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<title>Integer Composition, Connection Appell Constants and Bell polynomials: Integer Composition, Connection Appell Constants and Bell polynomials</title>
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<h1>Integer Composition, Connection Appell Constants and Bell polynomials</h1>
<p class="authors">
<span class="author">Nataliia Luno\(^\ast \)</span>
</p>
<p class="date">October 10, 2021; accepted: November 26, 2021; published online: February 17, 2022.</p>
</div>
<div class="abstract"><p> We introduce an explicit form of the connection coefficients for Appell polynomial sequences via Toeplitz-Hessenberg matrix determinants. Generalising, we give an explicit form of the connection coefficients for arbitrary polynomial sequences and explain the combinatorial meaning of both constants in terms of integer composition. </p>
<p><b class="bf">MSC.</b> 54AXX. </p>
<p><b class="bf">Keywords.</b> Appell polynomials, generating functions, connection coefficients, integer composition, connection problems, Bell polynomials. </p>
</div>
<p>\(^\ast \)Faculty of Mathematics and Computer Sciences, Vasyl’ Stus Donetsk University, 21, 600-richchia Street, 21021, Vinnytsia, Ukraine, e-mail: <span class="tt">nlunio@ukr.net</span>. </p>
<h1 id="a0000000002">1 Introduction</h1>
<p> In <span class="cite">
	[
	<a href="#Appell" >3</a>
	]
</span>, P. Appell introduced polynomials \(A_n(x)\) defined by the exponential generating function </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A07FEC650>">
<p>
  <div class="equation_content">
    \begin{equation} \label{gen_Ap} \exp (xt)A(t)= \sum _{n=0}^{\infty } A_n(x)\tfrac {t^n}{n!}, \end{equation}
  </div>
  <span class="equation_label">1</span>
</p>
</div>
<p> where \(A(t)\) is a formal power series </p>
<div class="equation" id="a0000000003">
<p>
  <div class="equation_content">
    \begin{equation}  A(t)= \sum _{n=0}^{\infty } a_n \tfrac {t^n}{n!}, \:  \:  a_0\neq 0, \end{equation}
  </div>
  <span class="equation_label">2</span>
</p>
</div>
<p> which are known as <i class="itshape">the Appell polynomials</i> today. </p>
<p>Besides, it was shown there exists a one-to-one correspondence in the form </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A07FEC230>">
<p>
  <div class="equation_content">
    \begin{equation} \label{n_poly} A_n(x)= \textstyle {n \choose 0}a_{n} x^0 + {n \choose 1}a_{n-1}x^1 + {n \choose 2}a_{n-2}x^2 +\dots + {n \choose n}a_0 x^n. \end{equation}
  </div>
  <span class="equation_label">3</span>
</p>
</div>
<p>We call the formal power series \(A(t)\) <i class="itshape">the transfer sequence</i> of the Appell sequence \(\{ A_n(x)\} _{n\geq 0}.\) </p>
<p>Throughout the text, we will use the equivalent for transfer sequence in the form </p>
<div class="equation" id="tvirna">
<p>
  <div class="equation_content">
    \begin{equation} \label{tvirna} A(t)= \sum _{n=0}^{\infty } a_n {t^n}, \:  \:  a_0\neq 0, \end{equation}
  </div>
  <span class="equation_label">4</span>
</p>
</div>
<p> whence </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A07FEE990>">
<p>
  <div class="equation_content">
    \begin{equation} \label{n_poly} A_n(x)= \sum _{i=0}^{n} \textstyle {n \choose i}(n-i)!a_{n-i} x^i. \end{equation}
  </div>
  <span class="equation_label">5</span>
</p>
</div>
<p>The classical Appell polynomials include the monomials, the Bernoulli polynomials, the Euler polynomials, the Hermite polynomials. All of them, in turn, participate in a big number of modern generalisations such as the Bernoulli-Apostol polynomials, the Euler-Apostol polynomials, the Gould-Hopper polynomials, the generalised hypergeometric Appell polynomials, etc. </p>
<p>The Appell polynomials is a special case of the Sheffer polynomials, basic properties of the latter were widely studied in <span class="cite">
	[
	<a href="#Roman" >22</a>
	]
</span> from the point of view of the umbral calculus. Nowdays, the Appell polynomials are of great interest again, new modifiers of the existing definitions and properties are proposed, for instance, the Dattoli’s school <span class="cite">
	[
	<a href="#Dattoli" >12</a>
	]
</span> is focused on the realisation of the Wheyle algebras with special functions, matrix <span class="cite">
	[
	<a href="#Aceto" >1</a>
	]
</span> and determinantal approaches <span class="cite">
	[
	<a href="#Adell" >2</a>
	]
</span> came out as well. As a consequence, new polynomial and combinatorial identities are obtained <span class="cite">
	[
	<a href="#Costabile" >10</a>
	, 
	<a href="#Nguyen" >19</a>
	, 
	<a href="#Pan" >20</a>
	, 
	<a href="#Belbachir" >5</a>
	]
</span>. </p>
<p>For two given arbitrary polynomial sequences \(\{ p_n(x)\} \) and \(\{ q_n(x)\} \) of degree \(n,\) each member of every sequence can be expressed as a linear combination of the second one: </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A07FA3A10>">
<p>
  <div class="equation_content">
    \begin{equation} \label{Con_prob} p_n(x)=\sum _{k=0}^n c_k(n)q_k(x). \end{equation}
  </div>
  <span class="equation_label">6</span>
</p>
</div>
<p>We call expression ?? <i class="itshape">the connection problem</i> for polynomial sequences \({\{ }{{{p}}}_{n}({}{{{x}}}){\} }\) and \(\{ q_n(x)\} .\) The unknown numbers \(c_k(n)\) that need to be found are called <i class="itshape">the connection coefficients</i> or the <i class="itshape">connection constants</i>. </p>
<p>When \(p_n(x)=x^n,\) the connection problem ?? is called <i class="itshape">the inverse problem</i>: </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A080687D0>">
<p>
  <div class="equation_content">
    \begin{equation} \label{Inv_prob} x^n=\sum _{k=0}^n c_k(n)q_k(x). \end{equation}
  </div>
  <span class="equation_label">7</span>
</p>
</div>
<p>In literature, large variety of methods are proposed to solve the connection problem, and choosing the proper method depends on what special classes both sequences belong to. Great amount of solutions were constructed considering the classical orthogonal polynomials, we only mention the ones based on NaViMa and other algorithms <span class="cite">
	[
	<a href="#Lopez" >16</a>
	, 
	<a href="#Koepf" >14</a>
	, 
	<a href="#Sanchez" >25</a>
	]
</span> or on the generalised hypergeometric function <span class="cite">
	[
	<a href="#Lewa" >15</a>
	]
</span>. Sometimes the results obtained by the recurrence methods are recurrent themselves <span class="cite">
	[
	<a href="#Ronv" >24</a>
	, 
	<a href="#Godoy" >13</a>
	]
</span>. </p>
<p>The explicit form of several connection problem solutions (the Laguerre polynomials, the Abel polynomials, the Gould polynomials, the falling and the rising factorials, etc.) was presented in the fundamental article by Roman and Rota <span class="cite">
	[
	<a href="#Roman" >22</a>
	]
</span>. </p>
<p>Here, we will use the results on Appell polynomials presented in <span class="cite">
	[
	<a href="#Cheikh" >11</a>
	]
</span>. </p>
<p><div class="theorem_thmwrapper " id="teAppApp">
  <div class="theorem_thmheading">
    <span class="theorem_thmcaption">
    Theorem
    </span>
    <span class="theorem_thmlabel">1</span>
    <span class="theorem_thmtitle">Cheikh and Chaggara</span>
  </div>
  <div class="theorem_thmcontent">
  <p>  Given two Appell sequences \(p_n(x),\) \(deg\left( p_n\right)=n,\) and \(q_n(x),\) \(deg\left( q_n\right)=n,\) with transfer sequences \(A(t)\) and \(B(t),\) respectively, the solution of the connection problem ?? has the form </p>
<div class="equation" id="a0000000004">
<p>
  <div class="equation_content">
    \begin{equation}  p_n(x)=\sum _{i=0}^n \tfrac {n!}{(n-i)!}c_{i}q_{n-i}(x), \textit{ where } \:  {\tfrac {A(t)}{B(t)}=\sum _{i=0}^{\infty } c_it^i}. \end{equation}
  </div>
  <span class="equation_label">8</span>
</p>
</div>

