
\documentclass[twoside]{article}
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\markboth{\hfil Analytic solutions of n-th order differential equations 
\hfil EJDE--2002/12}
{EJDE--2002/12\hfil Brian Haile \hfil}
\begin{document}
\title{\vspace{-1in}\parbox{\linewidth}{\footnotesize\noindent
{\sc  Electronic Journal of Differential Equations},
Vol. {\bf 2002}(2002), No. 12, pp. 1--14. \newline
ISSN: 1072-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu
\newline ftp  ejde.math.swt.edu  (login: ftp)}
 \vspace{\bigskipamount} \\
 %
  Analytic solutions of n-th order differential equations at a
  singular point 
 %
\thanks{ {\em Mathematics Subject Classifications:} 30A99, 34A30,  34M35, 46E15.
\hfil\break\indent
{\em Key words:} linear differential equation, regular
 singular point, analytic solution.
\hfil\break\indent
\copyright 2002 Southwest Texas State University. \hfil\break\indent
Submitted July 28, 2001. Published February 4, 2002.} }
\date{}
%
\author{Brian Haile}
\maketitle

\begin{abstract} 
 Necessary and sufficient conditions are be given for the
 existence of analytic solutions of the nonhomogeneous n-th order
 differential equation at a singular point. Let $L$ be a linear
 differential operator with coefficients analytic at zero.
 If $L^*$ denotes the operator conjugate to $L$, then we will show
 that the dimension of the kernel of $L$ is equal to the dimension
 of the kernel of $L^*$.  Certain representation theorems from
 functional analysis will be used to describe the space of linear
 functionals that contain the kernel of $L^*$.  These results will
 be used to derive a form of the Fredholm Alternative that will
 establish a link between the solvability of $Ly = g$ at a singular
 point and the kernel of $L^*$. The relationship between the roots
 of the indicial equation associated with $Ly=0$ and the kernel of
 $L^*$  will allow us to show that the kernel of $L^*$ is spanned
 by a set of polynomials.
\end{abstract}

\newtheorem{theorem}{Theorem}[section]
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\section{Introduction} 

In 1969, Harris, Sibuya and Weinberg \cite{h3} proved a theorem, based
on certain techniques of functional analysis, that contains as
corollaries the existence theorems of O. Perron and F.
Lettenmeyer.  Harris, Sibuya and Weinberg were able to show, under
certain conditions, that there exists a polynomial $f(z)$ such
that the linear differential system
\[z^D\frac{dy}{dz} - A(z)y = f(z),\]
where $A(z)$ is analytic at $z=0$, and $D=diag\{d_1,\dots, d_n\}$
with nonnegative integers $d_i$, has a solution analytic at $z=0$.
Two years later, H.L. Turrittin \cite{t2} posed the following problem:
Given the equation
\[
\frac{dW}{dz} = \sum_{j=0}^{\infty}\,z^{-j}A_j\,W +
\sum_{j=1}^{\infty}\,z^{-j}B_j
\]
where both series converge if $|z|\ge z_0 > 0$, with a formal solution
\[
W(z) = \sum_{j=0}^{\infty}\,z^{-j}C_j,
\]
what are the necessary and sufficient conditions that the formal solution
converges?  At the same time Turrittin speculated that the afore mentioned paper of Harris, Sibuya and Weinberg might lead to an answer to this question.

L.J. Grimm and L.M. Hall answered the question posed by Turrittin in \cite{g2}.  Although their initial work was inspired by the Harris, Sibuya and Weinberg paper, Grimm and Hall actually employed the theory of normally solvable and Noetherian operators, much as Korobe\u inik did, to derive an analogue of the Fredholm alternative for certain systems of functional differential operators.  Then they used A.E. Taylor's representation of Banach spaces of analytic functions \cite{t1} to obtain conditions for the solvability of certain nonhomogeneous
equations they had studied previously in \cite{g3}.

The primary difficulty encountered when applying the results of \cite{g2} comes when attempting to describe the cokernel (see \cite{g2}, \cite{h1}, \cite{h2}) of the operator.

In this paper we will completely describe the cokernel of the
operator $L$, defined by
\begin{equation} \label{eq1}
Ly(z) = z^ny^{(n)}(z)+z^{n-1}a_1(z)y^{(n-1)}(z)+\cdots+a_n(z)y(z)
\end{equation}
where $a_1(z),\dots, a_n(z)$ are analytic at the point $z=0$.

We will produce solvability conditions for the nonhomogeneous
Bessel equation, that are independent of the order, but match
those of \cite{h2} if it is an equation of integer order.

First, we will define a collection of Banach spaces, each
containing functions analytic at the origin, and such that $L$ is
a continuous linear operator on this collection. We will show that
the dimension of the kernel of $L$ is equal to the dimension of
the cokernel of $L$. Then we will use Taylor's representation of
Banach spaces of analytic functions \cite{t1} to essentially set up a
relationship between the roots of the indicial equation (from the
Frobenius method) and the necessary form of the nonhomogeneous
term $g$ that allows us to find a solution to $Ly=g$ analytic at
the origin.

\section{Definitions and Preliminaries}

Let $B_1$ and $B_2$ be Banach spaces and let $T: B_1 \to B_2$ be a
continuous linear operator with domain $B_1$.  Denote the
conjugate of $T$ by $T^\ast $.
\paragraph{Definition}
 The operator $T$ is normally solvable if $T(B_1)$ is  closed in $B_2$.
\smallskip 

The following lemma, due to Korobe\u inik \cite{j1}, gives another
characterization of normal solvability.  The annihilator of the
set $W$ will be denoted by $W^{\,\perp}$.
\begin{lemma} \label{Lm2.1}
Let $B_1$ and $B_2$ be Banach spaces, and let $T:B_1 \to B_2$ be a
continuous linear operator.  Then the following two properties are
equivalent. \begin{enumerate}

\item[(a)]  $T$ is normally solvable.

