In mathematics , Hermite numbers are values of Hermite polynomials at zero argument. Typically they are defined for physicists' Hermite polynomials.
Formal definition
The numbers H n = H n (0), where H n (x ) is a Hermite polynomial of order n , may be called Hermite numbers.
The first Hermite numbers are:
H
0
=
1
{\displaystyle H_{0}=1\,}
H
1
=
0
{\displaystyle H_{1}=0\,}
H
2
=
−
2
{\displaystyle H_{2}=-2\,}
H
3
=
0
{\displaystyle H_{3}=0\,}
H
4
=
+
12
{\displaystyle H_{4}=+12\,}
H
5
=
0
{\displaystyle H_{5}=0\,}
H
6
=
−
120
{\displaystyle H_{6}=-120\,}
H
7
=
0
{\displaystyle H_{7}=0\,}
H
8
=
+
1680
{\displaystyle H_{8}=+1680\,}
H
9
=
0
{\displaystyle H_{9}=0\,}
H
10
=
−
30240
{\displaystyle H_{10}=-30240\,}
Recursion relations
Are obtained from recursion relations of Hermitian polynomials for x = 0:
H
n
=
−
2
(
n
−
1
)
H
n
−
2
.
{\displaystyle H_{n}=-2(n-1)H_{n-2}.\,\!}
Since H 0 = 1 and H 1 = 0 one can construct a closed formula for H n :
H
n
=
{
0
,
if
n
is odd
(
−
1
)
n
/
2
2
n
/
2
(
n
−
1
)
!
!
,
if
n
is even
{\displaystyle H_{n}={\begin{cases}0,&{\mbox{if }}n{\mbox{ is odd}}\\(-1)^{n/2}2^{n/2}(n-1)!!,&{\mbox{if }}n{\mbox{ is even}}\end{cases}}}
where (n - 1)!! = 1 × 3 × ... × (n - 1).
Usage
From the generating function of Hermitian polynomials it follows that
exp
(
−
t
2
+
2
t
x
)
=
∑
n
=
0
∞
H
n
(
x
)
t
n
n
!
{\displaystyle \exp(-t^{2}+2tx)=\sum _{n=0}^{\infty }H_{n}(x){\frac {t^{n}}{n!}}\,\!}
Reference gives a formal power series :
H
n
(
x
)
=
(
H
+
2
x
)
n
{\displaystyle H_{n}(x)=(H+2x)^{n}\,\!}
where formally the n -th power of H , H , is the n -th Hermite number, H n . (See Umbral calculus .)
Notes
^ Weisstein, Eric W. "Hermite Number." From MathWorld--A Wolfram Web Resource. http://mathworld.wolfram.com/HermiteNumber.html
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