  </div>
</div> </p>
<p>Recently, independently from the Cheikh and Chaggara, in <span class="cite">
	[
	<a href="#Carillo" >9</a>
	]
</span>, the authors presented the Sheffer and Appell families linear functionals based on the inverse problem closed form solution. </p>
<p><i class="itshape">The aim</i> of this paper is to give an <i class="itshape">explicit form</i> of the connection coefficients for the Appell sequences, together with generalizing it to an arbitrary polynomial sequences. We also give the combinatorial interpretation of the results based on integer compositions and discuss arising related questions, <i class="it">i.e.</i>, relations between the Toeplitz-Hessenberg matrices determinants and the classical Bell polynomials. </p>
<h1 id="a0000000005">2 Appell connection coefficients</h1>
<h2 id="a0000000006">2.1 Formal power series</h2>
<p>It is known, that that formal power series <a href="#tvirna" class="eqref">4</a> has a unique multiplicative inverse \({\frac{1}{A(t)}=A^{-1}(t)}\) if and only if \(a \neq 0.\) The explicit formula was firstly discovered by Brioshi <span class="cite">
	[
	<a href="#Brioshi" >8</a>
	]
</span> in 1858 and is re-discovered by different researchers from time to time. </p>
<p>Transforming <a href="#tvirna" class="eqref">4</a>, </p>
<div class="displaymath" id="<plasTeX.TeXFragment object at 0x0000020A080307D0>">
  \begin{multline} \label{Ob_Rec} {\tfrac {1}{A(t)}}= {\left(1+\sum _{n=0}^{\infty } a_n {t^n}\right)}^{-1}= \sum _{m=0}^{\infty } {(-1)}^{m}{\left(1+\sum _{n=0}^{\infty } a_n {t^n}\right)}^{m}= \\ {=\sum _{i=0}^{\infty } \sum _{\substack {m_1, \ldots , m_n {\gt} 0, \\ \begin{bgroup} m_1+2m_2+\ldots +im_i=i 

\end{bgroup}}} {(-1)}^{m_1+\ldots + m_n}\binom {m_1+ \ldots + m_i}{m_1, \ldots , m_n}a_1^{m_1}\ldots a_i^{m_i} t^i } \end{multline}
</div>
<p>The inner sum is precisely the expanded expression of an arbitrary \(n\)-th order determinant </p>
<div class="displaymath" id="detA">
  \begin{gather}  \label{detA} \sum _{\sigma \in S_n} \epsilon (\sigma )a_1^{\sigma (1)}\ldots a_n^{\sigma (n)} {\displaystyle =\sum _{\sigma _{1}, \sigma _{2},\ldots ,\sigma _{n}}(-1)^{N(\sigma _{1}\sigma _{2}\ldots \sigma _{n})}\cdot a_{1}^{\sigma _{1}}}\dots a_{n}^{\sigma _{n}}, \end{gather}
</div>
<p> where permutations \({\displaystyle \sigma _{1},\sigma _{2},\ldots ,\sigma _{n}}\) belong to \({\displaystyle S_1,S_2,\dots , S_n,}\) respectively, and \({\displaystyle N(\sigma _{1}\sigma _{2}\ldots \sigma _{n})}\) denotes the number of inversions in \({\displaystyle \sigma _{1}\sigma _{2}\ldots \sigma _{n}}.\) </p>
<p>The explicit form of the determinant <a href="#detA" class="eqref">12</a> is given (see, <i class="it">e.g.</i>, <span class="cite">
	[
	<a href="#Merca" >18</a>
	]
</span>) by one of the following expressions </p>
<div class="displaymath" id="ast">
  \begin{gather} \label{ast} {\delta }_{n+1}= \left| \begin{array}{ccccccccc} 0 & a_1 & a_2 & \ldots & a_{i-2} & a_{i-1} & a_i\\ 0 & a_0 & a_1 & \ldots & a_{i-3} & a_{i-2} & a_{i-1}\\ 0 & 0 & a_0 & \ldots & a_{i-4} & a_{i-3} & a_{i-2}\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ 0 & 0 & 0 & \ldots & a_0 & a_1 & a_2 \\ 0 & 0 & 0 & \ldots & a_0 & a_1 \\ 1 & 0 & 0 & \ldots & 0 & a_0 \end{array} \right|, \end{gather}
</div>
<p> or, equivalently, as the \(n\)-th order determinant of a Toeplitz-Hessenberg matrix </p>
<div class="displaymath" id="a0000000007">
  \begin{gather*}  {\delta }_n= \tfrac {{(-1)}^n}{a_0^{n+1}} \left| \begin{array}{ccccccccc} a_1 & a_2 & \ldots & a_{i-2} & a_{i-1} & a_i\\ a_0 & a_1 & \ldots & a_{i-3} & a_{i-2} & a_{i-1}\\ 0 & a_0 & \ldots & a_{i-4} & a_{i-3} & a_{i-2}\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ 0 & 0 & \ldots & a_0 & a_1 & a_2 \\ 0 & 0 & \ldots & 0 & a_0 & a_1 \\ \end{array} \right|. \end{gather*}
</div>
<p>We gather all previous statements into <div class="lemma_thmwrapper " id="Lemma1">
  <div class="lemma_thmheading">
    <span class="lemma_thmcaption">
    Lemma
    </span>
    <span class="lemma_thmlabel">2</span>
  </div>
  <div class="lemma_thmcontent">
  <p> The formal power series <a href="#tvirna" class="eqref">4</a> inverse has the following explicit form </p>
<div class="equation" id="a0000000008">
<p>
  <div class="equation_content">
    \begin{equation}  \tfrac {1}{A(t)}=\sum _{n=0}^{\infty }a_n^{\ast } t^n, \textit{where \: } a_0^{\ast }=1 \:  \textit{and \: } a_i^{\ast }={\delta }_{i+1} \textit{are defined by \eqref{detA}}. \end{equation}
  </div>
  <span class="equation_label">14</span>
</p>
</div>

  </div>
</div> Some first inverse coefficients are listed below. </p>
<div class="displaymath" id="a0000000009">
  \begin{gather*} \begin{array}{ccccccccc} a_0^{\ast }=1,\\ a_1^{\ast }=-a_1,\\ a_2^{\ast }=a_1^2-a_2,\\ a_3^{\ast }=-a_1^3+2a_2a_1-a_3,\\ a_4^{\ast }=a_1^4-3a_2a_1^2+2a_3a_1+a_2^2-a_4,\\ a_5^{\ast }=-a_1^5+4a_1^3a_2-3a_1^2a_3-3a_1a_2^2+2a_1a_4+2a_2a_3-a_5.\\ \end{array}\end{gather*}
</div>
<p>Recall, <i class="itshape">division</i> of two formal power series \(\frac{B(t)}{A(t)}\) is defined as a product \(B(t)A^{-1}(t)\) if \(A^{-1}(t)\) exists. </p>
<p>For \(A(t)=\sum _{n=0}^{\infty } a_n t^n, a_0=1\) and \(B(t)=\sum _{n=0}^{\infty }b_nt^n,\) we denote \(C(t)=\frac{B(t)}{A(t)}=\sum _{=0}^{\infty }c_it^i,\) then \({{\frac{1}{A(t)}}}=\sum _{n=0}^{\infty } a_n^{\ast } t^n\) and, with the Cauchy formula, </p>
<div class="displaymath" id="a0000000010">
  \begin{gather*}  C(t)=B(t)\tfrac {1}{A(t)}= \sum _{n=0}^{\infty }b_nt^n \cdot \sum _{n=0}^{\infty } a_n^{\ast } t^n= \sum _{n=0}^{\infty } \left( \sum _{p=0}^{n} b_{n-p}a^{\ast }_p \right)\:  t^n. \end{gather*}
</div>
<p> Considering the expressions <a href="#ast" class="eqref">13</a> for \(a^{\ast }_p\) and the properties of the determinants, we obtain </p>
<div class="displaymath" id="determin">
  \begin{gather} \label{determin} c_0=1, c_n= \displaystyle \tfrac {1}{a_0^{p+1}} \left| \begin{array}{cccccccc} b_p & a_1 & a_2 & \ldots & a_{p-2} & a_{p-1} & a_p\\ b_{p-1} & a_0 & a_1 & \ldots & a_{p-3} & a_{p-2} & b_{p-1}\\ b_{p-2} & 0 & a_0 & \ldots & a_{p-4} & a_{p-3} & b_{p-2}\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ b_2 & 0 & 0 & \ldots & a_0 & a_1 & a_2 \\ b_1 & 0 & 0 & \ldots & 0 & a_0 & a_1 \\ b_0 & 0 & 0 & \ldots & 0 & 0 & a_0 \end{array} \right|. \end{gather}
</div>
<p> Some first ratio coefficients are listed below. </p>
<div class="displaymath" id="a0000000011">
  \begin{gather*} \begin{array}{ccccccccc} c_0=1,\\ c_1=-a_1+_1,\\ c_2=a_1^2-a_1b_1-a_2+b_2,\\ c_3=-a_1^3+a_1^2b_1+2a_2a_1-a_1b_2-a_2b_1-a_3+b_3,\\ c_4^{\ast }=a_1^4-a_1^3b_1-3a_1^2a_2+a_1^2b_2+2a_1a_2b_1+2a_3a_1-a_1b_3+a_2^2-a_2b_2-\\ -a_3b_1-a_4+b_4. \end{array}\end{gather*}
</div>
<h2 id="a0000000012">2.2 Connection constants</h2>
<p> Thus, we derive the explicit form of two arbitrary formal power series ratio. <div class="lemma_thmwrapper " id="Lemma2">
  <div class="lemma_thmheading">
    <span class="lemma_thmcaption">
    Lemma
    </span>
    <span class="lemma_thmlabel">3</span>
  </div>
  <div class="lemma_thmcontent">
  <p> The ratio coefficients \(c_i\) of two given formal power series \(A(t)=\sum _{n=0}^{\infty } a_n t^n, a_0 \neq 0\) and \(B(t)=\sum _{n=0}^{\infty }b_nt^n\) are defined by formulas <a href="#determin" class="eqref">15</a>. </p>

