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$\displaystyle \int_{0}^{\frac{\pi}{2}} \ln(\sin(x))dx=-\frac{\pi}{2}\ln(2)$ is an integral that is common.

But, how can we show $\displaystyle\int_{0}^{\frac{\pi}{2}}\ln^{2}(\sin(x))dx=\frac{{\pi}^{3}}{24}+\frac{\pi}{2}\ln^{2}(2)$?.

Does anyone have any ideas on how to approach $\displaystyle\int_{0}^{\frac{\pi}{2}}\ln^{2}(\sin(x))dx$?.

Thank you very much.

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  • $\begingroup$ wolframalpha.com/input/… $\endgroup$ Commented Aug 20, 2011 at 14:30
  • $\begingroup$ The elementary calculations in the answers are not complete, because the justifications of interchanging of integration and differentiation, interchanging double sums are easy but non-trivial. At least some words about it, details can be left to the reader :-) $\endgroup$
    – vesszabo
    Commented Aug 29, 2012 at 16:26
  • $\begingroup$ I uploaded my proof $\endgroup$ Commented Nov 17, 2023 at 13:45
  • $\begingroup$ For future reference, this question is also addressed here and here (with a slight variation). $\endgroup$ Commented Mar 5 at 8:20

8 Answers 8

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Here is a completely different way to approach this integral, which relies on some elementary complex analysis (Cauchy's theorem). It is based on an approach which I have seen several times employed to compute $\int_0^{\pi/2}\log{(\sin{x})}\,dx$ (particularly, in Ahlfors's book).


The idea is to integrate the principal branch of $f(z) := \log^2{(1 - e^{2iz})} = \log^2{(-2ie^{iz}\sin{z})}$ over the contour below, and then let $R \to \infty$ and $\epsilon \to 0$.
Contour

First of all, $1 - e^{2iz} \leq 0$ only when $z = k\pi + iy$, where $k$ is integral and $y \leq 0$. Thus, in the region of the plane which is obtained by omitting the lines $\{k\pi + iy: y\leq 0\}$ for $k \in \mathbb Z$, the principal branch of $\log{(1-e^{2iz})}$ is defined and analytic. Note that, for each fixed $R$ and $\epsilon$, the contour we wish to integrate over is contained entirely within this region.

By Cauchy's theorem, the integral over the contour vanishes for each fixed $R$. Since $f(x + iR) = \log^2{(1 - e^{2ix}e^{-2R})} \to 0$ uniformly as $R \to \infty$, the integral over the segment $[iR,\pi/2 + iR]$ vanishes in the limit. Similarly, since $1 - e^{2iz} = O(z)$ as $z \to 0$, we have $f(z) = O(\log^2{|z|})$ for small enough $z$, which, since $\epsilon \log^2{\epsilon} \to 0$ with $\epsilon$, means that the the integral over the circular arc from $i\epsilon$ to $\epsilon$ vanishes as $\epsilon \to 0$.

From the vertical sides of the contour, we get the contribution $$ \begin{align*} \int_{[\pi/2,\pi/2 + iR]} + \int_{[iR,i\epsilon]} f(z)\,dz & = i\int_0^R f(\pi/2 + iy)\,dy -i\int_\epsilon^R f(iy)\,dy. \end{align*} $$ Since $f(iy)$ and $f(\pi/2 + iy)$ are real, this contribution is purely imaginary.

