Plots of S (x ) and C (x ) . The maximum of C (x ) is about 0.977451 424 . If the integrands of S and C were defined using π / 2 t 2 instead of t 2 , then the image would be scaled vertically and horizontally (see below).
The Fresnel integrals S (x ) and C (x ) , and their auxiliary functions F (x ) and G (x ) are transcendental functions named after Augustin-Jean Fresnel that are used in optics and are closely related to the error function (erf ). They arise in the description of near-field Fresnel diffraction phenomena and are defined through the following integral representations:
S
(
x
)
=
∫
0
x
sin
(
t
2
)
d
t
,
C
(
x
)
=
∫
0
x
cos
(
t
2
)
d
t
,
F
(
x
)
=
(
1
2
π
2
−
S
(
x
)
)
cos
(
x
2
)
−
(
1
2
π
2
−
C
(
x
)
)
sin
(
x
2
)
,
G
(
x
)
=
(
1
2
π
2
−
S
(
x
)
)
sin
(
x
2
)
+
(
1
2
π
2
−
C
(
x
)
)
cos
(
x
2
)
.
{\displaystyle {\begin{aligned}S(x)&=\int _{0}^{x}\sin \left(t^{2}\right)\,dt,\\C(x)&=\int _{0}^{x}\cos \left(t^{2}\right)\,dt,\\F(x)&=\left({\frac {1}{2}}{\sqrt {\frac {\pi }{2}}}-S\left(x\right)\right)\cos \left(x^{2}\right)-\left({\frac {1}{2}}{\sqrt {\frac {\pi }{2}}}-C\left(x\right)\right)\sin \left(x^{2}\right),\\G(x)&=\left({\frac {1}{2}}{\sqrt {\frac {\pi }{2}}}-S\left(x\right)\right)\sin \left(x^{2}\right)+\left({\frac {1}{2}}{\sqrt {\frac {\pi }{2}}}-C\left(x\right)\right)\cos \left(x^{2}\right).\end{aligned}}}
The parametric curve
(
S
(
t
)
,
C
(
t
)
)
{\displaystyle {\bigl (}S(t),C(t){\bigr )}}
is the Euler spiral or clothoid, a curve whose curvature varies linearly with arclength.
The term Fresnel integral may also refer to the complex definite integral
∫
−
∞
∞
e
±
i
a
x
2
d
x
=
π
a
e
±
i
π
/
4
{\displaystyle \int _{-\infty }^{\infty }e^{\pm iax^{2}}dx={\sqrt {\frac {\pi }{a}}}e^{\pm i\pi /4}}
where a is real and positive; this can be evaluated by closing a contour in the complex plane and applying Cauchy's integral theorem .