^{1/2})}$ are purely symbolic and do not assume the
existence  of the square roots of $A$). We note that the  condition
(H1) is  automatically satisfied with  $Y = X $,
the operators   $C(t)$,  $S(t)$, $AS(t) $ are  compact for  all
$t\in \mathbb{R}$, and
$ \|C(t)\| \leq \cosh {(t \|A\|^{1/2})}$ and
$ \|S(t)\| \leq \|A\|^{-1/2} \sinh{(t \|A\|^{1/2})}$  for all
$t\in \mathbb{R}$.

 The next proposition is a re-formulation  of Theorem \ref{theo1}.
In  this result,
$
\gamma=   \cosh{(a \|A\|^{1/2})}   +\|A\|^{-1/2} \sinh{(a\|A\|^{1/2})}
$
  and (H3*)  is the   condition,
\begin{itemize}
\item[(H3*)] The function $f(\cdot,y)$ is strongly measurable
for every  $y\in X$, $f(t,\cdot)$ is continuous a.e.  for
 $t\in I$ and $ g \in C(I\times X, X )$. There are positive constants
$c_{1}, c_{2}$,  an integrable  function  $m_{f}  : I \to [ 0,\infty )$
and a  continuous nondecreasing function
$W_f :[0,\infty ) \to (0,\infty )$ such that
$\| g(t, y ) \| \leq  c_{1} \| y \|+c_{2}$  and $ \| f(t, y ) \|
 \leq m_{f}(t) W_{f} ( \|  y\|) $  for all $ (t, y) \in I \times X$.
\end{itemize}

\begin{proposition}
 \label{P1} Assume  {\rm (H3*), (H6)} hold, and for all  $r>0$  the
set of functions $\{ { g(\cdot,u(\cdot) ) } :  u \in
B_{r}(0,C(I,\mathbb{R}^{n} ))\}$  is  equicontinuous on  $I$ and
\[
\limsup_{r\to \infty}\frac{\gamma  }{r}
[  N_{P}^{r} +    N_{Q}^{r} + W_{f}(r)a]
 +  c_{1}(1+ \gamma(1 +a \| A\| ) ) <1.
\]
Then there exists a mild solution $x(\cdot)$ of \eqref{2}-\eqref{4}.
If, in addition,
$$
\frac{d}{dt}C(t)g(0,x(0))\big|_{t=0}=0,
$$
 then $\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0}  =   Q(y_{0},x)$.
\end{proposition}


To complete this  section, we apply our abstract results on an concrete
second order partial differential equation.
Consider the  differential  system
\begin{gather}
\frac{\partial^2}{\partial t^2}\big[ u(t,\tau)-
 \int_{0}^{\pi} b(  \omega ,\tau ) u(t, \omega) d\omega \big]
=   \frac{\partial^2}{\partial \tau^2}u(t,\tau) +
F\big(t,u(t,\tau) \big), \label{eqe1} \\
u(t,0 ) =  u(t,\pi )=0,   \label{eqe2}  \\
u(0, \tau) =  x_{0}   (\tau) + \int_{0}^{a} p(u(s,\tau)) d s, \label{eqe3}\\ \label{eqe4}
\frac{\partial}{\partial t} u(0, \tau)= y_{0} (\tau)
+ \int_{0}^{a} q(u(s,\tau )) d s,
\end{gather}
for   $(t,\tau)\in I\times J=[0,a]\times [0,\pi]$.

To study this  system we chose the space  $X= L^2([0,\pi])$, and we
assume   $x_{0}, y_{0} \in X$.
 In addition, we consider  the  operator   $A:D(A) \subseteq X\to
X$   by $ A x= x'' $, where
$ D(A) = \{ x \in X :x'' \in X, x(0) = x(\pi) = 0\}$.
It is well-known that $A$ is the infinitesimal generator of a
strongly continuous cosine family $(C(t))_{t\in \mathbb{R}}$ on $X$.
Furthermore, $A$ has a discrete spectrum, the eigenvalues are $-n^2$,
for $n \in \mathbb{N}$,  with corresponding  eigenvectors
${ z_{n} (\tau) = \big(\frac{2}{\pi}\big)^{1/2} \sin (n \tau)}$,
the set of functions   $\{z_{n} : n \in  \mathbb{N}\}$ is an
orthonormal basis of $X$   and the
following properties hold.
\begin{itemize}
\item[(a)]
For $z \in X$,  $C(t)z =  \sum_{n=1}^{\infty} \cos{(nt)} \langle  z,
z_{n} \rangle z_{n}$ and   the  associated sine function is given by $S(t)
z = \sum_{n=1}^{\infty} \frac{\sin(nt)}{n} \langle z, z_{n}
\rangle z_{n}$. It follows from the last expression that $S(t)$  is
compact  for all  $t\in \mathbb{R}$ and $\|C(t)\| =\|S(t)\|=
 1$, for all  $ t \in \mathbb{R}$. In addition,
$A z =  - \sum_{n=1}^{\infty} n^2 \langle  z,
z_{n} \rangle z_{n}$, for  $z \in D(A)$.