Finally, the contribution from the bottom side of the contour, after letting $\epsilon \to 0$, is $$ \begin{align*} \int_0^{\pi/2} f(x)\,dx = \int_0^{\pi/2} \log^2{(-2ie^{ix}\sin{x})}\,dx, \end{align*} $$ and we know from the preceding remarks that the real part of this integral must vanish. For $x$ between $0$ and $\pi/2$, the quantity $2\sin{x}$ is positive. Writing $-ie^{ix} = e^{i(x - \pi/2)}$, we see that $x - \pi/2$ is the unique value of $\arg{(-2ie^{ix}\sin{x})}$ which lies in $(-\pi,\pi)$. Since we have chosen the principal branch of $\log{z}$, it follows from these considerations that $\log{(-2ie^{ix}\sin{x})} = \log{(2\sin{x})} + i(x-\pi/2)$, and therefore that $$ \begin{align*} \text{Re}{f(x)} &= \log^2{(2\sin{x})} - (x-\pi/2)^2 \\ &= \log^2{(\sin{x})} + 2\log{2}\log{(\sin{x})} + \log^2{2} - (x - \pi/2)^2. \end{align*} $$ By setting $\int_0^{\pi/2} \text{Re}f(x)\,dx = 0$ we get $$ \begin{align*} \int_0^{\pi/2} \log^2{(\sin{x})}\,dx &= \int_0^{\pi/2}(x-\pi/2)^2\,dx - 2\log{2}\int_0^{\pi/2} \log{(\sin{x})}\,dx -\frac{\pi}{2}\log^2{2} \\ & = \frac{1}{3}\left(\frac{\pi}{2}\right)^3 + \frac{\pi}{2} \log^2{2} \end{align*} $$ as expected


By similar methods, one can compute a variety of integrals of this form with little difficulty. Here are some examples I have computed for fun. All are proved by the same method, with the same contour, but different functions $f$.

  1. Take $f(z) = \log{(1 + e^{2iz})} = \log{(2e^{iz}\cos{z})}$ and compare imaginary parts to get $$ \int_0^\infty \log{(\coth{y})}\,dy = \frac{1}{2}\left(\frac{\pi}{2}\right)^2. $$
  2. Related to this question of yours (which incidentally led me here), one can show by taking $f(z) = \log^4(1 + e^{2iz})$ and comparing real parts that $$ \int_0^{\pi/2} x^2\log^2{(2\cos{x})}\,dx = \frac{1}{30}\left(\frac{\pi}{2}\right)^5 + \frac{1}{6}\int_0^{\pi/2} \log^4{(2\cos{x})}\,dx. $$ Assuming the result of the other question, we then get $$ \int_0^{\pi/2} \log^4{(2\cos{x})}\,dx = \frac{19}{15}\left(\frac{\pi}{2}\right)^5. $$
  3. Also related to the question cited in 2., taking $f(z) = z^2\log^2{(1 + e^{2iz})}$ and comparing real parts gives $$ \int_0^{\pi/2}x^2\log^2{(2\cos{x})}\,dx = \frac{1}{5}\left(\frac{\pi}{2}\right)^5 + \pi \int_0^\infty y\log^2{(1- e^{-2y})}\,dy. $$ Once more, assuming the result of the other question, we get $$ \int_0^\infty y\log^2{(1- e^{-2y})}\,dy = \frac{1}{45}\left(\frac{\pi}{2}\right)^4. $$

Actually, the integral in 3. has several interesting series expansions, and I would be very interested if someone could compute it without using the result from the question I cited. For one thing, that would give us a different proof of that result (which is why I started investigating it in the first place).

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  • $\begingroup$ Actually, to add to the examples listed above, I believe one can show that $$\int_{-\pi/2}^{\pi/2}\left(\log(2\cos{x}) + ix\right)^m\,dx =0$$ for all integers $m>0$, by taking $f(z) = \log^m(1 + e^{2iz})$ and integrating instead over the rectangle with vertices $-\pi/2 + Ri$, $-\pi/2$, $\pi/2$. (Of course, the corners must be omitted as before, but this should be a nonissue.) With this choice of contour, the contributions from the vertical sides will actually cancel. $\endgroup$ Commented Mar 15, 2012 at 9:02
  • $\begingroup$ Thanks a lot Nick. That's very insightful. $\endgroup$
    – Cody
    Commented Mar 19, 2012 at 21:15
  • $\begingroup$ I am pleased to report that this method can also be employed to answer the question I referenced in 2. and 3. See here. $\endgroup$ Commented Mar 31, 2012 at 18:15
  • $\begingroup$ @NickStrehlke, can I ask something? Why are you using $2ie^{iz}\sin(z)$ when it is supposed to be $\sin(z)$? $\endgroup$
    – Amad27
    Commented Dec 26, 2014 at 14:36
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Let $t=\sin(x)$. Then $\mathrm{d}t = \cos(x)\; \mathrm{d}x = \sqrt{1-t^2}\; \mathrm{d}x$. Now,

