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

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Discussion Overview

The discussion revolves around evaluating certain integrals related to Vardi's results, specifically integrals involving logarithmic functions of the tangent function. The scope includes mathematical reasoning and exploration of advanced integral calculus techniques.

Discussion Character

  • Exploratory, Technical explanation, Mathematical reasoning

Main Points Raised

  • One participant presents a classic result attributed to Vardi involving the integral of the logarithm of the logarithm of the tangent function and proposes further evaluations of related integrals.
  • Another participant outlines a method to evaluate Vardi's integral by defining a function and differentiating under the integral sign, leading to a complex analysis approach.
  • The second participant notes the challenge of finding the constant of integration and suggests a limit process to evaluate the integral at a specific point.
  • A third participant expresses appreciation for the outlined method, indicating engagement with the technical details presented.
  • A fourth participant offers a hint to assist others in the discussion, suggesting a collaborative atmosphere.

Areas of Agreement / Disagreement

Participants appear to engage with the topic constructively, but no consensus is reached on the evaluations or methods proposed, as differing approaches and ideas are presented without resolution.

Contextual Notes

The discussion involves complex integrals and advanced mathematical functions, with potential limitations in assumptions regarding convergence and the behavior of the integrals at specific limits.

DreamWeaver
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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) $.
 
Last edited:
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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