\item[(b)]  The equation $Ty = u$, $u \in B_2$, is solvable in $B_1$
if and only if   $u \in (\ker T^*)^\perp$.
\end{enumerate}
\end{lemma}

\paragraph{Definition}  % Defn2.2
The d-characteristic of  $T$ is the ordered pair
$(\alpha(T),\beta(T))$, where $\alpha(T) = \dim(\ker T)$ and
$\beta(T) = \dim(B_2/T(B_1)$.  $\beta(T)$ is called the defect
number of $T$. 

\paragraph{Definition}   % Defn2.3
The index of the operator $T$, denoted by $ind(T)$, is the number
 $\beta(T) - \alpha(T)$. 

\paragraph{Definition}  % Defn2.4
The operator $T$ is called a Noetherian operator if $T$ is
normally  solvable and if both $\alpha(T)$ and $\beta(T)$ are
finite. \smallskip 

\paragraph{Remark} 
If $\beta(T) < \infty$, then $\beta(T) = \dim(\mathop{\rm coker}
T) = \dim(\ker T^*)$.
\smallskip

The following theorem is due to I.C. Gohberg and M.G. Kre\u in \cite{g1}.

\begin{theorem} \label{Thm2.1}
Let $T: B_1 \to B_2$ be a continuous Noetherian operator, and let
$T_1: B_1 \to B_2$ be a compact operator.  Then $T_2 = T + T_1$ is
a Noetherian  operator from $B_1$ into $B_2$ with $\mathop{\rm
ind} (T_2) = \mathop{\rm ind}(T)$.
\end{theorem}


 For an arbitrary Noetherian operator the following theorem holds.

\begin{theorem}[Fredholm Alternative] \label{Thm2.2}
  If $B_1$ and $B_2$ are Banach spaces and $T:B_1\to B_2$ is a Noetherian
  operator with
  conjugate $T^*$, then \begin{enumerate}
\item[(i)] The equation $T\,y = u$ has a solution (in $B_1$) if and only if
            $u\in (\ker T^*)^\perp$.
\item[(ii)] The equation $T^*\,f = g$ has a solution (in $B_2^*$) if and only if
            $g\in (\ker T^{**})^\perp$.
\end{enumerate}
\end{theorem}

The proof of this theorem can be found in  Korobe\u inik \cite[Lemma 2.1]{j1}.

\section{Properties of the Operator}

Let $G = \{z: |z|<1\}$ and define $A_p$ to be the Banach space of
functions $\upsilon(z)$ analytic in $G$ and $p$ times continuously
differentiable on $\overline{G}$, with norm
\[\|\upsilon(z)\|_p = \{\max |\upsilon^{(i)}(z)|,\; 0 \leq i \leq p,\;
|z| = 1\}.\]

Consider the operator $L:A_n \to A_0$, defined in (\ref{eq1}), where the
$a_i$ are now in $A_0$. In order to apply Theorem \ref{Thm2.1} to the
operator $L$, we need the following two results.  A proof for each
of these two lemmas can be easily obtained by following the
techniques used by Korobe\u inik \cite{j1}.

\begin{lemma} \label{Lem3.1}
The operator $l_0:A_n \to A_0$ defined by $l_0y(z) \equiv
z^ny^{(n)}(z)$ is Noetherian with $\alpha(l_0) = \beta(l_0)$.
\end{lemma}

\begin{lemma} \label{Lm3.2}
The operator $l_i:A_n \to A_0$, $1 \leq i \leq n$, defined by \\
$l_iy(z) = z^{n-i}a_i(z)y^{(n-i)}(z)$, $a_i \in A_0$, is compact.
\end{lemma}


Now we are able to apply Theorem \ref{Thm2.1} to the operator $L$ to obtain the
following theorem.

\begin{theorem} \label{Thm3.1}
$L$ is a Noetherian operator with $\alpha(L) = \beta(L)$.
\end{theorem}

\section{Description of the Banach Spaces}

Let $\tilde{A}$ be the space of all functions that are analytic in
$G$. If $f \in \tilde{A}$, $f(z)$ can be expanded in a power
series in $z$,
$$f(z) = \sum_{k=0}^{\infty} f_kz^k , \quad
\mbox{convergent in }  G.$$

\paragraph{Definition} % Defn4.1
If $f$ and $g$ are elements of $\tilde{A}$ such that
$$f(z) = \sum_{k=0}^{\infty} f_kz^k \quad \mbox{and}\quad
 g(z) = \sum_{k=0}^{\infty} g_kz^k\,,$$
we define the Hadamard product of $f$ and $g$ by
$$B(f,g;z) = \sum_{k=0}^{\infty} f_kg_kz^k \,,\quad  z \in G.$$


The series $B(f,g;z)$, thus defined, is an element of $\tilde{A}$
and defines a continuous linear functional of $f$ over $A_0$.

\paragraph{Definition}  % Defn4.2
Define $A_0^0$ as the class of all $F \in \tilde{A}$ such that
$$\lim_{r \to 1^-}B(u,F;r)$$
exists for each $u \in A_0$. 

\begin{theorem} \label{Thm4.1}
$A_0^0$ is a Banach space if the norm is defined by
$$\|F\| = \lim_{r \to 1^-} \sup_{\|u\|_0=1} |B(u,F;r)|,\quad u \in A_0.$$
\end{theorem}

Let $A_0^*$ denote the space of all linear functionals defined on
$A_0$.  Recall that, as $u$ varies over $A_0$, $B(u,F;r)$ defines
a linear functional with norm $\sup_{\|u\|_0=1} |B(u,F;r)|,\;\; u
\in A_0$.  Then, if $F \in A_0^0$,
\begin{equation} \label{eq2}
\gamma(u) = \lim_{r \to 1} B(u,F;r), \;\; u \in A_0
\end{equation}
defines an element $\gamma$ of $A_0^*$.

