Generalized Appell polynomials explained

\{pn(z)\}

has a generalized Appell representation if the generating function for the polynomials takes on a certain form:

K(z,w)=A(w)\Psi(zg(w))=

infty
\sum
n=0

pn(z)wn

where the generating function or kernel

K(z,w)

is composed of the series

A(w)=

infty
\sum
n=0

anwn

with

a0\ne0

and

\Psi(t)=

infty
\sum
n=0

\Psintn

and all

\Psin\ne0

and

g(w)=

infty
\sum
n=1

gnwn

with

g1\ne0.

Given the above, it is not hard to show that

pn(z)

is a polynomial of degree

n

.

Boas–Buck polynomials are a slightly more general class of polynomials.

Special cases

g(w)=w

gives the class of Brenke polynomials.

\Psi(t)=et

results in the Sheffer sequence of polynomials, which include the general difference polynomials, such as the Newton polynomials.

g(w)=w

and

\Psi(t)=et

gives the Appell sequence of polynomials.

Explicit representation

The generalized Appell polynomials have the explicit representation

pn(z)=

n
\sum
k=0

zk\Psikhk.

The constant is

hk=\sumP

a
j0
g
j1
g
j2

g
jk

where this sum extends over all compositions of

n

into

k+1

parts; that is, the sum extends over all

\{j\}

such that

j0+j1++jk=n.

For the Appell polynomials, this becomes the formula

pn(z)=

n
\sum
k=0
an-kzk
k!

.

Recursion relation

Equivalently, a necessary and sufficient condition that the kernel

K(z,w)

can be written as

A(w)\Psi(zg(w))

with

g1=1

is that
\partialK(z,w)
\partialw

=c(w)K(z,w)+

zb(w)
w
\partialK(z,w)
\partialz

where

b(w)

and

c(w)

have the power series

b(w)=

w
g(w)
d
dw

g(w) =1+

infty
\sum
n=1

bnwn

and

c(w)=

1
A(w)
d
dw

A(w) =

infty
\sum
n=0

cnwn.

Substituting

K(z,w)=

infty
\sum
n=0

pn(z)wn

immediately gives the recursion relation

zn+1

d
dz

\left[

pn(z)
zn

\right]=

n-1
-\sum
k=0

cn-k-1pk(z)-z

n-1
\sum
k=1

bn-k

d
dz

pk(z).

For the special case of the Brenke polynomials, one has

g(w)=w

and thus all of the

bn=0

, simplifying the recursion relation significantly.

See also

References