  </div>
</div> Now, connection Appell coefficients are specified as follows. </p>
<p><div class="theorem_thmwrapper " id="teApp2">
  <div class="theorem_thmheading">
    <span class="theorem_thmcaption">
    Theorem
    </span>
    <span class="theorem_thmlabel">4</span>
  </div>
  <div class="theorem_thmcontent">
  <p> Given two Appell families \(p_n(x)\) and \(q_n(x)\) such that \(\operatorname {deg}{\left( p_n\right)}{=}\) \(=\operatorname { deg}\left( q_n\right)=n,\) with transfer sequences \(A(t)\) and \(B(t),\) respectively, </p>
<ul class="itemize">
  <li><p>\((i)\) solution of inverse problem for \(A_n(x)\) has the form </p>
<div class="equation" id="a0000000013">
<p>
  <div class="equation_content">
    \begin{equation}  x^i=\sum _{i=0}^n \tfrac {n!}{(n-i)!}a^{\ast }_{i}A_{n-i}(x), \end{equation}
  </div>
  <span class="equation_label">16</span>
</p>
</div>
<p> where connection constants \(a_i^{\ast }\) are defined by <a href="#Lemma1">lemma 2</a>; </p>
</li>
  <li><p>\((ii)\) solution of their connection problem has the form </p>
<div class="equation" id="conap">
<p>
  <div class="equation_content">
    \begin{equation}  \label{conap} B_n(x)=\sum _{i=0}^n \tfrac {n!}{(n-i)!}c_{i}A_{n-i}(x), \end{equation}
  </div>
  <span class="equation_label">17</span>
</p>
</div>
<p> where connection constants \(c_i\) are defined by <a href="#Lemma2">lemma 3</a>. </p>
</li>
</ul>

  </div>
</div> </p>
<p>The proof comes from <a href="#teAppApp">theorem 1</a>, <a href="#Lemma1">lemma 2</a> and <a href="#Lemma2">lemma 3</a>. </p>
<p><div class="example_thmwrapper " id="a0000000014">
  <div class="example_thmheading">
    <span class="example_thmcaption">
    Example
    </span>
    <span class="example_thmlabel">5</span>
  </div>
  <div class="example_thmcontent">
  <p>Considering two equal formal power series with \(a_i=b_i\) for all \(i \geq 0\), according to <a href="#teApp2">theorem 4</a> we have </p>
<div class="displaymath" id="a0000000015">
  \begin{gather*}  c_0=1,c_i= \tfrac {1}{a_0^{i+1}} \left| \begin{array}{cccccccc} b_i & b_1 & _2 & \ldots & b_{i-2} & b_{i-1} & _i\\ b_{i-1} & b_0 & b_1 & \ldots & b_{i-3} & b_{i-2} & b_{i-1}\\ b_{i-2} & 0 & b_0 & \ldots & b_{i-4} & b_{i-3} & b_{i-2}\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ b_2 & 0 & 0 & \ldots & b_0 & b_1 & b_2 \\ b_1 & 0 & 0 & \ldots & 0 & b_0 & b_1 \\ b_0 & 0 & 0 & \ldots & 0 & 0 & b_0 \end{array} \right|=0, \end{gather*}
</div>
<p> which turns the connection formula <a href="#conap" class="eqref">17</a> into the needed identity: </p>
<div class="displaymath" id="a0000000016">
  \[  A_n(x)=\sum _{i=0}^n \tfrac {n!}{(n-i)!}c_{i}B_{n-i}(x)=c_0B_{n-0}(x)=B_n(x).  \]
</div>

  </div>
</div> </p>
<p><div class="example_thmwrapper " id="a0000000017">
  <div class="example_thmheading">
    <span class="example_thmcaption">
    Example
    </span>
    <span class="example_thmlabel">6</span>
  </div>
  <div class="example_thmcontent">
  <p>Let us find the standard basis representation of an arbitrary Appell polynomial \(A_n(x)\) with transfer sequence \(A(t)=\sum _{n=0}^{\infty }a_nt^n,\) where \(a_n={ \tfrac {A_n(0)}{n!}}.\) For standard basis, we have \(B_n(x)=x^n\) with transfer sequence \(B(t)=\sum _{n=0}^{\infty }t^n,\) then </p>
<div class="displaymath" id="a0000000018">
  \begin{gather*}  c_0=1,c_i= \tfrac {1}{a_0^{i+1}} \left| \begin{array}{cccccccc} a_i & 0 & 0 & \ldots & 0 & 0\\ a_{i-1} & 1 & 0 & \ldots & 0 & 0\\ a_{i-2} & 0 & 1 & \ldots & 0 & 0\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ a_1 & 0 & 0 & \ldots & 0 & 1 & 0 \\ a_0 & 0 & 0 & \ldots & 0 & 0 & 1 \end{array} \right|=a_i \end{gather*}
</div>
<p> and the connection formula <a href="#conap" class="eqref">17</a> takes the form </p>
<div class="displaymath" id="a0000000019">
  \[  A_n(x)=\sum _{i=0}^n \tfrac {n!}{(n-i)!}a_{i}x^{n-i}= \sum _{i=0}^n \tfrac {n!}{(n-i)!}\tfrac {A_i(0)}{i!}x^{n-i}=\sum _{n=0}^{n}\textstyle {n \choose i}A_i(0)x^{n-i},  \]
</div>
<p> which reconstitute S. Roman’s umbral calculus result presented in <span class="cite">
	[
	<a href="#Roman" >22</a>
	]
</span>. </p>

  </div>
</div> </p>
<p><div class="remark_thmwrapper " id="a0000000020">
  <div class="remark_thmheading">
    <span class="remark_thmcaption">
    Remark
    </span>
    <span class="remark_thmlabel">7</span>
  </div>
  <div class="remark_thmcontent">
  <p>It is easy to see that the first \(k\) members of the ratio \(\frac{B(t)}{A(t)}=C(t)=\sum _{=0}^{\infty }c_it^i\) with \(A(t)=\sum _{i=0}^{\infty }a_it^i\) and \(B(t)=\sum _{i=0}^{\infty }b_it^i\) produce the simultaneous linear recurrent equations </p>
<div class="displaymath" id="a0000000021">
  \[  b_k=\sum _{j=0}^k a_j c_{k-j},\:  \text{where}\:  a_0\neq 0,  \]
</div>
<p> solutions of which in the form of determinants <a href="#determin" class="eqref">15</a> were given formulas ???(2.22) in the significant collection of combinatorial identities of H. W Gould <span class="cite">
	[
	<a href="#Gould2010" >21</a>
	]
</span>. <span class="qed">â–¡</span></p>