$$ \int_0^{\frac{\pi}{2}} \log^2(\sin(x)) \mathrm{d} x = \int_0^1 \frac{\log^2(t)}{\sqrt{1-t^2}} \mathrm{d} t $$

The latter form can be integrated by means of $\int_0^1 \frac{t^{s-1}}{\sqrt{1-t^2}} \mathrm{d} t = \frac{1}{2} \operatorname{B}\left(\frac12, \frac{s}{2}\right) = \dfrac{\sqrt{\pi}\, \Gamma\left(\frac{s}{2}\right)}{2 \Gamma\left(\frac{s+1}{2}\right)}$

Now differentiate with respect to $s$ twice and set $s=1$ which will get

$$ \frac{C^2 \pi}{8} + \frac{\pi^3}{24} + \frac{C \pi }{4} \psi\left(\frac12\right) + \frac{\pi}{8} \psi\left(\frac12\right)^2 = \frac{\pi^3}{24} + \frac{\pi}{2} \log(2)^2 $$

Added: $C$ stands for Euler-Mascheroni constant.

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  • $\begingroup$ ok clear i understood $\endgroup$ Commented Aug 20, 2011 at 16:01
  • $\begingroup$ Could you please explain what $C$ is? $\endgroup$ Commented Aug 20, 2011 at 16:28
  • $\begingroup$ I believe the C has something to do with the gamma constant, $\gamma$?. Because $psi(1/2)=-\gamma-2ln(2)$. This would then result in cancellations leaving only $\frac{{\pi}^{3}}{24}+\frac{\pi}{2}ln^{2}(2)$. Am I correct Sasha?. I like your solution. Very clever. Though, I must admit, the differentiation of the Gamma has me a little stymied. I will have to work through it. $\endgroup$
    – Cody
    Commented Aug 20, 2011 at 17:54
  • $\begingroup$ I ran through the differentiation and got: $\frac{{\pi}^{3}}{24}+\frac{\pi}{8}(\psi(1/2))^{2}+\frac{\pi \gamma}{4}\psi(1/2)+\frac{\pi {\gamma}^{2}}{8}$, which equals the correct result after simplifying. Very nice method, S. $\endgroup$
    – Cody
    Commented Aug 20, 2011 at 18:21
  • $\begingroup$ @Americo $C$ is Euler-Mascheroni constant, I edited the post to explain that. $\endgroup$
    – Sasha
    Commented Aug 20, 2011 at 19:39
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A third approach would be the Fourier series:

Namely, consider

$$\ln \left (2\sin \frac{x}{2}\right )=-\sum_{n=1}^{\infty}\frac{\cos nx}{n};(0<x<2\pi)$$

After squared:

$$\ln^2\left (2\sin \frac{x}{2}\right )=\sum_{n=1}^{\infty} \sum_{k=1}^{\infty}\frac{\cos kx\cos nx}{kn}$$

Now, integrate the last equation from $x=0$ to $x=\pi$

On the right side, we get:

$$\frac{\pi}{2}\sum_{k=1}^{\infty}\frac{1}{k^2}=\frac{\pi}{2}\frac{\pi^2}{6}=\frac{\pi^3}{12}$$

because $$I=\int_{0}^{\pi}\cos kx\cos nx\,dx=0;k\neq n$$ $$I=\frac{\pi}{2};k=n$$

On the left side:

$$\int_{0}^{\pi}\ln^2\left (2\sin \frac{x}{2}\right )\,dx= \ln^22 \int_{0}^{\pi}dx + 4\ln 2 \int_{0}^{\frac{\pi}{2}} \ln \left (\sin x\right )dx+2 \int_{0}^{\frac{\pi}{2}} \ln^2 \left (\sin x\right )dx $$

Since we know that $ \int_{0}^{\frac{\pi}{2}} \ln(\sin x)dx=-\frac{\pi}{2}\ln(2) $ then we get $ \int_{0}^{\frac{\pi}{2}}\ln^{2}(\sin x)dx $ from the equation.

