To give you context, I am currently attempting to derive the radial wavefunctions for a hydrogenic atom, from scratch. B.H. Bransden, C.J. Joachain - Physics of Atoms and Molecules states:
$$U_{p}(\rho, s) = \frac{(-s)^{p} e^{-\rho s /(1-s)}}{(1-s)^{p+1}} = \sum^{\infty}_{q=p} \frac{L^{p}_{q}(\rho)}{q!} s^q ; |s|<1$$ An explicit expression for $L_{n+l}^{2l+1} (\rho)$ is given by $$L_{n+l}^{2l+1} (\rho) = \sum^{n-l-1}_{k=0} (-1)^{k+1} \frac{[(n+l)!]^{2} \rho^{k}}{(n-l-1-k)! (2l+1+k)! k!} $$ and is easily verified by substitution into the above with $q = n + l$ and $p=2l+1$.
I am stuck on how to verify this by substitution. Perhaps this is a naive approach but here is what I have attempted so far:
$$ U_{p}(\rho, s) = \sum^{\infty}_{n-l-1=0} \frac{L_{n+l}^{2l+1}(\rho)}{(n+l)!} s^{n+l} $$ Any tips on how to progress would be very helpful.
Ultimately, I would also like to obtain $L^{2l+1}_{n-l-1}({\rho})$.
I found this question that is somewhat related to mine, but I would like to use the expressions provided in Joachim and Bransden for the moment.
Edit: Since I asked the question, I have also attempted the following: I first plugged in the taylor expansion of $e^{\rho s/(1-s)}$ and the binomial expansion of $(1-s)^{p+1}$ into the expression, giving:
$$ \sum^{2l+1}_{b=0} \sum^{\infty}_{a=0} \frac{(-s)^{2l+1-b+a} \rho^a b! (2l+1-b)!}{a!(2l+1)!(1-s)^a} $$
Then I tried to shift the summation index from $2l+1$ to $n-l-1$, introducing a new variable $k = b + (n-3l-2)$ but I am not sure what to do from this point. I also set $ a = n-l-1 $.