My question concerns the behavior of the incomplete Beta function
$$B_{1/2}(y+1,y)=\int_0^{1/2}x^y (1-x)^{y-1}dx$$
in the large $y$ limit. I have been looking everywhere, but I can't find anything. I was thinking that I can get a good approximation by letting $(1-x)^{y-1}\approx x^y$, thus yielding a solution of the form $\approx 1/(2^{2y+1})$. However, is there any reference that talks about the above function in the large argument limit?
This is straightforward steepest descent (or Laplace's method). Let $f(x):=\ln(x)+\ln(1-x),$ and $g(x)=(1-x)^{-1}$ so that the integral becomes:
$$\int_0^{1/2}g(x)e^{yf(x)}dx.$$
On $[0,1/2]$, $f$ achieves its maximum at $x_0=1/2$. Furthermore, $f''(x)=-1/x^2-1/(1-x)^2$, and $f''(x_0)<0$.
Then Laplace's method gives:
$$\int_0^{1/2}g(x)e^{yf(x)}dx\sim \sqrt{\frac{2\pi}{y\,|f''(x_0)|}}\,g(x_0)\,e^{yf(x_0)}$$ in the sense that the ratio of the LHS and RHS converges to $1$ when $y\to+\infty$.
Can you wrap it up from here? Note the extra $1/\sqrt{y}$ that's going to contribute.