\documentclass[reqno]{amsart}
\usepackage{hyperref}

\AtBeginDocument{{\noindent\small
\emph{Electronic Journal of Differential Equations},
Vol. 2013 (2013), No. 31, pp. 1--18.\newline
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu}
\thanks{\copyright 2013 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2013/31\hfil Solutions in several types of periodicity]
{Solutions in several types of periodicity for partial
 neutral integro-differential equation}

\author[J. C. dos Santos, S. M. Guzzo\hfil EJDE-2013/31\hfilneg]
{Jos\'e Paulo C. dos Santos, Sandro M. Guzzo}  % in alphabetical order

\address{Jos\'e Paulo C. dos Santos \newline
Instituto de  Ci\^encias Exatas - 
Universidade Federal de Alfenas,
Rua Gabriel Monteiro da Silva, 700,
37130-000 Alfenas - MG, Brazil}
\email{zepaulo@unifal-mg.edu.br}

\address{Sandro M. Guzzo \newline
Universidade Estadual do Oeste do Paran\'a - UNIOESTE,
Colegiado do curso de Mate\-m\'atica,
Rua Universit\'aria, 2069. Caixa Postal 711,
85819-110 Cascavel - PR, Brazil}
\email{smguzzo@gmail.com}

\thanks{Submitted August 4, 2012. Published January 28, 2013.}
\thanks{J. C. dos Santos was supported by  grant CEX-APQ-00476-09 
from FAPEMIG/Brazil.}
\subjclass[2000]{45K05, 34K40, 34K14, 45N05}
\keywords{Integro-differential equations;  neutral differential equations;
\hfill\break\indent  asymptotically almost periodic; asymptotic compact 
 almost automorphic;
\hfill\break\indent $S$-asymptotically $\omega$-periodic; 
asymptotically $\omega$-periodic}

\begin{abstract}
 In this article we study the existence of mild solutions in several types
 of periodicity for partial neutral integro-differential equations with
 unbounded delays.
\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{definition}[theorem]{Definition}
\newtheorem{example}[theorem]{Example}
\newtheorem{remark}[theorem]{Remark}
\allowdisplaybreaks

\section{Introduction}

In this article we study  the existence of  several types of
mild solutions for the partial neutral integro-differential equation
\begin{gather}
\frac{d}{dt} (x(t) + f(t,x_t)) = Ax(t)+ \int_{0}^{t} B(t-s)x(s) ds
 + g(t,x_t), \label{eqi1} \\
x_0 = \varphi \in   \mathcal{B}, \label{eqi2}
\end{gather}
where  $ A:D(A)\subset X\to X$ and  $B(t):D(B(t))\subset X\to X$, $t\geq 0$,
are closed linear  operators; $(X, \| \cdot \|) $ is a Banach  space;
 the history
$x_{t}:(-\infty,0]\to X$, $x_{t}(\theta)=x(t+\theta)$, belongs to an
abstract phase  space ${\mathcal{B}}$ defined
axiomatically,   and  $ f,g:I\times \mathcal{B} \to X $ are appropriated
 functions.


The literature relative to ordinary neutral
differential equations is very  extensive, thus  we suggest
the  Hale and Lunel book \cite{HA1} concerning this
matter. Referring to partial neutral functional differential
equations, we cite the pioneer articles Hale \cite{hale2} and   Wu
\cite{wu3,wu4,wu5}  for finite delay equations,
Hern\'{a}ndez and Henriquez \cite{HH2,HH1}, Hern\'{a}ndez \cite{HH3}  for the
unbounded delay,  Hern\'{a}ndez and dos Santos \cite{HJ2} and
Henr\'{\i}quez  et al. \cite{HJ1,Joseh3} and Dos Santos et al.
\cite{Dos,Dos1,DosSantos} for partial neutral integro-differential
equations with unbounded delay.

The existence of almost automorphic, asymptotically almost automorphic,
almost periodic, asymptotically almost periodic,
$S$-asymptotically $\omega$-periodic and asymptotically $\omega$-periodic
solutions to differential equations is among the most
attractive topics in mathematical analysis due to their possible applications
in areas such as physics, economics, mathematical
biology, engineering, etc.
(cf. \cite{Ravi, B, BD,Caiedo,lizama,HH11,TG,DDD,d1,Hui,Dos1,EN, H2008,HJEJ,
g2,g3,veech1,zaid1,zaki1}).
The concept of asymptotically almost automorphic,  was introduced in the
literature in the early eighties by N'Gu\'er\'ekata \cite{gaston}.
However, the literature concerning $S$-asymptotically $\omega$-periodic
functions with values in Banach spaces is recent
 (cf \cite{Caiedo,Cue1,Cue2,M1,H2008}).
 The existence of asymptotically almost automorpic,
$S$-asymptotically $\omega$-periodic functions and asymptotically
 $\omega$-periodic for the partial neutral system
\eqref{eqi1}-\eqref{eqi2} is an untreated topic in the literature
and this fact is the main motivation of the present work.

This paper is organized in four sections.  In Section
\ref{preliminaries} we
 mention a few results and notations related with  resolvent of operators and
 of  several types of
 periodicity. In Section \ref{ExistenceResults} we
 study the existence of  several types of
 periodicity  mild solutions
to the partial neutral system \eqref{eqi1}-\eqref{eqi2}. In Section
4, we discuss the existence and uniqueness of  several types of
 periodicity   solution to a concrete partial neutral
integro-differential equation with delay, as an illustration to our
abstract results.

\section{Preliminaries}\label{preliminaries}

 Let $(Z,\|\cdot\|_{Z})$ and $(W,\|\cdot\|_{W})$ be
Banach spaces. We denote by $\mathcal{L}(Z,W)$  the space of bounded linear operators from $Z$ into $W$ endowed with norm of
operators, and we write simply $\mathcal{L}(Z)$ when $Z = W$.
By $\mathbf{R}(Q)$ we denote  the range of a map $Q$ and for  a
closed linear operator $P: D(P)\subseteq Z \to W$, the notation $[D(P)]$ represents the domain of $P$ endowed with the graph
norm, $\|z\|_{1} = \|z\|_{Z} + \|P z\|_{W} $,  $z \in D(P)$. In the case $Z=W$,
the notation  $\rho(P) $ stands for the resolvent
set of $P$, and $R(\lambda, P) = (\lambda I - P)^{-1}$ is the resolvent
operator of $P$. Furthermore, for appropriate functions
$K :[0,\infty)\to Z$ and $S: [0,\infty)\to \mathcal{L}(Z,W)$, the notation
 $\widehat{K}$ denotes the Laplace transform of $K$,
and $S*K$ the convolution between $S$ and $K$, which is defined by
$S*K(t)=\int_{0}^{t} S(t-s) K(s) d s$. The notation,
$B_{r}(x,Z)$ stands for the closed ball with center at $x$ and radius $r>0$
in $Z$. As usual,  $C_0([0, \infty),Z)$
represents the sub-space  of $C_b([0, \infty),Z)$ formed by the functions
which vanish at infinity and $C_{\omega}([0,\infty),X)$ denote the
spaces $C_{\omega}([0,\infty),X)= \{x \in C_{b}([0,\infty),X ): x
 \,\,\text{is $\omega$-periodic } \}$.
If $k:\mathbb{R} \to W$, we denote
  $\|k \|_{W,\infty}=\sup_{s\in \mathbb{R}}\|
k(s)\|_{W}$ or if  $k:[0,\infty) \to W$, we denote
$\|k \|_{W,\infty}=\sup_{s\in [0,\infty)}\| k(s)\|_{W}$.

In this work we will employ an axiomatic definition of the phase
space $\mathcal{B}$ similar at those in   \cite{HMN}.   More
precisely, $\mathcal{B}$ will denote a   vector space of functions
defined from $(-\infty,0]$ into $X$ endowed with a semi-norm
denoted by $\|\cdot\|_{\mathcal{B}}$ and such that the following axioms hold:
\begin{itemize}
\item[(A1)] If $x:(-\infty,\sigma+b)\to X$ with
$b>0$ is continuous on $[\sigma,\sigma +b)$ and $x_{\sigma}\in \mathcal{B}$,
then for each $t\in [\sigma,\sigma+b)$ the following
conditions hold:
\begin{itemize}
\item[(i)] $x_{t}$ is in $\mathcal{B}$,
\item[(ii)] $\|x(t)\| \leq H \|x_{t}\|_{\mathcal{B}}$,
 \item[(iii)] $\|x_{t}\|_{\mathcal{B}} \leq K(t-\sigma) \sup\{\|
x(s)\|:\sigma\leq s\leq t\}+
 M(t-\sigma)\|x_{\sigma}\|_{\mathcal{B}}$,
\end{itemize}
where $H>0$ is a constant, and $K,M:[0,\infty) \mapsto [1,\infty)$
are functions such that $K(\cdot)$ and $M(\cdot)$ are
respectively continuous and locally bounded, and $H,K,M$ are independent
 of $x(\cdot)$.

 \item[(A2)] If $x(\cdot)$ is a
function as in (A1), then $x_{t}$ is a $\mathcal{B}$-valued
continuous function on $[\sigma,\sigma+b)$.

 \item[(B1)] The space $\mathcal{B}$ is complete.