  </div>
</div> </p>
<p><div class="remark_thmwrapper " id="a0000000022">
  <div class="remark_thmheading">
    <span class="remark_thmcaption">
    Remark
    </span>
    <span class="remark_thmlabel">8</span>
  </div>
  <div class="remark_thmcontent">
  <p>Another interesting method of obtaining determinants <a href="#ast" class="eqref">13</a> appeared in <span class="cite">
	[
	<a href="#Wheeler" >26</a>
	]
</span>. For two given formal power series </p>
<div class="displaymath" id="a0000000023">
  \[  g(x)=a_1x^1+a_2x^2+a_3x^3+\ldots +a_nx^n+\ldots , \]
</div>
<div class="displaymath" id="a0000000024">
  \[  f(x)=\tfrac {1}{1-x}=1+x^1+x^2+x^3+\ldots +x^n+\ldots , \]
</div>
<p> their compositional function \(F(x)=f\left(g(x)\right)\) has the expansion </p>
<div class="displaymath" id="a0000000025">
  \begin{gather*}  F(x)=1+a_1x^1+(a_1^2+a_2)x^2+(a_1^3+2a_1a_2+a_3)x^3+\\ +(a_1^4+3a_1^2a_2+a_2^2+2a_1a_3+a_4)x^4+\\ +(a_1^5+4a_1^3a_2+3a_1a_2^2+3a_1^2a_3+2a_2a_3+2a_1a_4+a_5)x^5+ \ldots \end{gather*}
</div>
<p> and the coefficients of the powers of \(n\) almost coincide with the connection determinants defined by <a href="#ast" class="eqref">13</a> (for total identity, choose \(f(x)=\frac{1}{1+x}.\)) </p>
<p>The reasons of choosing \(f(x)\) and \(g(x),\) due to N. Wheeler, is cored into the eigenvalue representation of unnamed Newton matrices identity: </p>
<div class="displaymath" id="a0000000026">
  \[  \operatorname {det} \left(\mathbb {I}-x\mathbb {A}\right){=}\exp \left( \operatorname {tr} \:  \operatorname {log} \left(\mathbb {I}-x\mathbb {A}\right)\right){=}{\exp }\left({-}T_1x-\tfrac {1}{2}T_2x^2-\tfrac {1}{3}T_3x^3+{\ldots } \right),  \]
</div>
<p> where \(T_k = tr ( {\mathbb {A}}^k).\) </p>
<p>Besides the relations between the connection determinants and the Toeplitz-Hessenberg matrix determinants, in <span class="cite">
	[
	<a href="#Wheeler" >26</a>
	]
</span>, the similarity of the Toeplitz-Hessenberg matrix determinants and the classical Bell polynomials are clarified. In the assumptions </p>
<div class="displaymath" id="a0000000027">
  \[ f(x)=\exp (x)=1+\tfrac {1}{1!}x^1+\tfrac {1}{2!}x^2+\tfrac {1}{3!}x^3+\ldots , \]
</div>
<div class="displaymath" id="a0000000028">
  \[  g(x)=b_1x^1+\tfrac {1}{2!}b_2x^2+\tfrac {1}{3!}b_3x^3+\ldots ,  \]
</div>
<p> one can obtain </p>
<div class="displaymath" id="a0000000029">
  \begin{gather*}  F(x)=1+\tfrac {1}{1!}b_1x^1+\tfrac {1}{2!}(b_1^2+b_2)x^2+\tfrac {1}{3!}(b_1^3+3b_1b_2+b_3)x^3+\\ +\tfrac {1}{4!}(b_1^4+6b_1^2b_2+3b_2^2+4_1b_3+b_4)x^4+\\ +\tfrac {1}{5!}(b_1^5+10b_1^3b_2+15b_1b_2^2+10b_1^2b_3+10b_2b_3+5b_1b_4+b_5)x^5+ \ldots = \end{gather*}
</div>
<div class="displaymath" id="a0000000030">
  \begin{gather*}  =1+\tfrac {1}{1!}B_1\left(b_1\right)x^1+\tfrac {1}{2!}B_2\left(b_1,b_2\right)x^2+\tfrac {1}{3!}B_3\left(b_1,b_2,b_3\right)x^3+\\ +\tfrac {1}{4!}B_4\left(b_1, b_2, b_3, b_4\right)x^4 +\tfrac {1}{5!}B_5\left(b_1, b_2, b_3, b_4, b_5\right)x^5+ \ldots , \end{gather*}
</div>
<p> where the \(B_n(\bullet )\) are the classical <i class="itshape">complete exponential Bell polynomials.</i> <span class="qed">â–¡</span></p>

  </div>
</div> </p>
<h1 id="a0000000031">3 Combinatorial meanings of Appell connection constants</h1>
<h2 id="a0000000032">3.1 Integer composition</h2>
<p>As far as classical Bell polynomials encode the information related to the ways a set (an integer number) can be partitioned, let us have a look on the inverse determinants <a href="#ast" class="eqref">13</a> from the combinatorial point of view. </p>
<p><i class="itshape">The partition</i> of the integer number \(n\) is a tuple of positive integers <span class="cite">
	[
	<a href="#Andrews" >4</a>
	]
</span>: \(\lambda =\left({\lambda }_1,{\lambda }_2, \ldots , {\lambda }_n\right) \) such that \({\lambda }_1+{\lambda }_2+ \ldots + {\lambda }_k=n\) and \({\lambda }_1\leq {\lambda }_2\leq \ldots \leq {\lambda }_k.\) The notation \(\lambda \vdash n\) means that \(\lambda \) is a partition of \(n.\) As usual, integer partitions are visualized with Young diagrams. </p>
<p>Two sums that differ only in the order of their summands are considered the same partition. For example, \(5\) can be partitioned in seven distinct ways: </p>
<div class="displaymath" id="a0000000033">
  \[  5=5, 5=4 + 1, 5=3 + 2, 5=3 + 1 + 1, 5=2 + 2 + 1, \]
</div>
<div class="displaymath" id="a0000000034">
  \[  5=2 + 1 + 1 + 1, 5=1 + 1 + 1 + 1+1. \]
</div>
<p>If the order of summands does matter, integer partition is called <i class="itshape">integer composition.</i> </p>
<p>In the case of integer composition of \(n,\) we move from the origin \((0, 0)\) to the east-north along the \(n \times n\) square diagonal. <i class="itshape">The step</i> is a pair \((x, y),\) where \(x\) is an east value, \(y\) is a north value. In integer compositions, only \((x, x)\) diagonal steps occur, with the length of the step equal to \(x.\) Thus, we associate every step \(\left({\lambda }_j, {\lambda }_j \right)\) with a member \({\lambda }_j\) of the certain partition \({\sum }_{j=1}^k {\lambda }_j=n.\) <i class="itshape">The pass</i> is a sequence of the diagonal steps with integer coordinate from the origin \((0, 0)\) to the point \((n, n).\) So, a path is a product of the steps of lengths \({\lambda }_i:\) \( \left({\lambda }_1, {\lambda }_1 \right) \left({\lambda }_2, {\lambda }_2 \right) \ldots \left({\lambda }_k, {\lambda }_k \right).\) Thus, there exists a one-to-one correspondence between the set of all compositions of \(n\) and the set of all different paths from \((0, 0)\) to the point \((n, n).\) </p>
<p>According to the composition definition, for \(n=5,\) the binary paths </p>
<div class="displaymath" id="a0000000035">
  \[  \left(1, 1 \right) \left(2,2 \right) \ldots \left(2, 2 \right) \text{and} \:  \left(2, 2 \right) \left(2,2 \right) \ldots \left(1, 1 \right)  \]
</div>
<p> are considered to be different, but, taking into account step product’s commutativity, we have three different paths of length \(1+2+2:\) </p>
<div class="displaymath" id="a0000000036">
  \begin{gather*}  (1,1)(2,2)(2,2)+(2,2)(1,1)(2,2)+(2,2)(2,2)(1,1)=\\ =3(1,1)(2,2)(2,2)=3(1,1){(2,2)}^2. \end{gather*}
</div>
<p> For \(n=5,\) we have sixteen distinct partitions, two of which are shown in Fig. 1 (a, b). </p>
<figure >
  <div class="centered"><figure class="subfigure" id="f1:n16mu2m1">
 <img src="img-0001.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_1(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption"> \(5=1+1+3\).</span>
</figcaption>
</figure>  <figure class="subfigure" id="f1:n16mu2m2">
 <img src="img-0002.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_2(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(5=2+1+2\).</span>
</figcaption>
</figure> <figcaption>
  <span class="caption_title">Figure</span> 
  <span class="caption_ref">1</span> 
  <span class="caption_text"></span> 
</figcaption>  </div>

