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

\AtBeginDocument{{\noindent\small {\em 
Electronic Journal of Differential Equations}, 
Vol. 2005(2005), No. 79, pp. 1--25.\newline 
ISSN: 1072-6691. URL: http://ejde.math.txstate.edu
or http://ejde.math.unt.edu
\newline ftp ejde.math.txstate.edu  (login: ftp)}
\thanks{\copyright 2005 Texas State University - San Marcos.}
\vspace{9mm}}

\begin{document}
\title[\hfilneg EJDE-2005/79\hfil Solutions approaching polynomials at infinity]
{Solutions approaching polynomials at infinity to nonlinear ordinary
differential equations}
\author[Ch. G. Philos, P. Ch. Tsamatos\hfil EJDE-2005/79\hfilneg]
{Christos G. Philos, Panagiotis Ch. Tsamatos}  % in alphabetical order

\address{Christos G. Philos \hfill\break
Department of Mathematics, University of Ioannina, P. O. Box 1186,
451 10 Ioannina, Greece} 
\email{cphilos@cc.uoi.gr}

\address{Panagiotis Ch. Tsamatos \hfill\break
Department of Mathematics, University of Ioannina, P. O. Box 1186,
451 10 Ioannina, Greece} 
\email{ptsamato@cc.uoi.gr}

\date{}
\thanks{Submitted February 13, 2005. Published July 11, 2005.}
\subjclass[2000]{34E05, 34E10, 34D05}
\keywords{Nonlinear differential equation; asymptotic properties;
\hfill\break\indent  
asymptotic expansions; asymptotic to polynomials solutions}

\begin{abstract}
 This paper concerns the solutions approaching polynomials at
 $\infty $ to $n$-th order ($n>1$) nonlinear ordinary differential
 equations, in which the nonlinear term depends  on  time $t$ and
 on $x,x',\dots ,x^{(N)}$, where $x$ is the unknown function and
 $N$ is an integer with $0\leq N\leq n-1$. For each given integer
 $m$ with $\max \{1,N\}\leq m\leq n-1$, conditions are given which
 guarantee that, for any real polynomial of degree at most $m$,
 there exists a solution that is asymptotic at $\infty $ to this
 polynomial. Sufficient conditions are also presented for every
 solution to be asymptotic at $\infty $ to a real polynomial of
 degree at most $n-1$. The results obtained extend those by the
 authors and by Purnaras \cite{p5} concerning the particular case
 $N=0$.
\end{abstract}

\maketitle
\numberwithin{equation}{section}
\newtheorem{theorem}{Theorem}[section]
\newtheorem{lemma}[theorem]{Lemma}
\newtheorem{corollary}[theorem]{Corollary}
\newtheorem{proposition}[theorem]{Proposition}
\newtheorem{example}[theorem]{Example}
\allowdisplaybreaks

\section{Introduction}

Since its invention by Isaac Newton around 1666, the theory of ordinary
differential equations has occupied a central position in the development of
mathematics. One reason for this is its widespread applicability in the
sciences. Another is its natural connectivity with other areas of
mathematics. In the theory of ordinary differential equations, the study of
the asymptotic behavior of the solutions is of great importance, especially
in the case of nonlinear equations. In applications of nonlinear ordinary
differential equations, any information about the asymptotic behavior of the
solutions is usually extremely valuable. Thus, there is every reason for
studying the asymptotic theory of nonlinear ordinary differential equations.

Very recently, the authors and Purnaras \cite{p5} studied solutions, which are
asymptotic at infinity to real polynomials of degree at most $n-1$, for the
$n$-th order ($n>1$) nonlinear ordinary differential equation
\begin{equation}
x^{(n)}(t)=f(t,x(t)),\quad t\geq t_{0}>0, \label{E0}
\end{equation}
where $f$ {\it is a continuous real-valued function on}
$[t_{0},\infty )\times \mathbb{R}$. The work in \cite{p5} is
essentially motivated by the recent one by Lipovan \cite{l2}
concerning the special case of the second order nonlinear ordinary
differential equation
\begin{equation}
x''(t)=f(t,x(t)),\quad t\geq t_{0}>0.
\label{tE0}
\end{equation}
The application of the main results in \cite{p5} to the second order nonlinear
ordinary differential equation \eqref{tE0} leads to
improved versions of the ones given in \cite{l2} (and of other previous related
results in the literature). Some closely related results for second order
nonlinear differential equations involving the derivative of the unknown
function have been given by Rogovchenko and Rogovchenko \cite{r1} (see, also,
Mustafa and Rogovchenko \cite{m2}).

It is the purpose of the present article to extend the results in \cite{p5} to
the more general case of the $n$-th order ($n>1$) nonlinear ordinary
differential equation
\begin{equation}
x^{(n)}(t)=f(t,x(t),x'(t),\dots ,x^{(N)}(t)),\quad t\geq t_{0}>0,  \label{EN}
\end{equation}
where $N$ {\it is an integer with} $0\leq N\leq n-1$, {\it and}
$f$
 {\it is a continuous real-valued function on} $[t_{0},\infty )\times
\mathbb{R}^{N+1}$. Note that our thoughts to extend the results in \cite{p5} for
the differential equation \eqref{EN}, in some future time, had been made
known in this paper.

Throughout the paper, we are interested in solutions of the
differential equation \eqref{EN} which are defined for all large
$t$, i.e., in solutions of \eqref{EN} on an interval $[T,\infty
)$, $T\geq t_{0}$, where $T$ may depend on the solution. For
questions about the global existence in the future of the
solutions of \eqref{EN}, we refer to standard classical theorems
in the literature (see, for example, Corduneanu \cite{c4}, Cronin
\cite{c5},
 and Lakshmikantham and Leela \cite{l1}).

The paper is organized as follows. In Section 2, for each given
integer $m$ with $\max \{1,N\}\leq m\leq n-1$, sufficient
conditions are presented in order that, for any real polynomial of
degree at most $m$, the differential equation \eqref{EN} has a
solution defined for all large $t$, which is asymptotic at $\infty
$ to this polynomial and such that the first $n-1$ derivatives of
the solution are asymptotic at $\infty $ to the corresponding
first $n-1$ derivatives of the given polynomial. Section 3 is
devoted to establishing conditions, which are sufficient for every
solution defined for all large $t$ of the differential equation
\eqref{EN} to be asymptotic at $\infty $ to a real polynomial of
degree at most $n-1$ (depending on the solution) and the first
$n-1$ derivatives of the solution to be asymptotic at $\infty $ to
the corresponding first $n-1$ derivatives of this polynomial.
Moreover, in Section 3, conditions are also given, which guarantee
that every solution $x$ defined for all large $t$ of \eqref{EN}
satisfies $[ x^{(j)}(t)/t^{n-1-j}] \to [c/(n-1-j)!] $ for $t\to
\infty $ ($j=0,1,\dots ,n-1$), where $c$ is some real number
(depending on the solution $x$). Section 4 contains the
application of the results to the special case of second order
nonlinear ordinary differential equations. For $n=2$ and $N=0$,
\eqref{EN} becomes \eqref{tE0}. Moreover, in the special case
where $n=2$ and $N=1$, \eqref{EN} can be written as
\begin{equation}
x''(t)=f(t,x(t),x'(t)),\quad t\geq t_{0}>0,  \label{tE1}
\end{equation}
where $f$ {\it is a continuous real-valued function on}
$[t_{0},\infty )\times \mathbb{R}^{2}$. Some general examples are
given in the last section (Section 5), which demonstrate the
applicability of the results (and, especially, of the main result
in Section 2).

The asymptotic theory of $n$-th order ($n>1$) nonlinear differential
equations has a very long history. A central role in this theory plays the
problem of the study of solutions which have a prescribed asymptotic
behavior via solutions of the equation $x^{(n)}=0$. In the special case of
second order nonlinear differential equations, a large number of papers have
appeared concerning this problem; see, for example, Cohen \cite{c1}, Constantin
\cite{c2}, Dannan \cite{d1}, Hallam \cite{h1}, Kamo and Usami \cite{k1},
 Kusano, Naito and Usami \cite{k2}, Lipovan \cite{l2}, Mustafa and
Rogovchenko \cite{m2}, Naito \cite{n1,n2,n3}, Philos
and Purnaras \cite{p4}, Rogovchenko and Rogovchenko \cite{r1,r2},
Rogovchenko \cite{r3},
Rogovchenko and Villari \cite{r4}, Souplet \cite{s2}, Tong \cite{t1},
 Waltman \cite{w1}, Yin
\cite{y1}, and Zhao \cite{z1}. For higher order differential equations (ordinary or,
more generally, functional), the above mentioned problem has also been
investigated by several researchers; see, for example, Kusano and Trench
\cite{k3,k4}, Meng \cite{m1}, Philos \cite{p1,p2,p3},
Philos, Sficas and Staikos \cite{p6},
Philos and Staikos \cite{p7}, and the references cited in these papers. We also
mention the paper by Trench \cite{t2} concerning linear second order ordinary
differential equations as well as the paper by Philos and Tsamatos \cite{p8}
about the problem of the asymptotic equilibrium for nonlinear differential
systems with retardations.

Before closing this section, we note that it is especially interesting to
examine the possibility of generalizing the results of the present paper in
the case of the $n$-th order ($n>1$) nonlinear delay differential equation
\[
x^{(n)}(t)=f(t,x(t-\tau _{0}(t)),x'(t-\tau
_{1}(t)),\dots ,x^{(N)}(t-\tau _{N}(t))),\quad t\geq t_{0}>0,
\]
where $\tau _{k}$ ($k=0,1,\dots ,N$) are nonnegative continuous
real-valued functions on $[t_{0},\infty )$ such that $\lim_{t\to
\infty }[t-\tau _{k}(t)]=\infty $ ($k=0,1,\dots ,N$).

\section{Conditions for the Existence of Solutions that are Asymptotic to
Polynomials at Infinity}

Our results in this section are the theorem below and its corollary.

