Spherical harmonics

The spherical harmonics $Y_{l}^{m}(\theta ,\phi )$ are the angular portion of the solution to Laplace's equation in spherical coordinates. The first few spherical harmonics are given by:

$Y_{0}^{0}(\theta ,\phi )={\frac {1}{2}}{\frac {1}{\sqrt {\pi }}}$

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle Y_{1}^{-1}(\theta ,\phi )={\frac {1}{2}}{\sqrt {\frac {3}{2\pi }}}\sin \theta e^{-i\phi }}

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle Y_{1}^{0}(\theta ,\phi )={\frac {1}{2}}{\sqrt {\frac {3}{\pi }}}\cos \theta }

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle Y_1^1 (\theta,\phi) = -\frac{1}{2} \sqrt{\frac{3}{2\pi}} \sin \theta e^{i\phi} }

See also

• M. E. Rose "Elementary theory of angular momentum", John Wiley & Sons (1967) Appendix III
• Spherical Harmonic -- from Wolfram MathWorld
• I. Nezbeda, J. Kolafa and S. Labík "The spherical harmonic expansion coefficients and multidimensional integrals in theories of liquids", Czechoslovak Journal of Physics 39 pp. 65-79 (1989)