The operator representing the computation of a derivative,
(1)
|
sometimes also called the Newton-Leibniz operator. The second derivative is then denoted ,
the third
,
etc. The integral is denoted
.
The differential operator satisfies the identity
(2)
|
where
is a Hermite polynomial (Arfken 1985, p. 718),
where the first few cases are given explicitly by
(3)
| |||
(4)
| |||
(5)
| |||
(6)
| |||
(7)
| |||
(8)
|
The symbol
can be used to denote the operator
(9)
|
(Bailey 1935, p. 8). A fundamental identity for this operator is given by
(10)
|
where
is a Stirling number of the second
kind (Roman 1984, p. 144), giving
(11)
| |||
(12)
| |||
(13)
| |||
(14)
|
and so on (OEIS A008277). Special cases include
(15)
| |||
(16)
| |||
(17)
|
A shifted version of the identity is given by
(18)
|
(Roman 1984, p. 146).