\begin{theorem} \label{thm1}
Let $m$ be an integer with $\max\{1,N\}\leq m\leq n-1$, and assume that

\begin{multline}\label{e2.1}
\left| f(t,z_{0},z_{1},\dots ,z_{N})\right| \leq
\sum_{k=0}^{N}p_{k}(t)g_{k}\big( \frac{\left| z_{k}\right| }{t^{m-k}}%
\big) +q(t) \\
\text{\textit{for all} }(t,z_{0},z_{1},...,z_{N})\in [t_{0},\infty )
\times \mathbb{R}^{N+1},
\end{multline}
where $p_{k}$ $(k=0,1,\dots ,N)$ and $q$ are nonnegative
continuous real-valued functions on $[t_{0},\infty )$ such that
\begin{equation} \label{e2.2}
\int_{t_{0}}^{\infty }t^{n-1}p_{k}(t)dt<\infty \quad
(k=0,1,\dots ,N), \quad\text{and}\quad
\int_{t_{0}}^{\infty }t^{n-1}q(t)dt<\infty ,
\end{equation}
and $g_{k}$ $(k=0,1,\dots ,N)$ are nonnegative continuous
real-valued functions on $[0,\infty )$ which are not identically
zero. Let $c_{0},c_{1},\dots ,c_{m}$ be real numbers and $T$
 be a point with $T\geq t_{0}$, and suppose that there
exists a positive constant $K$ so that
\begin{equation} \label{e2.3}
\begin{aligned}
&\max_{k=0,1,\dots ,N}\Big\{ \sum_{\ell =0}^{N}\Big[ \int_{T}^{\infty }\frac{
(s-T)^{n-1-k}}{(n-1-k)!}p_{\ell }(s)ds\Big] \Theta _{\ell }(c_{\ell
},c_{\ell +1},\dots ,c_{m};T;K) \\
 &+\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}q(s)ds\Big\} \leq K,
\end{aligned}
\end{equation}
where
\begin{equation} \label{e2.4}
\Theta _{0}(c_{0},c_{1},\dots ,c_{m};T;K)=\sup \big\{ g_{0}(z):\text{ }0\leq
z\leq \frac{K}{T^{m}}+\sum_{i=0}^{m}\frac{| c_{i}| }{T^{m-i}}
\big\}
\end{equation}
and, provided that $N>0$,
\begin{multline}\label{e2.5}
\Theta _{\ell }(c_{\ell },c_{\ell +1},...,c_{m};T;K) \\
=\sup \big\{ g_{\ell }(z):0\leq z\leq \frac{K}{T^{m-\ell }}
+\sum_{i=\ell }^{m}\frac{i(i-1)...(i-\ell +1)\left| c_{i}\right|}{T^{m-i}}
\big\} \\
(\ell =1,...,N).
\end{multline}
Then the differential equation \eqref{EN} has a solution $x $ on
the interval $[T,\infty )$, which is asymptotic to the polynomial
$c_{0}+c_{1}t+\dots +c_{m}t^{m}$ as $t\to \infty $;
 i.e.,
\begin{equation} \label{e2.6}
x(t)=c_{0}+c_{1}t+\dots +c_{m}t^{m}+o(1)\quad \text{as } t\to
\infty ,
\end{equation}
and satisfies
 \begin{equation} \label{e2.7}
x^{(j)}(t)=\sum_{i=j}^{m}i(i-1)\dots (i-j+1)c_{i}t^{i-j}+o(1)
\quad \text{as } t\to \infty \quad (j=1,\dots ,m)
\end{equation}
and, provided that $m<n-1$,
\begin{equation} \label{e2.8}
x^{(\lambda )}(t)=o(1)\quad \text{as } t\to \infty \quad
(\lambda =m+1,\dots ,n-1).
\end{equation}
\end{theorem}

\begin{corollary} \label{coro1}
Let $m$ be an integer with $\max\{1,N\}\leq m\leq n-1$, and assume
that \eqref{e2.1} is satisfied, where $p_{k}$ $(k=0,1,\dots ,N)$
 and $q$, and $g_{k}$ $(k=0,1,\dots ,N)$ are as in Theorem $\ref{thm1}$.
Then, for any real numbers $c_{0},c_{1},\dots ,c_{m}$, the
differential equation \eqref{EN} has a solution $x$ on an interval
$[T,\infty )$ $($where $T\geq \max \{t_{0},1\}$ depends on
$c_{0},c_{1},\dots ,c_{m}$$)$, which is asymptotic to the
polynomial $c_{0}+c_{1}t+\dots +c_{m}t^{m}$ as $t\to \infty $;
i.e., \eqref{e2.6}  holds, and satisfies \eqref{e2.7} and
\eqref{e2.8} $($provided that $m<n-1$$)$.
\end{corollary}

The method which will be applied in the proof of Theorem \ref{thm1} is based on the
use of the well-known Schauder fixed point theorem (Schauder \cite{s1}). This
theorem can be found in several books on functional analysis (see, for
example, Conway \cite{c3}).

\begin{theorem}[Schauder theorem] \label{thmschauder}
Let $E$ be a Banach space and $X$ be any non\-empty convex and
closed subset of $E$. If $S$ is a continuous mapping of $X$ into
itself and $SX$ is relatively compact, then the mapping $S$ has at
least one fixed point $($i.e., there exists an $x\in X$ with $x=Sx
$$)$.
\end{theorem}

We need to consider the Banach space $BC([T,\infty ),\mathbb{R})$ of all
bounded continuous real-valued functions on the given interval
 $[T,\infty )$, endowed with the sup-norm $\|\cdot\|$:
\[
\| h\| =\sup_{t\geq T}| h(t)| \quad
\text{for }h\in BC([T,\infty ),\mathbb{R}).
\]

In the proof of Theorem \ref{thm1}, we will  use the set
$(BC)^{N}([T,\infty ),\mathbb{R})$ defined as follows:
($BC)^{0}([T,\infty ),\mathbb{R})$ coincides with $BC([T,\infty
),\mathbb{R})$; for $N>0$, $(BC)^{N}([T,\infty ),\mathbb{R})$ is
the set of all bounded continuous real-valued functions on the
interval $[T,\infty )$, which have bounded continuous $k$-order
derivatives on $[T,\infty )$\ for each $k=1,\dots ,N$. Clearly,
$(BC)^{N}([T,\infty ),\mathbb{R})$\ is a Banach space endowed with
the norm $\|\cdot\|_N$ defined by
\[
\| h\| _{N}=\max_{k=0,1,\dots ,N}\| h^{(k)}\|\quad \text{for }h\in
(BC)^{N}([T,\infty ),\mathbb{R}).
\]

To present a compactness criterion for subsets of the space
$(BC)^{N}([T,\infty ),\mathbb{R})$, we first give some well-known definitions
of notions referred to sets of real-valued functions. Let $U$ be a set of
real-valued functions defined on the interval $[T,\infty )$. The set $U$ is
called \textit{uniformly bounded }if there exists a positive constant $M$
such that, for all functions $u$ in $U$,
\[
| u(t)| \leq M\quad \text{for every }t\geq T.
\]
Also, $U$ is said to be \textit{equicontinuous} if, for each $\epsilon >0$,
there exists a $\delta \equiv \delta (\epsilon )>0$ such that, for all
functions $u$ in $U$,
\[
| u(t_{1})-u(t_{2})| <\epsilon \quad\text{for every }
t_{1},t_{2}\geq T\text{ with }| t_{1}-t_{2}| <\delta .
\]
Moreover, $U$ will be called \textit{equiconvergent at }$\infty $
if all functions in $U$ are convergent in $\mathbb{R}$ at the
point $\infty $ and, for each $\epsilon >0$, there exists a
$T_{\epsilon }\geq T$ such that, for all functions $u$ in $U$,
\[
| u(t)-\lim_{s\to \infty}u(s)| <\epsilon
\quad\text{for every }t\geq T_{\epsilon }.
\]

We have the following compactness criterion for subsets of
$(BC)^{N}([T,\infty ),\mathbb{R})$.

\begin{lemma}[Compactness criterion] \label{lemcompact}
Let $H$ be a subset of the Banach space \break $(BC)^{N}([T,\infty
),\mathbb{R})$ endowed with the norm $\|\cdot \| _{N}$. Define
$H^{(0)}=H$ and, provided that $N>0$, $H^{(k)}=\{h^{(k)}:h\in H\}
$ for $k=1,\dots ,N$. If $H^{(k)}$ $(k=0,1,\dots ,N)$ are
uniformly bounded, equicontinuous and
 equiconvergent at $\infty$, then $H$ is relatively compact.
\end{lemma}

In the special case $N=0$, i.e., in the case of the Banach space
$BC([T,\infty ),\mathbb{R})$, the above compactness criterion is
well-known (see Avramescu \cite{a1}, Staikos \cite{s3}). The
method used in the proof of our compactness criterion is a
generalization of the one applied in proving this criterion in the
special case of the Banach space $BC([T,\infty),\mathbb{R})$.

\begin{proof}[Proof of Lemma \ref{lemcompact}]
 First, we notice that the sets $H^{(k)}$ ($k=0,1,\dots ,N$)
are uniformly bounded if and only if the set $H$ is
uniformly bounded in $(BC)^{N}([T,\infty ),\mathbb{R})$ in the sense that
there exists a positive constant $M$ such that, for all functions $h$ in $H$,
\[
\vert h^{(k)}(t)\vert \leq M\quad \text{for every }t\geq T\quad
(k=0,1,\dots ,N).
\]
Also, we observe that $H^{(k)}$ ($k=0,1,\dots ,N$) are equicontinuous if and
only if $H$ is equicontinuous in $(BC)^{N}([T,\infty ),\mathbb{R})$, that
is, for each $\epsilon >0$, there exists a
$\delta \equiv \delta (\epsilon)>0$ such that, for all functions $h$ in $H$,
\[
\vert h^{(k)}(t_{1})-h^{(k)}(t_{2})\vert <\epsilon \quad\text{for
every }t_{1},t_{2}\geq T\text{ with }\vert t_{1}-t_{2}\vert
<\delta \quad(k=0,1,\dots ,N).
\]
Moreover, $H^{(k)}$ ($k=0,1,\dots ,N$) are equiconvergent at
$\infty $ if and only if $H$ is equiconvergent at $\infty $ in
$(BC)^{N}([T,\infty ),\mathbb{R})$ in the sense that all functions in $H$ are
convergent in $\mathbb{R}$ at the point $\infty $ and, provided that $N>0$,
 the first $N$ derivatives of every function in $H$ tend to zero at
$\infty$, and, for each $\epsilon >0$, there exists a
$T_{\epsilon}\geq T$ such that, for all functions $h$ in $H$,
\[
\vert h(t)-\lim_{s\to \infty}h(s)\vert
<\epsilon \quad\text{for every }t\geq T_{\epsilon }
\]
and, provided that $N>0$,
\[
| h^{(k)}(t)| <\epsilon \quad \text{for every }t\geq
T_{\epsilon }\quad (k=1,\dots ,N).
\]

Let $(BC)_{\ell }^{N}([T,\infty ),\mathbb{R})$ be the subspace of
$(BC)^{N}([T,\infty ),\mathbb{R})$ consisting of all functions $h$ in
$(BC)^{N}([T,\infty ),\mathbb{R})$ such that
$\lim_{t\to \infty }h(t)$ exists in $\mathbb{R}$
and, provided that $N>0$,
\[
\lim_{t\to \infty }h^{(k)}(t)=0\text{\ \ \ }(k=1,\dots ,N).
\]
Note that $(BC)_{\ell }^{N}([T,\infty ),\mathbb{R})$ is a closed subspace
of $(BC)^{N}([T,\infty ),\mathbb{R})$.

Consider the Banach space $C([0,1],\mathbb{R})$ of all continuous
real-valued functions on the interval $[0,1]$, endowed with the sup-norm
$\|\cdot\| ^{0}$:
\[
\| h\| ^{0}=\sup_{0\leq t\leq 1} | h(t)|
\quad\text{for }h\in C([0,1],\mathbb{R}).
\]
Consider, also, the set $C^{N}([0,1],\mathbb{R})$ defined as follows:
$C^{0}([0,1],\mathbb{R})$ coincides with $C([0,1],\mathbb{R})$; for $N>0$,
$C^{N}([0,1],\mathbb{R})$ is the set of all $N$-times continuously
differentiable real-valued functions on the interval $[0,1]$. Clearly,
$C^{N}([0,1],\mathbb{R})$ is a Banach space endowed with the norm $\| _{
\text{ }}\| _{N}^{0}$ defined by
\[
\| h\| _{N}^{0}=\max_{k=0,1,\dots ,N}\| h^{(k)}\| ^{0}\quad
\text{for }h\in C^{N}([0,1],\mathbb{R}).
\]

By the Arzel\`{a}-Ascoli theorem, a subset of the Banach space $C^{N}([0,1],
\mathbb{R})$ is relatively compact if and only if it is uniformly bounded
and equicontinuous. Note that a subset $H_{0}$ of $C^{N}([0,1],\mathbb{R})$
is called uniformly bounded if there exists a positive constant $M$ such
that, for all functions $h_{0}$ in $H_{0}$,
\[
| h_{0}^{(k)}(t)| \leq M\quad \text{for every }t\in [ 0,1]
\quad (k=0,1,\dots ,N).
\]
Also, a subset $H_{0}$ of $C^{N}([0,1],\mathbb{R})$ is said to be
equicontinuous if, for each $\epsilon >0$, there exists a $\delta \equiv
\delta (\epsilon )>0$ such that, for all functions $h_{0}$ in $H_{0}$,
\[
| h_{0}^{(k)}(t_{1})-h_{0}^{(k)}(t_{2})| <\epsilon
\]
for every $t_{1},t_{2}\in [ 0,1]$  with
$| t_{1}-t_{2}|<\delta$ $(k=0,1,\dots ,N)$.