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  • $\begingroup$ How you wrote $$ \sum_{n=1}^\infty \sum_{k=1}^\infty \frac{1}{nk} = \sum_{k=1}^\infty \frac{1}{k^2} $$ ? $\endgroup$ Commented Jul 20, 2023 at 12:11
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Perform the change of variable \begin{align}y=\dfrac{\pi}{2}-x\end{align}

\begin{align}J&=\int_0^{\frac{\pi}{2}}\ln^2\left(\sin x\right) \,dx\\ &=\int_0^{\frac{\pi}{2}}\ln^2\left(\cos x\right)\,dx\\\end{align}

Consider the integrals,

\begin{align}A&=\int_0^{\frac{\pi}{2}}\ln^2\left(\tan x\right)\,dx\\ B&=\int_0^{\frac{\pi}{2}}\ln^2(\sin x\cos x)\,dx\end{align}

observe that,

\begin{align}A+B=4J\end{align}

Perform the change of variable \begin{align}y=\tan x\end{align}

\begin{align}A&=\int_0^\infty \frac{\ln^2 x}{1+x^2}\,dx\end{align}

Consider the double integral

\begin{align} K&=\int_0^\infty \int_0^\infty \frac{\ln^2(xy)}{(1+x^2)(1+y^2)}\,dx\,dy\\ &=2\int_0^\infty \int_0^\infty \frac{\ln^2 x}{(1+x^2)(1+y^2)}\,dx\,dy\\ &=\pi A \end{align}

since,

\begin{align} \int_0^\infty \frac{\ln x}{1+x^2}\,dx=0\end{align}

On the other hand, perform the change of variable $u=xy$,

\begin{align}K&=\int_0^\infty \int_0^\infty \frac{y\ln^2 u}{(u^2+y^2)(1+y^2)}\,du\,dy\\\end{align}

Perform the change of variable $v=y^2$,

\begin{align}K&=\frac{1}{2}\int_0^\infty \int_0^\infty \frac{\ln^2 u}{(u^2+v)(1+v)}\,du\,dv\\ &=\frac{1}{2}\int_0^\infty\left[\frac{\ln\left(\frac{v+1}{v+u^2}\right)}{u^2-1}\right]_{v=0}^{\infty}\ln^2 u\,du\\ &=\int_0^\infty\frac{\ln^3 u}{u^2-1}\,du\\ &=\int_0^1\frac{\ln^3 u}{u^2-1}\,du+\int_1^\infty\frac{\ln^3 u}{u^2-1}\,du\\ \end{align}

In the latter integral perform the change of variable $z=\dfrac{1}{u}$,

\begin{align}K&=2\int_0^1\frac{\ln^3 u}{u^2-1}\,du\\ &=2\int_0^1\frac{\ln^3 u}{u-1}\,du-\int_0^1\frac{2u\ln^3 u}{u^2-1}\,du \end{align}

In the latter integral perform the change of variable $z=u^2$,

\begin{align}K&=\left(2-\frac{1}{8}\right)\int_0^1\frac{\ln^3 u}{u-1}\,du\\ &=-\frac{15}{8}\int_0^1\left( \sum_{n=0}^\infty u^{n}\right)\ln^3 u\,du\\ &=-\frac{15}{8}\sum_{n=0}^\infty\int_0^1 u^{n}\ln^3 u\,du\\ &=\frac{45}{4} \sum_{n=0}^\infty\frac{1}{(n+1)^4}\\ &=\frac{45}{4}\zeta(4)\\ \end{align}

therefore,

\begin{align}A&=\frac{K}{\pi}\\ &=\frac{45}{4\pi}\zeta(4)\end{align}

\begin{align} B&=\int_0^{\frac{\pi}{2}}\ln^2\left(\frac{\sin(2x)}{2}\right)\,dx \end{align}