\item[(C1)] If $(\varphi^n )_{n\in\mathbb{N}}$ is a sequence in $C_{b}((-\infty,0],X) $  formed by  functions with compact
support such that { $\varphi^{n}\to \varphi$} uniformly on compact, then $\varphi \in \mathcal{B}$ and $\|\varphi^n -
\varphi\|_{\mathcal{B}} \to 0$ as $n \to \infty$.
\end{itemize}

\begin{definition}  \rm
Let  $S(t):\mathcal{B} \to \mathcal{B}$ be the $C_{0}$-semigroup defined
 by $S(t)\varphi (\theta)= \varphi(0)$ on $[-t,0]$ and
 $ S(t)\varphi (\theta)=\varphi( t + \theta )$ on $(-\infty, -t]$.
The phase space $\mathcal{B}$ is called a fading memory if $\|
S(t)\varphi\|_{\mathcal{B}}\to 0$ as $t \to \infty$ for each
 $\varphi \in \mathcal{B}$ with $\varphi (0)=0$.
\end{definition}

\begin{remark} \label{rem2} \rm
In this work we assume there exists  positive
$\mathfrak{K}$ such that
$$
\max\{K(t), M(t)\}\leq \mathfrak{K}
$$
for each $t\geq 0$. Observe that this condition is  verified, for example,
if $\mathcal{B}$ is a fading memory,  see \cite[Proposition 7.1.5]{HMN}.
\end{remark}


\begin{example} \label{example1} \rm
 The phase space $ C_{r} \times L^{p}(\rho,X)$.
 Let $r \geq 0$, $1 \leq p < \infty$ and let
$\rho:(-\infty,-r] \to \mathbb{R}$ be a
 nonnegative measurable function which satisfies the conditions
(g-5), (g-6) in the terminology  of \cite{HMN}.   Briefly, this means that
 $\rho$ is locally integrable and  there exists a non-negative,
 locally bounded function $\gamma$ on $(- \infty, 0]$ such that
$\rho(\xi+\theta) \leq \gamma(\xi) \rho(\theta)$,
 for all $ \xi \leq 0$ and $ \theta \in (- \infty , -r)\setminus N_{\xi }$,
where $N_{\xi} \subseteq (- \infty, -r)$ is a set with Lebesgue measure zero.
 The space  $C_{r} \times L^{p}(\rho,X)$ consists of all classes of functions
$\varphi: (- \infty , 0] \to X $ such that $ \varphi $ is
continuous on $[- r,0]$, Lebesgue-measurable, and $\rho \|\varphi\|^{p} $
is Lebesgue  integrable on $ (- \infty , -r )$. The
seminorm in  $ C_{r}\times L^{p}(\rho,X)$ is defined by
$$
\| \varphi \|_{\mathcal{B}}
:= \sup \{ \|\varphi(\theta)\| : -r \leq \theta \leq 0 \}
 +\Big( \int_{- \infty }^{-r} \rho(\theta ) \|\varphi(\theta)\|^{p} d\theta
\Big)^{1/p}.
$$
The space  $\mathcal{B} = C_{r} \times L^{p}(\rho;X) $ satisfies axioms
(A1), (A2), (B1).   Moreover, when $ r=0$ and $p=2$,
we can take $H = 1$, $M(t) = \gamma(-t)^{1/2}$ and
${ K(t) = 1 + (\int_{-t}^{0} \rho(\theta) \,d \theta )^{1/2}}$, for
$t \geq 0$ and
$$
\mathfrak{K} = \Big(\sup_{s\leq 0} |\gamma(s)^{1/2}|+ \Big(1+
(\int_{-\infty}^0 \rho(\theta) d\theta)^{1/2}\Big)\Big).
$$
See \cite[Theorem 1.3.8]{HMN} for details.
 \end{example}

 For better comprehension of the
 subject we shall introduce the following definitions,  hypothesis and results.
Throughout the rest of the paper we always assume that the abstract
integro-differential problem
\begin{gather}
\frac{dx(t)}{dt}  = Ax(t)+ \int_{0}^{t} B(t-s)x(s) \, ds, \label{eqa1} \\
x(0)  =  x \in X. \label{eqa2}
\end{gather}

\begin{definition} \label{D3} \rm
 A  one-parameter family of bounded linear operators
$(\mathcal{R}(t))_{t\geq 0} $  on $X$  is called a resolvent
operator  of  \eqref{eqa1}-\eqref{eqa2} if the following  conditions
are satisifed.
\begin{itemize}
\item[(a)] Function $\mathcal{R}(\cdot): [0, \infty) \to \mathcal{L}(X)$
 is strongly continuous and $\mathcal{R}(0)x=x$ for all $x\in X$.

\item[(b)] For  $x \in D(A) $,  $\mathcal{R}(\cdot)x \in C([0,\infty), [D(A)])
\cap C^{1}([0,\infty),X)$, and
\begin{gather}\label{eqrp1}
\frac{d \mathcal{R}(t)x}{dt}
= A \mathcal{R}(t)x + \int_{0}^{t} B(t-s) \mathcal{R} (s) x d s, \\
\label{eqrp2}
\frac{d \mathcal{R}(t)x}{dt}  =  \mathcal{R}(t) A x
+ \int_{0}^{t} \mathcal{R}(t-s) B(s)x d s,
\end{gather}
for every  $t\geq 0 $,

\item[(c)] There exists  constants $M>0,\delta$ such that
$\|\mathcal{R}(t)\| \leq M e^{\delta t}$ for every $ t\geq 0$.
\end{itemize}
\end{definition}

\begin{definition} \label{def3} \rm
A resolvent operator $(\mathcal{R}(t))_{t\geq 0}$ of \eqref{eqa1}-\eqref{eqa2}
 is called exponentially stable if there exists
positive constants $M, \beta$ such that
$\| \mathcal{R}(t) \| \leq M e^{- \beta t}$.
\end{definition}

In this work we  assume that the following conditions are satisfied:
\begin{itemize}
\item[(H1)] Operator $A : D(A)\subseteq X \to X $ is  the infinitesimal
generator of  an analytic semigroup $(T(t))_{t\geq 0}$  on $X$, and there
are constants  $M_{0} >0, \omega \in \mathbb{R}$ and
  $\vartheta  \in (\pi/2,\pi) $   such that
$  \rho(A) \supseteq
\Lambda_{ \omega, \vartheta } = \{ \lambda \in \mathbb{C}:
\lambda \neq \omega, \, |\arg(\lambda - \omega)| < \vartheta \} $ and
$\| R(\lambda,A) \| \leq \dfrac{M_{0}}{|\lambda - \omega|} $
for all  $\lambda \in \Lambda_{\omega, \vartheta}$.

\item[(H2) ] For all  $t\geq 0$, $B(t):D(B(t)) \subseteq X \to X $
is a closed linear operator, $D(A) \subseteq D(B(t)) $ and $B(\cdot)x $
is  strongly measurable on $(0,\infty) $ for each $x \in D(A)$.
There exists  $b(\cdot) \in L^{1}([0,\infty)) $ such that
$\widehat{b}(\lambda)$ exists for $\operatorname{Re}(\lambda) > 0$ and
$\| B(t) x \| \leq b(t) \|x\|_{1} $ for all  $t>0 $ and  $x \in D(A)$.
 Moreover, the operator valued function
$\widehat{B} : \Lambda_{\omega,\pi/2} \to \mathcal{L}([D(A)],X)$
 has an analytical extension (still denoted by $\widehat{B}$) to
$\Lambda_{\omega, \vartheta}$ such that $\| \widehat{B}(\lambda) x \|
\leq \|\widehat{B}(\lambda)\| \, \|x\|_{1}$ for all
$x \in D(A)$, and $\|\widehat{B}(\lambda)\| = O(\frac{1}{|\lambda|})$ as
 $| \lambda | \to \infty$.

\item[(H3)]  There exists a subspace   $D \subseteq D(A) $   dense in
$[D(A)] $   and   positive constants  $C_{i}$, $i=1,2$, such that
 $A(D) \subseteq D(A) $, $\widehat{B}(\lambda)(D) \subseteq D(A)$,
 $\|A \widehat{B}(\lambda) x \| \leq   C_{1} \|x\|$ for
every $x\in D$ and  all $ \lambda \in \Lambda_{\omega, \vartheta}$.
\end{itemize}


For  $r>0$, $ \theta \in (\frac{\pi}{2}, \vartheta )$ and $w \in \mathbb{R}$, set
$$
\Lambda_{r, \omega, \theta}= \{ \lambda \in \mathbb{C}:
\lambda \neq \omega, |\lambda| >r,
\,|\arg(\lambda-\omega)| < \theta  \} ,
$$
 and $\omega+\Gamma^{i}_{r,\theta }$, $i=1,2,3$, the paths
\begin{gather*}
\omega+\Gamma^{1}_{r,\theta }  =\{\omega + t e^{i\theta}: t \geq r \}, \\
\omega+\Gamma^{2}_{r,\theta }  =\{\omega + re^{i\xi}:  -\theta \leq \xi \leq \theta \}, \\
\omega+\Gamma^{3}_{r,\theta }  =\{\omega + t e^{-i\theta}: t \geq r \},
\end{gather*}
with $\omega+\Gamma_{r,\theta }=\bigcup_{i=1}^{3}\omega+\Gamma^{i}_{r,\theta }$
oriented counterclockwise. In addition,  $\Psi(G)$ is the set
$$
\Psi(G) = \{ \lambda \in \mathbb{C}: G(\lambda):=(\lambda I- A -
\widehat{B}(\lambda) )^{-1} \in \mathcal{L}(X)\}.
 $$

 The next results  establish that  the operator
family   $(\mathcal{R}(t))_{t\geq 0} $ defined by
\begin{equation}\label{defnresolv1}
\mathcal{R}(t) =  \begin{cases}
\frac{1}{2\pi i } \int_{\omega+\Gamma_{r,\theta}} e^{\lambda t}
 G(\lambda)  d\lambda,  & t>0,  \\
I, & t=0.
\end{cases}
\end{equation}
is  an exponentially stable resolvent operator for \eqref{eqa1}-\eqref{eqa2}.

\begin{theorem}[{\cite[Corollary 3.1]{Dos1}}]   \label{constnresolvente}
Suppose that  conditions {\rm (H1)--(H3)}  are
satisfied. Then, the function $\mathcal{R}(\cdot) $ is a  resolvent
operator for system  \eqref{eqa1}-\eqref{eqa2}.
If $ \omega+r < 0$, the function $\mathcal{R}(\cdot)$ is an exponentially
 stable  resolvent operator for
  system  \eqref{eqa1}-\eqref{eqa2}.
\end{theorem}