Next, we consider the function
$\Phi :(BC)_{\ell }^{N}([T,\infty ),\mathbb{R})\to C^{N}([0,1],\mathbb{R})$
defined by the formula
\[
(\Phi x)(t)=\begin{cases}
x( T+\frac{t}{1-t}), & \text{if }0\leq t<1 \\
\lim_{s\to \infty}x(s), & \text{if }t=1.
\end{cases}
\]
It is not difficult to check that $\Phi $ is a homeomorphism
between the Banach spaces $(BC)_{\ell }^{N}([T,\infty
),\mathbb{R})$ and $C^{N}([0,1],\mathbb{R})$.
 So, it follows that a subset of the space
$(BC)_{\ell}^{N}([T,\infty ),\mathbb{R})$ is relatively compact if
and only if it is uniformly bounded, equicontinuous and equiconvergent
at $\infty $.

Now, assume that the sets $H^{(k)}$ ($k=0,1,\dots ,N$) are uniformly bounded,
equi\-continuous and equiconvergent at $\infty $. Then $H$ is uniformly
bounded, equicontinuous and equiconvergent at $\infty $, in
$(BC)^{N}([T,\infty ),\mathbb{R})$. Thus, $H$ is a relatively compact subset
of $(BC)_{\ell }^{N}([T,\infty ),\mathbb{R})$. Since $(BC)_{\ell
}^{N}([T,\infty ),\mathbb{R})$ is a closed subspace of $(BC)^{N}([T,\infty ),
\mathbb{R})$, we can be led to the conclusion that $H$ is also relatively
compact in $(BC)^{N}([T,\infty ),\mathbb{R})$.
The proof of the lemma is complete.
\end{proof}

\begin{proof}[Proof of Theorem \ref{thm1}]
 Set
\[
P_{m}(t)=c_{0}+c_{1}t+\dots +c_{m}t^{m}\equiv \sum_{i=0}^{m}c_{i}t^{i}
\quad\text{for }t\in \mathbb{R}.
\]
We have

\begin{equation*}
P_{m}^{(j)}(t)=\sum_{i=j}^{m}i(i-1)...(i-j+1)c_{i}t^{i-j}\quad \text{for }
t\in \mathbb{R}\quad  (j=1,...,m)
\end{equation*}

and, provided that $m<n-1$,
\[
P_{m}^{(\lambda )}(t)=0\quad \text{for }t\in \mathbb{R}\quad
(\lambda=m+1,\dots ,n-1).
\]
Furthermore, we see that the substitution
$y=x-P_{m}$
transforms the differential equation \eqref{EN} into the equation
\begin{equation}
y^{(n)}(t)=f( t,y(t)+P_{m}(t),y'(t)+P_{m}'(t),\dots
,y^{(N)}(t)+P_{m}^{(N)}(t)) .\label{ENast}
\end{equation}
 We observe that
\begin{gather*}
y(t)=x(t)-(c_{0}+c_{1}t+\dots +c_{m}t^{m}), \\
y^{(j)}(t)=x^{(j)}(t)-\sum_{i=j}^{m}i(i-1)\dots (i-j+1)c_{i}t^{i-j}\quad
(j=1,\dots ,m),
\end{gather*}
and, provided that $m<n-1$,
\[
y^{(\lambda )}(t)=x^{(\lambda )}(t)\quad (\lambda =m+1,\dots ,n-1).
\]
So, by taking into account \eqref{e2.6}, \eqref{e2.7} and \eqref{e2.8},
we can be led to the conclusion that what we have to prove is that the
differential equation \eqref{ENast} has a solution $y$ on the interval
$[T,\infty )$, which satisfies
\begin{equation} \label{e2.9}
\lim_{t\to \infty }y^{(\rho )}(t)=0\quad (\rho =0,1,\dots ,n-1).
\end{equation}

Let $E$ denote the Banach space $(BC)^{N}([T,\infty ),\mathbb{R})$\ endowed
with the norm $\|\cdot\| _{N}$, and let us define
\[
Y=\{y\in E:\text{ }\| y\| _{N}\leq K\}.
\]
It is clear that $Y$ is a nonempty convex and closed subset of $E$.

Consider, now, an arbitrary function $y$ in $Y$. Then
$| y(t)| \leq K$ for every $t\geq T$ and, provided that $N>0$,
\[
| y^{(\ell )}(t)| \leq K \quad \text{for every }t\geq T\quad (\ell
=1,\dots ,N).
\]
Thus, for every $t\geq T$, we obtain
\[
\frac{| y(t)+P_{m}(t)| }{t^{m}}\leq \frac{| y(t)| }{
t^{m}}+\sum_{i=0}^{m}\frac{| c_{i}| }{t^{m-i}}\leq \frac{K}{T^{m}}
+\sum_{i=0}^{m}\frac{| c_{i}| }{T^{m-i}}
\]
and, provided that $N>0$,
\begin{align*}
\frac{| y^{(\ell )}(t)+P_{m}^{(\ell )}(t)| }{t^{m-\ell }}
&\leq \frac{| y^{(\ell )}(t)| }{t^{m-\ell }}+\sum_{i=\ell }^{m}\frac{
i(i-1)\dots (i-\ell +1)| c_{i}| }{t^{m-i}} \\
&\leq \frac{K}{T^{m-\ell }}+\sum_{i=\ell }^{m}\frac{i(i-1)\dots (i-\ell
+1)| c_{i}| }{T^{m-i}}\quad(\ell =1,\dots ,N\text{).}
\end{align*}
Hence, we have
\[
g_{0}\big( \frac{| y(t)+P_{m}(t)| }{t^{m}}\big) \leq \Theta
_{0}(c_{0},c_{1},\dots ,c_{m};T;K)\quad\text{for }t\geq T,
\]
where $\Theta _{0}(c_{0},c_{1},\dots ,c_{m};T;K)$ is defined by
\eqref{e2.4}; moreover, provided that $N>0$, we have
\[
g_{\ell }\big( \frac{| y^{(\ell )}(t)+P_{m}^{(\ell )}(t)| }{
t^{m-\ell }}\big) \leq \Theta _{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)
\quad\text{for }t\geq T\quad (\ell =1,\dots ,N),
\]
where $\Theta _{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)$ are defined by
\eqref{e2.5}. But, from \eqref{e2.1} it follows that
\begin{align*}
&\big| f\big( t,y(t)+P_{m}(t),y'(t)+P_{m}'(t),\dots ,y^{(N)}(t)+P_{m}^{(N)}(t)
\big) \big| \\
&\leq p_{0}(t)g_{0}\big( \frac{| y(t)+P_{m}(t)| }{t^{m}}\big)
+p_{1}(t)g_{1}\big( \frac{| y'(t)+P_{m}'(t)| }{
t^{m-1}}\big) \\
&\quad+\dots +p_{N}(t)g_{N}\big( \frac{| y^{(N)}(t)+P_{m}^{(N)}(t)| }{
t^{m-N}}\big) +q(t)
\end{align*}
for all $t\geq T$. So, we have
\begin{multline} \label{e2.10}
| f( t,y(t)+P_{m}(t),y'(t)+P_{m}'(t),\dots ,y^{(N)}(t)+P_{m}^{(N)}(t)) | \\
\leq \sum_{\ell =0}^{N}p_{\ell }(t)\Theta _{\ell }(c_{\ell },c_{\ell
+1},\dots ,c_{m};T;K)\quad\text{for every }t\geq T.
\end{multline}
This inequality, together with \eqref{e2.2}, guarantee that
\[
\int_{T}^{\infty }\frac{(s-T)^{n-1}}{(n-1)!}f(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)) ds
\]
exists in $\mathbb{R}$. More generally, for each $\rho \in \{0,1,\dots ,n-1\}$,
\[
\int_{T}^{\infty }\frac{(s-T)^{n-1-\rho }}{(n-1-\rho )!}f(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)) ds
\]
exists in $\mathbb{R}$. Next, we use \eqref{e2.10} to obtain, for any $k\in
\{0,1,\dots ,N\}$ and for every $t\geq T$,
\begin{align*}
& \Big| \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!}f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds\Big| \\
& \leq \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!}\Big| f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) \Big| ds \\
& \leq \int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}\Big| f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) \Big| ds \\
& \leq \sum_{\ell =0}^{N}\Big[ \int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{
(n-1-k)!}p_{\ell }(s)ds\Big] \Theta _{\ell }(c_{\ell },c_{\ell
+1},\dots ,c_{m};T;K) \\
& \quad +\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}q(s)ds\,.
\end{align*}
Hence, by using \eqref{e2.3}, we have
\begin{multline} \label{e2.11}
\big| \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!}f\big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\big) ds\big| \\
\leq K  \quad \text{for all }t\geq T\quad (k=0,1,\dots ,N).
\end{multline}

We have thus proved that every function $y$ in $Y$ is such that
(2.12) holds. So, it is not difficult to check that the formula
\begin{align*}
(Sy)(t)&=(-1)^{n}\int_{t}^{\infty }\frac{(s-t)^{n-1}}{(n-1)!} \\
&\quad \times f\big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\big) ds
\quad \text{for }t\geq T
\end{align*}
defines a mapping $S$ of $Y$ into itself. Our purpose is to apply
the Schauder theorem for this mapping. We shall prove that $S$
satisfies the assumptions of the Schauder theorem.