Define the mapping $\Lambda: A_0^0 \to A_0^*$ by $\Lambda(F) =
\gamma$. Let $\phi \in A_0^*$ and define the function
$$H(z) = \sum_{k=0}^{\infty} \phi(z^k)z^k,\quad  z \in G.$$

\begin{theorem} \label{Thm4.2}
$H(z) \in A_0^0$. \end{theorem}

Now, we may also define the mapping $\Gamma: A_0^* \to A_0^0$ by
$\Gamma(\phi) = H$.

\begin{theorem} \label{Thm4.3}
The mapping $\Lambda$ is an isometric isomorphism and
$\Lambda^{-1} = \Gamma$. \end{theorem}

Therefore, as a result of theorems \ref{Thm4.2} and \ref{Thm4.3}, each linear
functional in $A_0^*$ can be uniquely represented (or determined)
by an element in $A_0^0$.  We restate this result in the following
theorem.


\begin{theorem} \label{Thm4.4}
Every linear functional $\gamma \in A_0^*$ is representable in the form
\begin{equation} \label{eq3}
\gamma(u) = \lim_{r \to 1}\frac{1}{2\pi}\int_{0}^{2\pi}u(\rho e^{i\theta})
    F \big(\frac{r}{\rho}e^{-i\theta} \big)d \theta,\quad u \in A_0,
\end{equation}
where $r < \rho < 1$ and $F \in A_0^0$.  $F$ uniquely determines
and is uniquely determined by $\gamma$, and $\|\gamma\| = \|F\|$.
\end{theorem}

\section{Description of the Cokernel}

Using the results of Theorem \ref{Thm4.4}, we can apply the Fredholm
Alternative to obtain the following theorem which gives necessary
and sufficient conditions for the solvability of $Ly = g$, $g \in
A_0$.

\begin{theorem} \label{Thm5.1}
For $g \in A_0$, the equation $Ly = g$ has a solution in $A_n$ if and only if
\begin{equation} \label{eq4}
\lim_{r \to 1} B(g,f;r) = 0
\end{equation}
for all $f \in A_0^0$ such that
\begin{equation} \label{eq5}
\lim_{r \to 1} B(Ly,f;r) = 0
\end{equation}
for all $y \in A_n$. \end{theorem}

\paragraph{Proof.}  Define the space ${\cal F}(L)$ by ${\cal F}(L) =
\Gamma(\ker(L^*))$.  Hence ${\cal F}(L)$ is a subspace of $A_0^0$
and can be represented by
\begin{equation}     \label{eq6}
{\cal F}(L) = \{f \in A_0^0:  \mbox{$f$ satisfies (\ref{eq5}) for all }y
\in A_n \}.
\end{equation}
Now, from Theorem \ref{Thm2.2}, the equation $Ly = g$ has a solution in
$A_n$ if and only if $u$ is in $ker(L^*)^{\perp}$,  and $u$ is in
$ker(L^*)^{\perp}$ if and only if $\gamma(u) = 0$ for all $\gamma
\in ker(L^*)$. But by Theorem \ref{Thm4.4} this means
$$\gamma(u) = \lim_{r \to 1} B(g,f;r) = 0$$
for every $f \in \Gamma(\ker(L^*)) = {\cal F}(L)$.
\hfill$\diamondsuit$

    Equation (\ref{eq5}) characterizes the cokernel of $L$ $(\ker(L^*))$ and 
equation (\ref{eq4})
characterizes the annihilator of the cokernel of $L$
$(\ker(L^*)^{\perp})$.
 Next, we will use theorems \ref{Thm3.1} and \ref{Thm5.1} to 
describe completely the structure of
the cokernel of $L$.  We will do this by developing a rather
intriguing relationship between the coefficients of a Frobenius
series solution for $Ly = 0$ and the coefficients of a series for
any member of $A_0^0$ that satisfies (\ref{eq5}).

%-----  Definition 5.1  -----
\paragraph{Definition}
The ``factorial function'' $r^{(k)}$ is defined as follows,
according to the value of $k$: \begin{enumerate}

\item[(a)] if $k=1,2,3,\dots$, then $r^{(k)}=r(r-1)(r-2) \cdots
(r-k+1)$,
\item[(b)] if $k=0$, then $r^{(0)}=1$,
\item[(c)] if $k=-1,-2,-3,\dots$, then
$r^{(k)}=\frac{1}{(r+1)(r+2)\cdots (r-k)}$,
\item[(d)] if $k$ is not an integer, then
$r^{(k)} = \frac{\Gamma(r+1)}{\Gamma(r-k+1)}$.
\end{enumerate}\smallskip 


    If we seek a Frobenius series solution for $Ly = 0$ of the form \newline
$w(z) = \sum_{k=0}^{\infty}c_kz^{k+r}$, the indicial equation will
be
$$F(r) = r^{(n)}+r^{(n-1)}a_{1_0}+ \cdots
                 +r^{(2)}a_{(n-2)_0}+r^{(1)}a_{(n-1)_0}+a_{n_0} = 0.$$

The following theorem is an immediate consequence of theorem \ref{Thm3.1} 
and \ref{Thm5.1}.


