I recently came across the series
$$G(t):=\sum_{n=0}^\infty\frac{t^{n}}{B(n+1,\xi+1)}$$ defined for $t\in(0,1)$ and $\xi+1>0$. I am trying to get a better-looking form for this sum, something more "usable" in general, but I don't know how to handle the beta function. I am pretty sure that this is the power series for $g(t)=\frac{1}{(1-t)^{2+\xi}}$, but I can't prove it. Right now I have only noticed that for $\xi=0$ we get $G(t)=\sum_{n\geq0}(n+1)t^{n}=\frac{1}{(1-t)^2}$, the derivative of the geometric series. Any ideas on how to deal with this sum?
Both of the other answers are nice, but I think this is what I was looking for, so I'm answering my question:
It can be easily shown with induction that $$B(n+1,\xi+1)=\frac{n!}{(\xi+1)\cdots(\xi+n+1)}$$ for all $n$. All it takes is an integration by parts on the formula of the Beta function:
Now we consider the function $\psi(t)=(\xi+1)(1-t)^{-(\xi+2)}$. Again, by induction it is easily proved that $$\psi^{(n)}(t)=(\xi+1)\cdots(\xi+n+1)(1-t)^{-(\xi+n+2)}$$ So $\psi^{(n)}(0)/n!=1/B(n+1,\xi+1)$. This shows that our series is exactly the power series for $\psi(t)$, i.e. $$G(t)=\sum_{n=0}^\infty\frac{\psi^{(n)}(0)}{n!}t^n=\psi(t)=\frac{\xi+1}{(1-t)^{\xi+2}} $$