Perform the change of variable $y=2x$,

\begin{align} B&=\frac{1}{2}\int_0^{\pi}\ln^2\left(\frac{\sin x}{2}\right)\,dx\\ &=\frac{1}{2}\int_0^{\frac{\pi}{2}}\ln^2\left(\frac{\sin x}{2}\right)\,dx+\frac{1}{2}\int_{\frac{\pi}{2}}^{\pi}\ln^2\left(\frac{\sin x}{2}\right)\,dx\\ \end{align}

In the latter integral perform the change of variable $y=\pi-x$,

\begin{align} B&=\int_0^{\frac{\pi}{2}}\ln^2\left(\frac{\sin x}{2}\right)\,dx\\ &=\int_0^{\frac{\pi}{2}}\ln^2\left(\sin x\right)\,dx-2\ln 2\int_0^{\frac{\pi}{2}}\ln(\sin x)\,dx+\frac{\pi}{2}\ln^2 2\\ &=J+\frac{3\pi}{2}\ln^2 2 \end{align}

Therefore,

\begin{align}\frac{45}{4}\zeta(4)+J+\frac{3\pi}{2}\ln^2 2=4J \end{align}

Thus,

\begin{align}J&=\frac{15}{4\pi}\zeta(4)+\frac{1}{2}\pi\ln^2 2 \end{align}

If you know that,

\begin{align}\zeta(4)=\frac{\pi^4}{90}\end{align}

therefore,

\begin{align}\boxed{J=\frac{\pi^3}{24}+\frac{1}{2}\pi\ln^2 2} \end{align}

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Alternative solution:

\begin{align} A&=\int_0^{\frac{\pi}{2}}x\ln^2(\sin x)dx\\ &\overset{y=\sin x}=\int_0^1 \frac{\ln^2 y\arcsin y}{\sqrt{1-y^2}}dy\\ &\overset{\text{IBP}}=\left[\left(\int_0^y \frac{\ln^2 t}{\sqrt{1-t^2}}dt\right)\arcsin y\right]_0^1-\int_0^1 \frac{1}{\sqrt{1-y^2}}\left(\int_0^y \frac{\ln^2 t}{\sqrt{1-t^2}}dt\right)dy \\ &=\frac{\pi}{2}\int_0^1 \frac{\ln^2 t}{\sqrt{1-t^2}}dt-\int_0^1 \int_0^1 \frac{y\ln^2(ty)}{\sqrt{1-y^2}\sqrt{1-t^2y^2}}dtdy\\ &=\frac{\pi}{2}\int_0^1 \frac{\ln^2 t}{\sqrt{1-t^2}}dt+\int_0^1 \int_0^1 \frac{y\ln^2 y}{\sqrt{1-y^2}\sqrt{1-t^2y^2}}dtdy-\\&\int_0^1 \int_0^1 \frac{y\ln^2 t}{\sqrt{1-y^2}\sqrt{1-t^2y^2}}dtdy- 2\underbrace{\int_0^1 \int_0^1 \frac{y\ln y\ln(ty)}{\sqrt{1-y^2}\sqrt{1-t^2y^2}}dtdy}_{u=ty}\\ &=\frac{\pi}{2}\int_0^1 \frac{\ln^2 t}{\sqrt{1-t^2}}dt+\int_0^1 \left[\frac{\arcsin(ty)}{\sqrt{1-y^2}}\right]_{t=0}^{t=1}\ln^2 ydy+\\&\int_0^1 \frac{1}{t}\left[\text{arcsinh}\left(\frac{t\sqrt{1-y^2}}{\sqrt{1-t^2}}\right)\right]_{y=0}^{y=1}\ln^2 tdt-2\int_0^1 \frac{\ln y}{\sqrt{1-y^2}}\left(\int_0^y \frac{\ln t}{\sqrt{1-t^2}}dt\right)dy\\ &=\frac{\pi}{2}\int_0^1 \frac{\ln^2 t}{\sqrt{1-t^2}}dt+A-\underbrace{\int_0^1 \frac{\text{arcsinh}\left(\frac{t}{\sqrt{1-t^2}}\right)\ln^2 t}{t}dt}_{\text{IBP}}-\left(\int_0^1 \frac{\ln y}{\sqrt{1-y^2}}dy\right)^2\\ &=\frac{\pi}{2}\int_0^1 \frac{\ln^2 t}{\sqrt{1-t^2}}dt+A+\frac{1}{3}\int_0^1 \frac{\ln^3 t}{1-t^2}dt-\left(\int_0^1 \frac{\ln y}{\sqrt{1-y^2}}dy\right)^2\\ \end{align} Moreover, \begin{align} \int_0^1 \frac{\ln y}{\sqrt{1-y^2}}dy&=\int_0^{\frac{\pi}{2}}\ln(\sin x)dx=-\frac{\pi}{2}\ln 2\\ \int_0^1 \frac{\ln^3 t}{1-t^2}dt&=-\frac{45}{8}\zeta(4)=-\frac{\pi^4}{16} \end{align}