\begin{theorem} \label{Thm5.2}
If the equation $F(r) = 0$ does not have a nonnegative integer
root, then the equation $Ly = g$ has a solution in $A_n$ for any
$g \in A_0$. \end{theorem}

\paragraph{Proof.}  We know that $dim(\ker(L^*)) = 0$ from 
Theorem \ref{Thm3.1}.
So $f \equiv 0$ is the
only solution to  (\ref{eq5}) and (\ref{eq4}) is satisfied for any $g \in A_0$. Therefore, by 
Theorem \ref{Thm5.1}, equation $Ly = g$ has a solution in $A_n$ for any\\
$g \in A_0$.  \hfill $\diamondsuit$ \smallskip

Now assume that the indicial equation, $F(r) = 0$, has at least
one nonnegative integer root.  We will show that the cokernel of
$L$ is always spanned by a set of polynomials and therefore the
existence of a solution to $Ly = g$ in $A_n$ depends only on a
finite number of the coefficients in the series expansion of
$g(z)$.
    First, we need to rewrite equation (\ref{eq5}). Let
$$f(z)= \sum_{k=0}^{\infty}f_kz^k \quad\mbox{and}\quad
 a_i(z)= \sum_{k=0}^{\infty}a_{i_k}z^k, \quad  i=1,\dots,n.$$
Then another form of (\ref{eq5}) is:
\begin{equation} \label{eq7}
\begin{array}{c}
\vspace{.15cm}
F(0)f_0 + \sum_{k=1}^\infty a_{n_k}\,f_k = 0 \\
\vspace{.15cm}
F(1)f_1 + \sum_{k=1}^\infty \left[a_{(n-1)_k}+a_{n_k}\right]f_{k+1} = 0\\
\vspace{.15cm}
F(2)f_2 + \sum_{k=1}^\infty \left[2a_{(n-2)_k}+2a_{(n-1)_k}+a_{n_k}\right]f_{k+2} = 0\\
F(3)f_3 + \sum_{k=1}^\infty
                 \left[6a_{(n-3)_k}+6a_{(n-2)_k}+3a_{(n-1)_k}+a_{n_k}\right]f_{k+3} = 0\\
\vdots \\
F(n)f_n + \sum_{k=1}^\infty
 \left[n^{(n-1)}a_{1_k}+n^{(n-2)}a_{2_k}+\cdots +na_{(n-1)_k}+a_{n_k}\right]f_{k+n}=0\\
\vdots \\
F(r)f_r + \sum_{k=1}^\infty
 \left[r^{(n-1)}a_{1_k}+r^{(n-2)}a_{2_k}+\cdots +ra_{(n-1)_k}+a_{n_k}\right]f_{k+r}=0\\
\vdots \end{array}
\end{equation}

\begin{theorem} \label{Thm5.3}
If the equation $F(r) = 0$ has exactly one nonnegative integer
root, $r$, then the cokernel of $L$ is spanned by a polynomial of
degree $r$. \end{theorem}

\paragraph{Proof.} Since there is only one nonnegative integer root,
$r$, we may reduce (\ref{eq7}) to
\begin{equation} \label{eq8}
\begin{array}{c}
\vspace{.15cm}
F(0)f_0 + \sum_{k=1}^r a_{n_k}\,f_k = 0 \\
\vspace{.15cm}
F(1)f_1 + \sum_{k=1}^{r-1} \left[a_{(n-1)_k}+a_{n_k}\right]f_{k+1} = 0\\
\vspace{.15cm}
F(2)f_2 + \sum_{k=1}^{r-2} \left[2a_{(n-2)_k}+2a_{(n-1)_k}+a_{n_k}\right]f_{k+2} = 0\\
F(3)f_3 + \sum_{k=1}^{r-3}
                 \left[6a_{(n-3)_k}+6a_{(n-2)_k}+3a_{(n-1)_k}+a_{n_k}\right]f_{k+3} = 0\\
\vdots \\
F(r-1)f_{r-1} +
 \left[(r-1)^{(n-1)}a_{1_1} +
                                \cdots + (r-1)^{(1)}a_{(n-1)_1}+a_{n_1}\right]f_r = 0\\
F(r)f_r = 0
\end{array}
\end{equation}
by setting $f_k = 0$ for $k > r$. Back substitution for $f_k,\,\,
k < r$, yields a polynomial of degree $r$ in the cokernel of $L$.
We also know that $dim(\ker(L)) = 1$, which implies, from 
Theorem \ref{Thm3.1}, that $\dim(\ker(L^*)) = 1$. 
Therefore the cokernel of $L$ is
spanned by a polynomial of degree $r$. \hfill
$\diamondsuit$\smallskip