We will show that $SY$ is relatively compact. Define $(SY)^{(0)}=SY$ and,
provided that $N>0$, $(SY)^{(k)}=\{(Sy)^{(k)}:y\in Y\}$ for $k=1,\dots ,N$.
By the given compactness criterion, in order to show that $SY$ is relatively
compact, it suffices to establish that each one of the sets $(SY)^{(k)}$ (
$k=0,1,\dots ,N$) is uniformly bounded, equicontinuous, and equiconvergent at
$\infty $. Let $k$ be an arbitrary integer in $\{0,1,\dots ,N\}$. Since
$SY\subseteq Y$, we obviously have $\| (Sy)^{(k)}\| \leq K$ for
all $y\in Y$, and consequently $(SY)^{(k)}$ is uniformly bounded. Moreover,
in view of \eqref{e2.10}, we obtain, for any function $y\in Y$
 and every $t\geq T$,
\begin{align*}
| (Sy)^{(k)}(t)-0|
&=\Big| \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!}\\
&\quad\times f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds\Big| \\
&\leq \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!} \\
&\quad\times \Big|f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) \Big| ds
\\
&\leq \sum_{\ell =0}^{N}\Big[ \int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{
(n-1-k)!}p_{\ell }(s)ds\Big] \Theta _{\ell }(c_{\ell },c_{\ell
+1},\dots ,c_{m};T;K) \\
&\quad +\int_{t}^{\infty }\frac{(s-t)^{n-1-k}}{(n-1-k)!}q(s)ds.
\end{align*}
Thus, by \eqref{e2.2}, it follows easily that ($SY)^{(k)}$ is
equiconvergent at $\infty $. Furthermore, by using again \eqref{e2.10}, for any
$y\in Y$ and for every $t_{1},t_{2}$ with $T\leq t_{1}<t_{2}$, we have:
\begin{align*}
&| (Sy)^{(n-1)}(t_{2})-(Sy)^{(n-1)}(t_{1})| \\
&=\Big| \int_{t_{2}}^{\infty }f\Big( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,
y^{(n-1)}(s)+P_{m}^{(n-1)}(s)\Big) ds \\
&\quad -\int_{t_{1}}^{\infty }f\Big( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,
y^{(n-1)}(s)+P_{m}^{(n-1)}(s)\Big) ds\Big| \\
&=\Big| -\int_{t_{1}}^{t_{2}}f\Big( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),
\dots ,y^{(n-1)}(s)+P_{m}^{(n-1)}(s)\Big) ds\Big| \\
&\leq \int_{t_{1}}^{t_{2}}f\Big( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),
\dots ,y^{(n-1)}(s)+P_{m}^{(n-1)}(s)\Big) \Big| ds
\\
&\leq \sum_{\ell =0}^{n-1}\Big[ \int_{t_{1}}^{t_{2}}p_{\ell }(s)ds\Big]
\Theta _{\ell }(c_{\ell },c_{\ell
+1},\dots ,c_{m};T;K)+\int_{t_{1}}^{t_{2}}q(s)ds,
\end{align*}
if $k=n-1$ (and so $N=n-1$); and
\begin{align*}
&| (Sy)^{(k)}(t_{2})-(Sy)^{(k)}(t_{1})| \\
&=\Big| \int_{t_{2}}^{\infty }\frac{(s-t_{2})^{n-1-k}}{(n-1-k)!}f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds \\
&\; -\int_{t_{1}}^{\infty }\frac{(s-t_{1})^{n-1-k}}{(n-1-k)!}f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds\Big| \\
&=\Big| \int_{t_{2}}^{\infty }\Big[ \int_{r}^{\infty }\frac{(s-r)^{n-2-k}
}{(n-2-k)!}f( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\\
&\quad \dots ,y^{(N)}(s)+P_{m}^{(N)}(s)) ds\Big] dr \\
&\quad -\int_{t_{1}}^{\infty }\Big[ \int_{r}^{\infty }\frac{(s-r)^{n-2-k}}{
(n-2-k)!}f( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),  \\
&\quad \dots ,y^{(N)}(s)+P_{m}^{(N)}(s)) ds\Big] dr\Big| \\
&=\Big| -\int_{t_{1}}^{t_{2}}\Big[ \int_{r}^{\infty }\frac{(s-r)^{n-2-k}}{
(n-2-k)!}f\big( s,y(s)+P_{m}(s),y'(s)+P_{m}'(s), \\
&\quad \dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\big) ds\Big] dr\Big| \\
&\leq \int_{t_{1}}^{t_{2}}\Big[ \int_{r}^{\infty }\frac{(s-r)^{n-2-k}}{
(n-2-k)!}\Big| f(s,y(s)+P_{m}(s),y'(s)+P_{m}'(s), \\
&\quad \dots ,y^{(N)}(s)+P_{m}^{(N)}(s))\Big| ds\Big] dr \\
&\leq \sum_{\ell =0}^{N}\Big\{ \int_{t_{1}}^{t_{2}}\Big[ \int_{r}^{\infty
}\frac{(s-r)^{n-2-k}}{(n-2-k)!}p_{\ell }(s)ds\Big] dr\Big\} \Theta
_{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K) \\
&\quad+\int_{t_{1}}^{t_{2}}\Big[ \int_{r}^{\infty }\frac{(s-r)^{n-2-k}}{(n-2-k)!
}q(s)ds\Big] dr,
\end{align*}
if $k<n-1$. Hence, it is not difficult to verify that the set $(SY)^{(k)}$
is equicontinuous. We have thus proved that $SY$ is relatively compact.

It remains to prove that the mapping $S$ is continuous. To this end, let us
consider a $y\in Y$ and an arbitrary sequence $( y_{\nu }) _{\nu\geq 1}$ in
$Y$ with
\[
\| \cdot \| _{N}-\lim_{\nu \to \infty }y_{\nu }=y.
\]
Then we obviously have $\| \cdot \| -\lim_{\nu \to \infty }y_{\nu
}=y$ and, provided that $N>0$,
\[
\| \cdot \| -\lim_{\nu \to \infty }y_{\nu}^{(k)}=y^{(k)}\quad (k=1,\dots ,N).
\]
On the other hand, by \eqref{e2.10}, we have, for all $\nu \geq 1$,
\begin{align*}
&\Big| f\Big( t,y_{\nu }(t)+P_{m}(t),y_{\nu }'(t)+P_{m}'(t),\dots ,
y_{\nu }^{(N)}(t)+P_{m}^{(N)}(t)\Big) \Big| \\
&\leq \sum_{\ell =0}^{N}p_{\ell }(t)\Theta _{\ell }(c_{\ell },c_{\ell
+1},\dots ,c_{m};T;K)+q(t)\quad\text{for every }t\geq T.
\end{align*}
So, because of \eqref{e2.2}, one can apply the Lebesgue dominated convergence
theorem to obtain, for every $t\geq T$,
\begin{align*}
&\lim_{\nu \to \infty }\int_{t}^{\infty }\frac{(s-t)^{n-1}
}{(n-1)!}f( s,y_{\nu }(s)+P_{m}(s),y_{\nu }'(s)+P_{m}'(s),\dots ,y_{\nu }^{(N)}(s)+P_{m}^{(N)}(s)) ds \\
&=\int_{t}^{\infty }\frac{(s-t)^{n-1}}{(n-1)!}f(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)) ds.
\end{align*}
This ensures the pointwise convergence
$\lim_{\nu \to \infty }(Sy_{\nu })(t)=(Sy)(t)$ for $t\geq T$.
Next, we  establish that
\begin{equation} \label{e2.12}
\|\cdot\| _{N}-\lim_{\nu \to \infty }Sy_{\nu }=Sy.
\end{equation}
For this purpose, we consider an arbitrary subsequence
$( Sy_{\mu _{\nu}}) _{\nu \geq 1}$ of $( Sy_{\nu }) _{\nu \geq 1}$. Since
$SY$ is relatively compact, there exists a subsequence
$( Sy_{\mu _{\lambda_{\nu }}}) _{\nu \geq 1}$ of
$( Sy_{\mu _{\nu }}) _{\nu\geq 1}$\ and a $u\in E$ so that
\[
\|\cdot\| _{N}-\lim_{\nu \to \infty }
Sy_{\mu _{\lambda _{\nu }}}=u.
\]
Since the $\|\cdot\| _{N}-$convergence implies the uniform
convergence and, in particular, the pointwise one to the same
limit function, we must have $u=Sy$. This means that (2.13) holds
true. We have thus proved that the mapping $S$ is continuous.

Now, by applying the Schauder theorem, we conclude that there
exists a $y\in Y $ with $y=Sy$. That is,
\begin{align*}
y(t)&=(-1)^{n}\int_{t}^{\infty }\frac{(s-t)^{n-1}}{(n-1)!}\\
&\quad\times f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds
\quad \text{ for }t\geq T.
\end{align*}
This yields
\[
y^{(n)}(t)=f( t,y(t)+P_{m}(t),y'(t)+P_{m}'(t),\dots
,y^{(N)}(t)+P_{m}^{(N)}(t))\quad \text{ for }t\geq T
\]
and so $y$ is a solution on $[T,\infty )$ of the differential equation
\eqref{ENast}. Furthermore, for each $\rho =0,1,\dots ,n-1$, we have
\begin{multline*}
(-1)^{n-\rho }y^{(\rho )}(t) \\
=\int_{t}^{\infty }\frac{(s-t)^{n-1-\rho }}{(n-1-\rho )!}f\Big(
s,y(s)+P_{m}(s),y'(s)+P_{m}'(s),\dots ,y^{(N)}(s)+P_{m}^{(N)}(s)\Big) ds
\end{multline*}
for all $t\geq T$. Thus, it follows that the solution $y$ satisfies
\eqref{e2.9}.
The proof of the theorem is now complete.
\end{proof}

\begin{proof}[Proof of Corollary \ref{coro1}]
Let $c_{0},c_{1},\dots ,c_{m}$ be given real
numbers. By taking into account the hypothesis that $g_{k}$ ($k=0,1,\dots ,N$)
are not identically zero on $[0,\infty )$, we can consider a positive
constant $K$ so that
\[
\Theta _{0}^{0}\equiv \sup \big \{ g_{0}(z):\text{ }0\leq z\leq
K+\sum_{i=0}^{m}| c_{i}|\big \} >0
\]
and, provided that $N>0$,
\[
\Theta _{\ell }^{0}\equiv \sup \big\{ g_{\ell }(z):\text{ }0\leq z\leq
K+\sum_{i=0}^{m}i(i-1)\dots (i-\ell +1)| c_{i}| \big\} >0
\quad(\ell =1,\dots ,N).
\]
Furthermore, by \eqref{e2.2}, we can choose a point $T\geq \max \{t_{0},1\}$
such that
\[
\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}p_{\ell }(s)ds\leq
 \frac{K}{2(N+1)\Theta _{\ell }^{0}}\quad(k,\ell =0,1,\dots ,N)
\]
and
\[
\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}q(s)ds\leq \frac{K}{2}
\quad(k=0,1,\dots ,N).
\]
Since $T\geq 1$, we have
\[
\frac{K}{T^{m}}+\sum_{i=0}^{m}\frac{| c_{i}| }{T^{m-i}}
\leq K+\sum_{i=0}^{m}| c_{i}|
\]
and, provided that $N>0$,
\[
\frac{K}{T^{m-\ell }}+\sum_{i=\ell }^{m}\frac{i(i-1)\dots (i-\ell
+1)| c_{i}| }{T^{m-i}}\leq K+\sum_{i=\ell }^{m}i(i-1)\dots (i-\ell
+1)| c_{i}|
\]
 for $\ell =1,\dots ,N$. Consequently,
\[
\Theta _{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)\leq \Theta
_{\ell }^{0} \quad (\ell =0,1,\dots ,N),
\]
where $\Theta _{0}(c_{0},c_{1},\dots ,c_{m};T;K)$ is defined by \eqref{e2.4}
 and, in the case where $N>0$,
$\Theta _{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)$
 ($\ell =1,\dots ,N$) are defined by \eqref{e2.5}. Now, we obtain
\begin{align*}
&\max_{k=0,1,\dots ,N}\Big\{ \sum_{\ell =0}^{N}\Big[
\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}p_{\ell
}(s)ds\Big] \Theta
_{\ell }(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)  \\
&+\int_{T}^{\infty }\frac{(s-T)^{n-1-k}}{(n-1-k)!}q(s)ds\Big\}  \\
&\leq \sum_{\ell =0}^{N}\frac{K}{2(N+1)\Theta _{\ell }^{0}}\Theta _{\ell
}(c_{\ell },c_{\ell +1},\dots ,c_{m};T;K)+\frac{K}{2} \\
&=\sum_{\ell =0}^{N}\frac{K}{2(N+1)}\cdot \frac{\Theta _{\ell }(c_{\ell
},c_{\ell +1},\dots ,c_{m};T;K)}{\Theta _{\ell }^{0}}+\frac{K}{2} \\
&\leq \frac{K}{2(N+1)}(N+1)+\frac{K}{2}=K,
\end{align*}
which implies  \eqref{e2.3}. Hence, the corollary follows from
Theorem \ref{thm1}.
\end{proof}

