A closed form for the dilogarithm integral $\int _{ 0 }^{ 1 }{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right) \right) }{ x } dx } $ $$\int _{ 0 }^{ 1 }{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right)  \right)  }{ x } dx } $$
when I was solving an infinite series by using the beta function I encountered the above dilogarithm integral which has a quadratic term. I tried to apply u-substitution and other dilogarithm identities to evaluate it, Unfortunately, I didn't get it. Since the infinite series has a closed-form in terms of Apery$\zeta \left( 3 \right)$  and Catalan constant $G$, The result of this integral would be to in such constants.
I hope if anyone could come up with a good method to evaluate this integral.
 A: We know that $\text{Li}_2(x)=-\int_0^1 \frac{x\ln(y)}{1-xy}dy$
so
$$\int_0^1 \frac{\text{Li}_2(2x(1-x))}{x}dx=-2\int_0^1 \ln(y)\left[\int_0^1 \frac{1-x}{1-2x(1-x)y}dx\right]dy$$
$$=-2\int_0^1 \frac{\ln(y)\arctan\sqrt{\frac{y}{2-y}}}{\sqrt{y(2-y)}}dy\overset{\sqrt{\frac{y}{2-y}}=x}{=}-4\int_0^1\frac{\ln\left(\frac{2x^2}{1+x^2}\right)\arctan(x)}{1+x^2}dx$$
$$\overset{x=\tan\theta}{=}-4\int_0^{\pi/4}\theta\ln(2\sin^2 \theta)\ d\theta=-4\ln(2)\int_0^{\pi/4}\theta\ d\theta-8\int_0^{\pi/4}\theta\ln(\sin\theta)\ d\theta$$
$$=-4\ln(2)\left(\frac{\pi^2}{32}\right)-8\left(\frac{35}{128}\zeta(3)-\frac{\pi^2}{32}\ln(2)-\frac{\pi}{8}G\right)$$
$$=\pi G-\frac{35}{16}\zeta(3)+\frac{\pi^2}{8}\ln(2).$$
The last integral follows from using the Fourier series of $\ln(\sin\theta)=-\ln(2)-\sum_{n=1}^\infty\frac{\cos(2n\theta)}{n}$.
A: Mathematica gives 
$$
\pi  C+\frac{1}{16} \left(\pi ^2 \log (4)-35 \zeta (3)\right).
$$
A: Considering
$$I(x)=\int{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right)  \right)  }{ x } dx }$$
please find (and enjoy) the antiderivative.
Using it
$$I(1)=-2 \zeta (3)-\frac{1}{6} \pi ^2 \log (2)$$
$$I(0)=-\pi  C+\frac{3 \zeta (3)}{16}-\frac{7}{24} \pi ^2 \log (2)$$
$$J=\int_0^1{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right)  \right)  }{ x } dx }=\pi  C-\frac{35}{16} \zeta (3)+\frac{1}{8} \pi ^2 \log (2)$$
Edit
Consider that $$\text{Li}_2(t)=\sum_{n=1}^\infty \frac t {n^2}\implies \text{Li}_2(2x(1-x))=\sum_{n=1}^\infty \frac {\big[2x(1-x)\big]^n} {n^2}$$
$$\int{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right)  \right)  }{ x } dx }=\sum_{n=1}^\infty \frac {2^n}{n^2} \int (1-x)^n x^{n-1}\,dx $$
$$J=\int_0^1{ \frac { \operatorname{Li}_2\left( 2x\left( 1-x \right)  \right)  }{ x } dx }=\sum_{n=1}^\infty\frac{2^n}{n^2}\frac{\Gamma (n) \,\,\Gamma (n+1)}{\Gamma (2 n+1)}=\sqrt{\pi }\sum_{n=1}^\infty\frac{ 2^{-n}\,\, \Gamma (n)}{n^2 \,\Gamma \left(n+\frac{1}{2}\right)}$$
$$J=\, _4F_3\left(1,1,1,1;\frac{3}{2},2,2;\frac{1}{2}\right)=\pi  C-\frac{35 \zeta (3)}{16}+\frac{1}{8} \pi ^2 \log (2)$$