In the next result we denote by $(-A)^{\vartheta}$ the fractional
power of the operator $(-A)$, (see \cite{PA} for details).


\begin{theorem}[{\cite[Corollary 3.2]{Dos1}}]    \label{estpr1}
Suppose that conditions {\rm (H1)--(H3)}  are satisfied. Then
there  exists a positive number $ C$ such that
\begin{equation} \label{despderr}
  \| (-A)^{\vartheta}\mathcal{R}(t) \|  \leq
   \begin{cases}
 C e^{(r+\omega) t},  & t\geq1, \\
 Ce^{(r+\omega)t}t^{-\vartheta},   & t \in  (0,1),
\end{cases}
\end{equation}
for all  $ \vartheta \in (0,1)$. If $ \omega +r< 0$ and $\vartheta
\in(0,1)$, then there  exists $\phi \in L^1([0,\infty))$ such that
\begin{equation} \label{estnec}
\|(-A)^{\vartheta}\mathcal{R}(t)\| \leq \phi (t).
\end{equation}
\end{theorem}

In the remaining  of this section  we discuss the  existence  of
solutions to
\begin{gather} \label{eqanhp1}
 \frac{dx(t)}{dt}
= Ax(t)+ \int_{0}^{t} B(t-s)x(s) \ d s + f(t), \quad   t \in [0,a],     \\
\label{eqanhp2}    x(0) = z \in X,
\end{gather}
where $f\in L^{1}([0,a],  X) $.  In the sequel, $\mathcal{R}(\cdot)$
is the operator  function defined by \eqref{defnresolv1}. We begin
by introducing the following concept of classical solution.

\begin{definition}  \label{D1} \rm
A function  $x : [0,b] \to X $, $0<b\leq a $,  is called  a
classical solution of   \eqref{eqanhp1}-\eqref{eqanhp2} on $[0,b] $  if
$ x \in  C([0,b],  [D(A)]) \cap C^{1}((0,b], X) $, the condition
\eqref{eqanhp2} holds and the equation  \eqref{eqanhp1} is satisfied
on $[0,a]$.
\end{definition}

\begin{theorem}[{\cite[Theorem 2]{Grimmer4}}] \label{formvarconstnr}
Let $z\in X$. Assume that $f \in C([0,a],X)$  and  $x(\cdot) $ is a
classical  solution of  \eqref{eqanhp1}-\eqref{eqanhp2} on
$[0, a]$. Then
\begin{equation}  \label{formulavariation}
x(t) = \mathcal{R}(t) z  +  \int_{0}^{t} \mathcal{R}(t-s) f(s) \, d
s,  \quad  t \in [0,a].
\end{equation}
\end{theorem}

 Motivated by  \eqref{formulavariation}, we introduce the following concept.

\begin{definition}  \label{D2} \rm
A function $u \in C([0,a],X) $ is called  a mild solution of
\eqref{eqanhp1}-\eqref{eqanhp2} if
$$
u(t) = \mathcal{R}(t)z + \int_{0}^{t} \mathcal{R}(t-s) f(s)\, d s,
\quad t\in[0,a].
$$
\end{definition}

To establish our existence result, motivated  by the  previous facts,
we introduce the following assumptions.
 \begin{itemize}
\item[(P1)] There exists a Banach space  $(Y,\|\cdot\|_{Y}) $
 continuously included in $X$ such that the following conditions are verified.
\begin{itemize}

\item[(a)] For every   $t\in (0,\infty)$,
$ \mathcal{R}(t)\in\mathcal{L}(X)\cap
\mathcal{L}(Y,[D(A)])$  and  $ B(t) \in \mathcal{L}(Y,X)$. In
addition, $A\mathcal{R}(\cdot)x, B(\cdot )x \in C((0,\infty),X) $
 for every   $ x \in Y$.
\item[(b)] There are positive constants
  $ M, \beta$ such that
  $$
\|\mathcal{R}(s) \|  \leq   M e^{-\beta s}, \quad s\geq 0.
$$
\item[(c)] There exists $ \phi \in L^1([0,\infty))$ such that
 $\| A\mathcal{R}(t) \|_{\mathcal{L}(Y,X)}  \leq  \phi(t),  \ \  t\geq0$.
\end{itemize}
\item[(PF)]
   $f: \mathbb{R} \times \mathcal{B}\to  Y$
is a continuous function and there exists a
continuous non decreasing function
  $L_{f} :[0,\infty)\to [0,\infty), $   such that
$$
\| f(t,\psi_1) - f(t,\psi_2) \|_{Y} \leq
L_{f} (r) \| \psi_1 - \psi_2 \|_{\mathcal{B}}, \quad
  (t,\psi_j) \in   \mathbb{R} \times B_{r}(0, \mathcal{B} ).
$$
   \item[(PG)]    $g: \mathbb{R} \times \mathcal{B} \to X$ is a continuous
function  and there exists a continuous and non decreasing function
$ L_{g}:[0, \infty)\to [0, \infty)$ such that
$$
\| g(t,\psi_1) -g(t,\psi_2) \| \leq L_g (r)
 \| \psi_1 - \psi_2 \|_{\mathcal{B}}, \quad (t,\psi_j)\in  \mathbb{R}
\times B_{r}(0 , \mathcal{B}).
$$
\item[(P2)]
\begin{align*}
&\sup_{r>0} \big[\frac{ r}{2 \mathfrak{K}}- L_f(2\mathfrak{K}r )r \mu
 - \frac{M}{\beta}L_g(2\mathfrak{K}r )r\big] \\
&\geq  \frac{1}{2 \mathfrak{K}} (M \|\varphi\|_{\mathcal{B}}
 + M \|f(0,\varphi)\| + \sup_{t \in [0,\infty)}\|f(t,0)\|_Y \mu
+ \frac{M}{\beta}\sup_{t \in [0,\infty)}\|g(t,0)\| ),
\end{align*}
where $\mu =(  \|i_c\|_{\mathcal{L}(Y,X)} +  \|\phi\|_{L^1}
+  \frac{M}{\beta} \|b\|_{L^1} )$.
\end{itemize}

Motivated by the theory of resolvent operator, we introduce  the
following concept of mild solution for \eqref{eqi1}-\eqref{eqi2}.

 \begin{definition}  \rm
A  function  $u:(-\infty, b] \to X$,
$0<b\leq a$, is  called a mild solution  of \eqref{eqi1}-\eqref{eqi2}
on $[0,b]$, if  $u_0=\varphi \in \mathcal{B}$;
$ u|_{[0,b]} \in C([0,b]:X)$; the functions
$\tau \mapsto A\mathcal{R}(t-\tau)f(\tau,u_\tau)$
and
 $\tau \mapsto \int_{0}^{\tau}B(\tau-\xi )f(\xi ,u_{\xi }) d \xi $
are integrable on  $[0,t)$  for every $t \in (0,b]$ and
\begin{align*} \label{solfraca}
u(t) &=  \mathcal{R}(t)(\varphi(0)+f(0,\varphi))-f(t,u_{t})
 -\int_{0}^{t}A\mathcal{R}(t-s)f(s,u_{s})ds \\
&\quad - \int_{0}^{t}\mathcal{R}(t-s) \int_{0}^{s}
 B(s- \xi)f(\xi, u_{\xi}) d\xi ds+ \int_{0}^{t}\mathcal{R}(t-s)g(s,u_{s})ds,
\quad t \in [0,b].
\end{align*}
\end{definition}

Now, we need to  introduce some concepts, definitions and technicalities on
asymptotically almost periodical  functions, $S$-asymptotically
$\omega$-periodic, asymptotically $\omega$-periodic asymptotically and
almost automorphic  functions.

\begin{definition} \rm
A  function $f\in C(\mathbb{R},Z) $ is almost periodic (a.p.) if for
every   $ \varepsilon > 0$ there exists a relatively dense subset of
$\mathbb{R}$, denoted by $\mathcal{H}( \varepsilon, f,Z)$, such that
 $$
\| f(t+ \xi ) - f(t) \|_{Z} < \varepsilon, \quad   t \in\mathbb{R},\,
 \xi \in \mathcal{H}( \varepsilon, f,Z).$$
\end{definition}

\begin{definition} \rm
A  function $f\in C([0, \infty),Z) $ is
asymptotically almost periodic (a.a.p.) if there exists  an almost
 periodic function $g(\cdot)$ and $w
 \in C_0([0, \infty),Z)$ such that $f(\cdot) = g(\cdot) + w(\cdot)$.
\end{definition}

In this paper,  $AP(Z)$ and $AAP(Z)$  are the spaces
 \begin{gather*}
  AP(Z)=\{f\in C(\mathbb{R},Z): f \text{ is a.p. }\},  \\
  AAP(Z)= \{f\in C([0,\infty ),Z): f \text{ is a.a.p. }\},
 \end{gather*}
endowed with the norm of the uniform convergence.
We  know from the result in \cite{z5} that  $AP(Z)$ and $AAP(Z)$ are
Banach spaces.

\begin{definition} \label{def4} \rm
 A  function $u\in C_{b}([0, \infty),X) $ is   said
$S$-asymptotically $\omega$-periodic  if
\[
\lim_{t \to \infty} (u(t+\omega )-u(t)   )=0.
\]
\end{definition}
In the rest of this paper,  the notation  $SAP_{\omega}(X)$ stands for the
 space 
$$
SAP_{\omega}(X) = \{f\in C_b(\mathbb{R},X): f \text{ is $S$-asymptotically 
$\omega$-periodic }\},
 $$
endowed with the norm of the uniform convergence. 
It is  clear that $SAP_{\omega}(X)$ is a  Banach space.