\section{Sufficient Conditions for all Solutions to be Asymptotic to
Polynomials at Infinity}

Our results in this section are formulated as a proposition and a theorem.
Our proposition is interesting of its own as a new
result. Moreover, this proposition will be used, in a basic way, in proving
Theorem \ref{thm2}.

\begin{proposition} \label{prop3.0}
Assume that
\begin{multline} \label{e3.1}
| f(t,z_{0},z_{1},\dots ,z_{N})|\leq
\sum_{k=0}^{N}p_{k}(t)g_{k}\big( \frac{| z_{k}| }{t^{n-1-k}} \big
) +q(t)\\
\quad \text{for all } (t,z_{0},z_{1},\dots ,z_{N})\in [
t_{0},\infty)\times \mathbb{R}^{N+1},
\end{multline}
where $p_{k}$ $(k=0,1,\dots ,N)$ and $q$ are nonnegative
continuous real-valued functions on $[t_{0},\infty )$ such that
\begin{equation} \label{e3.2}
\int_{t_{0}}^{\infty }p_{k}(t)dt<\infty \quad (k=0,1,\dots ,N), \quad
\text{and}\quad \int_{t_{0}}^{\infty }q(t)dt<\infty ;
\end{equation}
and $g_{k}$ $(k=0,1,\dots ,N)$ are continuous real-valued
functions on $[0,\infty )$, which are positive and increasing on
$(0,\infty )$ and such that
\begin{equation} \label{e3.3}
\int_{1}^{\infty }\frac{dz}{\sum_{k=0}^{N}g_{k}(z)}=\infty .
\end{equation}
Then every solution $x$ on an interval $[T,\infty )$,
$T\geq t_{0}$, of the differential equation \eqref{EN}
satisfies
\begin{equation} \label{e3.4}
x^{(j)}(t)=\frac{c}{(n-1-j)!}t^{n-1-j}+o(t^{n-1-j})\quad\text{as }
t\to \infty \quad (j=0,1,\dots ,n-1),
\end{equation}
where $c$ is some real number $($depending on the solution $x$$)$.
\end{proposition}

\begin{theorem} \label{thm2}
Assume that \eqref{e3.1} is satisfied, where $p_{k}$ $(k=0,1,\dots
,N)$ and $q$  are as in Theorem $\ref{thm1}$,
 i.e., nonnegative continuous real-valued functions on
$[t_{0},\infty)$ such that
\begin{equation} \label{e3.5}
\int_{t_{0}}^{\infty }t^{n-1}p_{k}(t)dt<\infty\quad (k=0,1,\dots
,N), \quad \textit{and} \quad \int_{t_{0}}^{\infty
}t^{n-1}q(t)dt<\infty ,
\end{equation}
and $g_{k}$ $(k=0,1,\dots ,N)$ are as in Proposition
$\ref{prop3.0}$. Then every solution $x$ on an interval $[T,\infty
)$, $T\geq t_{0}$, of the differential equation \eqref{EN} is
asymptotic to a polynomial $c_{0}+c_{1}t+\dots +c_{n-1}t^{n-1}$
 as $t\to \infty $; i.e.,
\begin{equation} \label{e3.6}
x(t)=c_{0}+c_{1}t+\dots +c_{n-1}t^{n-1}+o(1)\quad \textit{as}\quad
t\to \infty ,
\end{equation}
and satisfies
\begin{equation} \label{e3.7}
x^{(j)}(t)=\sum_{i=j}^{n-1}i(i-1)\dots
(i-j+1)c_{i}t^{i-j}+o(1)\quad \textit{as}\quad t\to \infty \quad
(j=1,\dots ,n-1),
\end{equation}
where $c_{0},c_{1},\dots ,c_{n-1}$ are real numbers $($depending
on the solution $x$$)$. More precisely, every solution $x$ on an
interval $[T,\infty )$, $T\geq t_{0}$, of \eqref{EN}
 satisfies
\begin{equation} \label{e3.8}
x(t)=C_{0}+C_{1}(t-T)+\dots +C_{n-1}(t-T)^{n-1}+o(1)\quad
\textit{as}\quad t\to \infty
\end{equation}
and
\begin{equation}\label{e3.9}
x^{(j)}(t)=\sum_{i=j}^{n-1}i(i-1)\dots
(i-j+1)C_{i}(t-T)^{i-j}+o(1)\quad \textit{as}\quad t\to \infty
\quad (j=1,\dots ,n-1),
\end{equation}
 where
\begin{multline} \label{e3.10}
C_{i}=\frac{1}{i!}\Big[ x^{(i)}(T)+(-1)^{n-1-i}\int_{T}^{\infty
}\frac{ (s-T)^{n-1-i}}{(n-1-i)!}f( s,x(s),x'(s),\dots ,x^{(N)}(s))
ds\Big]\\\quad (i=0,1,\dots ,n-1).
\end{multline}
\end{theorem}

Combining  Corollary \ref{coro1}  and Theorem \ref{thm2}, we
obtain the following result.\smallskip

{\it Assume that} \eqref{e3.1} {\it is satisfied, where} $p_{k}$
($k=0,1,\dots ,N$) {\it and} $q$  {\it are nonnegative continuous
real-valued functions on} $[t_{0},\infty )$ {\it such that}
\eqref{e3.5}
 {\it holds, and} $g_{k}$ ($k=0,1,\dots ,N$) {\it are nonnegative continuous
real-valued functions on} $[0,\infty )$ {\it which are not
identically zero. Then, for any real polynomial of degree at most}
$n-1$, {\it the differential equation} \eqref{EN} {\it has a
solution defined for all large} $t$, {\it which is asymptotic at}
$\infty $ {\it to this polynomial and such that the first} $n-1$
{\it derivatives of the solution are asymptotic at} $\infty $ {\it
to the corresponding first} $n-1$ {\it derivatives of the given
polynomial. Moreover, if, in addition,} $g_{k}$ ($k=0,1,\dots ,N$)
{\it are positive and increasing on} $(0,\infty )$ {\it and such
that} \eqref{e3.3} {\it holds, then every solution defined for all
large} $t$ {\it of the differential equation }\eqref{EN} {\it is
asymptotic at} $\infty $ {\it to a real polynomial of degree at
most} $n-1$ $(${\it depending on the solution}$)${\it and
 the first} $n-1$ {\it derivatives of the solution are
asymptotic at} $\infty $ {\it to the corresponding first} $n-1$
{\it derivatives of this polynomial.} \smallskip


The following lemma plays an important role in proving our proposition. This
lemma is the well-known Bihari's lemma (see Bihari \cite{b1}; see, also,
Corduneanu \cite{c4}) in a simple form which suffices for our needs.

\begin{lemma}[Bihari] Assume that
\[
h(t)\leq M+\int_{T_{0}}^{t}\mu (s)g(h(s))ds\quad \text{for }
t\geq T_{0},
\]
where $M$ is a positive constant, $h$ and $\mu $
 are nonnegative continuous real-valued functions on
$[T_{0},\infty )$, and $g$ is a continuous real-valued
function on $[0,\infty )$, which is positive and increasing on
$(0,\infty )$ and such that
\[
\int_{1}^{\infty }\frac{dz}{g(z)}=\infty .
\]
Then
\[
h(t)\leq G^{-1}\Big( G(M)+\int_{T_{0}}^{t}\mu (s)ds\Big) \quad
\text{for } t\geq T_{0},
\]
where $G$ is a primitive of $1/g$ on $(0,\infty)$ and $G^{-1}$
 is the inverse function of $G$.
\end{lemma}
\begin{proof}[Proof of Proposition 3.1\label{prop3.1}]
Consider an arbitrary solution $x$ on
an interval\textit{\ }$[T,\infty )$, $T\geq t_{0}$, of the differential
equation \eqref{EN}. From \eqref{EN} it follows that
\[
x^{(k)}(t)=\sum_{i=k}^{n-1}\frac{(t-T)^{i-k}}{(i-k)!}x^{(i)}(T)+\int_{T}^{t}
\frac{(t-s)^{n-1-k}}{(n-1-k)!}f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds
\]
($k=0,1,\dots ,N$) for $t\geq T$. Therefore, in view of \eqref{e3.1},
for any $k\in \{0,1,\dots ,N\}$ and
every $t\geq T$, we obtain
\begin{align*}
&| x^{(k)}(t)|  \\
&\leq \sum_{i=k}^{n-1}\frac{(t-T)^{i-k}}{(i-k)!}|
x^{(i)}(T)| +\int_{T}^{t}\frac{(t-s)^{n-1-k}}{(n-1-k)!}|
f( s,x(s),x'(s),\dots ,x^{(N)}(s)) | ds \\
&\leq \sum_{i=k}^{n-1}\frac{t^{i-k}}{(i-k)!}|
x^{(i)}(T)| +t^{n-1-k}\int_{T}^{t}| f(
s,x(s),x'(s),\dots ,x^{(N)}(s)) | ds \\
&\leq \sum_{i=k}^{n-1}\frac{t^{i-k}}{(i-k)!}|
x^{(i)}(T)| +t^{n-1-k}\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell
}(s)g_{\ell }\Big( \frac{| x^{(\ell )}(s)| }{s^{n-1-\ell
}}\Big) +q(s)\Big] ds \\
&\leq \Big[ \sum_{i=k}^{n-1}\frac{t^{i-k}}{(i-k)!}|
x^{(i)}(T)| +t^{n-1-k}\int_{T}^{t}q(s)ds\Big]  \\
&\quad +t^{n-1-k}\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell
}(s)g_{\ell }\Big( \frac{| x^{(\ell )}(s)| }{s^{n-1-\ell
}}\Big) \Big] ds.
\end{align*}
Thus, for any $k\in \{0,1,\dots ,N\}$, we have
\begin{align*}
&\frac{| x^{(k)}(t)| }{t^{n-1-k}} \\
&\leq \Big[ \sum_{i=k}^{n-1}\frac{1}{(i-k)!t^{n-1-i}}|
x^{(i)}(T)| +\int_{T}^{\infty }q(s)ds\Big]
+\int_{T}^{t}\Big[\sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell }
\Big( \frac{| x^{(\ell )}(s)| }{s^{n-1-\ell }}\Big) \Big] ds
\end{align*}
for every $t\geq T$. So, by taking into account \eqref{e3.2}, we immediately
conclude that, for each $k\in \{0,1,\dots ,N\}$, there exists a positive
constant $M_{k}$ such that
\[
\frac{| x^{(k)}(t)| }{t^{n-1-k}}\leq M_{k}+\int_{T}^{t}
\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell }\Big( \frac{|
x^{(\ell )}(s)| }{s^{n-1-\ell }}\Big) \Big] ds\quad\text{for }
t\geq T.
\]
Hence, by setting $M=\max_{k=0,1,\dots ,N}M_{k}$ \ ($M$ is a
positive constant), we obtain
\begin{align*}
\frac{| x^{(k)}(t)| }{t^{n-1-k}}\leq M+\int_{T}^{t}\Big[
\sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell }\Big ( \frac{| x^{(\ell
)}(s)| }{s^{n-1-\ell }}\Big ) \Big] ds \quad\text{for}\quad t\geq
T \quad (k=0,1,\dots ,N).
 \end{align*}
 That is,
\begin{equation} \label{e3.11}
\frac{| x^{(k)}(t)| }{t^{n-1-k}}\leq h(t)\quad
\text{for every } t\geq T\quad (k=0,1,\dots ,N),
\end{equation}
where
\[
h(t)=M+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell
}\Big( \frac{| x^{(\ell )}(s)| }{s^{n-1-\ell }}\Big ) \Big] ds
\quad\text{for }t\geq T.
\]
Furthermore, by using \eqref{e3.11} and the hypothesis that $g_{k}$
($k=0,1,\dots ,N$) are increasing on $(0,\infty )$, we obtain for
 every $t\geq T$
\begin{align*}
h(t) &\equiv M+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell
}\Big( \frac{| x^{(\ell )}(s)| }{s^{n-1-\ell }}\Big) \Big] ds \\
&\leq M+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)g_{\ell }(
h(s)) \Big] ds \\
&\leq M+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)\Big]
\Big[\sum_{\ell =0}^{N}g_{\ell }( h(s)) \Big] ds.
\end{align*}
Consequently,
\begin{equation} \label{e3.12}
h(t)\leq M+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)\Big] g(
h(s)) ds\quad\text{for }t\geq T,
\end{equation}
where $g=\sum_{\ell =0}^{N}g_{\ell }$.
Clearly, $g$ is a continuous real-valued function on $[0,\infty )$, which is
positive and increasing on $(0,\infty )$. Moreover, because of \eqref{e3.3}, $g$ is
such that
\begin{equation} \label{e3.13}
\int_{1}^{\infty }\frac{dz}{g(z)}=\infty .
\end{equation}
Next, we consider the function
\[
G(z)=\int_{M}^{z}\frac{du}{g(u)}\quad \text{for }z\geq M.
\]
We observe that $G$ is a primitive of the function $1/g$ on $[M,\infty )$.
It is obvious that $G(M)=0$ and that $G$ is strictly increasing on
$[M,\infty )$. Also, by \eqref{e3.13}, we have $G(\infty )=\infty $. So, it follows
that $G([M,\infty ))=[0,\infty )$. Thus, the inverse function $G^{-1}$ of $G$
is defined on $[0,\infty )$. Moreover, $G^{-1}$ is also strictly increasing
on $[0,\infty )$, and $G^{-1}([0,\infty ))=[M,\infty )$. Furthermore, we can
take into account \eqref{e3.12} and use the Bihari lemma to conclude that $h$
satisfies
\[
h(t)\leq G^{-1}\Big( G(M)+\int_{T}^{t}\Big[ \sum_{\ell =0}^{N}p_{\ell }(s)
\Big] ds\Big) =G^{-1}\Big( \sum_{\ell =0}^{N}\int_{T}^{t}p_{\ell
}(s)ds\Big)
\]
for $t\geq T$. Therefore, in view of \eqref{e3.2}, it follows that
\[
h(t)\leq G^{-1}\Big( \sum_{\ell =0}^{N}\int_{T}^{\infty }p_{\ell
}(s)ds\Big) \quad\text{for every }t\geq T;
\]
i.e., there exists a positive constant $\Lambda $ such that
$h(t)\leq \Lambda$  for $t\geq T$.
So, \eqref{e3.11} yields
\begin{equation} \label{e3.14}
\frac{| x^{(k)}(t)| }{t^{n-1-k}}\leq \Lambda \quad
\text{for all }t\geq T\quad (k=0,1,\dots ,N).
\end{equation}