</figure>
<h2 id="a0000000037">3.2 Toeplitz-Hessenberg matrix determinants via integer composition</h2>
<p> As far, as Toeplitz-Hessenberg matrix determinants <a href="#ast" class="eqref">13</a> and, consequently, the formulas ??, describe integer partition of natural number \(i,\) it implies the combinatorial meaning of the connection coefficients \(a_i^{\ast }\) defined by <a href="#Lemma1">lemma 2</a>.‘ We match every step \(\left( {\lambda }_j, {\lambda }_j \right)\) the member \(a_{{\lambda }_j}\) of the transfer function \(A(t)={\sum }_{n=0}^n a_it^i.\) Then, the expressions for \(a_i^{\ast }\) <a href="#ast" class="eqref">13</a> of the inverse problem are literally the “<i class="itshape">connection</i>” coefficients, each of \(a_i^{\ast }\) is formed as a sum of all different paths connecting the origin \((0, 0)\) with the point \((n, n).\) The latter coincides with all integer compositions of \(n.\) </p>
<p>For instance, if \(n=5,\) from <a href="#ast" class="eqref">13</a>, </p>
<div class="displaymath" id="a0000000038">
  \begin{equation*}  c_5=-a_1^5+4a_1^3a_2-3a_1^2a_3-3a_1a_2^2+2a_1a_4+2a_2a_3-a_5. \end{equation*}
</div>
<p> Here the summands multiplied by a number \(k\) contain \(k\) different paths, <i class="it">i.e.</i>, </p>
<div class="displaymath" id="a0000000039">
  \[ 3a_1a_2^2=a_1a_2a_2+a_2a_1a_2+a_2a_2a_1 \]
</div>
<p> binary path corresponding to the second summand in the latter sum are shown in Fig. 1(a)??, </p>
<div class="displaymath" id="a0000000040">
  \[ 3a_1^2a_3=a_1a_1a_3+a_1a_3a_1+a_3a_1a_1 \]
</div>
<p> binary path corresponding to the first summand in the latter sum are shown in Fig. 1(b)???, and we have sixteen different binary paths in total. </p>
<p>Moreover, those coefficients \(a_i^{\ast }\) <a href="#ast" class="eqref">13</a> form the corresponding line in the analogue of Pascal triangle, similiar constructions occure for special polynomial structures (<span class="cite">
	[
	<a href="#Bonneux" >7</a>
	]
</span>). In the case of the inverse problem, we have the analogue of Pascal’s triangle for compositions (as far as the order of the summands matters, some coefficients are multiplied by a number \(k\)): </p>
<div class="displaymath" id="a0000000041">
  \[  {{{ {{{ \begin{array}{ccccccccccccccccccccccccc}& & & & &  \!  {{{1 }}}\\ & & & & &  \!  {{{-}}}a_{(1)} \\ & & & & \!  {{{a}}}_{(1^2)} & &  \!  {{{-}}}{{{a}}}_{(2)} \\ & & &  \!  {{{-}}}{{{a}}}_{(1^3)} & &  \!  {{2}}{{{a}}}_{(2,1)} & &  \!  {{{-a}}}_{(3)} \\ & &  \!  {{{a}}}_{(1^4)} & &  \!  {{{-}}}{{3}}{{{a}}}_{(2,1^2)} &  \!  a_{(2^2)} &  \!  2a_{(3,1)} & &  \!  {{{-a}}}_{(4)} \\ & \!  {{{-a}}}_{{{(1^5)}}} & &  \!  {4{a_{{{(2,1^3)}}}}} &  \!  {{{-}}}{3}a_{{{(2^2,1)}}} &  \!  {{{-}}}{3}a_{{{(3,1^2)}}} &  \!  {2}a_{{{(3,2)}}} &  \!  {2}a_{{{(4,1)}}} & &  \!  {{{-}}}a_{(5)} \end{array}}}} }}}  \]
</div>
<p> where \(a_{\left(\lambda _i \vdash n\right)}=\prod _{i} a_i^{m_i},\) <i class="it">i.e.</i>, \( a_{(2,1^3)}=a_2a_1^3.\) </p>
<p>Here, some summands have negative signs. Combinatorially, it means when making the odd number of paths we change the direction into the opposite one. </p>
<p>Let us denote the number of all different paths corresponding to integer \(n\) by \(W(n),\) the properties of the Pascal triangle implies \(W(n)=2^{n-1}.\) Thus, we have </p>
<p><div class="proposition_thmwrapper " id="proposition1">
  <div class="proposition_thmheading">
    <span class="proposition_thmcaption">
    Proposition
    </span>
    <span class="proposition_thmlabel">9</span>
  </div>
  <div class="proposition_thmcontent">
  <p> The number of all different paths corresponding to each \(a_i^{\ast }\) in determinants <a href="#ast" class="eqref">13</a> is equal to \(2^{i-1}.\) </p>

  </div>
</div> </p>
<p>Combinatorially, the expressions for \(c_i\) from the <i class="itshape">connection problem solution</i> given by <a href="#teApp2">theorem 4</a> are formed in the following manner. Starting from the origin \((0, 0),\) the first step correspondent to \(b_i\) always ought to be made <i class="itshape">over</i> the main diagonal of the big square to the east-north (marked by blue), and it can be absent. The rest of the steps corresponding to \({\prod }_{k=1}^{n-i} a_k\) are made <i class="itshape">under</i> the main diagonal of the big square to the point \((n, n)\) (marked by red). </p>
<p>In other words, connection coefficient \(c_n\) is represented by the set of all paths, each of the latter consists of no more than one upper binary step and the rest \((n-i)\) lower steps, both all upper and lower steps are the members of the same integer partition. If we match every upper step \(\left( {\beta }_i, {\beta }_i\right)\) with the coefficient \({b}_{{\beta }_i}\) of the transfer function \(B(t)\) and we match the rest \((n-i)\) of the lower steps with the product of the coefficients \({a}_{{\alpha }_1}, \ldots , {a}_{{\alpha }_{n-i}} \) of the transfer function \(A(t),\) then the path \(\left({\beta }_i, {\beta }_i \right) \left({\alpha }_1, {\alpha }_1 \right) \ldots , \left({\alpha }_{n-i}, {\alpha }_{n-i} \right)\) is matched with a product \({b}_{{\beta }_i},{a}_{{\alpha }_1}, \ldots , {a}_{{\alpha }_{n-i}},\) where \({\beta }_{i}+{\alpha }_1+ \ldots + {\alpha }_{n-i}=n.\) </p>
<p>For instance, if \(n=4,\) due to <a href="#determin" class="eqref">15</a>, </p>
<div class="displaymath" id="a0000000042">
  \[ c_4=a_1^4-a_1^3b_1-3a_1^2a_2+a_1^2b_2+2a_1a_2b_1+2a_1a_3-a_1b_3+a_2^2-a_2b_2-a_3b_1-a_4+b_4. \]
</div>
<p> Here the summands multiplied by a number \(k\) contain \(k\) different paths, starting with \(b_i\) \((0\leq i \leq n),\) <i class="it">i.e.</i>, </p>
<div class="displaymath" id="a0000000043">
  \[ 2a_1a_2b_1=b_1a_1a_2+b_1a_2a_1 \]
</div>
<p> the paths corresponding to both summands are shown in Fig. 2(a,b). </p>
<figure >
  
<div class="centered"><figure class="subfigure" id="f1:n16mu2m1">
 <img src="img-0003.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_3(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(b_1a_1a_2\).</span>
</figcaption>
</figure>  <figure class="subfigure" id="f1:n16mu2m2">
 <img src="img-0004.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_4(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(b_1a_2a_1\).</span>
</figcaption>
</figure> <figcaption>
  <span class="caption_title">Figure</span> 
  <span class="caption_ref">2</span> 
  <span class="caption_text"></span> 
</figcaption>  </div>

</figure>
<p><div class="proposition_thmwrapper " id="a0000000044">
  <div class="proposition_thmheading">
    <span class="proposition_thmcaption">
    Proposition
    </span>
    <span class="proposition_thmlabel">10</span>
  </div>
  <div class="proposition_thmcontent">
  <p>The number of all different paths corresponding to each connection coefficient \(c_i\) in determinants <a href="#ast" class="eqref">13</a> is equal to \(2^{i}.\) </p>

  </div>
</div> <div class="proof_wrapper" id="a0000000045">
  <div class="proof_heading">
    <span class="proof_caption">
    Proof
    </span>
    <span class="expand-proof">â–¼</span>
  </div>
  <div class="proof_content">
  