    We now assume that the indicial equation for $Ly = 0$ has $q > 1$ nonnegative
integer roots, $r_1,\, \dots,\, r_q$. Assume $r_1 > r_2 >  \cdots
> r_q$ and let $N = r_1 - r_q$.  Under these assumptions we are
guaranteed, following the standard Frobenius series solution
technique, at least one solution in $A_n$.  If there is to be more
than one linearly independent solution in $A_n$, it can be
determined by using the smaller root, $r_q$, of the indicial
equation and calculating the first $N + 1$ coefficients of the
Frobenius series.  If $c_0,\,c_1,\dots,c_N$ denote these
coefficients and $H=(h_{i,j})$ is the upper-triangular matrix
where
$$h_{i,j}= \left\{ \begin{array}{ll}
 0, & \mbox{if $i>j$}\\
 F(r_1-i+1), & \mbox{if $i=j$}\\
 (r_1-j+1)^{(n-1)}a_{1_{j-i}} + \cdots \\
 +(r_1-j+1)^{(1)}a_{(n-1)_{j-i}}+a_{n_{j-i}}, & \mbox{if $i<j$}
 \end{array} \right. $$
then  the system of equations, $H\vec{c} = \vec{0}$, 
\begin{equation} \label{eq9}
%\hspace*{.2cm}
\left[\begin{array}{cccccc}
\hspace{-.2cm}F(r_1)&h_{1,2} &h_{1,3} &\cdots & h_{1,N}  & h_{1,N+1}\hspace{-.2cm}\\
\hspace{-.2cm}0     &F(r_1-1)&h_{2,3} &\cdots & h_{2,N}  & h_{2,N+1}\hspace{-.2cm}\\
\hspace{-.2cm}0     &   0    &F(r_1-2)&\cdots & h_{3,N}  & h_{3,N+1}\hspace{-.2cm}\\
\hspace{-.2cm}\vdots&\cdots  &  0     &\ddots & \cdots   &  \vdots  \hspace{-.2cm}\\
\hspace{-.2cm}0     &\cdots  &\vdots  &\ddots & F(r_q+1) & h_{N,N+1}\hspace{-.2cm}\\
\hspace{-.2cm}0     &   0    &  0     &\cdots &  0       & F(r_q)   \hspace{-.2cm}
  \end{array}\right] \hspace{-.2cm}
  \left[\begin{array}{c}
\hspace{-.2cm}c_N\hspace{-.2cm} \\\hspace{-.2cm}c_{N-1}\hspace{-.2cm}\\\hspace{-.2cm}
 c_{N-2}\hspace{-.2cm} \\\hspace{-.2cm} \vdots \hspace{-.2cm}\\\hspace{-.2cm} c_1
\hspace{-.2cm} \\\hspace{-.2cm} c_0 \hspace{-.2cm}
  \end{array}\right]
= \left[\begin{array}{c}
 \hspace{-.2cm}0\hspace{-.2cm} \\\hspace{-.2cm} 0\hspace{-.2cm} \\
\hspace{-.2cm} 0\hspace{-.2cm} \\\hspace{-.2cm} \vdots \hspace{-.2cm} \\
\hspace{-.2cm} 0\hspace{-.2cm} \\\hspace{-.2cm} 0 \hspace{-.2cm}
  \end{array}\right]
\end{equation}
determines these coefficients.
In other words, the number of linearly independent solutions to  (\ref{eq9}) 
coincides with the number of linearly independent solutions in $A_n$ of 
$Ly= 0$.

\paragraph{Definition} 
Let
$$B = \left[\begin{array}{cccc}
                b_{1,1} & b_{1,2} & \cdots & b_{1,n} \\
                b_{2,1} & b_{2,2} & \cdots & b_{2,n} \\
                \vdots & \vdots & \ddots & \vdots \\
                b_{n,1} & b_{n,2} & \cdots & b_{n,n}
            \end{array} \right],$$
then define the backward transpose of $B$ as
$$B^t = \left[\begin{array}{cccc}
                b_{n,n} & \cdots & b_{2,n} & b_{1,n} \\
                \vdots & \ddots & \vdots & \vdots \\
                b_{n,2} & \cdots & b_{2,2} & b_{1,2} \\
                b_{n,1} & \cdots & b_{2,1} & b_{1,1}
             \end{array} \right].$$


    Return to the infinite set of equations (\ref{eq7}) which determine the cokernel of $L$. We want to consider the system of equations
\begin{equation} \label{eq10}
%\hspace*{.4cm}
\left[\begin{array}{cccccc}
\hspace{-.2cm}F(r_q)&h_{N,N+1}&h_{N-1,N+1}&\cdots &h_{2,N+1} &h_{1,N+1}\hspace{-.2cm}\\
\hspace{-.2cm}0     &F(r_q+1) &h_{N-1,N}  &\cdots &h_{2,N}   &h_{1,N}  \hspace{-.2cm}\\
\hspace{-.2cm}0     & 0       &F(r_q+2)   &\cdots &h_{2,N-1} &h_{1,N-1}\hspace{-.2cm}\\
\hspace{-.2cm}\vdots&\cdots   &  0        &\ddots &\cdots    & \vdots  \hspace{-.2cm}\\
\hspace{-.2cm}0     &\cdots   &\vdots     &\ddots &F(r_1-1)  &h_{1,2}  \hspace{-.2cm}\\
\hspace{-.2cm}0     &   0     &  0        &\cdots & 0        &F(r_1)   \hspace{-.2cm}
   \end{array}\right] \hspace{-.2cm}
  \left[\begin{array}{c}
  \hspace{-.2cm}f_{r_q}\hspace{-.2cm} \\\hspace{-.2cm} f_{r_q+1}\hspace{-.2cm} \\
  \hspace{-.2cm} f_{r_q+2}\hspace{-.2cm} \\\hspace{-.2cm} \vdots\hspace{-.2cm} \\
  \hspace{-.2cm} f_{r_1-1}\hspace{-.2cm} \\\hspace{-.2cm} f_{r_1}\hspace{-.2cm}
  \end{array}\right]
= \left[\begin{array}{c}
  \hspace{-.2cm}0\hspace{-.2cm} \\\hspace{-.2cm} 0\hspace{-.2cm} \\
  \hspace{-.2cm} 0\hspace{-.2cm} \\\hspace{-.2cm} \vdots\hspace{-.2cm} \\
  \hspace{-.2cm} 0\hspace{-.2cm} \\\hspace{-.2cm} 0 \hspace{-.2cm}
  \end{array}\right]
\end{equation}
given specifically by the $r_qth$ through the $r_1th$ equations of (\ref{eq7}).
The coefficient matrix for this system of equations will be denoted by $H^t$ since it
is the backward transpose of the matrix $H$ in (\ref{eq9}).


