Bessel functions

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Bessel functions of the first kind Jn(x) are defined as the solutions to the Bessel differential equation

x2d2ydx2+xdydx+(x2−n2)y=0

which are nonsingular at the origin. They are sometimes also called cylinder functions or cylindrical harmonics. The Bessel function Jn(z) can also be defined by the contour integral

Jn(z)=12πi∮e(z/2)(t−1/t)t−n−1dt

Applications in statistical mechanics

See also