Therefore, \begin{align} \boxed{\displaystyle \int_0^1 \dfrac{\ln^2 t}{\sqrt{1-t^2}}dt=\int_0^{\frac{\pi}{2}}\ln^2(\sin x)dx=\dfrac{\pi\ln^2 2}{2}+\dfrac{\pi^3}{24}} \end{align}

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Note $\int_{0}^{\frac\pi2} \ln^2(\tan x)dx = \frac{d^2}{da^2} (\int_{0}^{\frac\pi2} \tan^a x \ dx)_{a=0} =\frac{d^2}{da^2} (\frac\pi2\sec\frac{\pi a}2)_{a=0}=\frac{\pi^3}8 $ \begin{align} I=& \int_{0}^{\frac{\pi}{2}}\ln^2(2\sin x)\ dx =\int_{0}^{\frac{\pi}{2}}\ln^2(2\cos x)\ dx\\ =&\ \frac14 \int_{0}^{\frac\pi2} [\overset{2x\to x}{\ln^2(2\sin 2x)}+\ln^2(\tan x)]\ dx = \frac14 I + \frac14\cdot \frac{\pi^3}8 =\frac{\pi^3}{24} \end{align} which, along with $\int_{0}^{\frac{\pi}2}\ln(2\sin x)dx =0$, leads to $$\int_{0}^{\frac{\pi}{2}}\ln^2(\sin x)\ dx = \frac{{\pi}^3}{24}+\frac\pi2 \ln^{2}2 $$