  </div>
</div>Let us count the number of all paths correspondent to the connection coefficient<a href="#ast" class="eqref">13</a>. </p>
<ul class="itemize">
  <li><p>If multiplier \(b_i\) is absent, the corresponding summands look like \({\prod }_ka_k\) and the number of all correspondent paths describes integer composition of \(n,\) and it is equal to \(W(n)\); </p>
</li>
  <li><p>for \(b_1,\) the correspondent multipliers \({\prod }_ka_k\) describe integer composition of \(n-1,\) d the number of correspondent paths is equal to \(W(n-1)\), and we have \(1 \cdot W(n-1)\) paths in total; </p>
</li>
  <li><p>for \(b_2,\) the correspondent multipliers \({\prod }_ka_k\) describe integer composition of \(n-2,\) d the number of correspondent paths is equal to \(W(n-2)\), and we have \(1 \cdot W(n-1)\) paths in total; and so on; </p>
</li>
  <li><p>for \(b_{n-1},\) we have \(1 \cdot W(1)\) paths; </p>
</li>
  <li><p>finally, for \(b_{n},\) we have only one possible path. </p>
</li>
</ul>
<p> Summing up, we obtain from <a href="#proposition1">proposition 9</a>: </p>
<div class="displaymath" id="a0000000046">
  \begin{gather*}  W(n)+1 \cdot W(n-1)+1 \cdot W(n-2)+ \cdots + 1 \cdot W(2)+ 1 \cdot W(1) +1=\\ 2^{n-1}+2^{n-2}+\cdots + 2^{1}+ 2^{0}+1. \end{gather*}
</div>
<p> The latter sum is known to be equal to \(2^n,\) which completes the proof. </p>
<h1 id="a0000000047">4 Connection coefficients for arbitrary polynomials</h1>
<h2 id="<plasTeX.TeXFragment object at 0x0000020A0835DC10>">4.1 Expressions for arbitrary connection constants</h2>
<p>Connection between two orthogonal polynomial families </p>
<div class="displaymath" id="a0000000048">
  \begin{align*} \label{P_Q} P_n(x)=\sum _{k=0}^n {a}_{n,k}x^k, \quad \quad Q_n(x)=\sum _{k=0}^m {\overline{a}}_{m,k}x^m, \:  {a}_{n,k}, {\overline{a}}_{m,k} \in \mathbb {R} \end{align*}
</div>
<p> can be established as a connection between corresponding vectors \(\vec{P}_n^t\) and \(\vec{Q}_n^t\) by the lower-triangle matrix of unknown coefficients \(C_m(n)\) (see <span class="cite">
	[
	<a href="#Ronv" >24</a>
	]
</span>): </p>
<div class="displaymath" id="a0000000049">
  \[  \vec{P}_n = \left[C_{m,n}\right] \vec{Q}_n \:  \textit{where} \:  C_{m,n}=C_m(n), \]
</div>
<p> or, equivalently: </p>
<div class="displaymath" id="a0000000050">
  \begin{equation*} \begin{pmatrix}  P_0(x)

\\ P_1(x)

\\ \cdots 

\\ P_n(x) 

\end{pmatrix}= \begin{pmatrix}  C_0(0) 

& 0 

& \cdots 

& 0

\\ C_1(0) 

& C_1(1) 

& \cdots 

& C_1(0)

\\ \cdots 

& \cdots 

& \cdots 

& \cdots 

\\ C_n(0) 

& C_n(1) 

& \cdots 

& C_n(n) 

\end{pmatrix}\begin{pmatrix}  Q_0(x)

\\ Q_1(x)

\\ \cdots 

\\ Q_n(x) 

\end{pmatrix}\end{equation*}
</div>
<p>We will search for the solution of the connection problem ?? in the form </p>
<div class="equation" id="<plasTeX.TeXFragment object at 0x0000020A082E6870>">
<p>
  <div class="equation_content">
    \begin{equation} \label{con_con} P_n(x) = \begin{pmatrix}  d_0(n) 

& d_1(n) 

& d_2(n) 

& \cdots 

& d_n(n) 

\end{pmatrix} \begin{pmatrix}  Q_n(x)

\\ Q_{n-1}(x)

\\ Q_{n-2}(x)

\\ \cdots 

\\ Q_0(x) 

\end{pmatrix}. \end{equation}
  </div>
  <span class="equation_label">18</span>
</p>
</div>
<p>Solving the Appell connection problem in the previous section was based on the simultaneously linear recurrence equations </p>
<div class="displaymath" id="a0000000051">
  \[  b_k=\sum _{j=0}^k a_j c_{k-j},\:  \text{where}\:  a_0\neq 0, \:  0 \leq k \leq n,  \]
</div>
<p>Unlike the Appell polynomials, the generating function of an arbitrary polynomial family depends on two variable \(x\) and \(t,\) which can not be "divided" into two independent series, for instance, the Chebyshev polynomials \(T_n(x)\) of the first kind have the following generating function </p>
<div class="displaymath" id="a0000000052">
  \[  \sum _{n=0}^{\infty }T_n(x)t^n=\frac{1-tx}{1-2tx+t^2}.  \]
</div>
<p> Let </p>
<div class="equation" id="explicit">
<p>
  <div class="equation_content">
    \begin{equation}  \label{explicit} P_n(x)=\sum _{i=0}^{n} c_i(n) {x^{n-i}} \text{\: and} \: \:  Q_i(x)=\sum _{j=0}^{i} b_j(i) {x^{i-j}}, 0\leq i \leq n \end{equation}
  </div>
  <span class="equation_label">19</span>
</p>
</div>
<p> be two families of arbitrary polynomials given in the standard basis. For the fixed \(n,\) coefficients \(d_i(n) \) and \(c_i(n) \) can be treated as one-indexed, so we denote \(d_i(n):=d_i,\) \(c_i(n):=c_i.\) After substituting <a href="#explicit" class="eqref">19</a> into ??, we obtain simultaneously two-indexed recurrence equations </p>
<div class="equation" id="simult">
<p>
  <div class="equation_content">
    \begin{equation} \label{simult} b_i=\sum _{j=0}^i a_j c_{i-j}(n-j),\:  \text{where}\:  b_0(i) \neq 0, \:  0 \leq i \leq n. \end{equation}
  </div>
  <span class="equation_label">20</span>
</p>
</div>
<p> Since \(\operatorname {deg}(Q_i(x))=i,\) then \(b_0(i)\neq 0,\) and, by the Cramer’s rule, <a href="#simult" class="eqref">20</a> has unique solution. <div class="lemma_thmwrapper " id="a0000000053">
  <div class="lemma_thmheading">
    <span class="lemma_thmcaption">
    Lemma
    </span>
    <span class="lemma_thmlabel">11</span>
  </div>
  <div class="lemma_thmcontent">
  <p>Solutions \(c_i(n)\) of the simultaneously two-indexed recurrence equations <a href="#simult" class="eqref">20</a> are defined by the \((n+1)\)-order determinants </p>
<div class="displaymath" id="prosto">
  \begin{gather} \label{prosto} \displaystyle { c_i(n)=\frac{1}{a_0(n)a_0(n-1)\ldots a_0(1)a_0(0)}}\times \\ \times \left| \begin{array}{ccccccc} b_i & a_1(n-i+1) & a_2(n-i+2) & \ldots & a_{i-1}(n-i) & a_i(n)\\ b_{i-1} & a_0(n-i+1) & a_1(n-i+2) & \ldots & a_{i-2}(n-i) & a_{i-1}(n)\\ b_{i-2} & 0 & a_0(n-i+2) & \ldots & a_{i-3}(n-i) & a_{i-2}(n)\\ \ldots & \ldots & \ldots & \ldots & \ldots & \ldots \\ b_0 & 0 & 0 & \ldots & 0 & a_0(n) \end{array} \right|.\notag \end{gather}
</div>

  </div>
</div> </p>
<p>Now, we are ready to establish the explicit formula of the connection problem ?? in general case. </p>
<p><div class="theorem_thmwrapper " id="a0000000054">
  <div class="theorem_thmheading">
    <span class="theorem_thmcaption">
    Theorem
    </span>
    <span class="theorem_thmlabel">12</span>
  </div>
  <div class="theorem_thmcontent">
  <p>For two polynomial families given in the standard basis </p>
<div class="displaymath" id="a0000000055">
  \begin{equation*}  P_n(x)=\sum _{i=0}^{n} b_i(n) {x^{n-i}}, \:  Q_i(x)=\sum _{j=0}^{i} a_j(i) {x^{i-j} }, \:  b_0(i) \neq 0, \: 0\leq i \leq n, \end{equation*}
</div>
<p> the unknown connection coefficients \(c_i(n)\) of the connection problem ?? </p>
<div class="displaymath" id="a0000000056">
  \begin{equation*}  P_n(x)=\sum _{i=0}^n c_i(n)Q_i(x) \end{equation*}
</div>
<p> are defined via determinants <a href="#prosto" class="eqref">21</a>. </p>