  If we set $f_k = 0$, $k > r_1$, then the number of linearly independent
solutions to (\ref{eq10}) coincides with the number of linearly independent
polynomials in the cokernel of $L$.  The following lemma is the basis of a very
lucrative relationship between the number of linearly independent solutions in
$A_n$ of $Ly = 0$ and the number of linearly independent polynomials in the
cokernel of $L$.

\begin{lemma} \label{Lma5.1}
Let $B$ be an $n \times n$ matrix and $B^t$ be its backward
transpose, then \\ $B^t \sim B$. \end{lemma}

\paragraph{Proof.} Denote the $n \times n$ backward identity by
P, i.e.,
$$P = \left[\begin{array}{ccccc}
        0      & \cdots &   0   &   0   &   1    \\
        0      & \cdots &   0   &   1   &   0    \\
        \vdots &        &\cdots &       & \vdots \\
        0      &   1    &   0   &\cdots &   0    \\
        1      &   0    &   0   &\cdots &   0
      \end{array}\right].$$
Then $B^t = PB^TP$ where $B^T$ is the usual transpose of $B$.  It
is known that $B^T \sim B$ which implies that there exists a
nonsingular matrix $R$ such that $B^T = RBR^{-1}$.  So, if we let
$Q = PR$ then $Q$ is a nonsingular matrix such that $B^t =
QBQ^{-1}$. \hfill $\diamondsuit$\smallskip

Now, from Lemma \ref{Lma5.1}, we know that $H \sim H^t$.  In other words,
there exists a nonsingular matrix, $Q$, such that $QH = H^tQ$.
Therefore, equations (\ref{eq9}) and (\ref{eq10}) will have the same number of
linearly independent solutions directly related to each other by
the matrix $Q$. We state this result in the following lemma.


\begin{lemma} \label{Lma5.2}
If $Q$ is a nonsingular matrix such that $QH = H^tQ$ and 
 $[c_N  \cdots  c_0]^T$ is
a solution of (\ref{eq9}) then $Q[c_N \cdots c_0]^T$ is a solution of
 (\ref{eq10}).
\end{lemma}

Together, lemmas \ref{Lma5.1} and \ref{Lma5.2} describe the unique relationship
between the kernel and cokernel of the operator $L$. Thus, we can
completely describe the structure of the cokernel of $L$ when
$F(r) = 0$ has two or more nonnegative integer roots.  These
results are presented in the following theorem.


\begin{theorem} \label{Thm5.4}
Assume the indicial equation, $F(r) = 0$, has $q$ $(q \leq n)$
nonnegative integer roots,
$r_1,\, \dots,\,r_q$, with $r_1 > r_2 > \, \cdots > r_q$. Let $N_i = r_i - r_{i+1}$ and \\
$\eta(p) = \sum_{i=1}^{p} N_i$, $p \in \{1, \dots, q-1\}$. Then,
if $Ly = 0$ has $m + 1$ $(m+1 \leq q)$ linearly independent
solutions in $A_n$, there exist integers $p_1 < p_2 < \cdots < p_m
\leq q-1$ such that the cokernel of $L$ is spanned by the
functions $f_0(z)$ $\cup$ $\{f_j(z)\}_{j=1}^{m}$ where $f_0(z)$ is
a polynomial of degree $r_q$ and $f_j(z)$ is a polynomial of
degree $r_q + \eta(p_j)$.
\end{theorem}

\paragraph{Proof.} Following the Frobenius method for solving $Ly =
0$ we find a solution in $A_n$ associated with the largest root,
$r_1$.  Then we check for a solution in $A_n$ associated with each
of the smaller roots.  With the hypotheses above we will get
solutions associated with the following $m + 1$ roots,
$$\{r_1, r_1 - \eta(p_1), r_1 - \eta(p_2), \dots, r_1 - \eta(p_m) \},$$
where $p_1, p_2, \dots, p_m$ are integers such that $1 \leq p_1 <
p_2 < \cdots < p_m \leq q-1$, and these will be linearly
independent. Thus (\ref{eq9}) will have $m + 1$ linearly independent
solutions, where each of the coefficients
$$\{c_N, c_{N-\eta(p_1)}, c_{N-\eta(p_2)}, \dots, c_{N-\eta(p_m)} \}$$
are arbitrary. From lemmas \ref{Lma5.1} and \ref{Lma5.2}, 
we will get $m+1$ linearly  independent
solutions to (\ref{eq10}), where each of the coefficients
$$\{f_{r_q}, f_{r_q+\eta(p_1)}, f_{r_q+\eta(p_2)}, \dots, f_{r_q+\eta(p_m)} \}$$
are arbitrary.

Therefore, each of the polynomials
\begin{equation} \label{eq11}
\begin{array}{c}
f_0(z) = f_{0_0} + f_{0_1}z + \cdots + f_{0_{r_q}}z^{r_q} \vspace{.1cm} \\
f_1(z) = f_{1_0} + f_{1_1}z + \cdots + f_{1_{r_q+\eta(p_1)}}z^{r_q+\eta(p_1)}\vspace{.1cm}\\
f_2(z) = f_{2_0} + f_{2_1}z + \cdots + f_{2_{r_q+\eta(p_2)}}z^{r_q+\eta(p_2)} \\
\vdots \\
f_m(z) = f_{m_0} + f_{m_1}z + \cdots + f_{m_{r_q+\eta(p_m)}}z^{r_q+\eta(p_m)}
  \end{array}
\end{equation}
is an element of $\ker(L^*)$.  But, from Theorem \ref{Thm3.1} we know that
$$\dim(\ker  L^*) = \dim(\ker  L) = m + 1.$$
Hence, the cokernel of $L$ is spanned by the polynomials in (\ref{eq11}).
\hfill $\diamondsuit$ \smallskip

