Central Beta function Β(x). Imagine we wanted to find a series expansion for $\left(x^2\,B(x,x)\right)^\frac nx, n\in\Bbb N $ which would be particularly difficult because it uses the Beta function. Let there be the rule that any strategies can be used to find a series expansion for $0\le x\le 1$ as long as the series terms are not too complicated and have some pattern. Here is how I would do it using a Taylor expansion at x=a which all give beautiful results. One simple and amazing expansion would be at x=0, but to include all cases, I will use x=a as all cases for $0\lt a\le 1$ have the radius of convergence which works for $0\lt x\le 1$:
$$\left(x^2\,B(x)\right)^\frac nx=\left(x^2\,B(x,x)\right)^\frac nx =\frac{x!^\frac{2n}{x}}{Γ(2x)^\frac nx}=Γ^{-\frac nx}(2x)\sum_{n=0}^\infty \frac{\left(\frac{d^n}{dx^n}x!^\frac {2n}x\right)_{x=a}(x-a)^n}{n!}$$
Here comes the problem where I am unsure about the radius of convergence for the usual Taylor series of $Γ(2x) ^{-\frac nx}$. The problem is this steep change due to the x in the denominator of $\left(\frac{(2x)!}{2x}\right)^{-\frac nx}$. If it was the factorial instead of the gamma, there would not be such a small derivative at $x≈0$ which would imply the series representation working. For example here is the graph of $\frac{1}{Γ(2x)^\frac 1x}$ for $n=1$:
This all relates to the series of $x^\frac 1x$ of which I still do not know the convergence for. It amazingly has an explicit form for the Taylor Series at $x=1$ at OEIS A008405. How can I do the rest or have a new series?
It does not have to be a Taylor Series.
Please correct me and give me feedback!

$\textstyle\displaystyle{\frac{1}{\Gamma(x)}=x\prod_{k=1}^{\infty}\frac{1+\frac{x}{n}}{\left(1+\frac{1}{n}\right)^x}}$
$\implies\textstyle\displaystyle{x^2\Gamma^2(x)=\prod_{k=1}^{\infty}\frac{\left(1+\frac{1}{n}\right)^{2x}}{\left(1+\frac{x}{n}\right)^2}}$
Using the same formula we can get,
$\textstyle\displaystyle{\frac{1}{\Gamma(2x)}=2x\prod_{k=1}^{\infty}\frac{1+\frac{2x}{n}}{\left(1+\frac{1}{n}\right)^{2x}}}$
Finally their ratio would be
$\textstyle\displaystyle{\frac{x^2\Gamma^2(x)}{\Gamma(2x)}}$
$=x^2B(x,x)$
$\textstyle\displaystyle{=2x\prod_{k=1}^{\infty}\frac{1+\frac{2x}{n}}{\left(1+\frac{x}{n}\right)^2}}$
$\textstyle\displaystyle{\implies\frac{n}{x}\ln(x^2B(x,x))=\frac{n\ln(2x)}{x}+\frac{n}{x}\sum_{k=1}^{\infty}\ln\left(\frac{n(n+2x)}{(n+x)^2}\right)}$
Obviously this not the infinite sum for the function you wanted but rather the log of it. So I would call this a partial answer.
Edit:
Technically you can find the series representation of the function using what I derived previously, but it would produce a messy double summation-
If we take $e$ to be the base on both sides then the $LHS$ would be $(x^2B(x,x))^\frac{n}{x}$ and the $RHS$ would be (using the series representation of $e^x$)-
$\textstyle\displaystyle{(x^2B(x))^\frac{n}{x}=\sum_{j=0}^{\infty}\frac{1}{j!}\left(\frac{n\ln(2x)}{x}+\frac{n}{x}\sum_{k=1}^{\infty}\ln\left(\frac{n(n+2x)}{(n+x)^2}\right)\right)^j}$
And for the series representation of $\textstyle\displaystyle{\Gamma(2x)^{-\frac{n}{x}}}$, I will do a similar thing, this time I am going to use weierstrass' formula for the gamma function-
So, $\Gamma(2x)^{-\frac{n}{x}}=e^{-\frac{n}{x}\ln(\Gamma(2x))}$
$\textstyle\displaystyle{=\sum_{k=0}^{\infty}\frac{1}{k!}\left(-\frac{n}{x}\ln(\Gamma(2x))\right)^k}$
$\textstyle\displaystyle{=\sum_{k=0}^{\infty}\frac{(-1)^kn^k}{k!x^k}\ln^k\left(\frac{1}{2xe^{2{\gamma}x}}\prod_{j=1}^{\infty}\frac{e^\frac{2x}{j}}{1+\frac{2x}{j}}\right)}$
$\textstyle\displaystyle{=\sum_{k=1}^{\infty}\frac{(-1)^kn^k}{k!x^k}\left(-\ln(2x)-2\gamma x+\sum_{j=1}^{\infty}\left(\frac{2x}{j}-\ln\left(1+\frac{2x}{j}\right)\right)\right)^k}$
If I am able to do better than this, then I would add it to the answer.