Let's declare $\mathcal{G}$ is constant of Catalanand the $\mathcal{H}_m-st$ mharmonic term. Let it be shown that:
$$\displaystyle{\sum_{m=1}^{\infty} \frac{(-1)^m \mathcal{H}_{2m} }{2m+1} -\frac{1}{2} \sum_ {m=1}^{\infty} \frac{(-1)^m \mathcal{H}_m}{2m+1} = \frac{\pi \log 2}{8} - \frac{\mathcal {G}}{2}}$$
My try
Since $$\displaystyle{{H_{2m}} - \frac{1}{2}{H_m} = \left( {1 + \frac{1}{2} + \frac{1}{3} + .. + \ frac{1}{{2m}}} \right) - \frac{1}{2}\left( {1 + \frac{1}{2} + \frac{1}{3} + .. + \ frac{1}{m}} \right) = \sum\limits_{n = 1}^m {\frac{1}{{2n - 1}}} }$$ we have:
$$\displaystyle{S = \sum\limits_{m = 1}^\infty {\frac{{{{\left( { - 1} \right)}^m}}}{{2m + 1}}\left( {{H_{2m}} - \frac{1}{2}{H_m}} \right)} = \sum\limits_{m = 1}^\infty {\frac{{{{\left( { - 1 } \right)}^m}}}{{2m + 1}}\sum\limits_{n = 1}^m {\frac{1}{{2n - 1}}} } = }$$ $$\displaystyle{\sum\limits_{m = 1}^\infty {{{\left( { - 1} \right)}^m}\sum\limits_{n = 1}^m {\frac{1}{ {2n - 1}}} \int\limits_0^1 {{x^{2m}}dx} } = \int\limits_0^1 {\left( {\sum\limits_{m = 1}^\infty {{ {\left( { - 1} \right)}^m}\left( {\sum\limits_{n = 1}^m {\frac{1}{{2n - 1}}} } \right){x ^{2m}}} } \right)dx} }$$
We consider the function
$$\displaystyle{f\left( x \right) = \sum\limits_{m = 1}^\infty {{{\left( { - 1} \right)}^m}\left( {\sum\limits_{ n = 1}^m {\frac{1}{{2n - 1}}} } \right){x^{2m}}} = \sum\limits_{m = 1}^\infty {{a_m} \cdot {x^{2m}}} }$$ with $$\displaystyle{{a_m} = {\left( { - 1} \right)^m}\left( {\sum\limits_{n = 1}^m {\frac{1}{{2n - 1}}} } \right)}$$
Then $$\displaystyle{a_m} = {\left( { - 1} \right)^m}\left( {\sum\limits_{n = 1}^m {\frac{1}{{2n - 1}}} } \right) \Rightarrow {a_{m + 1}} = - {\left( { - 1} \right)^m}\left( {\sum\limits_{n = 1}^{m + 1} { \frac{1}{{2n - 1}}} } \right) = $$ $$\displaystyle{ - {\left( { - 1} \right)^m}\left( {\frac{1}{{2m + 1}} + \sum\limits_{n = 1}^m {\frac{ 1}{{2n - 1}}} } \right) = - {a_m} - \frac{{{{\left( { - 1} \right)}^m}}}{{2m + 1}}}$$
\begin{gathered} * {\text{This equality holds}}:\frac{{\arctan \left( x \right)}}{{1 + {x^2}}} = - \sum\limits_{n = 1}^\infty {{{\left( { - 1} \right)}^n}} \left( {{H_{2n}} - \frac{1}{2}{H_n}} \right){x^{2n - 1}}\left( {\left| x \right| \leqslant 1} \right) \hfill \\ \Leftrightarrow - \frac{{x\arctan \left( x \right)}}{{1 + {x^2}}} = \sum\limits_{n = 1}^\infty {{{\left( { - 1} \right)}^n}} \left( {{H_{2n}} - \frac{1}{2}{H_n}} \right){x^{2n}} \hfill \\ {\text{Now, integrate both side w}}{\text{.r}}{\text{.t }}x{\text{ from }}0{\text{ to }}1: \hfill \\ \Rightarrow - \int\limits_0^1 {\frac{{x\arctan \left( x \right)}}{{1 + {x^2}}}dx} = \sum\limits_{n = 1}^\infty {{{\left( { - 1} \right)}^n}} \left( {{H_{2n}} - \frac{1}{2}{H_n}} \right)\int\limits_0^1 {{x^{2n}}} dx = \sum\limits_{n = 1}^\infty {\frac{{{{\left( { - 1} \right)}^n}}}{{2n + 1}}} \left( {{H_{2n}} - \frac{1}{2}{H_n}} \right) = S \hfill \\ * I = \int\limits_0^1 {\frac{{x\arctan \left( x \right)}}{{1 + {x^2}}}dx} ,{\text{ let}}:x = \tan \left( t \right) \Rightarrow dx = \left( {1 + {{\tan }^2}\left( t \right)} \right)dt \Rightarrow \frac{{dx}}{{1 + {x^2}}} = dt \hfill \\ \Rightarrow I = \int\limits_0^{\frac{\pi }{4}} {t\tan \left( t \right)dt} \xrightarrow{{{\text{IBP}}}}\left. { - t\ln \left( {\cos \left( t \right)} \right)} \right|_0^{\frac{\pi }{4}} + \int\limits_0^{\frac{\pi }{4}} {\ln \left( {\cos \left( t \right)} \right)dt} = \frac{\pi }{8}\ln \left( 2 \right) + \frac{G}{2} - \frac{\pi }{4}\ln \left( 2 \right) = \frac{G}{2} - \frac{\pi }{8}\ln \left( 2 \right) \hfill \\ \because \int\limits_0^{\frac{\pi }{4}} {\ln \left( {\cos \left( t \right)} \right)dt} = \frac{G}{2} - \frac{\pi }{4}\ln \left( 2 \right){\text{ is well}} - {\text{known, and can be found in this site}}{\text{.}} \hfill \\ \Rightarrow S = - I = \frac{\pi }{8}\ln \left( 2 \right) - \frac{G}{2} \hfill \\ \end{gathered}