Theorems \ref{Thm5.1}, \ref{Thm5.2}, \ref{Thm5.3}, and \ref{Thm5.4}
 describe  completely the cokernel of
the operator $L$, which is either zero dimensional or is spanned
by polynomials.  Therefore, if the nonhomogeneous term in $Ly = g$
is represented by the series
\begin{equation} \label{eq12}
g(z) = \sum_{k=0}^{\infty} g_kz^k,
\end{equation}
the solvability in $A_n$ of $Ly = g$ is determined by a finite number of
the coefficients in (\ref{eq12}).

\section{Examples}

In this section we will illustrate some of the preceding results.
Consider the nonhomogeneous Bessel equation of order $\nu$.
%----- Example 6.1 -----

\begin{example} \rm
 Let $L_1:A_2 \to A_0$ be defined by
$$L_1\,y(z) = z^2\,y'' (z) + zy' (z) + (z^2-\nu^2)y(z).$$
\end{example}

If we use the Frobenius method to solve $L_1y = 0$ we obtain the
indicial function $F(r) = (r - \nu)(r + \nu)$, so $\nu$ and $-\nu$
are the roots of the indicial equation. Without loss of generality
assume that $\nu \geq 0$. If $\nu$ is not an integer, $F(r) = 0$
will not have a nonnegative integer root. Thus, by Theorem \ref{Thm5.2},
$Ly = g$ will have a solution in $A_2$ for any function $g \in
A_0$. If $\nu$ is an integer, then $F(r) = 0$ has exactly one
nonnegative integer root, $\nu$. Thus, by Theorem \ref{Thm5.3}, the
cokernel of $L_1$ is spanned by a polynomial of degree $\nu$.
Following the proof of Theorem \ref{Thm5.3} we are able to produce this
polynomial. First, we derive the finite system of equations
$$\begin{array}{c}
F(0)f_0 + \sum_{k=1}^{\nu} a_{n_k}\,f_k = 0 \vspace{.1cm} \\ \vspace{.1cm}
F(1)f_1 + \sum_{k=1}^{\nu -1} \left[a_{(n-1)_k}+a_{n_k}\right]f_{k+1} = 0\\\vspace{.1cm}
F(2)f_2 + \sum_{k=1}^{\nu -2} \left[2a_{(n-2)_k}+2a_{(n-1)_k}+a_{n_k}\right]f_{k+2} = 0\\
F(3)f_3 + \sum_{k=1}^{\nu -3}
                 \left[6a_{(n-3)_k}+6a_{(n-2)_k}+3a_{(n-1)_k}+a_{n_k}\right]f_{k+3} = 0\\
\vdots \\
F(\nu -1)f_{\nu -1} +
 \left[(\nu -1)^{(n-1)}a_{1_1} +
                       \cdots + (\nu -1)^{(1)}a_{(n-1)_1}+a_{n_1}\right]f_{\nu} = 0\\
F(\nu)f_{\nu} = 0,
\end{array}  $$
similar to those in (\ref{eq8}); then, back substitution yields the polynomial
$$f(z) = z^{\nu} + \sum_{m=1}^{\lfloor \frac{\nu}{2} \rfloor}
   \frac{(\nu - m -1)!}{2^{2m}\, m!(\nu - 1)!} z^{\nu -2m},$$
which spans the cokernel of $L_1$. So, by Theorem \ref{Thm5.1}, $L_1y = g$
will have a solution in $A_2$ if and only if the coefficients in
the series expansion of $g(z) = \sum_{k=0}^\infty g_kz^k$ satisfy
$$g_{\nu} + \sum_{m=1}^{\lfloor \frac{\nu}{2} \rfloor}
   \frac{(\nu - m -1)!}{2^{2m}\, m!(\nu - 1)!} g_{\nu -2m} = 0. $$

%----- Remark 6.1 -----

\paragraph{Remark}
This example was given previously by Hall \cite{h2}. However, by
applying the techniques developed in this article, we have
obtained solvability conditions for $L_1y=g$, the nonhomogeneous
Bessel equation of order $\nu$, independent of the value of $\nu$.
We obtained this condition, which matches that of \cite{h2} if $\nu$ is
an integer, without converting the equation to a system.
\smallskip

%----- Example 6.2 -----

\begin{example} \rm
 Let $L_2:A_2 \to A_0$ be defined by
$$L_2\,y(z) = z^2\,y''(z) - 2z(z-2)y'(z) + 2(2-3z)y(z).$$
 \end{example}

Here, $F(r) = 0$ has roots $r_1 = 4$, $r_2 = 1$ and $N = r_1 - r_2
= 3$. We will use Theorem \ref{Thm5.4} to describe the cokernel of the
operator $L_2$. First, we obtain the coefficient matrices of (\ref{eq9})
and (\ref{eq10}).
$$H = \left[\begin{array}{cccc}
                    0 & 0 & 0 & 0 \\
                    0 & -2 & -2 & 0 \\
                    0 & 0 & -2 & -4 \\
                    0 & 0 & 0 & 0
             \end{array}\right] \quad and \quad
H^t = \left[\begin{array}{cccc}
                      0 & -4 & 0 & 0 \\
                      0 & -2 & -2 & 0 \\
                      0 & 0 & -2 & 0 \\
                      0 & 0 & 0 & 0
             \end{array}\right].$$

Then, from Lemma \ref{Lma5.1}, we know that $H \sim H^t$ and so there exists a nonsingular matrix
$$Q = \left[\begin{array}{cccc}
                    1 & -2 & 2 & 8 \\
                    0 & 1 & 0 & -2 \\
                    0 & 0 & 1 & 2 \\
                    0 & 0 & 0 & 1
             \end{array}\right]$$
such that $QH = H^tQ$.

