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
$$ \begin{align} & \sum_{i=1}^{n-1}\dfrac{\Gamma(i-d)\Gamma(n-i+d)}{\Gamma(i+1)\Gamma(n-i)(n-i-d)} \\ &= \dfrac{\Gamma(-d)\Gamma(n+d)}{(n-d)\Gamma(n)} \left(\dfrac{d\Gamma(2d)\Gamma(n)\Gamma(d-n+1)}{\Gamma(n+d)\Gamma(2d-n+1)} - 1\right), \\ &\sum_{i=1}^{n-1} \dfrac{\Gamma(n-d-i)\Gamma(i+d)}{(i-d)\Gamma(i+1)\Gamma(n-i)} \\ &=-\dfrac{\Gamma(d)\Gamma(n-d)}{d\Gamma(n)} \left(\ \dfrac{\Gamma(n)\Gamma(n-2d)\Gamma(1-d)^2}{\Gamma(1-2d)\Gamma(n-d)^2} -1\right). \end{align} $$