\begin{definition} \label{def7}\rm
A continuous function $f:[0,\infty)\times Z \to W$  is said
uniformly $S$-asymptotically $\omega$-periodic  on  bounded sets if
 $f(\cdot, x)$ is bounded
for each $x \in Z$, and for every $\varepsilon >0$ and for all bounded 
set $K \subseteq Z $, there exists  $L(K,\varepsilon) \geq 0$
such that $ \| f(t,x)-f(t+\omega ,x)\|_{W}\leq \varepsilon$ for 
every $t\geq L(K,\varepsilon) $ and all  $x\in K$.
\end{definition}

\begin{definition}  \label{def8} \rm
 A  continuous function
$f:[0,\infty) \times Z\to W$  is said asymptotically  uniformly continuous 
on  bounded  sets, if for every $\varepsilon>0$ and for all bounded
 set $K\subseteq Z $ there exist constants $L(K,\varepsilon) \geq 0$ and
$\delta = \delta(K,\varepsilon) > 0$ such that 
$\|f(t,x) - f(t,y)\|_{W} \leq \varepsilon$ for
 all
$t \geq L(K,\varepsilon)$ and every   $x,y \in K$ with 
$\| x-y \|_{Z} \leq  \delta$.
\end{definition}



\begin{lemma}[{\cite[Lemma 4.1]{M1}}] \label{composition}
Assume that $f:[0,\infty)\times Z\to W$ is a function
 uniformly $S$-asymptotically $\omega$-periodic  on bounded sets and
asymptotically uniformly continuous on bounded sets. Let $u\in SAP_{\omega}(Z)$,
 then the function $\theta: \mathbb{R} \to W$
defined by $\theta(t) = f(t,u(t))$ is $S$-asymptotically $\omega$-periodic.
\end{lemma}

By using a similar procedure  to the proof of  the 
\cite[Lemma 3.5]{H2008}, we prove the next result.

\begin{lemma} \label{lema4H}
Suppose that condition  {\rm (P1)(b)}  holds  and   $ f\in SAP_{\omega}(X)$.
 Let  $F:[0,\infty)\to X$ be the function defined by
$$ 
F(t):=\int_{0}^{t} \mathcal{R}(t-s) f(s)d s. 
$$
Then $F \in SAP_{\omega}(X)$.
\end{lemma}

\begin{lemma}[{\cite[Lemma 2.10]{H2008}}]   \label{lem8H}
Assume that  $\mathcal{B}$ is a fading memory space and 
$u \in C(\mathbb{R},X)$ is such that $u_0 \in \mathcal{B}$ and 
$u|_{[0,\infty)} \in SAP_{\omega}(X)$, then 
$ t \mapsto u_t \in SAP_{\omega}(\mathcal{B})$.
\end{lemma}

\begin{definition} \label{def6}\rm
A  function $u\in C_{b}([0, \infty),X) $ is  called  asymptotically 
$\omega$-periodic if there exists an $\omega$-periodic
function $v$ and $w \in C_{0}([0, \infty), X)$ such that $u = v + w$.
\end{definition}

 \begin{remark} \rm
 In \cite{H2008} the authors have shown
that the set of the asymptotically $\omega$-periodic functions is
 properly contained in $SAP_{\omega}(W)$.
\end{remark}

\begin{lemma}[{\cite[Remark 3.13]{H2008}}] \label{caiedo0}
 If $u\in C_{b}([0,\infty),  X)$ is a function such that
$\lim_{t\to \infty}(u(t +n \omega)-u(t))=0$, uniformly for 
$n \in \mathbb{N}$, then $u(\cdot)$ is asymptotically  $\omega$-periodic.
\end{lemma}

In the rest of this paper,  $S_{\omega}(X)$ stands for the  space 
$$ 
S_{\omega}(X) = \{f\in C_b([0,\infty),X): \lim_{t\to \infty}f(t +n \omega)-f(t)=0,
 \text{ uniformly for }  n \in \mathbb{N}  \}, 
$$
endowed with the norm of the uniform convergence.

\begin{lemma}[{\cite[Lemma 2.3]{Caiedo}}] \label{caiedo1}
Let  $f : [0,\infty)\times Z \to W$  be asymptotically uniformly continuous 
on bounded sets. Suppose that for all bounded subset
$K \subset Z$, the set $\{f(t,z)\geq 0, z \in K \}$ is bounded and 
$  \lim_{t\to \infty} \| f(t+n\omega, z) - f(t,z) \| = 0$, uniformly
 for $z \in K$ and $n \in \mathbb{N}$. If $ u \in S_{\omega}(Z)$, 
 then $ f(\cdot, u(\cdot)) \in S_{\omega}(W)$.
\end{lemma}

\begin{lemma}\cite[Lemma 3.7]{Caiedo}  \label{caiedo2}
Suppose that condition  {\rm (P1)(b)}  holds  and
$f \in S_{\omega}(X)$.
 If $F$ is the function defined by $F(t):=\int_{0}^t \mathcal{R}(t-s) f(s)ds$, 
$t\geq 0$, then $F \in S_{\omega}(X)$.
\end{lemma}

We now introduce some  notion of asymptotically almost automorphic.

\begin{definition} \rm
A  function $f\in C( \mathbb{R} , X)$
 is said to be almost automorphic if for every sequence
of real numbers $(s'_{n})_{n \in \mathbb{N}}$, there exists a
subsequence $(s_{n})_{n \in \mathbb{N}} \subset (s'_{n})_{n \in
\mathbb{N}}$ such that
$$ 
g(t):= \lim_{n \to \infty} f(t+s_{n}) 
$$
is well defined for  each  $t \in \mathbb{R}$, and
$$ 
f(t) = \lim_{n \to \infty} g(t-s_{n}) 
$$
for all $t \in \mathbb{R}$.
\end{definition}

It is well known that  the range of an almost automorphic function
is relatively compact on $X$, and hence it is bounded. Moreover, the
space of all   almost automorphic functions, denoted by $AA(X)$,
endowed with the norm of the uniform convergence is a Banach space
\cite{g2}.

\begin{definition} \rm
A function $f\in C( [0, \infty) ,  Z)$ is said to be asymptotically
almost automorphic if it can
 be written as $f=g+h$ where $g \in AA(Z)$  and $ h \in
C_0([0,\infty),Z)$. Denote by $AAA(Z)$ the set of all such
functions.
\end{definition}

\begin{definition}  \label{def1} \rm
A function $f\in C( \mathbb{R}, Z)$ is said to be compact almost
automorphic if for every sequence of real numbers $(\sigma_{n})_{n
\in \mathbb{N}}$ there exists a subsequence $(s_{n})_{n \in
\mathbb{N}} \subset (\sigma_{n})_{n \in \mathbb{N}}$ such that
\begin{gather*}
g(t): = \lim_{n \to \infty} f(t+s_{n}),\\
f(t)= \lim_{n \to \infty} g(t-s_{n})
\end{gather*}
uniformly on compact subsets  of  $\mathbb{R}$. The collection of 
those functions will be denoted by $AA_c(Z)$.
\end{definition}

\begin{definition} \label{def2} \rm
A   function $f\in C( \mathbb{R} \times  Z, W)$  is said to be
compact almost automorphic in $t \in \mathbb{R}$, if for every
sequence of real numbers $(\sigma_{n})_{n \in \mathbb{N}}$ there
exists a subsequence $(s_{n})_{n \in \mathbb{N}} \subset
(\sigma_{n})_{n \in \mathbb{N}}$ such that
\begin{gather*}
g(t,z):= \lim_{n \to \infty} f(t+s_{n}, z), \\
 f(t,z) = \lim_{n \to \infty} g(t-s_{n},z),
\end{gather*}
where the limits are uniform on compact subset of $\mathbb{R}$,
 for each $z \in Z$. The space of such functions will be denoted 
by $AA_c(Z, W)$.
\end{definition}

\begin{definition} \rm
 A continuous function $f\in C( [0, \infty),   Z)$ is said to be compact
 asymptotically almost automorphic if it
can be written as $f=g+h$ where $g \in AA_c(Z)$   and $ h \in
C_0(\mathbb{R}^{+},Z)$. Denote by $AAA_c(Z)$ the set of all such
functions.
\end{definition}

\begin{definition} \rm
  Let $K\subset Z$ and $I \subset \mathbb{R}$. Let $C_{K}(I\times Z,
W)$ denote the collection of functions $f:I\times Z\to W$
such that $f(t, \cdot)$ is uniformly continuous on $K$ for every $t
\in I \subseteq \mathbb{R}$.
\end{definition}

 \begin{definition} \rm
 A function $f\in C([0, \infty) \times Z,W)$ is said to be compact
asymptotically almost automorphic if it can be written as $f=g+h, $
where $g\in AA_c(Z,W)$   and $h \in C_0([0, \infty)\times  Z, W) $.
Denote by $AAA_c(Z,W)$ the set of all such functions.
\end{definition}


\begin{lemma}[{\cite[Lemma 3.3]{Jose3}}] \label{lemaJ1}
Let $u \in AAA_c(Z)$ and $f\in AAA_c(Z, W)\cap C_{R}(\mathbb{R}\times Z,W)$,
 where $R=\overline{\{ u(t): t \in \mathbb{R} \}}$.
Then the function
 $\Phi: \mathbb{R} \to W$ defined by $\Phi(t) = f (t , u(t)) \in AAA_c(W)$.
\end{lemma}


\begin{lemma}[{\cite[Lemma 3.4]{Jose3}}] \label{lemaJ2}  %\label{Jose3}
 Suppose that condition  (P1)-$(b) $ holds  and  $f \in AAA_c(X)$. If
 $F$ is the function defined by
 $$ 
F(t):=\int_{0}^t \mathcal{R}(t-s) f(s)ds, \quad t\geq 0,
$$
 then $F \in AAA_c(X)$.
\end{lemma}


\begin{lemma}[{\cite[Lemma 3.5]{Jose3}}] \label{lemaJ3}
If $u\in AA_c(X)$, then  the function $s \mapsto
u_{s}$ belongs to $AA_c(\mathcal{B})$.
Moreover, if $\mathcal{B}$ is a fading memory space and 
$u \in C(\mathbb{R},X)$ is such that $u_0 \in \mathcal{B}$ and 
$u|_{[0,\infty)} \in AAA_c(X)$, then $ t \mapsto u_t \in AAA_c(\mathcal{B})$.
\end{lemma}

\section{Several types of
 periodicity of mild solutions} \label{ExistenceResults}

In this section we establish the existence of several type of
periodicity for solutions to partial neutral
integro-differential equations system \eqref{eqi1}-\eqref{eqi2}. For
that, we need  to introduce a few preliminaries and important
results. Following, we consider the problem of the existence of
compact asymptotically almost automorphic solutions.

