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fixing latex rendering
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bonevbs committed Oct 24, 2023
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### Spherical harmonics

The [spherical harmonics](https://en.wikipedia.org/wiki/Spherical_harmonics) are special functions defined on the two-dimensional sphere $S^2$ (embedded in three dimensions). They form an orthonormal basis of the space of square-integrable functions defined on the sphere ($L^2(S^2)$) and are comparable to the harmonic functions defined on a circle/torus. The spherical harmonics are defined as
The [spherical harmonics](https://en.wikipedia.org/wiki/Spherical_harmonics) are special functions defined on the two-dimensional sphere $S^2$ (embedded in three dimensions). They form an orthonormal basis of the space of square-integrable functions defined on the sphere $L^2(S^2)$ and are comparable to the harmonic functions defined on a circle/torus. The spherical harmonics are defined as

$$
Y_l^m(\theta, \lambda) = \sqrt{\frac{(2l + 1)}{4 \pi} \frac{(l - m)!}{(l + m)!}} \, P_l^m(\cos \theta) \, \exp(im\lambda),
Y_l^m(\theta, \lambda) = \sqrt{\frac{(2l + 1)}{4 \pi} \frac{(l - m)!}{(l + m)!}} P_l^m(\cos \theta) \exp(im\lambda),
$$

where $\theta$ and $\lambda$ are colatitude and longitude respectively, and $P_l^m$ the normalized, [associated Legendre polynomials](https://en.wikipedia.org/wiki/Associated_Legendre_polynomials).
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in longitude and a Legendre transform

$$
\hat{f}_l^m = \frac{1}{2} \int_{0}^\pi \hat{f}^m(\theta) \, \overline{P_l^m} (\cos \theta) \, \sin \theta \;\mathrm{d} \theta
\hat{f}_l^m = \frac{1}{2} \int_{0}^\pi \hat{f}^m(\theta) \, \overline{P_l^m} (\cos \theta) \, \sin \theta \; \mathrm{d} \theta
$$

in latitude.
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