I find that the graph of $f(x)=\Gamma(x)^{1/x}$ or $(x!)^{1/x}$ is nearly a line when $x$ is large enough. And when $x$ gets larger, $f'$ will come to a limit. For example:
x f'(x)
1 -0.577216
2 0.211392
3 0.290511
4 0.316217
... ...
10 0.349503
20 0.358720
... ...
1000 0.367695
2000 0.367787
... ...
9000 0.367859
(calculated using SymPy)
The answer given by WolframAlpha is $1/e$. It is amazing, and why is it?
PS. $f'(x)=(\mathrm{polygamma}(0,x)/x-\ln(\Gamma(x))/x^2)*\Gamma(x)^{1/x}$

It is shown in https://doi.org/10.1007/s00013-010-0146-9 that $$ \Gamma (x) \sim \left( {\frac{x}{e}\left( {1 + \frac{1}{{12x^2 }} + \cdots } \right)} \right)^x \sqrt {\frac{{2\pi }}{x}} $$ for large positive $x$. Combining this with $$ \sqrt[x]{{\sqrt {\frac{{2\pi }}{x}} }} = \exp \left( {\frac{1}{{2x}}\log \left( {\frac{{2\pi }}{x}} \right)} \right) = 1 + \frac{1}{{2x}}\log \left( {\frac{{2\pi }}{x}} \right) + \frac{1}{{8x^2 }}\log ^2 \left( {\frac{{2\pi }}{x}} \right) + \cdots $$ we find $$ (\Gamma (x))^{1/x} \sim \frac{x}{e}\left( {1 + \frac{{\log (2\pi /x)}}{{2x}} + \frac{{3\log ^2 (2\pi /x) + 2}}{{24x^2 }} + \cdots } \right) $$ as $x\to +\infty$. You can see that, at leading order, $$ \frac{d}{{dx}}(\Gamma (x))^{1/x} \sim \frac{d}{{dx}}\frac{x}{e} = \frac{1}{e}. $$