Now, by taking into account \eqref{e3.1} and \eqref{e3.14},
we obtain for $t\geq T$
\begin{align*}
| f\big( t,x(t),x'(t),\dots ,x^{(N)}(t)\big) |
&\leq \sum_{k=0}^{N}p_{k}(t)g_{k}\Big(\frac{| x^{(k)}(t)| }{t^{n-1-k}
}\Big) +q(t) \\
&\leq \sum_{k=0}^{N}p_{k}(t)\big[ \sup_{0\leq z\leq \Lambda }
g_{k}(z)\big] +q(t)
\end{align*}
and consequently, in view of \eqref{e3.2},
\[
\int_{T}^{\infty }f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds
\quad\text{exists in }\mathbb{R}.
\]
On the other hand, from \eqref{EN} it follows that
\[
x^{(n-1)}(t)=x^{(n-1)}(T)+\int_{T}^{t}f( s,x(s),x'(s),\dots ,x^{(N)}(s)) ds
\quad\text{for }t\geq T,
\]
which gives
\[
\lim_{t\to \infty }x^{(n-1)}(t)=x^{(n-1)}(T)
+\int_{T}^{\infty }f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds\equiv c,
\]
where $c$ is a real number (depending on the solution $x$). Finally, by
applying the L'Hospital rule, we obtain
\[
\lim_{t\to \infty }\frac{x^{(j)}(t)}{t^{n-1-j}}=\frac{1}{
(n-1-j)!}\lim_{t\to \infty }x^{(n-1)}(t)=\frac{c}{(n-1-j)!
}\quad (j=0,1,\dots ,n-1),
\]
which implies that $x$ satisfies \eqref{e3.4}.
The proof of the proposition is complete.
\end{proof}

\begin{proof}[Proof of Theorem \ref{thm2}]
Let $x$ be an arbitrary solution on an interval $[T,\infty )$,
$T\geq t_{0}$,\ of the differential equation \eqref{EN}. Since
\eqref{e3.5} implies \eqref{e3.2}, as in the proof of Proposition
3.1, we can be led to the conclusion that \eqref{e3.14} holds,
where $\Lambda $ is some positive constant. This conclusion is
also a consequence of Proposition 3.1 itself; in fact, from this
proposition it follows that, for each $k=0,1,\dots ,N$,
$\lim_{t\to \infty }[ x^{(k)}(t)/t^{n-1-k}] $ exists (as a real
number). By using \eqref{e3.1} and \eqref{e3.14}, we obtain
\begin{align*}
| f\big( t,x(t),x'(t),\dots ,x^{(N)}(t)\big) |
&\leq \sum_{k=0}^{N}p_{k}(t)g_{k}\Big( \frac{| x^{(k)}(t)| }{t^{n-1-k}
}\Big) +q(t) \\
&\leq \sum_{k=0}^{N}p_{k}(t)\big[ \sup_{0\leq z\leq \Lambda }
g_{k}(z)\big] +q(t)
\end{align*}
for every $t\geq T$. This, together with \eqref{e3.5}, guarantee that
\[
L_{i}\equiv \int_{T}^{\infty }\frac{(s-T)^{n-1-i}}{(n-1-i)!}f\big(
s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds\quad (i=0,1,\dots ,n-1)
\]
are real numbers.
Now, \eqref{EN} gives,  for $t\geq T$,
\begin{equation} \label{e3.15}
x(t)=\sum_{i=0}^{n-1}\frac{(t-T)^{i}}{i!}x^{(i)}(T)+\int_{T}^{t}\frac{
(t-s)^{n-1}}{(n-1)!}f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds.
\end{equation}
Following the same procedure as in the proof of the corresponding theorem in
Philos, Purnaras and Tsamatos \cite{p5}, we can show that
\begin{align*}
&\int_{T}^{t}\frac{(t-s)^{n-1}}{(n-1)!}f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)
\big)ds \\
&=\sum_{i=0}^{n-1}\frac{(t-T)^{i}}{i!} (-1)^{n-1-i}L_{i}
+(-1)^{n}\int_{t}^{\infty }\frac{(s-t)^{n-1}}{(n-1)!}f\big(
s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds
\end{align*}
for all $t\geq T$. So, \eqref{e3.15} becomes
\begin{align*}
x(t)&=\sum_{i=0}^{n-1}\frac{(t-T)^{i}}{i!}\big[ x^{(i)}(T)+(-1)^{n-1-i}L_{i}
\big] \\
&\quad +(-1)^{n}\int_{t}^{\infty }\frac{(s-t)^{n-1}}{(n-1)!}f\big(
s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds\quad\text{for }t\geq T.
\end{align*}
Taking into account the definition of $L_{i}$ ($i=0,1,\dots ,n-1$) as well
as \eqref{e3.10}, we see that the above equation can be written as
\begin{equation} \label{e3.16}
x(t)=\sum_{i=0}^{n-1}C_{i}(t-T)^{i}+(-1)^{n}\int_{t}^{\infty }\frac{
(s-t)^{n-1}}{(n-1)!}f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds
\end{equation}
for all $t\geq T$. We have
\[
\lim_{t\to \infty }\int_{t}^{\infty }\frac{(s-t)^{n-1}}{
(n-1)!}f\big( s,x(s),x'(s),\dots ,x^{(N)}(s)\big) ds=0
\]
and thus \eqref{e3.16} implies that the solution $x$ satisfies
\eqref{e3.8}. Furthermore, \eqref{e3.16} gives
\begin{equation} \label{e3.17}
\begin{aligned}
x^{(j)}(t)=&\sum_{i=j}^{n-1}i(i-1)\dots (i-j+1)C_{i}(t-T)^{i-j} \\
&\quad +(-1)^{n-j}\int_{t}^{\infty
}\frac{(s-t)^{n-1-j}}{(n-1-j)!}f( s,x(s),x'(s),\dots ,x^{(N)}(s))
ds\\ &\quad\text{for}\quad t\geq T\quad (j=1,\dots ,n-1).
\end{aligned}
\end{equation}
Since
\[
\lim_{t\to \infty }\int_{t}^{\infty }\frac{(s-t)^{n-1-j}}{
(n-1-j)!}f( s,x(s),x'(s),\dots ,x^{(N)}(s)) ds=0\quad
(j=1,\dots ,n-1),
\]
it follows from \eqref{e3.17} that the solution $x$ satisfies, in addition,
\eqref{e3.9}. Finally, we observe that
\[
C_{0}+C_{1}(t-T)+\dots +C_{n-1}(t-T)^{n-1}\equiv c_{0}+c_{1}t+\dots
+c_{n-1}t^{n-1}
\]
for some real numbers $c_{0},c_{1},\dots ,c_{n-1}$. So, the solution $x$
satisfies \eqref{e3.6} and  \eqref{e3.7}.
The proof is complete.
\end{proof}




\section{Application of the Results to Second Order
Nonlinear Ordinary Differential Equations}

This section is devoted to the application of the results to the special
case of the second order nonlinear ordinary differential equations
\eqref{tE0} and \eqref{tE1}.

