A few tricky integrals.... Or are they?

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The discussion focuses on evaluating Vardi-type integrals, specifically the integrals of the form \(\int_{\pi/4}^{\pi/2}\log^n[\log(\tan x)]\,dx\) for \(n = 2\) and \(n = 3\). The results are expressed in terms of the Dirichlet Beta function \(\beta(x)\) and the Gamma function, with specific evaluations leading to expressions involving \(\beta''(1)\), \(\beta'''(1)\), and constants like \(\gamma\) and \(\zeta(3)\). The method involves differentiating under the integral sign and using complex analysis techniques to evaluate the integrals.

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Here are a few Vardi-type integrals I recently posted on another forum (some of you might have seen them)...Assuming the following classic result - due to Vardi - holds...\int_{\pi/4}^{\pi/2}\log\log(\tan x)\,dx=\frac{\pi}{2}\log\left[\sqrt{2\pi}\frac{\Gamma(3/4)}{\Gamma(1/4)}\right]Prove that:
\int_{\pi/4}^{\pi/2}\log^2[\log(\tan x)]\,dx=

\beta''(1)+\frac{\pi^3}{24}-\frac{\pi\gamma^2}{4}-\pi\gamma\log\left[\sqrt{2\pi}\frac{\Gamma(3/4)}{\Gamma(1/4)}\right]and...\int_{\pi/4}^{\pi/2}\log^3[\log(\tan x)]\,dx=

\beta'''(1)-3\gamma\,\beta''(1)+\frac{\pi\gamma^3}{2}-\frac{\pi}{2}\zeta(3) + \left(\frac{\pi^3}{4}+\frac{3\pi\gamma^2}{2}\right)\log\left[\sqrt{2\pi}\frac{\Gamma(3/4)}{\Gamma(1/4)}\right]
Where $$\beta(x)\,$$ is the Dirichlet Beta function, defined by:$$\beta(x)=\sum_{k=0}^{\infty}\frac{(-1)^k}{(2k+1)^x}$$
 
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I saw your other post, so I'm not going to say much.

But here's a brief outline of a way to evaluate Vardi's integral.Let $ \displaystyle I(a) = \int_{0}^{\infty}\frac{\ln(a^{2}+x^{2})}{\cosh x} \ dx $ and differentiate inside of the integral to get $ \displaystyle I'(a) = \int_{0}^{\infty} \frac{2a}{(a^{2}+x^{2}) \cosh x} \ dx $.

$I'(a)$ can be evaluated be letting $ \displaystyle f(z) = \frac{2a}{(a^{2}+z^{2}) \cosh z}$ and integrating around a rectangle or circle in the upper-half complex plane.

After somewhat tedious calculations, you''ll find that $ \displaystyle I'(a) = \Big[ \psi \Big(\frac{3}{4} + \frac{a}{2 \pi} \Big) - \psi \Big(\frac{1}{4} + \frac{a}{2 \pi} \Big) \Big]$

Then integrate back with respect to $a$.

Finding the constant of integration is tricky. It involves rewriting the integral and letting $a$ go to $\infty$.

But it will turn out that $ \displaystyle I(a) = 2 \pi \ln \Bigg[ \sqrt{2 \pi} \frac{\Gamma(\frac{3}{4} + \frac{a}{2 \pi})}{\Gamma(\frac{1}{4} + \frac{a}{2 \pi})} \Bigg] $

Then $ \displaystyle \lim_{a \to 0^{+}} I(a) = 2 \int_{0}^{\infty} \frac{\ln x}{\cosh x} \ dx = 2 \pi \ln \Bigg[ \sqrt{2 \pi} \frac{\Gamma(\frac{3}{4})}{\Gamma(\frac{1}{4})} \Bigg] $

Finally make the change of variables $x = \ln (\tan u) $.
 
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Very nice, RV! (Rock)
 
No worries if not, but just in case anyone's interested, here's a little hint to get you started in the right direction...

(Bandit)
Consider the integral:$$\int_0^{\infty}\frac{x^{q-1}}{\cosh x}\,dx$$for the real parameter $$q\in\mathbb{R}^+$$
 

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