In the following, we let $\mathcal{A}(Z)$ stands for one of the 
spaces $AAA_{c}(Z)$, $SAP_{\omega}(Z)$ or $S_{\omega}(Z)$.


\begin{lemma} \label{apide1}
Assume the condition {\rm(P1)} is fulfilled.
Let   $u \in \mathcal{A}(Y)$ and    $G(\cdot ):[0,\infty )\to X$ be the
function defined by 
$$  
G(t)=\int_{0}^t \mathcal{R}(t-s) \int_0^s B(s-\tau)u(\tau) \ d\tau ds,\quad
t\geq 0. 
$$ 
Then $  G(\cdot) \in \mathcal{A}(X)$.
\end{lemma}

\begin{proof}
First we consider the $AAA_{c}(Y)$ case. By Lemma \ref{lemaJ2}  
is sufficient to prove  that $H(t)=\int_0^t B(t-s) u(s) ds \in AAA_c(Y)$. 
Suppose $u=k+h$ where $k \in AA_c(Y)$ and $ h \in C_0([0,\infty),Y)$. Then
\begin{align*}
H(t)&=  \int_{-\infty}^t B(t-s) k(s)ds -
\int_{-\infty}^0 B(t-s) k(s)ds +  \int_{0}^t B(t-s) h(s)ds \\
&=  w(t) + q(t),
\end{align*}
where
\begin{gather*}
w(t) = \int_{-\infty}^t B(t-s) k(s)ds, \\
q(t) = \int_{0}^t B(t-s) h(s)ds - \int_{-\infty}^0 B(t-s) k(s)ds.
\end{gather*}

For a given  sequence $(\sigma_{n})_{n \in \mathbb{N}}$ of real
numbers, fix a subsequence $(s_{n})_{n \in \mathbb{N}}$, and a
continuous functions $v\in C_b(\mathbb{R}, Y)$ such that
$k(t+s_{n})$ converges to $v(t)$ in $Y$, and $v(t-s_{n})$ converges
to $k(t)$ in $Y$, uniformly on compact sets of $\mathbb{R}$.

From the Bochner's criterion related to integrable functions and the
estimate
\begin{eqnarray}\label{est1}
\|B(t-s)k(s)\|  = \| B(t-s)\|_{\mathcal{L}({Y,X})}\|k(s) \|_{{Y}}   \leq
 b(t-s) \|k(s) \|_{{Y}} \label{des3}
\end{eqnarray}
it follows that the function $s \mapsto B(t -s ) k(s) $ is integrable
 over $(-\infty, t)$ for each $t\in \mathbb{R}$.
Furthermore, since
$$
 w(t+s_{n}) =  \int^t_{-\infty} B(t-s)  k(s+s_{n})ds, \quad t\in \mathbb{R}, \;
 n \in \mathbb{N}, 
$$
using the estimate \eqref{est1} and the Lebesgue Dominated Convergence Theorem, 
it follows that $w(t+s_{n})$ converges to
${z(t)= \int^t_{-\infty}B(t-s) v(s) ds}$ for each $t\in \mathbb{R}$.

 The remaining task consists of  showing that the convergence is uniform 
on all compact subsets  of
$\mathbb{R}$ and that $ q (\cdot) \in  C_0([0,\infty), X)$. Let 
$K \subset \mathbb{R}$ be an arbitrary compact and let 
$\varepsilon >0$. Since $ h \in C_0([0,\infty), Y)$ and $ k(\cdot) \in AA_c(Y)$, 
there exists a constant $L$ and $N_{\varepsilon}$ such that
   $K \subset [\frac{-L}{2},\frac{L}{2}]$ with
\begin{gather*}
\int_{\frac{L}{2}}^{\infty} b(s) ds  < \varepsilon, \\
\| k(s+s_{n})-v(s)\|_{Y}  \leq \varepsilon, \quad n \geq N_{\varepsilon}, \; s \in [-L,L], \\
\| h(s) \|_{Y}   \leq \varepsilon, \quad  s \geq L.
\end{gather*}
For each $t\in K$, one has
\begin{align*}
&\|w(t+s_{n})-z(t)\| \\
& \leq \int^t_{-\infty} \|B(t-s)\|_{\mathcal{L}(Y,X)} 
 \|k(s+s_{n})-v(s)\|_{Y} ds \\
& \leq \int^{-L}_{-\infty} b(t-s)\| k(s+s_{n})-v(s)\|_{Y} ds 
 + \int^t_{-L} b(t-s) \| k(s+s_{n})-v(s)\|_{Y} ds \\
& \leq 2\|k\|_{Y,\infty} \int^{\infty}_{t+L}  b(s) ds 
 + \varepsilon\,\int^{\infty}_{0} b(s) ds \\
& \leq 2\|k\|_{Y,\infty} \int^{\infty}_{\frac{L}{2}} b(s) ds 
  + \varepsilon\,\int^{\infty}_{0}  b(s) ds \\
& \leq \varepsilon\Big(2\| k \|_{Y,\infty} +\int^{\infty}_{0}    b(s) ds\Big),
\end{align*}
which proves that the convergence is uniform on $K$, from  the fact
that the last estimate is independent of $t\in K$. Proceeding as
previously, one can similarly prove that $z(t-s_{n})$  converges to
$w$ uniformly on all compact subsets of $\mathbb{R}$. Next,  let us
show that $q(\cdot) \in  C_0([0,\infty), X)$. For all $t \geq 2L$ we
obtain
\begin{align*}
\|q(t) \| 
& \leq \int_{-\infty}^0 \|B(t-s)\|_{\mathcal{L}(Y,X)} \|k(s)\|_{Y} ds + \int_0^t \|B(t-s)\|_{\mathcal{L}(Y,X)} \|h(s)\|_{Y}ds \\
& \leq \int_{-\infty}^0  b(t-s)\| k(s)\|_{Y} ds  
 + \int_{t/2}^t b(t-s)\| h(s)\|_{Y} ds 
 + \int_0^{t/2}  b(t-s)\| h(s)\|_{Y} ds \\
& \leq \int_{\frac{L}{2}}^{\infty} b(s) ds\| k\|_{Y,\infty} 
 + \varepsilon \int_{t/2}^t  b(s) ds
  + \int_{\frac{L}{2}}^{\infty} b(s) ds\| h \|_{Y,\infty} \\
& \leq \varepsilon ( \|k\|_{Y,\infty} + \int^{\infty}_{0}  b(s) ds
  + \| h \|_{Y,\infty} ).
\end{align*}

Now we consider the $SAP_{\omega}(Y)$ case. From  Lemma \ref{lema4H}
 is sufficient to prove that 
$$ 
H(t) = \int_{0}^{t} B(t-s) u(s) ds
 $$ 
is $SAP_{\omega}(X)$. For all $t \geq 0$,
\begin{align*}
\|H(t)\| 
& \leq \int_{0}^{t} \|B(t-s) \|_{\mathcal{L}(Y,X)} \|u(s)\|_Y d\tau \\
& \leq \int_{0}^{t} b(t-s) \|u(s)\|_Y ds \\
& \leq \|u\|_{Y,\infty} \int_0^{\infty}b(s) ds.
\end{align*}
This shows that $H \in C_{b}([0,\infty), X)$. Furthermore, for 
$\omega \geq 0$,  we have for  $t \geq L > 0$,
\begin{align*}
&\| H(t+\omega) - H(t) \| \\
& = \| \int_{0}^{t+\omega} B(t+\omega-s) u(s) ds 
 - \int_{0}^{t} B(t-s) u(s) ds \| \\
& \leq \int_{0}^{\omega} b(t+\omega-s) \|u(s)\|_Y ds + \|
\int_{0}^{t} B(t-s) u(s+\omega) ds - \int_{0}^{t} B(t-s) u(s) ds \| \\
& \leq \|u\|_{Y,\infty} \int_{0}^{\omega} b(t+\omega-s) ds 
 + \int_{0}^{t} \|B(t-s)( u(s+\omega) - u(s) )\|ds \\
& \leq  \|u\|_{Y,\infty} \int_{0}^{\omega} b(t+\omega-s) ds 
 + \int_{0}^{L} b(t-s) \|u(s+\omega) - u(s)\|_Y ds \\
& \quad + \int_{L}^{t} b(t-s) \|u(s+\omega) - u(s)\|_Y ds.
\end{align*}
For all $\varepsilon >0$, we choose  $L$ sufficiently large such
that $\|u(s+\omega)-u(s)\|_Y < \varepsilon$ for all $s \geq L$ and
$\int_{L}^{\infty} b(s) ds < \varepsilon$. Hence, for $t \geq 2L$ we
obtain
\begin{align*}
\| H(t+\omega) - H(t) \|
& \leq \|u\|_{Y,\infty} \int_{t}^{t+\omega} b(s) ds 
 + 2\|u\|_{Y,\infty} \int_{t-L}^{t} b(s) ds + \varepsilon \int_{0}^{t-L} b(s) ds\\
& \leq \|u\|_{Y,\infty} \varepsilon + 2\|u\|_{Y,\infty} \varepsilon 
 + \varepsilon \int_{0}^{t-L} b(s) ds\\
& \leq \varepsilon \Big( 3\|u\|_{Y,\infty} + \int_{0}^{\infty} b(s)
ds \Big).
\end{align*}

