Determinants and Their Applications in Mathematical Physics

(Chris Devlin) #1
A.6 The Generalized Geometric Series and Eulerian Polynomials 323

Rodrigues formula.


Pn(x)=

1

2

n
n!

D

n
(x

2
−1)

n
,D=

d

dx

;

Generating function relation.


(1− 2 xh+h

2
)


1

(^2) =


n=0
Pn(x)h
n
;
Recurrence relations.
(n+1)Pn+1(x)−(2n+1)xPn(x)+nPn− 1 (x)=0,
(x
2
−1)P

n(x)=n[xPn(x)−Pn−^1 (x)];
Differential equation.
(1−x
2
)P
′′
n
(x)− 2 xP

n
(x)+n(n+1)Pn(x)=0;
Appell relation.If
φn(x)=(1−x
2
)
−n/ 2
Pn(x),
then
φ

n
(x)=nF φn− 1 (x),
where
F=(1−x
2
)
− 3 / 2
.


A.6 The Generalized Geometric Series and


Eulerian Polynomials


The generalized geometric seriesφm(x) and the closely related function


ψm(x) are defined as follows:


φm(x)=



r=0

r

m
x

r
, (A.6.1)

ψm(x)=



r=1

r

m
x

r

. (A.6.2)


The two sums differ only in their lower limits:


φm(x)=ψm(x),m> 0 ,

φ 0 (x)=

1

1 −x

,

ψ 0 (x)=

x

1 −x

=xφ 0 (x)

=φ 0 (x)− 1. (A.6.3)
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