Is there closed form for
$$\sum_{n=1}^\infty\frac{\overline{H}_n}{n^2}x^n\ ?$$
where $\overline{H}_n=\sum_{k=1}^n\frac{(-1)^{k-1}}{k}$ is the alternating harmonic number.
My approach,
In this paper page $95$ Eq $(5)$ we have
$$\sum_{n=1}^\infty \overline{H}_n\frac{x^n}{n}=\operatorname{Li}_2\left(\frac{1-x}{2}\right)-\operatorname{Li}_2(-x)-\ln2\ln(1-x)-\operatorname{Li}_2\left(\frac12\right)$$
Divide both sides by $x$ then integrate we get
$$\sum_{n=1}^\infty\frac{\overline{H}_n}{n^2}x^n=\int\frac{\operatorname{Li}_2\left(\frac{1-x}{2}\right)}{x}\ dx-\operatorname{Li}_3(-x)+\ln2\operatorname{Li}_2(x)-\operatorname{Li}_2\left(\frac12\right)\ln x$$
and my question is how to find the remaining integral? Thanks
Maybe you wonder why I have it as an indefinite integral, I meant so as I am planning to plug $x=0$ to find the constant after we find the closed form of the integral if possible.
I tried Mathematica, it gave
Edit
With help of $Mathematica$ I was able to find
\begin{align} \sum_{n=1}^\infty\frac{\overline{H}_n}{n^2}x^n&=-\frac13\ln^3(2)+\frac12\ln^2(2)\ln(1-x)-\frac12\zeta(2)\ln(x)+\frac32\ln^2(2)\ln(x)\\ &\quad-\ln(2)\ln(x)\ln(1-x)-\frac12\ln(2)\ln^2(x)-\frac12\ln^2(2)\ln(1-x)\\ &\quad-\ln^2(2)\left(\frac{x}{1+x}\right)+\ln(2)\ln\left(\frac{x}{1+x}\right)[\ln(1-x)+\ln(x)]\\ &\quad+\ln(x)\ln(1-x)\ln(1+x)+\ln(x)\operatorname{Li}_2\left(\frac{1-x}{2}\right)+\ln\left(\frac{x}{1+x}\right)\operatorname{Li}_2(x)\\ &\quad+\ln(1+x)\operatorname{Li}_2(x)+\operatorname{Li}_2\left(\frac{x}{1+x}\right)\ln\left(\frac{2x}{1+x}\right)-\operatorname{Li}_2\left(\frac{2x}{1+x}\right)\ln\left(\frac{2x}{1+x}\right)\\ &\quad+\operatorname{Li}_2\left(\frac{1+x}{2}\right)\ln\left(\frac{x}{2}\right)-\ln\left(\frac{x}{1+x}\right)\operatorname{Li}_2\left(\frac{1+x}{2}\right)-\operatorname{Li}_3(x)-\operatorname{Li}_3\left(\frac{x}{1+x}\right)\\ &\quad+\operatorname{Li}_3\left(\frac{2x}{1+x}\right)-\operatorname{Li}_3\left(\frac{1+x}{2}\right)-\operatorname{Li}_3(-x)+\ln(2)\operatorname{Li}_2(x)+\frac{7}{8}\zeta(3) \end{align}


Starring with Landens identity
$$\operatorname{Li}_2(1-t)+\operatorname{Li}_2\left(\frac{t-1}{t}\right)=-\frac12\ln^2t$$
set $1-t=\frac{1-x}{2}$ we get
$$\operatorname{Li}_2\left(\frac{1-x}{2}\right)=-\operatorname{Li}_2\left(-\frac{1-x}{1+x}\right)-\frac12\ln^2\left(\frac{1+x}{2}\right)$$
$$\Longrightarrow \int\frac{\operatorname{Li}_2\left(\frac{1-x}{2}\right)}{x}\ dx=-\int\frac{\operatorname{Li}_2\left(-\frac{1-x}{1+x}\right)}{x}\ dx-\frac12\int\frac{\ln^2\left(\frac{1+x}{2}\right)}{x}\ dx=-\mathcal{J}-\frac12\mathcal{K}$$
For $\mathcal{J}$, set $\frac{1-x}{1+x}=y$
$$\mathcal{J}=-2\int\frac{\operatorname{Li}_2(-y)}{1-y^2}\ dy\overset{IBP}{=}\ln\left(\frac{1-y}{1+y}\right)\operatorname{Li}_2(-y)+\int\frac{\ln\left(\frac{1-y}{1+y}\right)\ln(1+y)}{y}\ dy$$
$$=\ln\left(\frac{1-y}{1+y}\right)\operatorname{Li}_2(-y)+\underbrace{\int\frac{\ln(1-y)\ln(1+y)}{y}\ dy}_{\mathcal{\large J}_1}-\underbrace{\int\frac{\ln^2(1+y)}{y}\ dy}_{\mathcal{\large J}_2}$$