Now, $\left[\begin{array}{cccc} 1 & 2 & -2 & 1 \end{array}\right]^T$ is a solution to
$H\vec(c) = \vec{0}$ which implies, by Lemma \ref{Lma5.2}, that
$Q\left[\begin{array}{cccc} 1 & 2 & -2 & 1 \end{array}\right]^T =
\left[\begin{array}{cccc} 1 & 0 & 0 & 1 \end{array}\right]^T$
is a solution to \\
$H^t\left[\begin{array}{cccc} f_1 & f_2 & f_3 & f_4
\end{array}\right]^T = \vec{0}$. Thus, by setting $f_k = 0$, $k >
4$, in (\ref{eq7}) we can use back substitution to get $\displaystyle{f_0
= {3 \over 2}f_1}$. So, we
get two linearly independent polynomials, $f_1(z) = z^4$  and \\
$f_2(z) = z + {3 \over 2}$ that span the cokernel of $L_2$.

Thus, by Theorem \ref{Thm5.1}, $L_2y = g$ will have a solution in $A_2$  if
and only if the coefficients in the series expansion of $g(z)$
satisfy both $g_4 = 0$ and $g_1 = -{3 \over 2}g_0$.
%----- Remark 6.2 -----
\paragraph{Remark}
Back substitution is necessary to find the $f_k$, $k < r_q=1$,
since the equation $H^t\left[\begin{array}{cccc} f_1 & f_2 & f_3 &
f_4 \end{array}\right]^T = \vec{0}$ is derived from the first
through the fourth equations of (\ref{eq7}).
\smallskip

%----- Example 6.3 -----

\begin{example} \rm
Let $L_3:A_4 \to A_0$ be defined by
$$L_3\,y(z) = z^4\,y^{(4)}(z) + z^3a_1(z)y^{(3)}(z)
               + z^2a_2(z)y''(z)
                   + za_3(z)y' + a_4(z)y(z),$$
where $a_1(z) = z^4-4$, $a_2(z) = 12z^2-\frac{1}{2}z+6$, $a_3(z) =
-3z^3+13z^2-z-1$, and $a_4(z) = 6z^4+z^2-11z+1$.
\end{example}
In this case, $F(r) = 0$ has roots $r_1=5$, $r_2=4$,
$r_3=1$, and $r_4=0$. So, by Theorem \ref{Thm5.4}, we know that the
cokernel of $L_3$ is spanned by the function $f_0(z) = 1$ and,
possibly as many as three more polynomials, $f_j(z)$, of degree
$\eta(p_j)$, $1 \leq p_j \leq 3$. To apply Theorem \ref{Thm5.4}, i.e.,
determine the polynomials in the cokernel of $L_3$, it is enough
to find the matrix $H^t$ of (\ref{eq10}) and solve
$H^t\left[\begin{array}{cccccc} f_0&f_1&f_2&f_3&f_4&f_5
\end{array}\right]^T = \vec{0}$.
$$H^t = \left[\begin{array}{cccccc}
                        0 & -11 & 1 & 0 & 6 & 0 \\
                        0 & 0 & -12 & 14 & -3 & 6 \\
                        0 & 0 & 12 & -14 & 3 & -6 \\
                        0 & 0 & 0 & 12 & -17 & 112 \\
                        0 & 0 & 0 & 0 & 0 & -21 \\
                        0 & 0 & 0 & 0 & 0 & 0
            \end{array}\right]$$
Thus, $\left[\begin{array}{cccccc} f_0&f_1&f_2&f_3&f_4&f_5 \end{array}\right]^T =
       \left[\begin{array}{cccccc} \alpha&\frac{533}{11}\beta&101\beta&102\beta&72\beta&0 \end{array}\right]^T$
is a solution to $H^t\left[\begin{array}{cccccc}
f_0&f_1&f_2&f_3&f_4&f_5 \end{array}\right]^T = \vec{0}$, where
$\alpha$ and $\beta$ are arbitrary constants.

Therefore, by setting $f_k = 0$, $k > 5$, we get two linearly
independent polynomials, $f_0(z) = 1$ and $f_1(z) =
\frac{533}{11}z + 101z^2 + 102z^3 + 72z^4$ that span the cokernel
of $L_3$. So there exists only one integer, $p_1=2$, such that the
cokernel of $L_3$ is spanned by $f_0(z)$, a polynomial of degree
$r_4=0$, and $f_1(z)$, a polynomial of degree $r_4+
\eta(p_1)=0+(1+3)$. So, by Theorem \ref{Thm5.1}, $L_3y = g$ will have a
solution in $A_4$ if and only if the
coefficients in the series expansions of $g(z)$ satisfy the conditions
$g_0 = 0$ and
$\frac{533}{11}g_1 + 101g_2 + 102g_3 + 72g_4 = 0$.


\paragraph{Acknowledgments.}
I wish to express my gratitude to Professor Leon Hall for his guidance.
This paper stems from work done under his direction as part of my dissertation
at the University of Missouri at Rolla.

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\end{thebibliography}


\noindent{\sc Brian Haile}\\
Department of Mathematics and Statistics\\
Northwest Missouri state university \\
800 University Drive\\
Maryville, MO 64468 USA\\
e-mail: bhaile@mail.nwmissouri.edu

\end{document}