An evaluation using contour integration is also possible.
Consider the function $$ f(z) = \frac{\pi \cot (\pi z) [ \psi(-z)+\gamma] \ \psi_{1}(-z)}{z^3}, $$ where $\psi(z)$ is the digamma function, $\gamma$ is the Euler-Mascheroni constant, and $\psi_{1}(z)$ is the trigamma function.
The function $f(z)$ has poles at the positive integers of order 4, simple poles at the negative integers, and a pole of order 7 at the origin.
On the sides of a square with vertices at $z= (N+\frac{1}{2})\pm i (N+ \frac{1}{2})$ (call it $C_{N}$), $\cot (\pi z)$ is uniformly bounded.
And when $z$ is large in magnitude and not on the positive real axis, $\psi(-z) \sim \log(-z)$ and $\psi_{1}(-z) \sim - \frac{1}{z}$.
So $ \displaystyle \int_{C_{N}} f(z) \ dz \to 0$ as $N \to \infty$ through the positive integers, and therefore
$$ \sum_{n=-\infty}^{\infty} \text{Res}[f(z), n] = 0.$$
Expanding at the positive integers, we get
$$ \begin{align} f(z) &= \frac{1}{z^{3}} \Bigg[ \Bigg(\frac{1}{z-n} - 2 \zeta(2) (z-n) + \mathcal{O} \Big((z-n)^{3} \Big) \Bigg) \Bigg(\frac{1}{z-n} + H_{n} - \Big(H_{n}^{(2)}+\zeta(2) \Big)(z-n)\\ &+ \Big(H_{n}^{(3)} - \zeta(3) \Big) \cdot(z-n)^{2}+ \mathcal{O} \big((z-n)^{3} \Bigg) \Bigg( \frac{1}{(z-n)^{2}} + \Big( H_{n}^{2} + \zeta(2) \Big) - 2 \Big(H_{n}^{3} - \zeta(3) \Big) \\ & \cdot (z-n) + \mathcal{O} \Big( (z-n)^{2} \Big) \Bigg) \Bigg] \\ &= \frac{1}{z^{3}} \left(\frac{1}{(z-n)^{4}} + \frac{H_{n}}{(z-n)^{2}} - \frac{2 \zeta(2)}{(z-n)^{2}} + \frac{H_{n}^{(2)} H_{n}}{z-n} - \frac{\zeta(2) H_{n}}{z-n} + \frac{\zeta(3)}{z-n} - \frac{H_{n}^{(3)}}{z-n} + \mathcal{O}(1) \right) .\end{align}$$
So at the positive integers, $$ \begin{align} \text{Res}[f(z),n] &= \text{Res} \left[ \frac{1}{z^{3}} \frac{1}{(z-n)^{4}}, n \right] + \text{Res} \left[ \frac{1}{z^{3}} \frac{H_{n}}{(z-n)^{3}}, n \right] + \text{Res} \left[ \frac{-2 \zeta(2)}{z^{3}} \frac{1}{(z-n)^{2}}, n \right] \\ &+ \text{Res} \Big[ \frac{H_{n}^{(2)} H_{n}}{z^{3}} \frac{1}{z-n}, n \Big] + \text{Res} \Big[ \frac{- \zeta(2) H_{n}}{z^{3}} \frac{1}{z-n}, n \Big] + \text{Res} \Big[ \frac{\zeta(3)}{z^{3}} \frac{1}{z-n}, n \Big] \\ &+ \text{Res} \Big[ \frac{-H_{n}^{(3)}}{z^{3}} \frac{1}{z-n}\Big] \\ &= - \frac{10}{n^{5}} + \frac{6 H_{n}}{n^{5}} + \frac{6 \zeta(2)}{n^{4}} + \frac{H_{n}^{(2)}H_{n}}{n^{3}} - \frac{\zeta(2) H_{n}}{n^{3}} + \frac{\zeta(3)}{n^{3}} - \frac{H_{n}^{(3)}}{n^{3}} .\end{align} $$
