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Plane wave expansion : ウィキペディア英語版
Plane wave expansion
In physics, the plane wave expansion expresses a plane wave as a sum of spherical waves,
: e^ = \sum_^\infty (2 \ell + 1) i^\ell j_\ell(k r) P_\ell(\hat \cdot \hat),
where
* is the imaginary unit,
* is a wave vector of length ,
* is a position vector of length ,
* are spherical Bessel functions,
* are Legendre polynomials, and
* the hat denotes the unit vector.
In the special case where is aligned with the z-axis,
: e^ = \sum_^\infty (2 \ell + 1) i^\ell j_\ell(k r) P_\ell(\cos \theta),
where is the spherical polar angle of .
== Expansion in spherical harmonics ==

With the spherical harmonic addition theorem the equation can be rewritten as
: e^} = 4 \pi \sum_^\infty \sum_^\ell i^\ell j_\ell(k r) Y_\ell^m),
where
* are the spherical harmonics and
* the superscript denotes complex conjugation.
Note that the complex conjugation can be interchanged between the two spherical harmonics due to symmetry.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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