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In today's exercises, we complete the tasks from yesterday, which unfortunately had ambiguous and confusing instructions!
Recall that the HO wavefunctions are given by \begin{equation} R_{nl}(r) = \frac{A_{nl}}{b^{3/2}}x^le^{-x^2/2}L_{n}^{l+1/2}(x^2)\,, \end{equation}
where the oscillator length $b\equiv \sqrt{\hbar/(m\omega)}$, and the dimensionless variable $x\equiv r/b$. The normalization constant is given by
\begin{equation} A_{nl}=\sqrt{\frac{2^{n+l+2}n!}{\pi^{1/2}(2n+2l+1)!!}} \end{equation}