Two series involving the Gamma function The last piece I am left with in my proof is to compute the following two series:
$$\sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)}, \sum_{i=1}^{n-1} \dfrac{\Gamma(n-d-i)\Gamma(i+d)}{(i-d)\Gamma(i+1)\Gamma(n-i)},$$
here $n\geq 2$, $d\in(-0.5, 0.5)$. According to Maple that would be
$$
\begin{align}
& \sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)}= \\ 
&=\dfrac{\Gamma(-d)}{2}\left[\dfrac{d\Gamma(-d)\Gamma(d)\Gamma(n-2d)\Gamma(n)-2\Gamma(n+d)\Gamma(n-d)\Gamma(-2d)}{(n-d)\Gamma(n)\Gamma(n-d)\Gamma(-2d)}\right] \\
&= \dfrac{d\Gamma(-d)^2\Gamma(d)\Gamma(n-2d)}{2\Gamma(n-d+1)\Gamma(-2d)}-\dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)}
\end{align}
$$
and
$$
\begin{align}
&\sum_{i=1}^{n-1} \dfrac{\Gamma(n-d-i)\Gamma(i+d)}{(i-d)\Gamma(i+1)\Gamma(n-i)}= \\ &=\dfrac{\Gamma(d)}{2}\dfrac{d\Gamma(-d)^2\Gamma(n-2d)\Gamma(n)+2\Gamma(n-d)^2\Gamma(-2d)}{d\Gamma(-2d)\Gamma(n-d)\Gamma(n)} \\
&= \dfrac{\Gamma(d)\Gamma(-d)^2\Gamma(n-2d)}{2\Gamma(-2d)\Gamma(n-d)} + \dfrac{\Gamma(n-d)\Gamma(d)}{d\Gamma(n)}.
\end{align}
$$
I have already simplified these series as much as possible and could not find any more elementary properties of the $\Gamma$ function that would make these expressions more convenient. Therefore, I thought I should use one of the definitions of the $\Gamma$ function. Also I believe it should be something that involves integrals or sums (rather than products) in order to change the order of summation and apply $\sum_{i=1}^{n-1}$ first. 
However, writing the first series as 
$$
\sum_{i=1}^{n-1}\dfrac{\int_0^\infty e^{-u}u^{i-d-1}du\int_0^\infty e^{-v}v^{n-i+d-1}dv}{(n-i-d)\int_0^\infty e^{-z}z^idz\int_0^\infty e^{-w}w^{n-i-1}dw\int_0^\infty e^{-r}r^{n-i-d-1}dr} = 
$$
$$
\sum_{i=1}^{n-1}\dfrac{\int^\infty_0 \int^\infty_0 e^{-u-v}u^{i-d-1}v^{n-i+d-1}dudv}{(n-i-d) \int^\infty_0 \int^\infty_0 \int^\infty_0 e^{-z-w-r}z^{i}w^{n-i-1}r^{n-i-d-1}dzdwdr}
$$
does not help at all because of denominator. 
I also tried to rewrite it (both the series and the desired result) using the Beta function:
$$
\begin{align}
\sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)} &= \sum_{i=1}^{n-1}\dfrac{B(d+1,i-d)B(n-i+d,1-d)B(n-i-d,1) (i-n)}{\Gamma(1+d)\Gamma(-d)d}\\ 
&= \dfrac{B(-d,-d)B(n-2d,d)B(n-i-d,1)  + 2B(-d,n+d)}{2(n-d)}
\end{align}
$$
and to use a couple of definitions:
$$
    B(x,y) = 2\int_0^{\pi/2}(\sin\theta)^{2x-1}(\cos\theta)^{2y-1}\,d\theta, \qquad \mathrm{Re}(x)>0,\ \mathrm{Re}(y)>0,
$$
$$
    B(x,y) = \int_0^\infty\dfrac{t^{x-1}}{(1+t)^{x+y}}\,dt, \qquad \mathrm{Re}(x)>0,\ \mathrm{Re}(y)>0.
$$
However, even though they allowed me to use geometric progression, resulting expressions were too cumbersome (or should I try harder?). Even if this is a correct way, I cannot see how to go from a triple integral (geometric progression, cumbersome expression) to a triple + single integral, i.e. 
$$
\dfrac{B(-d,-d)B(n-2d,d)B(n-i-d,1)  + 2B(-d,n+d)}{2(n-d)}
$$
(here I ignore requirements $\mathrm{Re}(x)>0$, $\mathrm{Re}(y)>0$, which can be easily satisfied).
In case all this is not terribly difficult I would like only a hint first.

This does not really help, but since there seems to be some particular way to evaluate this kind of series I tried to take some simpler one first and just got annoyed by such an elegant answer (the one I got from Maple, of course):
$$\sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)i}{\Gamma(i+1)\Gamma(n-i)}=\Gamma(1-d)\Gamma(1+d)(n-1)=\dfrac{d(1-n)\pi}{\sin(\pi(1+d))}$$
(comparing with the very first series above $\frac{1}{n-d-i}$ here is just replaced with $i$).

Edit:
the desired results also can be rewritten to
$$
\begin{align}
& \sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)} \\ 
&= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} \left(\dfrac{d\Gamma(2d)\Gamma(n)\Gamma(d-n+1)}{\Gamma(n+d)\Gamma(2d-n+1)} - 1\right), \\
&\sum_{i=1}^{n-1} \dfrac{\Gamma(n-d-i)\Gamma(i+d)}{(i-d)\Gamma(i+1)\Gamma(n-i)} \\ 
&=-\dfrac{\Gamma(d)\Gamma(n-d)}{d\Gamma(n)} \left(\ \dfrac{\Gamma(n)\Gamma(n-2d)\Gamma(1-d)^2}{\Gamma(1-2d)\Gamma(n-d)^2} -1\right).
