I came across the following integral \begin{equation} \int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} \, , \end{equation} where in the above $P_{\ell}(x)$ is the Legendre polynomial, and $(x)_a$ is the Pochhammer symbol, $(x)_a = \tfrac{\Gamma(x+a)}{\Gamma(x)}$. $\ell$ is a non-negative integer number and $n$ is an integer bigger or equal to $-1$.
After running it for some values in Mathematica
it is easy to observe that it vanishes when
- $n+\ell$ is any even number,
- $\ell \geq n+2$.
The command that defines the integral is
int[n_, l_] :=
Integrate[
LegendreP[l, 1 - (2 t)/(n + 4)] Pochhammer[-t + 2, n + 1], {t, 0,
n + 4}]
and then two examples for $n=-1$ and $n=0$
Table[int[-1, l], {l, 0, 5}] // FunctionExpand
Table[int[0, l], {l, 0, 5}] // FunctionExpand
and of course, more values can be checked in a straightforward manner.
I managed to prove that the integral yields $0$ when $n+\ell$ is equal to any even number, however, I have not managed to derive a proof that the integral vanishes for $\ell \geq n+2$.
I was wondering if there are any suggestions on how to prove that the integral, also, vanishes for $\ell \geq n+2$.
The proof I managed that shows the integral being equal to $0$ when $n + \ell$ is any even number is as follows:
- make the substitution \begin{equation*} t = -t^{\prime}+n+4 \, , \end{equation*}
- use the identity $P_{\ell}(-x) = (-1)^{\ell}P_{\ell}(x)$ in order to re-write \begin{equation} P_{\ell}\left(-1 + \frac{2t^{\prime}}{n+4}\right) = P_{\ell}\left(- \left(1 - \frac{2t^{\prime}}{n+4}\right) \right) = (-1)^{\ell} P_{\ell}\left(1 - \frac{2t^{\prime}}{n+4}\right) \end{equation}
- we can use $(-x)_m = (-1)^m (x-m+1)_m$ in order to re-express the Pochhammer as \begin{equation} (2+t^{\prime}-n-4)_{n+1} = (-2 + t^{\prime} -n)_{n+1} = (-1)^{n+1} (-t^{\prime}+2)_{n+1} \end{equation}
Having all the above, we can express the original integral in terms of the $t^{\prime}$ variable in the following manner:
\begin{equation}
\int^0_{n+4} - dt^{\prime} (-1)^{\ell} P_{\ell}\left(1 - \frac{2t^{\prime}}{n+4}\right) (-1)^{n+1} (-t^{\prime}+2)_{n+1}
\end{equation}
and we can now swap the integration limits in the above to get
\begin{equation}
(-1)^{1+n+\ell} \int^{n+4}_0 dt^{\prime} P_{\ell}\left(1 - \frac{2t^{\prime}}{n+4}\right)
(-t^{\prime}+2)_{n+1}
\, .
\end{equation}
In the above we rename $t^{\prime} \rightarrow t$ and get
\begin{equation}\label{eq: integral_aux_02}
(-1)^{1+n+\ell} \int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} \, .
\end{equation}
So, what we have obtained so far is the following:
\begin{equation}
\begin{aligned}
&\int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} = \\
(-1)^{1+n+\ell} &\int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right) (-t+2)_{n+1} \Rightarrow
\\
\left(1 - (-1)^{1+n+\ell} \right) &\int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} = 0 \Rightarrow
\\
\left(1 + (-1)^{n+\ell} \right) &\int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} = 0
\, ,
\end{aligned}
\end{equation}
but for $n+\ell$ an even number $\left(1 + (-1)^{n+\ell} \right) =2$ and hence
\begin{equation}
\int^{n+4}_0 dt P_{\ell}\left(1 - \frac{2t}{n+4}\right)(-t+2)_{n+1} = 0
\, .
\end{equation}
Mathematica
can return the correct values, see here. Thanks for helping me clarify this! – Sep 01 '23 at 16:17