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Spherical Harmonics

This table gives low-order spherical harmonics in the common physics convention.

The harmonics use the Condon–Shortley phase and are normalized by

∫02π∫0πYℓm∗(θ,ϕ)Yℓ′m′(θ,ϕ)sin⁡θ dθ dϕ=δℓℓ′δmm′.\int_0^{2\pi}\int_0^\pi Y_{\ell m}^*(\theta,\phi)Y_{\ell' m'}(\theta,\phi) \sin\theta\,d\theta\,d\phi =\delta_{\ell\ell'}\delta_{mm'}.

They obey

Yℓ,−m=(−1)mYℓm∗.Y_{\ell,-m}=(-1)^mY_{\ell m}^*.
HarmonicFormula
Y00Y_{00}14π\frac{1}{\sqrt{4\pi}}
Y10Y_{10}34πcos⁡θ\sqrt{\frac{3}{4\pi}}\cos\theta
Y1,±1Y_{1,\pm1}∓38πsin⁡θ e±iϕ\mp\sqrt{\frac{3}{8\pi}}\sin\theta\,e^{\pm i\phi}
Y20Y_{20}516π(3cos⁡2θ−1)\sqrt{\frac{5}{16\pi}}(3\cos^2\theta-1)
Y2,±1Y_{2,\pm1}∓158πsin⁡θcos⁡θ e±iϕ\mp\sqrt{\frac{15}{8\pi}}\sin\theta\cos\theta\,e^{\pm i\phi}
Y2,±2Y_{2,\pm2}1532πsin⁡2θ e±2iϕ\sqrt{\frac{15}{32\pi}}\sin^2\theta\,e^{\pm2i\phi}
OperatorEigenvalue Equation
L2L^2L2Yℓm=ℏ2ℓ(ℓ+1)YℓmL^2Y_{\ell m}=\hbar^2\ell(\ell+1)Y_{\ell m}
LzL_zLzYℓm=ℏmYℓmL_zY_{\ell m}=\hbar mY_{\ell m}
  • Dropping the Condon–Shortley phase and then comparing signs across sources.
  • Forgetting the angular measure sin⁡θ dθ dϕ\sin\theta\,d\theta\,d\phi.
  • Confusing YℓmY_{\ell m} with real tesseral harmonics used in chemistry.
  • Treating angular normalization as radial normalization.
  • A. R. Edmonds, Angular Momentum in Quantum Mechanics, Princeton University Press, 1957.
  • G. B. Arfken, H. J. Weber, and F. E. Harris, Mathematical Methods for Physicists, 7th ed., Academic Press, 2013.
  • D. A. Varshalovich, A. N. Moskalev, and V. K. Khersonskii, Quantum Theory of Angular Momentum, World Scientific, 1988.