for $\mathcal{J}_1$, use $\ln(1-y)\ln(1+y)=\frac14\ln^2(1-y^2)-\frac14\ln^2\left(\frac{1-y}{1+y}\right)$
$$ \mathcal{J}_1=\frac14\underbrace{\int\frac{\ln^2(1-y^2)}{y}\ dy}_{y^2\to t}-\frac14\underbrace{\int\frac{\ln^2\left(\frac{1-y}{1+y}\right)}{y}\ dy}_{\frac{1-y}{1+y}=u}$$
$$=\frac18\int\frac{\ln^2(1-t)}{t}\ dt+\frac12\int\frac{\ln^2u}{1-u^2}\ du$$
I managed here to prove
$$\int\frac{\ln^2(1-t)}{t}dt=\ln(1-t)\left[\operatorname{Li}_2(1-t)-\operatorname{Li}_2(t)+\zeta(2))\right]-2\operatorname{Li}_3(1-t)\tag{*}$$
substitute $t=y^2$ back
$$\frac14\int\frac{\ln^2(1-y^2)}{y}dt=\frac18\int\frac{\ln^2(1-t)}{t}\ dy$$
$$=\frac18\ln(1-y^2)\left[\operatorname{Li}_2(1-y^2)-\operatorname{Li}_2(y^2)+\zeta(2)\right]-\frac14\operatorname{Li}_3(1-y^2)\tag1$$
As for the second integral,
$$\int\frac{\ln^2u}{1-u^2}\ du\overset{IBP}{=}\frac12\ln\left(\frac{1+u}{1-u}\right)\ln u-\int\frac{\ln\left(\frac{1+u}{1-u}\right)\ln u}{u}\ du$$
$$=\frac12\ln\left(\frac{1+u}{1-u}\right)\ln u-\int\frac{\ln(1+u)\ln u}{u}\ du+\int\frac{\ln(1-u)\ln u}{u}\ du$$
$$=\frac12\ln\left(\frac{1+u}{1-u}\right)\ln u-[-\operatorname{Li}_3(-u)\ln u+\operatorname{Li}_3(-u)]+[-\operatorname{Li}_3(u)\ln u+\operatorname{Li}_3(u)]$$
$$=\frac12\ln\left(\frac{1+u}{1-u}\right)\ln u+\operatorname{Li}_3(-u)\ln u-\operatorname{Li}_3(-u)-\operatorname{Li}_3(u)\ln u+\operatorname{Li}_3(u)$$
substitute $u=\frac{1-y}{1+y}$ back
$$-\frac14\int\frac{\ln^2\left(\frac{1-y}{1+y}\right)}{y}\ dy=\frac12\int\frac{\ln^2u}{1-u^2}\ du$$
$$=-\frac14\ln y\ln\left(\frac{1-y}{1+y}\right)+\frac12\operatorname{Li}_3\left(-\frac{1-y}{1+y}\right)\ln\left(\frac{1-y}{1+y}\right)$$
$$-\frac12\operatorname{Li}_3\left(-\frac{1-y}{1+y}\right)-\frac12\operatorname{Li}_3\left(\frac{1-y}{1+y}\right)\ln\left(\frac{1-y}{1+y}\right)-\frac12\operatorname{Li}_3\left(\frac{1-y}{1+y}\right)\tag2$$
Combine $(1)$ and $(2)$ to get $\mathcal{J}_1$
$$\mathcal{J}_1=\frac18\ln(1-y^2)\left[\operatorname{Li}_2(1-y^2)-\operatorname{Li}_2(y^2)+\zeta(2)\right]-\frac14\operatorname{Li}_3(1-y^2)-\frac14\ln y\ln\left(\frac{1-y}{1+y}\right)$$ $$+\frac12\operatorname{Li}_3\left(-\frac{1-y}{1+y}\right)\ln\left(\frac{1-y}{1+y}\right)-\frac12\operatorname{Li}_3\left(-\frac{1-y}{1+y}\right)-\frac12\operatorname{Li}_3\left(\frac{1-y}{1+y}\right)\ln\left(\frac{1-y}{1+y}\right)-\frac12\operatorname{Li}_3\left(\frac{1-y}{1+y}\right)$$
For $\mathcal{J}_2$, use $(*)$
$$\small{\mathcal{J}_2=\int\frac{\ln^2(1+y)}{y}\ dy\overset{y=-t}{=}-\int\frac{\ln^2(1-t)}{t}\ dt=-\ln(1+y)\left[\operatorname{Li}_2(1+y)-\operatorname{Li}_2(-y)+\zeta(2)\right]+2\operatorname{Li}_3(1+y)}$$
Similarly
$$\mathcal{K}=\int\frac{\ln^2\left(\frac{1+x}{2}\right)}{x}\ dx$$
$$=\int\frac{\ln^2(1+x)}{x}\ dx-2\ln2\int\frac{\ln(1+x)}{x}\ dx+\ln^22\int\frac{1}{x}\ dx$$
$$=-\ln(1+x)\left[\operatorname{Li}_2(1+x)-\operatorname{Li}_2(-x)+\zeta(2))\right]+2\operatorname{Li}_3(1+x)+2\ln2\operatorname{Li}_2(-x)+\ln^22\ln x$$
and what is left is only combining results and simplification but that's too tedious so I am just going to leave it as it and I am not sure if my calculations is right or not.