 \item[(b)]  If $\Phi$ is the group of translations on $X$ defined
by $\Phi(t)x(y_{0})=\tilde{x}(y_{0}+t)$, where $\tilde{x}\cdot $ is the
extension of $x\cdot$ with period $2\pi$, then $C(t)=\frac{1}{2}(
\Phi(t)+\Phi(-t))$ and    $A=B^2$, where $B$ is the
infinitesimal generator of $\Phi$ and $ E=\{ x \in H^{1}(0,\pi) :
x(0) = x(\pi) = 0 \}$ (see \cite{Fa} for details). In particular,
we observe that the inclusion $\iota :E \to X$ is compact.
\end{itemize}

In what the follows, we assume that $x_{0}  \in H^{1}([0, \pi])$  and
the  conditions.
\begin{itemize}
\item[(i)] The function   $  b(\cdot)$ is of class $C^2$ on
$I\times J$ and  $b(  \omega, \pi)=b(  \omega,\, 0) = 0$
 for all  $    \omega  \in   I$.

 \item[(ii)] The function $F:I\times [0,\pi]\to \mathbb{R}$ is continuous
and there is $L_{f}>0$   such that
$$
|F(t,\tau_{1})- F(t,\tau_{2})|\leq L_{F}|\tau_{1}-\tau_{2} |, \quad
t\in I, \tau_{i}\in \mathbb{R}.
$$
  \item[(iii)] The function $p,q  :\mathbb{R} \to \mathbb{R} $ are
continuous  and there  are positive constants $L_{p}, L_{q}$ such that
\begin{gather*}
   | p (\mu_{1})- p (\mu_{2})| \leq   L_{p} |\mu_{1} - \mu_{2}|,
  \quad \mu_{i}\in \mathbb{R} , \\
   |q (\mu_{1})- q (\mu_{2})| \leq  L_{q} |\mu_{1} - \mu_{2}|,  \quad
\mu_{i}\in \mathbb{R} .
\end{gather*}
\end{itemize}

 Let  $f, g :  X \to X $ and  $P,Q:C(I, X)\to X$   be the functions
defined by $f(t,x)(\tau ) = F(t, x(\tau))$   and
\begin{gather*}
g(t,x)(\tau ) = \int_{0}^{\pi} b(\omega,\tau) x (  \omega) d \omega ,  \\
P(u)(\tau ) = x_{0}(\tau)   + \int_{0}^{a} p(u(s,\tau)) d s, \\
Q(u)(\tau ) = y_{0}(\tau)   + \int_{0}^{a} q(u(s,\tau)) d s.
\end{gather*}
Under the above conditions, the functions $f,P,Q$  are   Lipschitz
continuous functions with Lipschitz constants
$L_{F}, L_{P}a^{3/4}$ and $L_{Q}a^{3/4}$ respectively. In addition,
$g(\cdot)$ is continuous, $g(t,\cdot)$ is a bounded linear operator
for all $t\in I$,  $g $ is $D(A)$-valued,
$$
\sup_{t\in I}\| g(t,\cdot)\|_{\mathcal{L}(X, [D(A)])}
\leq L_{g}=\Big(\int_{0}^{\pi}\int_{0}^{\pi}(\frac{\partial^2}{\partial
 \tau^2} b( \omega ,\tau ) )^2  d\omega   d\tau\Big)^{1/2},
$$
$N_{[D(A)]}\leq 1$ and $\widetilde{N_{1}}\leq 1 $.

 The next result follows directly from Theorem  \ref{theo3}.
We remark that for $z\in X $,
 $\frac{d}{dt}C(t)g(0,z)=AS(t)g(0,z)=S(t)Ag(0,z)$  so that,
$\frac{d}{dt}C(t)g(0,z)\big|_{t=0}=0 $.

\begin{proposition}
If  $ \big[ L_{g} (1 + a)  + a L_{f} +  a^{3/4}(L_{P}+   L_{Q})\big]  < 1$,
 then there exists a unique mild solution of \eqref{eqe1}-\eqref{eqe4}.
Moreover, $\frac{d}{dt}(x(t)-g(t,x(t)))\big|_{t=0}=Q(y_{0},x )$ if
$ P(x_{0},x)\in Y$.
\end{proposition}

\begin{thebibliography}{00}

\bibitem{BY1} L. Byszewski, V. Lakshmikantham;
Theorem about the existence and uniqueness of a solution of a nonlocal abstract
Cauchy problem in a Banach space.  Appl. Anal. \textbf{40 } (1)(1991)
11-19.

\bibitem{BY4} Byszewski, Ludwik;
\emph{Application of properties of the right-hand sides of evolution
equations to an investigation of nonlocal evolution problems}.
Nonlinear Anal., 33 (1998), no. 5, 413-426.

 \bibitem{BY2} L. Byszewski;
\emph{Theorems about the existence and uniqueness
of solutions of a semilinear evolution nonlocal Cauchy problem}.
  J. Math. Anal. Appl. \textbf{162} (2) (1991)  494--505.