Finally, let us prove the $S_{\omega}(Y)$ case. From the Lemma \ref{caiedo2}  
is sufficient
 prove that  $\lim_{t\to \infty} H(t + n\omega) - H(t) = 0$,
uniformly in  $n \in \mathbb{N}$, where   $H(t)=\int_0^t B(t-s) u(s)
ds$. For all $\varepsilon >0$, we choose  $L$ sufficiently large
such that $\|u(s+n \omega)-u(s)\|_Y < \varepsilon$ for all $s \geq
L$ and  $\int_{L}^{\infty} b(s) ds < \varepsilon$. Hence, for $t
\geq 2L$ we obtain
\begin{align*}
&\| H(t+ n\omega) - H(t) \|\\
& \leq \| \int_0^{t+ n\omega} B(t+ n\omega-s) u(s) d s  
 -  \int_0^{t} B(t-s) u(s) ds \| \\
& \leq \|u\|_{Y,\infty} \int_{0}^{n\omega} b(t + n\omega - s) ds 
 + \int_{0}^{L} b(t-s) \|u(s+n \omega)-u(s)\|_Y ds \\
& + \quad \int_{L}^{t} b(t- s) \|u(s+n \omega)-u(s)\|_Y  ds \\
& \leq \|u\|_{Y,\infty} \int_{t}^{t +n\omega} b(s) ds 
 + 2\|u\|_{Y,\infty} \int_{t-L}^{t} b(s) ds 
 + \varepsilon \int_{0}^{\infty} b(s) ds\\
& \leq \varepsilon ( 3 \|u\|_{Y,\infty} + \int_{0}^{\infty} b(s) ds ) .
\end{align*}
This completes the proof.
\end{proof}


\begin{lemma}  \label{apide2}
Let condition  {\rm (P1)(c)}  hold and  $u$ be a function
in $\mathcal{A}(Y)$.  If  $I:[0,\infty )\to X$  is  the function defined
by $ I(t) = \int_{0}^t A\mathcal{R}(t-s)u(s)ds$, then $ I(\cdot)\in
\mathcal{A}(X)$.
\end{lemma}

\begin{proof}
All the $AAA_{c}(Y)$, $SAP_{\omega}(Y)$ and $S_{\omega}(Y)$ cases
 require small modifications in the proof of Lemma \ref{apide1}.
\end{proof}


\begin{theorem} \label{p1}
Let $f  \in  AAA_c([0,\infty) \times\mathcal{B},Y) $ and
 $g \in AAA_c([0,\infty) \times\mathcal{B}, X)$. Assume that
$\mathcal{B}$ is   a fading memory space and   
 {\rm (P1),  (P2), (PF), (PG)} hold.
 Then there exists $ \varepsilon >0$ such that for
 each  $\varphi \in B_{\varepsilon}(0,\mathcal{B})$ there exists  
a unique  mild
 solution $u(\cdot,\varphi) \in AAA_c(X)$ of \eqref{eqi1}-\eqref{eqi2}.
\end{theorem}

\begin{proof}
 By the hypothesis there exists a constant $r>0$ such that
 \begin{align*}
& [  r- L_f(2\mathfrak{K}r) 2 \mathfrak{K}r \mu 
- \frac{M}{\beta}L_g(2\mathfrak{K}r )2 \mathfrak{K}r] \\
&\geq  M \|\varphi\|_{\mathcal{B}} + M \|f(0,\varphi)\| 
+ \sup_{t \in [0,\infty)}\|f(t,0)\|_Y  \mu 
 + \frac{M}{\beta}\sup_{t \in [0,\infty)}\|g(t,0)\|,
\end{align*}
where $ \mathfrak{K}$ is the constant  introduced in  Remark \ref{rem2}. 
We affirm that the assertion holds for $ \varepsilon \leq  r$. 
Let $\varphi \in B_{\varepsilon}(0,\mathcal{B})$ and  the space
 $$
\mathfrak{D}= \{ x \in AAA_c(X): x(0) = \varphi(0), \|x(t)\| \leq  r,\,
 t\geq 0 \}
$$ 
endowed with the metric $d(u,v)=\|u-v\|_{\infty} $, we define the
operator $ \Gamma: \mathfrak{D}\to C([0,\infty);X )$ by
\begin{align*}
 \Gamma
u(t)&=\mathcal{R}(t)(\varphi(0)+f(0,\varphi))-f(t,\widetilde{u}_{t})
-\int_{0}^{t}A\mathcal{R}(t-s)f(s,\widetilde{u}_{s})ds   \\
&\quad -  \int_{0}^{t}\mathcal{R}(t-s) \int_{0}^{s}B(s- \xi)
 f(\xi, \widetilde{u}_{\xi}) d\xi ds+
\int_{0}^{t}\mathcal{R}(t-s)g(s,\widetilde{u}_{s})ds, \quad t\geq 0
\end{align*}
where $ \widetilde{u}:\mathbb{R} \to X$ is the
function defined by the relation  $\widetilde{u}_{0}= \varphi$ and
$\widetilde{u} = u$ on $[0, \infty)$.  From  the hypothesis  
(P1) (PF) and  (PG) we obtain that $\Gamma
u$ is well defined and that $\Gamma u \in C([0, \infty);X)$.
 Moreover, from Lemma \ref{lemaJ3}, we have that function 
$s \mapsto \widetilde{u}_s \in AAA_c(\mathcal{B})$. By  Lemma  \ref{lemaJ1},
 we conclude that 
$s \mapsto f(s,\widetilde{u}_s)    \in AAA_c([0,\infty),Y) $ and 
$s \mapsto g(s,\widetilde{u}_s)  \in  AAA_c([0,\infty),X)$. 
From  Lemmas \ref{lemaJ2}, \ref{apide1}, \ref{apide2}
and $\lim_{t \to \infty} \| \mathcal{R}(t)(\varphi(0)+f(0,\varphi)) \| =0$,
 we obtain that $ \Gamma u\in AAA_c(X)$.

Next, we prove that $\Gamma(\cdot)$ is a contraction from $\mathfrak{D}$  
into $\mathfrak{D}$. If   $u\in \mathfrak{D}$ and $t\geq 0$, we obtain
\begin{align*} %\label{iii}
&\|\Gamma u(t)\|\\
&\leq \| \mathcal{R}(t)(\varphi(0)+ f(0,\varphi)) \|
 + \|i_c\|_{\mathcal{L}(Y,X)}(\|f(t,\widetilde{u}_{t}) - f(t,0)\|_Y 
 + \|f(t,0)\|_Y) \\
&\quad + \int_{0}^{t}\|A\mathcal{R}(t-s)(f(s,\widetilde{u}_{s}) - f(s,0))\| ds   
 + \int_{0}^{t} \|A\mathcal{R}(t-s)f(s,0)\| ds \\
&\quad + \int_{0}^{t}\|\mathcal{R}(t-s) \int_{0}^{s}B(s- \xi)
 (f(\xi, \widetilde{u}_{\xi}) - f(\xi,0)) d\xi \| ds \\
&\quad + \int_{0}^{t}\|\mathcal{R}(t-s) \int_{0}^{s}B(s- \xi)f(\xi,0) d\xi \| ds \\
&\quad + \int_{0}^{t}\|\mathcal{R}(t-s)(g(s,\widetilde{u}_{s}) - g(s,0))\| ds
  + \int_{0}^{t}\| \mathcal{R}(t-s) g(s,0) \| ds \\
&\leq   M \|\varphi\|_{\mathcal{B}} + M \|f(0,\varphi)\|  
 + \|i_c\|_{\mathcal{L}(Y,X)} ( L_f(\| \widetilde{u}_{t} 
 \|_{\mathcal{B}})\|\widetilde{u}_{t}\|_{\mathcal{B}}
 + \sup_{t \in [0,\infty)} \|f(t,0)\|_Y ) \\
&\quad + \int_{0}^{t} \phi(t-s)L_f(\|\widetilde{u}_{s}\|_{\mathcal{B}}) 
 \|\widetilde{u}_{s}\|_{\mathcal{B}} ds 
 + \sup_{t \in [0,\infty)}\|f(t,0)\|_Y  \int_{0}^{t} \phi(s) ds \\
&\quad + \int_{0}^{t}Me^{-\beta(t-s)} \int_{0}^{s}b(s-\xi)L_f
 (\|\widetilde{u}_{\xi}\|_{\mathcal{B}}) \|\widetilde{u}_{\xi}\|_{\mathcal{B}} 
 d\xi ds \\
&\quad + \sup_{t \in [0,\infty)}\|f(t,0)\|_Y \int_{0}^{t} Me^{-\beta(t-s)} 
 \int_{0}^{s}b(s-\xi) d\xi ds \\
&\quad + \int_{0}^{t} Me^{-\beta(t-s)} L_g(\|\widetilde{u}_{s}\|_{\mathcal{B}}) 
 \|\widetilde{u}_{s}\|_{\mathcal{B}} ds 
 + \sup_{t \in [0,\infty)}\|g(t,0)\| \int_{0}^{t}M e^{-\beta(t-s)} ds \\
&\leq  M \|\varphi\|_{\mathcal{B}} + M \|f(0,\varphi)\| \\
&\quad + \sup_{t \in [0,\infty)}\|f(t,0)\|_Y ( \|i_c\|_{\mathcal{L}(Y,X)} 
 + \int_0^{\infty} \phi(s) ds + \frac{M}{\beta} \int_0^{\infty} b(s) ds ) \\
&\quad + \frac{M}{\beta}\sup_{t \in [0,\infty)}\|g(t,0)\| \\
&\quad + L_f(\|\widetilde{u}_{t}\|_{\mathcal{B}}) ( \|i_c\|_{\mathcal{L}(Y,X)} 
 + \int_0^{\infty} \phi(s) ds + \frac{M}{\beta} \int_0^{\infty} b(s) ds )
 \|\widetilde{u}_{t}\|_{\mathcal{B}} \\
&\quad + \frac{M}{\beta}L_g(\|\widetilde{u}_{t}\|_{\mathcal{B}}) 
 \|\widetilde{u}_{t}\|_{\mathcal{B}} \\
&\leq  M \|\varphi\|_{\mathcal{B}} + M \|f(0,\varphi)\| \\
&\quad + \sup_{t \in [0,\infty)}\|f(t,0)\|_Y( \|i_c\|_{\mathcal{L}(Y,X)} 
 + \|\phi\|_{L^1} + \frac{M}{\beta} \|b\|_{L^1}) \\
&\quad + \frac{M}{\beta}\sup_{t \in [0,\infty)}\|g(t,0)\| 
+ L_f(2\mathfrak{K}r) ( \|i_c\|_{\mathcal{L}(Y,X)} + \|\phi\|_{L^1}
  + \frac{M}{\beta} \|b\|_{L^1} )2\mathfrak{K}r \\
&\quad + \frac{M}{\beta}L_g(2\mathfrak{K}r)2 \mathfrak{K}r \leq r
\end{align*}
where the inequality $\|\widetilde{u}_t\| \leq 2\mathfrak{K}r $ has been used and $i_c:Y \to X$ represents the continuous
inclusion of $Y$ on $X$.
 Thus, $ \Gamma(\mathfrak{D}) \subset
 \mathfrak{D}$. On the other hand, for $ u,v \in \mathfrak{D} $ we
 see that
\begin{align*}
&\| \Gamma u(t)-\Gamma v(t) \| \\
&\leq \|i_c\|_{\mathcal{L}(Y,X)}  \| f(t,\widetilde{u}_t) - f(t, \widetilde{v}_t ) \|_Y \\
& \quad + \int_{0}^{t} \|A\mathcal{R}(t-s)\|_{\mathcal{L}(Y,X)} \|f(s,\widetilde{u}_s) - f(s, \widetilde{v}_s )\|_{Y} ds \\
& \quad + \int_{0}^{t} \| \mathcal{R}(t-s) \| ( \int_{0}^{s} \|B(s-\xi)\|_{\mathcal{L}(Y,X)}\| f(\xi,\widetilde{u}_\xi) - f(\xi,\widetilde{v}_\xi ) \|_{Y} d\xi ) ds \\
& \quad + \int_{0}^{t}\| \mathcal{R}(t-s) \| \| g(s,\widetilde{u}_s) - g(s,\widetilde{v}_s ) \| ds \\
&\leq \Big(L_{f}(2\mathfrak{K}r) \mathfrak{K} \mu + L_{g}(2\mathfrak{K}r) 
 \mathfrak{K}\frac{M}{\beta} \Big) \|u-v\|_{\infty} \\
&\leq \Big(L_{f}(2\mathfrak{K}r)2\mathfrak{K} \mu
  + L_{g}(2\mathfrak{K}r)2\mathfrak{K}\frac{M}{\beta} \Big)
\|u-v\|_{\infty},
\end{align*}
we observe that $r- L_f(2\mathfrak{K}r) 2\mathfrak{K}r \mu 
- \frac{M}{\beta}L_g(2\mathfrak{K}r )2 \mathfrak{K}r >0$, this implies that 
\[
 L_f(2\mathfrak{K}r)2 \mathfrak{K} \mu + \frac{M}{\beta}L_g(2\mathfrak{K}r )2
\mathfrak{K}<1,
\]
 which shows that $ \Gamma(\cdot)$  is a contraction from $\mathfrak{D}$ into
 $\mathfrak{D}$. The  assertion is now a   consequence of the
 contraction mapping principle. The proof is complete.
\end{proof}


