Abstract
The function Ω
n
(
x
) defined by the integral 1/
π
∫
π
0
sin (
x
sin
ϕ
—
nϕ
)
dϕ
), or, when
n
is an even integer, by 2/
π
∫
π
/2
0
sin (
x
sin
ϕ
) cos
nϕdϕ
is closely related to J
n
(
x
), which was first given by Bessel under the form 1/
π
∫
π
0
cos (
x
sin
ϕ
—
nϕ
)
dϕ
. The Ω function, although of less importance in its application than the J function, occurs in a number of problems in mathematical physics, more especially those relating to the interference and diffraction of light.
Cited by
2 articles.
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