\bibitem{BY3} L. Byszewski, H. Akca;
\emph{Existence of solutions of a
semilinear functional-differential evolution nonlocal problem}.
 Nonlinear Analysis TMA. \textbf{34} (1) (1998) 65-72.

\bibitem{Fa}  Fattorini, H. O.;
\emph{Second Order Linear Differential
Equations in Banach Spaces}, North-Holland Mathematics Studies,
Vol.  108, North-Holland, Amsterdam,  1985.

\bibitem{HH1}  Hern\'andez, Eduardo; Henr\'iquez, Hern\'an;
\emph{Existence of solutions of a  second order abstract functional cauchy
problem with nonlocal conditions}. Ann. Polon. Math.
 88 (2006), 141-159.

\bibitem{H4} Hern\'andez, Eduardo; Henr\'iquez, Hern\'an;
\emph{Existence results for a second order differential equation
with nonlocal conditions}. To appear in Funkcialaj  Ekvacioj.

\bibitem{H1} Hern\'andez, Eduardo; Henr\'iquez, Hern\'an R.;
\emph{Global solutions for a  functional second  order abstract  cauchy
problem with nonlocal conditions}.
Ann. Polon. Math. 83 (2004)  149-170. \label{14}

\bibitem{H2}  Hern\'andez, Eduardo;
\emph{Existence of solutions to a second order partial differential
equation with  nonlocal conditions}.
Electron. J. Differential Equations.
Vol. 2003 (2003), No. 51, pp. 1-10.

\bibitem{H3}  Hern\'{a}ndez, Eduardo;  Pelicer, Mauricio;
\emph{Existence results for a second-order
Existence results for a second-order abstract Cauchy problem
with nonlocal conditions}. Electron. J. Differential Equations.
  Vol. 2005 (2005), No. 73, pp. 1-17.

\bibitem{HH3}  Hern\'andez, E.; McKibben, M. A.;
\emph{Some comments on Existence of solutions of abstract nonlinear
second-order neutral functional integrodifferential equations},
in Comput. Math. Appl. 46 (8-9) (2003). Comput. Math.
Appl. 50 (5-6) (2005), 655-669.

\bibitem{Ki}  Kisy\'nski, J.;
\emph{On cosine operator functions and one
parameter group of operators}, Studia Math. 49 (1972), 93-105.

\bibitem{NT1} S. K. Ntouyas;
\emph{Global existence results for certain second order delay
integrodifferential equations with nonlocal conditions}.
Dynam. Systems Appl. \textbf{7} (3) (1998),  415-425.

\bibitem{NT2}  S. K. Ntouyas, P. Ch. Tsamatos;
\emph{Global existence for second order semilinear ordinary and delay
integrodifferential equations with nonlocal conditions}.
Appl. Anal. \textbf{67} (3-4) (1997), 245-257.

\bibitem{Ma} Martin, R. H.;
\emph{Nonlinear Operators and Differential
Equations in Banach Spaces}, Robert E. Krieger Publ. Co., Florida,
1987.

\bibitem{St1}  Stan\v ek, S.;
\emph{On solvability of nonlinear boundary value
problems for the equation $(x'+g(t,x,x'))'=f(t,x,x')$ with
one-sided growth restrictions on $f$.}  Arch. Math. (Brno) \textbf{
38 } (2) (2002),  129--148.

\bibitem{St2} Stan\v ek, S.;
\emph{The degree method for condensing operators in periodic boundary
value problems.}
Nonlinear Anal.  \textbf{48} (4)(2002),  535--550.

\bibitem{St3} Stan\v ek, S.;
\emph{Functional boundary value
problems for second order functional differential equations of the
neutral type.}  Glas. Mat. Ser. III \textbf{36} (56)(1) (2001),
73--84.

\bibitem{St4} Stan\v ek, S.;
\emph{Boundary value problems for
systems of second-order functional differential equations. }
 Proceedings of the 6th Colloquium on the Qualitative
 Theory of Differential Equations (Szeged, 1999), No. 28, 14
  pp. (electronic), Proc. Colloq. Qual. Theory Differ.
   Equ., Electron. J. Qual. Theory Differ. Equ., Szeged, 2000.

\bibitem{TW1}  Travis, C. C.,  Webb, G. F.;
\emph{Cosine families and abstract nonlinear second order differential
equations}.  Acta
Math. Acad. Sci. Hungaricae,  32 (1978),  76-96.

\bibitem{TW2}  Travis, C. C., Webb, G. F.;
\emph{Compactness, regularity,  and uniform continuity properties
of strongly continuous cosine families}, Houston J. Math. 3 (4) (1977)
555-567.

\bibitem{vasilev} Vasil'ev, V. V.; Piskarev, S. I.;
\emph{Differential equations in Banach spaces. II.
Theory of cosine operator  functions. Functional analysis.}
J. Math. Sci. (N. Y.),  122 (2004),
 no. 2, 3055-3174.

\end{thebibliography}

\end{document}