\begin{remark} \rm
 A similar result was obtained by Dos Santos et al.
\cite{Dos1} for the existence of asymptotically almost periodic
solutions for the system  \eqref{eqi1}-\eqref{eqi2}.
\end{remark}

\begin{proposition} \label{p2}
Let $f :[0,\infty) \times\mathcal{B}\to Y $ and 
$g:[0,\infty) \times\mathcal{B} \to X$ be uniformly $S$-asymptotically
$\omega$-periodic on bounded sets and asymptotically uniformly continuous 
on bounded sets.  Assume that $\mathcal{B}$ is  a fading memory space and
 {\rm (P1), (P2),  (PF),  (PG)} hold.
Then there exists $ \varepsilon >0$ such that for
 each  $\varphi \in B_{\varepsilon}(0,\mathcal{B})$ there exists  a unique  mild
 solution $u(\cdot,\varphi ) \in SAP_{\omega}(X)$ of \eqref{eqi1}-\eqref{eqi2}
 on $[0,\infty)$. 
\end{proposition}

\begin{proof}
Let  the space
$$
\mathfrak{D}_{\omega}= \{ x \in SAP_{\omega}(X): x(0)
 = \varphi(0), \| x(t) \| \leq  r, \, t\geq 0 \}
$$
endowed with the metric $d(u,v)=\| u-v \|_{\infty} $, 
we define the operator $ \Gamma: \mathfrak{D}_{\omega}\to C([0,\infty);X )$
by
\begin{align*}
 \Gamma u(t)
&=\mathcal{R}(t)(\varphi(0)+f(0,\varphi))-f(t,\widetilde{u}_{t})
-\int_{0}^{t}A\mathcal{R}(t-s)f(s,\widetilde{u}_{s})ds \\
&\quad -  \int_{0}^{t}\mathcal{R}(t-s) \int_{0}^{s}B(s- \xi)f(\xi,
\widetilde{u}_{\xi}) d\xi ds+
\int_{0}^{t}\mathcal{R}(t-s)g(s,\widetilde{u}_{s})ds, \quad t\geq
0, 
\end{align*}
 where $ \widetilde{u}:\mathbb{R} \to X$ is the
function defined by the relation  $\widetilde{u}_{0}= \varphi$ and
$\widetilde{u} = u$ on $[0, \infty)$.  From  the hypothesis 
(P1), (PF) and  (PG) we obtain that $\Gamma u$ is well defined and that
 $\Gamma u \in C([0, \infty);X)$.
 Moreover, from Lemma \ref{lem8H}, we have that function $s \mapsto
\widetilde{u}_s \in SAP_{\omega}(\mathcal{B})$. By Lemma
 \ref{composition}, we conclude that $s \mapsto f(s,\widetilde{u}_s)
 \in  SAP_{\omega}([0,\infty),Y) $ and $s \mapsto g(s,\widetilde{u}_s)  \in
SAP_{\omega}([0,\infty),X)$. From Lemmas \ref{lema4H}, \ref{apide1}
 and \ref{apide2}
it follows that $ \Gamma u\in SAP_{\omega}(X)$. Using the same argument of
 Theorem \ref{p1} proof,   we obtain that $\Gamma
(\mathfrak{D}_{\omega}) \subset \mathfrak{D}_{\omega}$ and $\Gamma$ 
is a contraction. This completes the proof.
\end{proof}

\begin{proposition} \label{p3}
Let $f :[0,\infty) \times\mathcal{B}\to Y $ and $g:[0,\infty)
\times\mathcal{B} \to X$ be 
 asymptotically uniformly continuous on bounded subset $K \subset \mathcal{B}$,
 and  $\lim_{t\to \infty} \| f(t + n\omega, \psi) - f(t, \psi) \|_Y = 0$,
$\lim_{t\to \infty} \| g(t + n\omega, \psi) - g(t, \psi) \| = 0 $
 uniformly for  $\psi \in K $ and $n \in \mathbb{N}$.
Assume that $\mathcal{B}$ is
  a fading memory space and    (P1), (P2), (PF) and  (PG)
hold. Then there exists $ \varepsilon >0$ such that for
 each  $\varphi \in B_{\varepsilon}(0,\mathcal{B})$ there exists  a unique 
 asymptotically $\omega$-periodic  mild
 solution $u(\cdot,\varphi)$ of \eqref{eqi1}-\eqref{eqi2}
 on $[0,\infty)$. 
\end{proposition}

\begin{proof}
 We define  the space
 $$
\mathfrak{D}_0= \{ x \in S_{\omega}(X): x(0) = \varphi(0), \| x(t) \| 
\leq  r,\, t\geq 0 \}
$$ 
endowed with the metric $d(u,v)=\| u-v \|_{\infty}$. It is easy see 
that $\mathfrak{D}_0$  is a closed subspace of $S_{\omega}$. We
define the operator $ \Gamma:\mathfrak{D}_0 \to C([0,\infty);X )$ by
\begin{align*}
 \Gamma u(t)&=\mathcal{R}(t)(\varphi(0)+f(0,\varphi))-f(t,\widetilde{u}_{t})
-\int_{0}^{t}A\mathcal{R}(t-s)f(s,\widetilde{u}_{s})ds  \\
&\quad -  \int_{0}^{t}\mathcal{R}(t-s) \int_{0}^{s}
 B(s- \xi)f(\xi, \widetilde{u}_{\xi}) d\xi ds+
\int_{0}^{t}\mathcal{R}(t-s)g(s,\widetilde{u}_{s})ds, \quad t\geq 0,
\end{align*}
where $ \widetilde{u}:\mathbb{R} \to X$ is the
function defined by the relation  $\widetilde{u}_{0}= \varphi$ and
$\widetilde{u} = u$ on $[0, \infty)$. 
We observe that $\mathcal{R}(\cdot)(\varphi(0)+f(0,\varphi)) 
\in C_b([0,\infty),X))$ and 
$$
\lim_{t \to \infty}(\mathcal{R}(t+n\omega) - R(t))(\varphi(0)+f(0,\varphi))=0,
$$
uniformly in $n \in \mathbb{N}$.
Moreover, from   \cite[Lemma 3.16]{Mi} and Lemma \ref{caiedo1}, we obtain 
that $\lim_{t \to \infty} \| f(t+n\omega,
\widetilde{u}_{t + n\omega}) - f(t, \widetilde{u}_{t}) \|_Y = 0$ and 
$\lim_{t \to \infty} \| g(t+n\omega, \widetilde{u}_{t+ n\omega}) 
- g(t, \widetilde{u}_{t}) \| = 0$, uniformly in 
$n \in \mathbb{N}$. By Lemmas \ref{caiedo2}, \ref{apide1} and
\ref{apide2} we have  that
$$ 
\lim_{t \to \infty} \Gamma x (t+n\omega) -\Gamma x(t)=0,
$$
uniformly in $n \in \mathbb{N}$. From  Lemma \ref{caiedo0} and using 
the same argument of the Theorem \ref{p1} proof we conclude
that  $u=\Gamma u \in \mathfrak{D}_0$ and $u$ is asymptotically 
$\omega$-periodic. The proof is ended.
\end{proof}