  </div>
</div> </p>
<h2 id="a0000000057">4.2 Combinatorial meanings of arbitrary connection constants</h2>
<p>In fact, the connection problem ?? includes one polynomial \(P_n(x)\) and the set of the polynomials \(\{ Q_i(x)\} _{i=0}^n,\) every of which, in turn, is defined by the set of two-indexed coefficients \(b_0(n), b_1(n),\) \( \ldots , b_n(n)\) and \(a_0(n), a_1(n), \ldots , a_n(n),\) \(a_0(n-1), a_1(n-1), \ldots , a_n(n-1),\) \(\ldots ,\) \(a_0(0), a_1(0), \ldots , a_n(0),\) respectively. </p>
<p>In the case when all zero-subscribed coefficients are equal to \(1,\) the connection coefficients <a href="#prosto" class="eqref">21</a> have combinatorial meanings. It looks like we need to arrange all implicit points \((i, n)\) associated with value \(a_i(n),\) and points \((i, i)\) associated with values \(b_i(n)\) along the \((n, n)\) square diagonal in a proper way. </p>
<p>More precisely, we associate each two-indexed coefficient \(b_i(n)\) (\(0 \leq i \leq n\)) with upper step (over the diagonal, marked blue) and each two-indexed coefficient \(a_i(i)\) (\(0 \leq i \leq n\)) with lower binary step (under the diagonal, marked red) into the west-south direction. The number in the parentheses denotes the starting point at the diagonal of the \((n, n)\) square, the number of subscript denotes the step size. </p>
<p>Then every connection coefficient \(c_i(n)\) (\(0 \leq i \leq n\)) in <a href="#prosto" class="eqref">21</a> represents the set of all possible paths from point \((n,n)\) to point \((n-i,n-i).\) Each path consists of no more than one upper step \(b_i(n)\) and the rest \((n-i)\) of lower steps \(a_i(i)\) (\(0 \leq i \leq n\)), both all upper and lower steps are the members of the same integer composition. </p>
<figure >
  <div class="centered"><figure class="subfigure" id="f1:n16mu2m1">
 <img src="img-0005.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_5(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(b_3(4) a_1(1)\).</span>
</figcaption>
</figure>  <figure class="subfigure" id="f1:n16mu2m2">
 <img src="img-0006.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_6(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(a_2(2) a_1(3) b_1(4)\).</span>
</figcaption>
</figure> <figcaption>
  <span class="caption_title">Figure</span> 
  <span class="caption_ref">3</span> 
  <span class="caption_text"></span> 
</figcaption>  </div>

</figure>
<p>If \(n=4,i=4,\) from <a href="#prosto" class="eqref">21</a>, </p>
<div class="displaymath" id="a0000000058">
  \begin{gather*}  c_4(4)=b_4(4) - b_3(4) a_1(1) + a_1(1) a_1(2) b_2(4) - a_2(2) b_2(4) -\notag \\ - a_1(1) a_1(2) a_1(3) b_1(4) + a_1(1) a_2(3) b_1(4) + a_2(2) a_1(3) b_1(4) - a_3(3) b_1(4)+\notag \\ + a_1(1) a_1(2) a_1(3) a_1(4) - a_1(1) a_1(2) a_2(4) - a_1(1) a_2(3) a_1(4) + a_1(1) a_3(4) -\notag \\ - a_2(2) a_1(3) a_1(4)+ a_2(2) a_2(4) + a_3(3) a_1(4) - a_4(4), \end{gather*}
</div>
<p> which implies sixteen different paths from \((4, 4)\) to \((0, 0)\), the ones representing the second and the seventh summands, respectively, are shown in Fig. 3(a, b). </p>
<p>If \(n=4,i=3,\) from <a href="#prosto" class="eqref">21</a>, </p>
<div class="displaymath" id="a0000000059">
  \begin{gather*}  c_3(4)=-a_1(3)a_1(2)a_1(4)+a_1(3)a_1(2)b_1(4)+a_2(3)a_1(4)-\notag \\ -a_2(3)b_1(4)+a_1(2)a_2(4)-b_2(4)a_1(2)+b_3(4)-a_3(4), \end{gather*}
</div>
<p> there are eight different binary paths from \((4, 4)\) to \((1, 1)\), the ones representing the second and the third summands, respectively, are shown in Fig. 4(a, b). </p>
<figure >
  <div class="centered"><figure class="subfigure" id="f1:n16mu2m1">
 <img src="img-0007.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_7(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(a_1(3)a_1(2)b_1(4)\).</span>
</figcaption>
</figure>  <figure class="subfigure" id="f1:n16mu2m2">
 <img src="img-0008.jpg" alt="\includegraphics[width=0.4\textwidth ]{part_8(2).jpg}" style="width:0.4" />

<figcaption>
<span class="subcaption">\(a_2(3)b_1(4)\).</span>
</figcaption>
</figure> <figcaption>
  <span class="caption_title">Figure</span> 
  <span class="caption_ref">4</span> 
  <span class="caption_text"></span> 
</figcaption>  </div>

</figure>
<p><div class="proposition_thmwrapper " id="a0000000060">
  <div class="proposition_thmheading">
    <span class="proposition_thmcaption">
    Proposition
    </span>
    <span class="proposition_thmlabel">13</span>
  </div>
  <div class="proposition_thmcontent">
  <p>The number of all different paths corresponding to each connection coefficient in the <a href="#prosto" class="eqref">21</a> is equal to \(2^{i}.\) </p>

  </div>
</div> </p>
<p><i class="itshape">The proof</i> is analogous to that of <a href="#proposition1">proposition 9</a>. </p>
<p><div class="remark_thmwrapper " id="a0000000061">
  <div class="remark_thmheading">
    <span class="remark_thmcaption">
    Remark
    </span>
    <span class="remark_thmlabel">14</span>
  </div>
  <div class="remark_thmcontent">
  <p>Choosing a proper numeration of the polynomial coefficients different from the standard one <a href="#explicit" class="eqref">19</a> one can obtain the binary paths correspondent to the connection coefficients that will start at origin \((0, 0)\) and will end at point \((n,n).\) <span class="qed">â–¡</span></p>

  </div>
</div> </p>
<p><div class="remark_thmwrapper " id="a0000000062">
  <div class="remark_thmheading">
    <span class="remark_thmcaption">
    Remark
    </span>
    <span class="remark_thmlabel">15</span>
  </div>
  <div class="remark_thmcontent">
  <p>In the case when zero-subscribed coefficients are not equal to \(1,\) the number of the summands does not increase, but the number of steps inside one summand does increase. Moreover, the divisors appear as well. That is why the question about combinatorial meanings of the connection coefficients \(c_i(n)\) when all \(a_0(i)\neq 0\) is still open. <span class="qed">â–¡</span></p>

