There are a number of slightly different definitions of the Fresnel integrals. In physics, the Fresnel integrals denoted and are most often defined by
(1)
| |||
(2)
|
so
(3)
| |||
(4)
|
These Fresnel integrals are implemented in the Wolfram Language as FresnelC[z] and FresnelS[z].
and are entire functions.
The and integrals are illustrated above in the complex plane.
They have the special values
(5)
| |||
(6)
| |||
(7)
|
and
(8)
| |||
(9)
| |||
(10)
|
An asymptotic expansion for gives
(11)
| |||
(12)
|
Therefore, as , and . The Fresnel integrals are sometimes alternatively defined as
(13)
| |||
(14)
|
Letting so , and
(15)
| |||
(16)
|
In this form, they have a particularly simple expansion in terms of spherical Bessel functions of the first kind. Using
(17)
| |||
(18)
| |||
(19)
|
where is a spherical Bessel function of the second kind
(20)
| |||
(21)
| |||
(22)
| |||
(23)
| |||
(24)
|
Related functions , , , and are defined by
(25)
| |||
(26)
| |||
(27)
| |||
(28)
|