At the negative integers, $$\begin{align} \text{Res}[f(z),-n] &= -\frac{\psi_{1}(n) \Big( \psi(n)+\gamma\Big)}{n^3} \\ &= - \frac{\Big(\zeta(2) - H_{n-1}^{(2)} \Big)H_{n-1}}{n^{3}} \\ &= -\frac{ \Big(\zeta(2)-H_{n}^{(2)}+ \frac{1}{n^{2}}\Big) \Big(H_{n}- \frac{1}{n} \Big)}{n^{3}} \\ &= - \frac{\zeta(2) H_{n}}{n^{3}} + \frac{\zeta(2)}{n^{4}} + \frac{H_{n}^{(2)} H_{n}}{n^{3}} - \frac{H_{n}^{(2)}}{n^{4}} - \frac{H_{n}}{n^{5}} + \frac{1}{n^{6}}. \end{align}$$
And expanding at the origin, we get $$ \begin{align} f(z) &= \frac{1}{z^{3}} \Big( \frac{1}{z} - 2 \zeta(2) z - 2 \zeta(4) z^{3} - 2 \zeta(6) z^{5} + \mathcal{O}(z^{7}) \Big) \Big( \frac{1}{z} - \zeta(2)z - \zeta(3) z^{2} - \zeta(4) z^{3}- \zeta(5) z^{4} \\ &- \zeta(6) z^{5} + \mathcal{O}(z^{6}) \Big) \Big( \frac{1}{z^{2}} + \zeta(2) + 2 \zeta(3) z + 3 \zeta(4) z^{2} + 4 \zeta(5)z^{3} + 5 \zeta(6)z^{4} + \mathcal{O}(z^{5}) \Big) \\ &= \frac{1}{z^{7}} - \frac{2 \zeta(2)}{z^{5}} + \frac{\zeta(3)}{2z^{4}} - \frac{\zeta^{2}(2)}{z^{3}} + \frac{3 \zeta(5)}{z^{2}} - \frac{5 \zeta(2) \zeta(3)}{z^{2}} - \frac{2 \zeta^{2}(3)}{z} + \frac{2 \zeta(6)}{z} - \frac{8 \zeta(2) \zeta(4)}{z} \\ &+ \frac{2 \zeta^{3}(2)}{z} + \mathcal{O}(1) .\end{align}$$
Therefore, $$ \text{Res}[f(z),0] = -2 \zeta^{2}(3) + 2 \zeta(6) - 8 \zeta(2) \zeta(4) + 2 \zeta^{3}(2) .$$
Summing up all the residues,
$$ \begin{align} &-10 \sum_{n=1}^{\infty} \frac{1}{n^{6}} + 6 \sum_{n=1}^{\infty} \frac{H_{n}}{n^{5}} + 6 \zeta(2) \sum_{n=1}^{\infty} \frac{1}{n^{4}} + \sum_{n=1}^{\infty} \frac{H_{n}^{(2)} H_{n}}{n^{3}} - \zeta(2) \sum_{n=1}^{\infty} \frac{H_{n}}{n^{3}} + \zeta(3) \sum_{n=1}^{\infty} \frac{1}{n^{3}} \\ &- \sum_{n=1}^{\infty} \frac{H_{n}^{(3)}}{n^{3}} - \zeta(2) \sum_{n=1}^{\infty} \frac{H_{n}}{n^{3}} + \zeta(2) \sum_{n=1}^{\infty} \frac{1}{n^{4}} + \sum_{n=1}^{\infty} \frac{H_{n}^{(2)} H_{n}}{n^{3}} - \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}}{n^{4}} - \sum_{n=1}^{\infty} \frac{H_{n}}{n^{5}} + \sum_{n=1}^{\infty} \frac{1}{n^{6}} \\ &- 2 \zeta^2(3) + 2 \zeta(6) - 8 \zeta(2) \zeta(4) + 2 \zeta^3(2) = 0, \end{align} $$
where $$ \sum_{n=1}^\infty \frac{H_n}{n^q}= \left(1+\frac{q}{2} \right)\zeta(q+1)-\frac{1}{2}\sum_{k=1}^{q-2}\zeta(k+1)\zeta(q-k) \tag{1}$$
and $$\sum_{n=1}^{\infty} \frac{H^{(k)}_n}{n^k}\, = \frac{\zeta{(2k)}+\zeta^{2}(k)}{2}. \tag{2}$$
Therefore, $$ 2 \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}H_{n}}{n^{3}} = -10 \zeta(6) + \frac{17}{2} \zeta(2) \zeta(4) + 4 \zeta^{2}(3) - 2 \zeta^{3}(2) + \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}}{n^{4}} .$$
To evaluate $ \displaystyle \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}}{n^{4}}$ consider $$ g(z) = \frac{\Big(\psi_{1}(-z) \Big)^{2}}{z^{\color{red}{3}}} $$ and integrate around the same contour.
