Just state the result here. $latex \displaystyle \exp(\vec{k}\cdot\vec{r} ) = \exp( \cos \theta ) = \sum_{l=0}^\infty (2l+1) i^l j_l(kr) P_l(\vec{k}\cdot\vec{r} ) $ where $latex j_l $ is spherical Bessel function, $latex P_l $ is the Legendre poly…
Just state the result here. where is spherical Bessel function, is the Legendre polynomial. Using the relation using the Riccati-Bessel Functions using Riccati-Hankel functions Long range behaviour: or
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