\section{Applications}\label{Examples}

 In this section we study the  existence of several type of
asymptotically periodicity solutions of  the partial neutral
integro-differential system
\begin{gather}
\begin{aligned}
&\frac{\partial}{\partial t}  \Big[ u(t, \xi) 
+  \int_{-\infty}^{t} \int_{0}^{\pi} b(s-t,\eta,\xi) u(s,\eta)d \eta ds\Big] 
 \\
& = (\frac{\partial^{2}} {\partial \xi^{2}} + \nu) \Big[u(t, \xi) 
+ \int_0^t  e^{- \gamma(t-s)} u(s,\xi) ds\Big]
+ \int_{-\infty}^{t} a_0(s-t) u(s, \xi)ds, 
\end{aligned} \label{eqexemcseg1} \\
u(t, 0)  = u(t, \pi)  =  0,   \quad
u(\theta, \xi)  = \varphi(\theta, \xi),  \label{eqexemcseg2}
\end{gather}
for $(t,\xi)\in [0,a] \times [0,\pi]$, $\theta\leq 0, \nu <0$ and
 $\gamma>0$.
Moreover, we have identified $\varphi(\theta)(\xi) =\varphi(\theta, \xi)$.

To represent  this system in the abstract form \eqref{eqi1}-\eqref{eqi2},  
we  choose  the spaces $X=L^{2}([0,\pi]) $ and
$\mathcal{B} = C_{0} \times L^{2}(\rho,X)$, see Example \ref{example1} 
for details. We also consider  the operators 
$A,B(t): D(A) \subseteq X \to X$, $t\geq 0 $,   given  by 
 $ A x= x'' + \nu x$, $ B(t)x = e^{-\gamma t} Ax $  
for $x\in D(A) = \{x \in X : x'' \in X,\, x(0) = x(\pi) = 0 \}$.
 Moreover, $A$ has discrete spectrum, the eigenvalues are $- n^{2}+\nu$,
  $n \in \mathbb{N}$, with corresponding  eigenvectors 
$z_{n} (\xi) = (\frac{2}{\pi})^{1/2} \sin (n \xi)$,  the set  of functions
  $\{z_{n} : n \in \mathbb{N} \}$ is an orthonormal basis of $X$ and
  $T(t)x = \sum_{n=1}^{\infty} e^{-(n^{2}- \nu)t} \langle x, z_{n} \rangle z_{n}$ 
for   $x\in  X$.  For $\alpha \in (0,1)$, from \cite{PA} we can define 
the fractional power $(-A)^{\alpha}: D((-A)^{\alpha}) \subset X \to X$ of $A$ 
 is given by
 $(-A)^{\alpha}x= \sum_{n=1}^{\infty} (n^2-\nu)^{\alpha} \langle x, z_{n}
 \rangle z_n$, where 
$D((-A)^{\alpha}) =\{ x \in X: (-A)^{\alpha}x \in X \}$. In the next Theorem 
we consider $Y=D((-A)^{1/2})$.  We observe that 
$\rho(A) \supset \{ \lambda \in \mathbb{C}: \operatorname{Re}(\lambda) \geq \nu\}$
 and $\|\lambda R(\lambda,A)\| \leq M_1$ for 
 $ \operatorname{Re}(\lambda)\geq \nu$, from 
\cite[Proposition 2.2.11]{Alessandra2}
 we obtain that $A$ is a sectorial operator satisfying 
$\|R(\lambda,A) \| \leq  \frac{M}{|\lambda -\nu|}, M>0$, therefore (H1) 
is satisfied. Moreover, it is easy to see that conditions 
(H2)--(H3) are satisfied with $b(t)= e^{-\gamma t}$, and
$D=C_{0}^{\infty}([0,\pi])$  the space of infinitely
differentiable functions that vanishes at $\xi =0$ and $\xi = \pi$.
Under the above conditions we can  represent   the system
\begin{gather}
\frac{\partial u(t,\xi)}{\partial t}= \Big(\frac{\partial^{2}}
{\partial \xi^{2}} + \nu\Big) \Big[u(t, \xi) + \int_0^t  e^{-
\gamma(t-s)} u(s,\xi) ds\Big], \label{sit1}  \\
u(t,\pi)  =  u(t,0)  = 0, \label{sit2}
\end{gather}
in the abstract for
\begin{gather*}
\frac{d x(t)}{dt}  =  A x(t) + \int_{0}^{t} B(t-s)x(s) ds, \\
x(0)  =  z \in X. 
\end{gather*}

 We define the functions $f, g : \mathcal{B}\to X$ by
\begin{gather*}
f(\psi)(\xi)  = \int_{-\infty}^{0}\int_{0}^{\pi} b(s,\eta,\xi) 
 \psi (s,\eta)d\eta ds, \\
g(\psi)(\xi)  = \int_{-\infty}^{0} a_0(s) \psi(s, \xi)ds,
\end{gather*}
where
 \begin{itemize}
\item[(i)]   The function  $a_{0}:\mathbb{R}\to
\mathbb{R}$  is continuous and $L_g := (\int_{-\infty}^{0}
\frac{(a_0(s))^{2}}{\rho (s)}ds )^{\frac{1}{2}} < \infty$.
\item[(ii)] The functions    $ b(\cdot)$,
   $ \frac{\partial b(s, \eta, \xi)} {\partial \xi} $
are  measurable,  $b(s, \eta, \pi) = b(s,\eta,\, 0) = 0$
for all $(s,\eta)$ and
 \[
 L_f:= \max \Big\{\Big(\int_{0}^{\pi} \int_{-\infty}^{0}
\int_{0}^{\pi}
\rho^{-1}(\theta)\Big(\frac{\partial^{i}}{\partial\xi ^{i}}
b(\theta, \eta, \xi)\Big)^2 d\eta d\theta d\xi
\Big)^{1/2}:i=0,1 \Big\}<\infty.
\]
\end{itemize}
 Moreover, $f, g $ are bounded linear operators, 
 $\|f\|_{\mathcal{L}(\mathcal{B},X)} \leq L_f$,
 $\|g\|_{\mathcal{L}(\mathcal{B},X)} \leq L_g$ and a
straightforward estimation using $\bf (ii)$ shows that 
$f(I\times \mathcal{B})\subset D((-A)^{\frac{1}{2}})$ and
 $$
\|(-A)^{\frac{1}{2}}f(t,\cdot)\|_{\mathcal{L}(\mathcal{B},X)} \leq L_f 
$$ 
for all $t\in I$.  { This allows us to rewrite }  the
system \eqref{eqexemcseg1}-\eqref{eqexemcseg2} in the  abstract 
form \eqref{eqi1}-\eqref{eqi2} with $u_0=\varphi \in
\mathcal{B}$.

\begin{theorem} \label{thm1}
Assume that the previous conditions are verified. 
Let $2<K<\gamma $ and $\nu<0$ such that 
$|\nu| > \max\{M(K+1+ \gamma ),\gamma\}$. 
If $ \frac{1}{2 \mathfrak{K}} \geq L_f\mu + \frac{M}{|r + \nu|}L_g$, 
where $\mu = ( \| (-A)^{-\frac{1}{2}}\| + M(2 + \dfrac{e^{r + \nu}}{|r + \nu|} 
+ \dfrac{1}{|r + \nu| \gamma} ) )$, then there exists $R>0$ such that if 
$\| \varphi \|_{\mathcal{B}}<R$,
\begin{itemize}
\item[(i)] there exists a unique mild solution $u(\cdot) \in AAA_c(X)$ of
\eqref{eqexemcseg1}-\eqref{eqexemcseg2}. % with $u_{0}=\varphi $.

\item[(ii)] there exists a unique mild solution $u(\cdot) \in  SAP_{\omega}(X)$
of \eqref{eqexemcseg1}-\eqref{eqexemcseg2}. 

\item[(iii)] there exists a unique asymptotically
 $\omega$-periodic mild solution $u(\cdot) $   of
 \eqref{eqexemcseg1}-\eqref{eqexemcseg2}.
\end{itemize}
\end{theorem}

\begin{proof}
By using a similar procedure   as in the proof of  \cite[Theorem 5.1]{Dos1}
 we obtain an exponentially  stable resolvent operator
 for the system \eqref{sit1}-\eqref{sit2}. 
 From the previous facts, Theorem \ref{constnresolvente} and 
Theorem \ref{estpr1},  the  assumption (P1) is satisfied.
Observing that 
$$ M \|\varphi\|_{\mathcal{B}} (1+L_f) <+\infty,
$$ 
since $ \frac{ r}{2 \mathfrak{K}} \geq L_f\mu +\frac{M}{\beta}L_g$, 
there exists a constant $r_0$ such that  if $R\geq r_0$, we have
$$ 
\frac{ R}{2 \mathfrak{K}} - L_f\mu R -
\frac{M}{\beta}L_gR > M \|\varphi\|_{\mathcal{B}} (1+L_f).
$$ 
Now, for $\|\varphi\|_{\mathcal{B}} <R$,  from  Theorem \ref{p1} we
obtain that there exists a unique mild solution of 
\eqref{eqexemcseg1}-\eqref{eqexemcseg2} such that 
 $u(\cdot) \in AAA_c(X)$. By
Proposition \ref{p2} there exists a unique mild solution 
$u(\cdot) \in SAP_{\omega}(X)$ of
\eqref{eqexemcseg1}-\eqref{eqexemcseg2} and from Proposition \ref{p3} 
it follows that there exists a unique asymptotically
 $\omega$-periodic mild solution $u(\cdot) $   of
 \eqref{eqexemcseg1}-\eqref{eqexemcseg2}.  The proof is complete.
\end{proof}


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