Böhmer integral

From HandWiki

In mathematics, a Böhmer integral is an integral introduced by (Böhmer 1939) generalizing the Fresnel integrals. There are two versions, given by C⁡(x,α)=∫x∞tα−1cos⁡(t)dtS⁡(x,α)=∫x∞tα−1sin⁡(t)dt

Consequently, Fresnel integrals can be expressed in terms of the Böhmer integrals as S⁡(y)=12−12π⋅S⁡(12,y2)C⁡(y)=12−12π⋅C⁡(12,y2)

The sine integral and cosine integral can also be expressed in terms of the Böhmer integrals Si⁡(x)=π2−S⁡(x,0)Ci⁡(x)=π2−C⁡(x,0)

References