On the integral $\int_{e}^{\infty}\frac{t^{1/2}}{\log^{1/2}\left(t\right)}\alpha^{-t/\log\left(t\right)}dt,\,\alpha>1.$

Solution 1:

A naif but probably efficient approach is to exploit the fact that the logarithm function is approximately constant on short intervals and $$ \frac{1}{\sqrt{N}}\int_{e^N}^{e^{N+1}}\sqrt{t}\,\alpha^{-t/N}\,dt =\frac{N\sqrt{\pi}}{2\log(\alpha)^{3/2}}\,\text{Erf}\left(\sqrt{\frac{e^N\log\alpha}{N}}\right)$$ can be efficiently approximated through the continued fraction for the error function.
We may also consider this fact: through the Laplace transform $$ \int_{0}^{+\infty}\sqrt{t}\exp\left(-\frac{t\log\alpha}{N}\right)\,dt = \int_{0}^{+\infty}\mathcal{L}^{-1}\left(\frac{1}{\sqrt{t}}\right)\,\mathcal{L}\left(t \exp\left(-\frac{t\log\alpha}{N}\right)\right)\,ds $$ we get the following integral: $$ \int_{0}^{+\infty}\frac{N^2}{\sqrt{\pi s}(Ns+\log\alpha)^2}\,ds =\frac{2}{\sqrt{\pi}}\int_{0}^{+\infty}\frac{1}{(s^2+\frac{\log\alpha}{N})^2}\,ds$$ that is simple to estimate in terms of $N$ and $\alpha$. The original integral is a weigthed sum of these integrals, that according to my computations should behave like $$\exp\left(-\log(\alpha)^{3/2}\right).$$ But I am probably over-complicating things, and we may recover the same bound by just applying a modified version of Laplace's method to the original integral.