Main Question:
What can we say about $f(x)=\prod_{n=2}^\infty(1-n^{-1/x})$?
Is $f(x)$ integrable from $0$ to $1$? Is it continuous? If we have an affirmative answer to the question on integrability...
$$I=\int_{0}^{1}f(x)\,dx=\int_{1}^{\infty}\frac{1}{x^2}\prod_{n=2}^{\infty}\left(1-\frac{1}{n^{x}}\right)dx$$
Can we get bounds on $I$? Can we get a closed form for I? Can we get a decent approximation for $I$?
Motivations
I saw this post wherein I found
$$ \prod_{n=2}^{\infty} \left(1 - \frac{1}{n^p}\right) = \prod_{\omega : \omega^p = 1} \frac{1}{\Gamma(2-\omega)}. $$
After plotting $f(x)$, I found myself unsatisfied when I couldn't get a handle on $I$ using desmos. Maybe the issue is that $f_m(x)=\prod_{n=2}^{m}(1-n^{-1/x})$ don't converge fast enough? As I run $m\to \infty$ I observe $I_m= \int_0^1 f_m(x)\,dx$ wiggling. I'm not quite sure how to proceed in my curiosities.
Thanks for any insights.
Can we get a decent approximation for I? - yeah, I think so.
The trapezoidal rule gives good results, because $f^{(n)}(0^+)=f^{(n)}(1^-)=0$ for each $n>0$.
Here are my computations, using the following PARI/GP script:
$$\small\begin{aligned} \color{blue}{0.}\color{gray}{5000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000}\\ \color{blue}{0.49}\color{gray}{52524522182130053179347592830935038182739178227155813430014853398627049802084168378189484744909907}\\ \color{blue}{0.4960}\color{gray}{462685813435659657410735621739971142678008217517627767029731808108723102454366861311477695706614}\\ \color{blue}{0.49600}\color{gray}{13263546360125317620145429003484306469288432684171247707533969912066396804032830035759621991914}\\ \color{blue}{0.4960022}\color{gray}{198625044032046958121794546131346992908777037660564955370118897334400210136224769456663842563}\\ \color{blue}{0.49600222206}\color{gray}{45758305327177461401946937544240845348719200390983304017261198780787928938707341701795960}\\ \color{blue}{0.496002222066503}\color{gray}{9435348385778735042737942407442787721881965817897194427569958858545529012872132030474}\\ \color{blue}{0.4960022220665038758722}\color{gray}{291597400222685547259341485206377189559616296300739040313598923621170596850242}\\ \color{blue}{0.496002222066503875872217752736}\color{gray}{8950707201277324066195674090515553311094699224292721471410927775290176}\\ \color{blue}{0.49600222206650387587221775273692568333606393}\color{gray}{08945109817369766264054491087707420065200842499692225784}\\ \color{blue}{0.496002222066503875872217752736925683336063939363714480500547}\color{gray}{9605585454983581866471891249689081986411}\\ \color{blue}{0.496002222066503875872217752736925683336063939363714480500547711451723047013043337657919}\color{gray}{1646691496229}\\ \color{blue}{0.4960022220665038758722177527369256833360639393637144805005477114517230470130433376579194899311327705}\end{aligned}$$