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) |