  </div>
</div> </p>
<p><small class="footnotesize">  </small></p>
<div class="bibliography">
<h1>Bibliography</h1>
<dl class="bibliography">
  <dt><a name="Aceto">1</a></dt>
  <dd><p><a href ="https://doi.org/10.1080/10652469.2015.1013035"> <i class="sc">L. Aceto</i>, <i class="sc">H.R. Malonek</i>, <i class="sc">Gr. Tomaz</i>, <i class="it">A unified matrix approach to the representation of Appell polynomials</i>, Integral Transforms. Spec. Funct., <b class="bf">26</b> (2015) no.&#160;6, pp.&#160;426–441, <a href="http://doi.org/10.1080/10652469.2015.1013035">http://doi.org/10.1080/10652469.2015.1013035</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Adell">2</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/j.jmaa.2017.06.077"> <i class="sc">J.A. Adell</i>, <i class="sc">A. Lekuona</i>, <i class="it">Binomial convolution and transformations of Appell polynomials</i>, J. Math. Anal. Appl., <b class="bf">456</b> (2017) no.&#160;1, pp.&#160;16–33, <a href="https://doi.org/10.1016/j.jmaa.2017.06.077">https://doi.org/10.1016/j.jmaa.2017.06.077</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Appell">3</a></dt>
  <dd><p><i class="sc">P. Appell</i>, <i class="it">On one class of polynomials</i>, Ann. Sci. Ec. Norm. Super., <b class="bf">9</b> (1880), 2e serie, pp.&#160;119–144. </p>
</dd>
  <dt><a name="Andrews">4</a></dt>
  <dd><p><i class="sc">G.E. Andrews</i>, <i class="it">The Theory of Partitions</i>, Encyclopedia of Mathematics and Its Applications, vol. 2, Addison-Wesley, 1976. </p>
</dd>
  <dt><a name="Belbachir">5</a></dt>
  <dd><p><a href ="http://www.doiserbia.nb.rs/img/doi/0354-5180/2018/0354-51801812155B.pdf"> <i class="sc">H. Belbachir</i>, <i class="sc">S. Haj Brahim</i>, <i class="sc">M. Rachidi</i>, <i class="it">On another approach for a family of Appell polynomials</i>, Filomat, <b class="bf">9</b> (2018), pp.&#160;4155–4164. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Bell">6</a></dt>
  <dd><p><i class="sc">E.T. Bell</i>, <i class="it">Partition Polynomials</i>, Ann. Math., Second Series, <b class="bf">29</b> (1927-1928), no.&#160;1/4, pp.&#160;38–46. </p>
</dd>
  <dt><a name="Bonneux">7</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/j.aam.2019.101932"> <i class="sc">N. Bonneux</i>, <i class="sc">Z. Hamaker</i>, <i class="sc">J. Stembridge</i>, <i class="sc">M. Stevensa</i>, <i class="it">Wronskian Appell polynomials and symmetric functions</i>, Adv. Appl. Math., <b class="bf">111</b> (2019), 101932, <a href="https://doi.org/10.1016/j.aam.2019.101932">https://doi.org/10.1016/j.aam.2019.101932</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Brioshi">8</a></dt>
  <dd><p><a href ="https://doi.org/10.1007/BF03197335"> <i class="sc">F. Brioschi</i>, <i class="it">Sulle funzioni Bernoulliane ed Euleriane</i>, Ann. Mat. Pura Appl., (1858), pp.&#160;260–263, <a href="https://doi.org/10.1007/BF03197335">https://doi.org/10.1007/BF03197335</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Carillo">9</a></dt>
  <dd><p><a href ="https://doi.org/10.5802/crmath.172"> <i class="sc">S.A. Carillo</i>, <i class="sc">M. Hurtado</i>, <i class="sc">J. Stembridge</i>, <i class="sc">M. Stevensa</i>, <i class="it">Appell and Sheffer sequences; on their characterizations through functionals and examples</i>, Comptes Rendus Math., (2021) no. 2, pp.&#160;205–217, <a href="https://doi.org/10.5802/crmath.172">https://doi.org/10.5802/crmath.172</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Costabile">10</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/j.cam.2010.02.033"> <i class="sc">F.A. Costabile</i>, <i class="sc">E. Longo</i>, <i class="it">A determinantal approach to Appell polynomials</i>, J. Comput. Appl. Math., <b class="bf">234</b> (2010) no. 2, pp.&#160;1528–1542, <a href="https://doi.org/10.1016/j.cam.2010.02.033">https://doi.org/10.1016/j.cam.2010.02.033</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Cheikh">11</a></dt>
  <dd><p><a href ="doi:10.1016/j.cam.2004.02.024"> <i class="sc">Y.B. Cheikh</i>, <i class="sc">H. Chaggara</i>, <i class="it">Connection problems via lowering operators</i>, J. Comput. Appl. Math., <b class="bfseries">178</b> (2005) nos. 1-2, pp.&#160;45–61, <a href="doi:10.1016/j.cam.2004.02.024">doi:10.1016/j.cam.2004.02.024</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Dattoli">12</a></dt>
  <dd><p><a href ="https://doi:10.1016/j.cam.2004.02.024"> <i class="sc">G. Dattoli</i>, <i class="it">Hermite-Bessel and Laguerre-Bessel functions: a by-product of the monomiality principle</i>, in: Advanced Special Functions and Applications, Proceedings of the Melfi School on Advanced Topics in Mathematics and Physics, J. Comput. Appl. Math., Aracne Editrici, Rome, (2005), pp.&#160;147–164, <a href="https://doi:10.1016/j.cam.2004.02.024">https://doi:10.1016/j.cam.2004.02.024</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Godoy">13</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/s0377-0427(97)00137-4"> <i class="sc">E. Godoy</i>, <i class="sc">A. Ronveaux</i>, <i class="sc">A. Zarzo</i>, <i class="sc">I. Area</i>, <i class="it">Minimal recurrence relations for connection coefficients between classical orthogonal polynomials: Continuous case</i>, J. Comput. Appl. Math., (1997) no. 84, pp.&#160;257–275, <a href="https://doi.org/10.1016/s0377-0427(97)00137-4">https://doi.org/10.1016/s0377-0427(97)00137-4</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Koepf">14</a></dt>
  <dd><p><a href ="http://dx.doi.org/10.1016/S0096-3003(01)00078-9"> <i class="sc">W. Koepf</i>, <i class="sc">D. Schmersau</i>, <i class="it">Recurrence equations and their classical orthogonal polynomials solutions</i>, Appl. Math. Comput., (2002) no. 128, pp.&#160;303–327, <a href="http://doi.org/10.1016/S0096-3003(01)00078-9">http://doi.org/10.1016/S0096-3003(01)00078-9</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Lewa">15</a></dt>
  <dd><p><a href ="https://doi.org/10.13140/RG.2.1.2993.3209"> <i class="sc">S. Lewanowicz</i>, <i class="it">The Hypergeometric functions approach to the connection problem for the classical orthogonal polynomials</i>, Inst. of Computer Sci., Univ. of Wroclaw, 2003, <a href="http://doi.org/10.13140/RG.2.1.2993.3209">http://doi.org/10.13140/RG.2.1.2993.3209</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Lopez">16</a></dt>
  <dd><p><i class="sc">J.C. Lopez</i>, sc R. Carreno, <i class="sc">R.M. Suarez</i>, <i class="sc">J.A. Mendoza</i>, <i class="it">Connection formulae among special polynomials</i>, Int. J. Math. Comput. Sci., <b class="bf">10</b> (2015) no. 1, pp.&#160;39–49. </p>
</dd>
  <dt><a name="Luno2020">17</a></dt>
  <dd><p><a href ="https://doi.org/10.15673/tmgc.v13i2.1733"> <i class="sc">N. Luno</i>, <i class="it">Connection problems for the generalized hypergeometric Appell polynomials</i>, Proceedings of the International Geometry Center, <b class="bf">13</b> (2020) no. 2, pp.&#160;1–18, <a href="https://doi.org/10.15673/tmgc.v13i2.1733">https://doi.org/10.15673/tmgc.v13i2.1733</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Merca">18</a></dt>
  <dd><p><a href ="https://eudml.org/doc/267216"> <i class="sc">M. Merca</i>, <i class="it">A note on the determinant of a Toeplitz-Hessenberg matrix</i>, Spec. Matrices, (2013), pp.&#160;10–16, <span class="tt">https://eudml.org/doc/267216</span>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Nguyen">19</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/j.jnt.2013.11.008"> <i class="sc">H.D. Nguyen</i>, <i class="sc">L.G. Cheong</i>, <i class="it">New convolution identities for hypergeometric Bernoulli polynomials</i>, J. Number Theory, <b class="bf">137</b> (2014), pp.&#160;201–221, <a href="https://doi.org/10.1016/j.jnt.2013.11.008">https://doi.org/10.1016/j.jnt.2013.11.008</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Pan">20</a></dt>
  <dd><p><a href ="https://doi.org/10.1016/j.jcta.2005.07.008"> <i class="sc">H. Pan</i>, <i class="sc">Zh. W. Sun</i>, <i class="it">New identities involving Bernoulli and Euler polynomials</i>, J. Combinatorial Theory, Series A, <b class="bf">113</b> (2006) no. 1, pp.&#160;156–175, <a href="https://doi.org/10.1016/j.jcta.2005.07.008">https://doi.org/10.1016/j.jcta.2005.07.008</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Gould2010">21</a></dt>
  <dd><p><i class="sc">J. Quaintance</i>, <i class="it">Combinatorial Identities for Stirling Numbers: The Unpublished Notes of H. W. Gould.</i>, World Scientific Publishing, Singapore, 2015. </p>
</dd>
  <dt><a name="Roman">22</a></dt>
  <dd><p><i class="sc">S. Roman</i>, <i class="sc">G.-C. Rota</i>, <i class="it">The umbral calculus</i>, Adv. Math., <b class="bf">27</b> (1978) no. 2, pp.&#160;95–188. </p>
</dd>
  <dt><a name="Roman2">23</a></dt>
  <dd><p><i class="sc">S. Roman</i>, <i class="it">The umbral calculus</i>, Dover Publ. Inc., New York, 2005. </p>
</dd>
  <dt><a name="Ronv">24</a></dt>
  <dd><p><i class="sc">A. Ronveaux</i>, <i class="it">Orthogonal polynomials: connection and linearisation coefficients</i>, Proceedings of the International Workshop on Orthogonal Polynomials in Mathematical Physics, Leganes, 24-26 June, 1996. </p>
<p><br /></p>
</dd>
  <dt><a name="Sanchez">25</a></dt>
  <dd><p><a href ="http://dx.doi.org/10.1016/S0377-0427(00)00679-8"> <i class="sc">J. Sánchez-Ruiz</i>, <i class="sc">J.S. Dehesa</i>, <i class="it">Some connection and linearization problems for the polynomials in and beyond the Askey scheme</i>, J. Comput. Appl. Math., (2001) no. 133, pp.&#160;579–591, <a href="http://dx.doi.org/10.1016/S0377-0427(00)00679-8">http://dx.doi.org/10.1016/S0377-0427(00)00679-8</a>. <img src="img-0009.png" alt="\includegraphics[scale=0.1]{ext-link.png}" style="width:12.0px; height:10.700000000000001px" />
</a> </p>
</dd>
  <dt><a name="Wheeler">26</a></dt>
  <dd><p><span class="tt">https://www.reed.edu/physics/faculty/wheeler/documents/</span> </p>
</dd>
</dl>


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