In the case of the differential equation \eqref{tE0}, Theorem
\ref{thm1}, Corollary \ref{coro1}, Proposition 3.1, and Theorem
\ref{thm2} are formulated as follows:

\begin{theorem} \label{thm1A}
Assume that
\begin{equation} \label{e4.1}
| f(t,z)| \leq p(t)g\big( \frac{| z| }{t}\big) +q(t)
\quad \text{for all } (t,z)\in [ t_{0},\infty )\times \mathbb{R},
\end{equation}
where $p$ and $q$ are nonnegative continuous
real-valued functions on $[t_{0},\infty )$ such that
\[
\int_{t_{0}}^{\infty }tp(t)dt<\infty \quad\text{and}\quad
\int_{t_{0}}^{\infty }tq(t)dt<\infty;
\]
and $g$ is a nonnegative continuous real-valued function
on $[0,\infty )$ which is not identically zero.
Let $c_{0},c_{1}$ be real numbers and $T$ be a
point with $T\geq t_{0}$, and suppose that there exists a positive
constant $K$ so that
\begin{align*}
&\Big[ \int_{T}^{\infty }(s-T)p(s)ds\Big] \sup\big\{ g(z):\text{
}0\leq z\leq \frac{K}{T}+\frac{| c_{0}| }{T}+| c_{1}| \big\}
+\int_{T}^{\infty }(s-T)q(s)ds\\
&\leq K.
\end{align*}
Then the differential equation \eqref{tE0}
 has a solution $x$ on the interval $[T,\infty )$, which
is asymptotic to the line $c_{0}+c_{1}t$ as $t\to \infty$;
 i.e.,
\begin{equation} \label{e4.2} %\label{e4.3}
x(t)=c_{0}+c_{1}t+o(1)\quad \text{as } \quad t\to \infty ,
\end{equation}
and satisfies
\begin{equation} \label{e4.3}
 x'(t)=c_{1}+o(1)\quad \text{as } \quad t\to \infty .
\end{equation}
\end{theorem}

\begin{corollary} \label{coroA}
Assume that \eqref{e4.1} is satisfied, where $p$, $q$, and $g$ are
as in Theorem $4.1$. Then, for any real numbers $c_{0},c_{1}$, the
differential equation \eqref{tE0} has a solution $x$ on an
interval $[T,\infty )$ $($where $T\geq \max\{t_{0},1\}$ depends on
$c_{0},c_{1}$$)$, which is asymptotic to the line $c_{0}+c_{1}t$
as $t\to \infty $; i.e., \eqref{e4.2} holds, and satisfies
\eqref{e4.3}.
\end{corollary}

\begin{proposition} \label{propA}
Assume that \eqref{e4.1} is satisfied,
where $p$ and $q$ are nonnegative continuous
real-valued functions on $[t_{0},\infty )$ such that
\[
\int_{t_{0}}^{\infty }p(t)dt<\infty \quad\text{and}\quad
\int_{t_{0}}^{\infty }q(t)dt<\infty ,
\]
and $g$ is a continuous real-valued function on
$[0,\infty )$, which is positive and increasing on $(0,\infty )$
and such that
\[
\int_{1}^{\infty }\frac{dz}{g(z)}=\infty .
\]
Then every solution $x$ on an interval $[T,\infty )$,
$T\geq t_{0}$, of the differential equation \eqref{tE0} satisfies
\[
x(t)=ct+o(t)\quad\text{and}\quad x'(t)=c+o(1), \quad \text{as }\quad
t\to \infty,
\]
where $c$ is some real number $($depending on the solution $x$$)$.
\end{proposition}

\begin{theorem} \label{thm2A}
Assume that \eqref{e4.1} is satisfied, where $p$ and $q$ are as in
Theorem $\ref{thm1A}$, and $g$ is as in Proposition $\ref{propA}$.
Then every solution $x$ on an interval $[T,\infty )$, $T\geq
t_{0}$, of the differential equation \eqref{tE0} is asymptotic to
a line $c_{0}+c_{1}t$ as $t\to \infty $;
 i.e., \eqref{e4.2} holds, and satisfies \eqref{e4.3}, where $c_{0},c_{1}$ are real numbers
$($depending on the solution $x$$)$. More precisely, every
solution $x$ on an interval $[T,\infty )$, $T\geq t_{0}$, of
\eqref{tE0} satisfies
\[
x(t)=C_{0}+C_{1}(t-T)+o(1) \quad{and}\quad x'(t)=C_{1}+o(1), \quad
\text{as } \quad t\to \infty,
\]
where
\[
C_{0}=x(T)-\int_{T}^{\infty }(s-T)f(s,x(s))ds\quad\text{and} \quad
C_{1}=x'(T)+\int_{T}^{\infty }f(s,x(s))ds.
\]
\end{theorem}

The above results have also been obtained in Philos, Purnaras and Tsamatos
\cite{p5} (as consequences of the main results given therein). Here, these
results are stated for the sake of completeness.

Now, we concentrate on the differential equation \eqref{tE1}. By
applying Theorem \ref{thm1},  Corollary \ref{coro1}, Proposition
3.1, and Theorem \ref{thm2} to the differential equation
\eqref{tE1}, we obtain following results:
\begin{theorem} \label{thm1B} Assume that
\begin{multline} \label{e4.5}
| f(t,z_{0},z_{1})| \leq p_{0}(t)g_{0}\big( \frac{|z_0| }{t}\big)
+p_{1}(t)g_{1}(| z_{1}| )+q(t)\\
\quad \text{for all }(t,z_{0},z_{1})\in [ t_{0},\infty
)\times\mathbb{R}^{2},
\end{multline}
where $p_{0}$, $p_{1}$, and $q$ are nonnegative
continuous real-valued functions on $[t_{0},\infty )$ such that
\[
\int_{t_{0}}^{\infty }tp_{0}(t)dt<\infty ,\quad
\int_{t_{0}}^{\infty }tp_{1}(t)dt<\infty , \quad
\text{and}\quad \int_{t_{0}}^{\infty }tq(t)dt<\infty;
\]
and $g_{0}$ and $g_{1}$ are nonnegative
continuous real-valued functions on $[0,\infty )$ which are not
identically zero.
Let $c_{0},c_{1}$ be real numbers and $T$ be a
point with $T\geq t_{0}$, and suppose that there exists a positive
constant $K$ so that
\begin{align*}
&\Big[ \int_{T}^{\infty }(s-T)p_{0}(s)ds\Big] \sup \big\{
g_{0}(z):\enskip
 0\leq z\leq \frac{K}{T}+\frac{| c_{0}| }{T}+| c_{1}|
\big\} \\
&+\Big[ \int_{T}^{\infty }(s-T)p_{1}(s)ds\Big] \sup \big\{
g_{1}(z):\enskip 0\leq z\leq K+| c_{1}| \big\}
+\int_{T}^{\infty}(s-T)q(s)ds\leq K
\end{align*}
and

\begin{align*}
&\Big[ \int_{T}^{\infty }p_{0}(s)ds\Big] \sup \big\{
g_{0}(z):\enskip 0\leq z\leq \frac{K}{T}+\frac{| c_{0}| }{T}+|
c_{1}|
\big\} \\
&+\Big[ \int_{T}^{\infty }p_{1}(s)ds\Big] \sup \big\{ g_{1}(z):\text{ }
0\leq z\leq K+| c_{1}| \big\} +\int_{T}^{\infty }q(s)ds\leq K\,.
\end{align*}
Then the conclusion of Theorem $\ref{thm1A}$ holds for the
differential equation \eqref{tE1}.
\end{theorem}

\begin{corollary} \label{coroB}
Assume that \eqref{e4.5} is satisfied, where $p_{0},p_{1}$, and
$q$, and $g_{0}$ and $g_{1}$ are as in Theorem $\ref{thm1B}$. Then
the conclusion of Corollary $\ref{coroA}$ holds for the
differential equation \eqref{tE1}.
\end{corollary}

\begin{proposition} \label{propB}
Assume that \eqref{e4.5} is satisfied, where $p_{0}$, $p_{1}$, $q$
are nonnegative continuous real-valued functions on $[t_{0},\infty
)$ such that
\[
\int_{t_{0}}^{\infty }p_{0}(t)dt<\infty ,\quad
\int_{t_{0}}^{\infty}p_{1}(t)dt<\infty ,\quad \text{and}\quad
\int_{t_{0}}^{\infty}q(t)dt<\infty ;
\]
and $g_{0}$ and $g_{1}$ are continuous
real-valued functions on $[0,\infty )$, which are positive and
increasing on $(0,\infty )$ and such that
\[
\int_{1}^{\infty }\frac{dz}{g_{0}(z)+g_{1}(z)}=\infty .
\]
Then the conclusion of Proposition $\ref{propA}$ holds for the
differential equation \eqref{tE1}.
\end{proposition}

\begin{theorem} \label{thm2B}
Assume that \eqref{e4.5} is satisfied, where $p_{0}$, $p_{1}$, $q$
are as in Theorem $\ref{thm1B}$, and $g_{0}$ and $g_{1}$ are as in
Proposition $\ref{propB}$. Then the conclusion of Theorem
$\ref{thm2A}$ holds for the differential equation \eqref{tE1} with
\[
C_{0}=x(T)-\int_{T}^{\infty }(s-T)f(s,x(s),x'(s))ds, \quad
C_{1}=x'(T)+\int_{T}^{\infty }f(s,x(s),x'(s))ds.
\]
\end{theorem}

\section{Examples}

\begin{example}[Philos, Purnaras, Tsamatos \cite{p5}] \label{ex1} \rm
Consider the second order superlinear Emden-Fowler equation
\begin{equation}
x''(t)=a(t)[x(t)]^{2}\mathop{\rm sgn}x(t),\quad t\geq t_{0}>0,  \label{D1}
\end{equation}
where $a$ {\it is a continuous real-valued function on}
$[t_{0},\infty )$.
\end{example}

Applying Theorem \ref{thm1} (or, in particular, Theorem \ref{thm1A}),
 we obtain the following result:

{\it Assume that}
\begin{equation} \label{e5.1}
\int_{t_{0}}^{\infty }t^{3}| a(t)| dt<\infty .
\end{equation}
{\it Let} $c_{0},c_{1}$ {\it be real numbers and} $T$ {\it be a
point with} $T\geq t_{0}$, {\it and suppose that there exists a
positive constant} $K$ {\it so that}
\begin{equation} \label{e5.2}
A(T)\Big( \frac{K}{T}+\frac{| c_{0}| }{T}+|c_{1}| \Big) ^{2}\leq K,
\end{equation}
{\it where}
\begin{equation} \label{e5.3}
A(T)=\int_{T}^{\infty }(s-T)s^{2}| a(s)| ds.
\end{equation}
{\it Then} \eqref{D1} {\it has a solution $x$ on the interval}
$[T,\infty )$, {\it which is asymptotic to the line}
$c_{0}+c_{1}t$ {\it as} $t\to \infty $; {\it i.e.,}
\begin{equation} \label{e5.4} % {e5.5}
x(t)=c_{0}+c_{1}t+o(1)\quad\text{{\it as }} \quad t\to \infty ,
\end{equation}
{\it and satisfies}
\begin{equation}
 x'(t)=c_{1}+o(1) \quad\text{{\it as} }\quad t\to
\infty \,.
\end{equation}

Now, assume that \eqref{e5.1} is satisfied, and let $c_{0},c_{1}$ be given real
numbers and $T\geq t_{0}$ be a fixed point. Moreover, let $A(T)$ be defined
by \eqref{e5.3}. As it has been proved in \cite{p5}, there exists a positive
constant $K$ so that \eqref{e5.2} holds if and only if
\begin{equation} \label{e5.6}
A(T)( | c_{0}| +| c_{1}| T) \leq \frac{T^{2}}{4}.
\end{equation}
Thus, we have the following result:

{\it Assume that} \eqref{e5.1} {\it is satisfied, and let}
$c_{0},c_{1}$
 {\it be real numbers and} $T\geq t_{0}$  {\it be a point so that}
\eqref{e5.6} {\it holds, where} $A(T)$ {\it is defined by}
\eqref{e5.3}. {\it Then} \eqref{D1} {\it has a solution} $x$ {\it
on the interval} $[T,\infty )$, {\it which satisfies}
\eqref{e5.4}{\it and} (5.6).