\end{align}
$$
 A: We can use the Generalized Hypergeometric function
\begin{equation*}
    \,{}_pF_q(a_1,\ldots,a_p;b_1,\ldots,b_q;z) = \sum_{n=0}^\infty \frac{(a_1)_n\dots(a_p)_n}{(b_1)_n\dots(b_q)_n} \, \frac {z^n} {n!},
\end{equation*}
with Pochhammer symbol defined by
\begin{align*} (a)_0 &= 1, \\ (a)_n &= a(a+1)(a+2)...(a+n-1)=\dfrac{\Gamma(a+n)}{\Gamma(a)}, && n \geq 1, \end{align*}
and evaluate the first series in the following way:
\begin{align*}
&\sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)} \\
&= \dfrac{\Gamma(1-d)\Gamma(n-1+d)}{\Gamma(n-1)(n-1-d)} {}_4F_3(1, 1 - d, 2 - n, 1 + d - n; 2, 2 + d - n, 2 - d - n; 1)) \\
&= \dfrac{\Gamma(1-d)\Gamma(n-1+d)}{\Gamma(n-1)(n-1-d)} \sum_{m=0}^\infty \dfrac{(1)_m(1-d)_m(2-n)_m(1+d-n)_m}{(2)_m(2+d-n)_m(2-d-n)_m}\dfrac{1}{m!} \\
&= \dfrac{\Gamma(1-d)\Gamma(n-1+d)}{\Gamma(n-1)(n-1-d)} \sum_{m=0}^\infty \dfrac{(1-d)_m(2-n)_m(1+d-n)_m}{(m+1)(2+d-n)_m(2-d-n)_m}\dfrac{1}{m!} \\
&= \dfrac{\Gamma(1-d)\Gamma(n-1+d)}{\Gamma(n-1)(n-1-d)} \sum_{m=0}^\infty \dfrac{(1-d)_m(2-n)_m(1+d-n)_m}{(2+d-n)_m(2-d-n)_m}\dfrac{1}{(m+1)!} \\
&= \dfrac{\Gamma(1-d)\Gamma(n-1+d)}{\Gamma(n-1)(n-1-d)} \dfrac{(1+d-n)(1-n-d)}{-d(1-n)(d-n)}\sum_{m=0}^\infty \dfrac{(-d)_{m+1}(1-n)_{m+1}(d-n)_{m+1}}{(1+d-n)_{m+1}(1-d-n)_{m+1}}\dfrac{1}{(m+1)!} \\
&= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} ({}_3F_2(-d,1-n,d-n;-d-n+1,d-n+1;1)-1) \\
&= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} \left(\dfrac{(2d-n+1)_{n-1}(1)_{n-1}}{(d-n+1)_{n-1}(d+1)_{n-1}}-1\right) \\
&= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} \left(\dfrac{\Gamma(2d)\Gamma(n)\Gamma(d-n+1)\Gamma(d+1)}{\Gamma(d)\Gamma(n+d)\Gamma(2d-n+1)} - 1\right)\\
&= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} \left(\dfrac{d\Gamma(2d)\Gamma(n)\Gamma(d-n+1)}{\Gamma(n+d)\Gamma(2d-n+1)} - 1\right),\\
\end{align*}
here we used Saalschütz's theorem:
\begin{equation*}
    {}_3F_2 (a,b, -n;c, 1+a+b-c-n;1)= \frac{(c-a)_n(c-b)_n}{(c)_n(c-a-b)_n}. 
\end{equation*}
In the same way we evaluate the second series:
\begin{align*}
&\sum_{i=1}^{n-1} \dfrac{\Gamma(n-d-i)\Gamma(i+d)}{(i-d)\Gamma(i+1)\Gamma(n-i)} \\
&= \dfrac{\Gamma(1+d)\Gamma(n-d-1)}{\Gamma(n-1)(1-d)} {}_4F_3(1, 1-d, 2-n, 1+d; 2, 2-d, d-n+2; 1)) \\
&= \dfrac{\Gamma(1+d)\Gamma(n-d-1)}{\Gamma(n-1)(1-d)} \dfrac{(1-d)(d-n+1)}{d^2(n-1)}({}_3F_2(-d,d,1-n;1-d,d-n+1,1)-1) \\
&= -\dfrac{\Gamma(d)\Gamma(n-d)}{d\Gamma(n)} \left(\ \dfrac{(1)_{n-1}(1-2d)_{n-1}}{((1-d)_{n-1})^2} -1\right) \\
&= -\dfrac{\Gamma(d)\Gamma(n-d)}{d\Gamma(n)} \left(\ \dfrac{\Gamma(n)\Gamma(n-2d)\Gamma(1-d)^2}{\Gamma(1-2d)\Gamma(n-d)^2} -1\right). \\
\end{align*}
A: I'm not sure how useful this hint will be, but here it is:
$$\text{Since we know that}\;\;\Gamma(s+1)=s\Gamma (s)\;,\;\;\text{we get that}$$
$$\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)}=\frac{\color{red}{\Gamma(i-d)}\cdot\prod_{k=1}^d(n-i+d-k)\color{green}{\Gamma(n-i)}}{\prod_{k=0}^d(k-d)\cdot\color{red}{\Gamma(i-d)}\color{green}{\Gamma(n-i)}\Gamma(n-i-d)}$$