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\begin{align*} I &= \int\limits_0^{\pi /2} {(\ln^2(\cos(x)))dx} \\ &= \int\limits_0^{\pi /2} {(\ln^2(\sin(y)))dy} \quad \text{where } y = \frac{\pi}{2} - x \\ &= \int\limits_0^{\pi /2} {(\ln^2(\sin(x)))dx} \\ J &= \int\limits_0^{\pi /2} {\ln(\cos(y))dy} \quad \text{where } y = \frac{\pi}{2} - x \\ &= \int\limits_0^{\pi /2} {\ln(\sin(x))dx} \\ \int\limits_0^{\pi /2} {\ln(\sin(2x))dx} &= \frac{1}{2} \int\limits_0^\pi {\ln(\sin(y))dy} \\ &= \frac{1}{2} \int\limits_0^{\pi /2} {\ln(\sin(x))dx} + \frac{1}{2} \int\limits_{\pi /2}^\pi {\ln(\sin(y))dy} \\ &= \frac{1}{2} \int\limits_0^{\pi /2} {\ln(\sin(x))dx} + \frac{1}{2} \int\limits_0^{\pi /2} {\ln(\sin(x))dx} \\ &= \int\limits_0^{\pi /2} {\ln(\sin(x))dx} = J \\ J &= \int\limits_0^{\pi /2} {\ln(\sin(2x))dx} \\ &= \int\limits_0^{\pi / 2} {\ln(2\sin(x)\cos(x))dx} \\ &= \int\limits_0^{\pi /2} {\ln(2)dx} + \int\limits_0^{\pi /2} {\ln(\sin(x))dx} + \int\limits_0^{\pi /2} {\ln(\cos(x))dx} \\ &= \frac{\pi}{2} \ln(2) + 2J \\ &\Rightarrow \boxed{J = \int\limits_0^{\pi /2} {\ln(\sin(x))dx} = \int\limits_0^{\pi /2} {\ln(\cos(x))dx} = -\frac{\pi}{2}\ln(2)} \\ \int\limits_0^{\pi /2} {(\ln^2(\sin(2x)))dx} &= \frac{1}{2} \int\limits_0^\pi {(\ln^2(\sin(y)))dy} \\ &= \frac{1}{2} \int\limits_0^{\pi /2} {(\ln^2(\sin(x)))dx} + \frac{1}{2} \int\limits_{\pi /2}^\pi {(\ln^2(\sin(y)))dy} \\ &= \frac{1}{2} \int\limits_0^{\pi /2} {(\ln^2(\sin(x)))dx} + \frac{1}{2} \int\limits_0^{\pi /2} {(\ln^2(\sin(x)))dx} \\ &= \int\limits_0^{\pi /2} {(\ln^2(\sin(x)))dx} = I \\ I &= \int\limits_0^{\pi /2} {(\ln^2(\sin(2x)))dx} \\ &= \int\limits_0^{\pi /2} {(\ln^2(2\sin(x)\cos(x)))dx} \\ &= \int\limits_0^{\pi /2} {(\ln^2(2) + \ln^2(\sin(x)) + \ln^2(\cos(x)))dx} \\ &= \ln^2(2)\frac{\pi}{2} + 2I + 4\ln(2)J + 2\int\limits_0^{\pi /2} {\ln(\sin(x))\ln(\cos(x))dx} \\ &= 2I + \ln^2(2)\frac{\pi}{2} - 2\pi\ln^2(2) + 2\int\limits_0^{\pi /2} {\ln(\sin(x))\ln(\cos(x))dx} \\ &\Rightarrow \boxed{I = \frac{3\pi}{2}\ln^2(2) - 2\int\limits_0^{\pi /2} {\ln(\sin(x))\ln(\cos(x))dx}} \\ \text{we have proved that} \\ \int\limits_0^{\pi /2} {\ln(\sin(x))\ln(\cos(x))dx} &= \frac{\pi}{2}\ln^2(2) - \frac{\pi^3}{48} \\ \text{then} \\ \int\limits_0^{\pi /2} {(\ln^2(\cos(x)))dx} &= \frac{\pi^3}{24} + \frac{\pi}{2}\ln^2(2) \end{align*}

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Let $I=\int_0^{\frac\pi 2}\ln^2\sin xdx$. By adding $(\ln\sin x\pm\ln\cos x)^2$ we have $$\ln^2\sin2x-2\ln2\ln\sin2x+\ln^22+\ln^2\tan x=2\ln^2\sin x+2\ln^2\cos x.$$ Integrating from $0$ to $\frac\pi 2$ $$I=\frac\pi 2\ln^2 2+\frac13\int_0^{\frac\pi 2}\ln^2\tan x dx$$ where $$\int_0^{\frac\pi 2}\ln^2\tan x dx= \int_0^{\infty}\frac{\ln^2y}{y^2+1} dy= \int_0^{\infty}\frac{x^2}{\cosh x} dx=4\beta(3)=\frac{\pi^3}8 $$ where $\beta(s)$ is Dirichlet's beta function.

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