In particular, let us consider  the differential equation
\eqref{D1} with
$a(t)=t^{\sigma }\mu (t)$ for $t\geq t_{0}$,
where $\sigma $ is a real number and $\mu $ is a continuous and bounded
real-valued function on $[t_{0},\infty )$. In this case, there exists a
positive constant $\theta $ so that
\[
| a(t)| \leq \theta t^{\sigma }\quad \text{for every }t\geq t_{0}.
\]
We see that \eqref{e5.1} is satisfied if $\sigma <-4$. Furthermore,
assume that $\sigma <-4$ and let $c_{0},c_{1}$ be real numbers and
$T\geq t_{0}$ be a point. Then (see \cite{p5}) it follows that \eqref{e5.6}
holds if
\[
T^{\sigma +2}( | c_{0}| +| c_{1}| T) \leq
\frac{(\sigma +3)(\sigma +4)}{4\theta }.
\]


\begin{example} \label{ex2}\rm
 Consider the $n$-th order ($n>1$) sublinear
Emden-Fowler equation
\begin{equation}
x^{(n)}(t)=a(t)| x(t)| ^{1/2}\mathop{\rm sgn}x(t),\quad t\geq
t_{0}>0,  \label{D2}
\end{equation}
where $a$ {\it is a continuous real-valued function on}
$[t_{0},\infty )$.
\end{example}

For the differential equation (5.8), we have the following result:

{\it Let} $m$ {\it be an integer with} $1\leq m\leq n-1$, {\it and
assume that}
\begin{equation} \label{e5.7}
\int_{t_{0}}^{\infty }t^{n-1+(m/2)}| a(t)| dt<\infty .
\end{equation}
{\it Then, for any real numbers} $c_{0},c_{1},\dots ,c_{m}$, {\it
the differential equation} \eqref{D2} {\it has a solution} $x$
{\it on the $($whole$)$ interval} $[t_{0},\infty )$, {\it which is
asymptotic to the polynomial} $c_{0}+c_{1}t+\dots +c_{m}t^{m}$
{\it as} $t\to \infty$; {\it i.e.,}
\begin{align*}
x(t)=c_{0}+c_{1}t+\dots +c_{m}t^{m}+o(1)\quad\text{{\it as} }\quad
t\to \infty ,
\end{align*}
{\it and satisfies}
\begin{align*}
x^{(j)}(t)=\sum_{i=j}^{m}i(i-1)\dots
(i-j+1)c_{i}t^{i-j}+o(1)\quad\text{{\it as}}\quad t\to \infty
\quad (j=1,\dots ,m)
\end{align*}
{\it and, provided that} $m<n-1$,
\[
 x^{(\lambda )}(t)=o(1)\quad \text{ {\it as}}\quad t\to \infty \quad  (\lambda =m+1,\dots ,n-1).
\]
 To prove the above result, we assume that \eqref{e5.7} is
satisfied and we consider arbitrary real numbers
$c_{0},c_{1},\dots ,c_{m}$. By Theorem \ref{thm1}, it is
sufficient to show that there exists a positive constant $K$ such
that
\begin{equation} \label{e5.8}
A(t_{0})\Big( \frac{K}{t_{0}^{m}}+\sum_{i=0}^{m}\frac{| c_{i}| }{
t_{0}^{m-i}}\Big) ^{1/2}\leq K,
\end{equation}
where
\[
A(t_{0})=\int_{t_{0}}^{\infty }\frac{(s-t_{0})^{n-1}}{(n-1)!}s^{m/2}|
a(s)| ds.
\]
In the trivial case $A(t_{0})=0$, \eqref{e5.8} holds for any
positive constant $K$. So, in the sequel, we suppose that $A(t_{0})>0$. We
see that \eqref{e5.8} is equivalent to
\begin{equation} \label{e5.9}
K^{2}-\frac{[ A(t_{0})] ^{2}}{t_{0}^{m}}K-[ A(t_{0})]
^{2}\sum_{i=0}^{m}\frac{| c_{i}| }{t_{0}^{m-i}}\geq 0.
\end{equation}
Let us consider the quadratic equation
\[
\Omega (\omega )\equiv \omega ^{2}-\frac{[ A(t_{0})] ^{2}}{
t_{0}^{m}}\omega -[ A(t_{0})] ^{2}\sum_{i=0}^{m}\frac{|
c_{i}| }{t_{0}^{m-i}}=0
\]
in the complex plane. The discriminant of this equation is
\[
\Delta =\Big [ -\frac{[ A(t_{0})] ^{2}}{t_{0}^{m}}\Big ]
^{2}-4\Big [ -[ A(t_{0})] ^{2}\sum_{i=0}^{m}\frac{|
c_{i}| }{t_{0}^{m-i}}\Big ] .
\]
We see that $\Delta >0$ and so the equation $\Omega (\omega )=0$ has
two real roots:
\[
\omega _{1}=\frac{[ A(t_{0})] ^{2}}{2t_{0}^{m}}-\frac{\sqrt{\Delta }}{2},\quad
\omega _{2}=\frac{[ A(t_{0})] ^{2}}{2t_{0}^{m}}+\frac{\sqrt{\Delta }}{2}
\]
with  $\omega _{1}<\omega _{2}$. Clearly, $\omega _{2}>0$. We have
$\Omega (\omega )\geq 0$ for all $\omega \geq \omega _{2}$.
Hence, \eqref{e5.9} (or, equivalently, \eqref{e5.8}) is satisfied for
every positive
constant $K$ with $K\geq \omega _{2}>0$. We have thus proved that, in both
cases where $A(t_{0})=0$ or $A(t_{0})>0$, there exists a positive constant
$K $ so that \eqref{e5.8} holds. So, our result has been proved.

\begin{example} \label{ex3} \rm
Consider the second order Emden-Fowler equation
\begin{equation}
x''(t)=a(t)| x(t)| ^{\gamma }\mathop{\rm sgn}
x(t)+b(t)| x'(t)| ^{\delta }\mathop{\rm sgn}x'(t)
,\quad t\geq t_{0}>0,  \label{D}
\end{equation}
where $a$ {\it and} $b$ {\it are continuous real-valued functions
on} $[t_{0},\infty )$, {\it and} $\gamma $ {\it and} $\delta$ {\it
are positive real numbers}.
\end{example}\par
By applying Theorem \ref{thm1} (or, in particular, Theorem \ref{thm1B})
to the differential equation \eqref{D}, we arrive at the next result:

 {\it Assume that}
\begin{equation} \label{e5.10}
\int_{t_{0}}^{\infty }t^{1+\gamma }| a(t)| dt<\infty \quad
\text{{\it and}}\quad \int_{t_{0}}^{\infty }t| b(t)| dt<\infty .
\end{equation}
{\it Let} $c_{0},c_{1}$  {\it be real numbers and} $T$ {\it be a
point with} $T\geq t_{0}$, {\it and suppose that there exists a
positive constant} $K$ {\it so that}
\begin{align*}
&\Big[ \int_{T}^{\infty }(s-T)s^{\gamma }| a(s)| ds\Big] \Big(
\frac{K}{T}+\frac{| c_{0}| }{T}+| c_{1}| \Big)^{\gamma }
+\Big[ \int_{T}^{\infty }(s-T)| b(s)| ds\Big] ( K+|c_{1}| ) ^{\delta }\\
&\leq K
\end{align*}
{\it and}
\[
\Big[ \int_{T}^{\infty }s^{\gamma }| a(s)| ds\Big] \Big(
\frac{K}{T}+\frac{| c_{0}| }{T}+| c_{1}| \Big) ^{\gamma }+\Big[
\int_{T}^{\infty }| b(s)| ds\Big] ( K+| c_{1}|) ^{\delta }\leq K.
\]
{\it Then} \eqref{D} {\it has a solution $x$ on the interval}
$[T,\infty )$, {\it which is asymptotic to the line}
$c_{0}+c_{1}t$ {\it as} $t\to \infty $; {\it i.e.,} \eqref{e5.4}
{\it holds, and satisfies} (5.6).

Moreover, an application of Corollary \ref{coro1}
 (or, in particular, of Corollary 4.6) to the
differential equation \eqref{D} leads to the following result:

{\it Assume that} \eqref{e5.10} {\it is satisfied. Then, for any
real numbers} $c_{0},c_{1}$, \eqref{D} {\it has a solution} $x$
{\it on an interval} $[T,\infty )$ ({\it where} $T\geq
\max\{t_{0},1\}$ {\it  depends on} $c_{0},c_{1}$), {\it which
satisfies} \eqref{e5.4} {\it and} (5.6).

Also, we can apply Proposition 3.1 (or, in particular, Proposition
$\ref{propB}$) for the differential equation \eqref{D} to obtain
the result:

{\it If}
\begin{equation} \label{e5.11}
\int_{t_{0}}^{\infty }t^{\gamma }| a(t)| dt<\infty \quad
\text{{\it and}}\quad \int_{t_{0}}^{\infty }| b(t)| dt<\infty ,
\end{equation}
{\it and} $\gamma \leq 1$ {\it and} $\delta \leq 1$, {\it then
every solution} $x$ {\it on an interval} $[T,\infty )$, $T\geq
t_{0}$,
 {\it of} \eqref{D} {\it satisfies}
\[
x(t)=ct+o(t) \quad\text{{\it and}}\quad x'(t)=c+o(1), \quad
\text{{\it as }} \quad t\to \infty,
\]
{\it where} $c$ {\it is some real number $($depending on the
solution} $x$).

Furthermore, applying Theorem \ref{thm2} (or, in particular,
Theorem \ref{thm2B}) to the differential equation (5.12), we
obtain the following result:

{\it Assume that} \eqref{e5.10} {\it is satisfied, and that}
$\gamma \leq 1$ {\it and} $\delta \leq 1$. {\it Then every
solution} $x$ {\it on an interval} $[T,\infty )$, $T\geq t_{0}$,
{\it of} \eqref{D} {\it is asymptotic to a line} $c_{0}+c_{1}t$
{\it as} $t\to \infty $;
 {\it i.e.,} \eqref{e5.4} {\it holds, and satisfies} $(5.6)$,
{\it where} $c_{0},c_{1}$ {\it are real numbers} ({\it depending
on the solution} $x$). {\it More precisely, every solution} $x$
{\it on an interval} $[T,\infty )$, $T\geq t_{0}$, {\it of}
\eqref{D} {\it satisfies}
\[
x(t)=C_{0}+C_{1}(t-T)+o(1) \quad and \quad x'(t)=C_{1}+o(1), \quad
as \quad t\to \infty,
\]
{\it where}
\begin{gather*}
C_{0}=x(T)-\int_{T}^{\infty }\! (s-T)a(s)| x(s)| ^{\gamma }\mathop{\rm sgn}
x(s)ds-\int_{T}^{\infty }(s-T)b(s)| x'(s)| ^{\delta }
\mathop{\rm sgn}x'(s)ds, \\
C_{1}=x'(T)+\int_{T}^{\infty }a(s)| x(s)| ^{\gamma }
\mathop{\rm sgn}x(s)ds+\int_{T}^{\infty }b(s)| x'(s)| ^{\delta
}\mathop{\rm sgn}x'(s)ds.
\end{gather*}

Before ending this example, we concentrate on the
Emden-Fowler equation \eqref{D} with
\[
a(t)=t^{\sigma }\mu (t)\quad \text{for }t\geq t_{0},
\quad\text{and}\quad b(t)=t^{\tau }\nu (t)\quad \text{for }t\geq
t_{0},
\]
where $\sigma $ and $\tau $ are real numbers, and $\mu $ and $\nu $ are
continuous and bounded real-valued functions on $[t_{0},\infty )$. In this
case, we have
\[
| a(t)| \leq \theta t^{\sigma }\quad \text{for }t\geq t_{0}, \quad
\text{and}\quad | b(t)| =\xi t^{\tau }\quad \text{for }t\geq
t_{0},
\]
where $\theta $ and $\xi $ are positive constants. We see that \eqref{e5.10}
is satisfied if
$\gamma +\sigma <-2$ and $\tau <-2$.
Moreover, we observe that \eqref{e5.11} holds if
$\gamma +\sigma <-1$ and $\tau <-1$.


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