In mathematics, the Jacobi–Anger expansion (or Jacobi–Anger identity) is an expansion of exponentials of trigonometric functions in the basis of their harmonics. It is useful in physics (for example, to convert between plane waves and cylindrical waves), and in signal processing (to describe FM signals). This identity is named after the 19th-century mathematicians Carl Jacobi and Carl Theodor Anger.
The most general identity is given by:[1] [2]
ei\equiv
infty | |
\sum | |
n=-infty |
inJn(z)ei,
where
Jn(z)
n
i
ei\equiv
infty | |
\sum | |
n=-infty |
Jn(z)ei.
Using the relation
J-n(z)=(-1)nJn(z),
n
ei\equivJ0(z)+2
infty | |
\sum | |
n=1 |
inJn(z)\cos(n\theta).
The following real-valued variations are often useful as well:[3]
\begin{align} \cos(z\cos\theta)&\equivJ0(z)+2
infty | |
\sum | |
n=1 |
(-1)nJ2n(z)\cos(2n\theta), \\ \sin(z\cos\theta)&\equiv-2
infty | |
\sum | |
n=1 |
(-1)nJ2n-1(z)\cos\left[\left(2n-1\right)\theta\right], \\ \cos(z\sin\theta)&\equivJ0(z)+2
infty | |
\sum | |
n=1 |
J2n(z)\cos(2n\theta), \\ \sin(z\sin\theta)&\equiv2
infty | |
\sum | |
n=1 |
J2n-1(z)\sin\left[\left(2n-1\right)\theta\right]. \end{align}
Similarly useful expressions from the Sung Series:[4] [5]
\begin{align}
infty | |
\sum | |
\nu=-infty |
J\nu(x)&=1, \\
infty | |
\sum | |
\nu=-infty |
J2(x)&=1, \\
infty | |
\sum | |
\nu=-infty |
J3(x)&=
1 | \left[1+2\cos{ | |
3 |
x\sqrt{3 | |