The function $g(z)$ has poles of order 4 at the positive integers and a pole of order 7 at the origin.
Then again because the integral vanishes as $ N \to \infty$ through the positive integers, $$\sum_{n=0}^{\infty} \text{Res}[g(z), n] =0.$$
Expanding at the positive integers, we get $$ \begin{align} g(z) &= \frac{1}{z^{3}} \Bigg[\frac{1}{(z-n)^{2}}+ \Big(H_{n}^{(2)} + \zeta(2) \Big) - 2 \Big(H_{n}^{(3)}-\zeta(3)\Big) (z-n) + \mathcal{O}\Big((z-n)^{2}\Big) \Bigg]^{2} \\ &= \frac{1}{z^{3}} \Bigg(\frac{1}{(z-n)^{4}} + \frac{2 H_{n}^{(2)}+2 \zeta(2)}{(z-n)^{2}} - \frac{4H_{n}^{(3)} -4 \zeta(3)}{z-n} + \mathcal{O}(1) \Bigg) .\end{align}$$
So at the positive integers, $$ \begin{align} \text{Res} [g(z),n] &= \text{Res} \Bigg[ \frac{1}{z^{3}} \frac{1}{(z-n)^{4}},n \Bigg] + \text{Res} \Bigg[ \frac{1}{z^{3}} \frac{2 H_{n}^{(2)} + 2 \zeta(2)}{(z-n)^{2}},n\Bigg] + \text{Res} \Bigg[ \frac{4 \zeta(3) - 4 H_{n}^{(3)}}{z-n},n\Bigg] \\ &= -\frac{10}{n^{6}} - \frac{6 H_{n}^{(2)}}{n^{4}} - \frac{6 \zeta(2)}{n^{4}} - \frac{4 H_{n}^{(3)}}{n^{3}} + \frac{4 \zeta(3)}{n^{3}} . \end{align}$$
And expanding at the origin, we get $$ \begin{align} g(z) &= \frac{1}{z^{3}} \Big( \frac{1}{z^{2}} + \zeta(2) + 2 \zeta(3) z + 3 \zeta(4) z^{2} + 4 \zeta(5) z^{3} + 5 \zeta(6)z^{4} + \mathcal{O}(z^{5}) \Big)^{2} \\ &= \frac{1}{n^{7}} + \frac{2 \zeta(3)}{z^{5}} + \frac{2 \zeta(3)}{z^{4}} + \frac{6 \zeta(4) + \zeta^{2}(z)}{z^{3}} + \frac{9 \zeta(5) + 4 \zeta(2) \zeta(3)}{z^{2}} \\ &+ \frac{10 \zeta(6) + 6 \zeta(2) \zeta(4)+ 4 \zeta^{2}(3)}{z} + \mathcal{O}(1) . \end{align}$$
Therefore, $$ \text{Res}[g(z),0] = 10 \zeta(6) + 6 \zeta(2) \zeta(4)+ 4 \zeta^{2}(3) .$$
Summing up all the residues, $$\displaystyle -10 \zeta(6) - 6 \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}}{n^{4}} - 6 \zeta(2) \zeta(4) - 4 \sum_{n=1}^{\infty} \frac{H_{n}^{(3)}}{n^{3}} + 4 \zeta^{2}(3) + 10 \zeta(6) + 6 \zeta(2) \zeta(4) + 4 \zeta^{2}(3) =0, $$
which implies $$ \displaystyle \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}}{n^{4}} = \zeta^{2}(3) - \frac{\zeta(6)}{3} .$$
Combining this result with the previous result, we get $$ \displaystyle \sum_{n=1}^{\infty} \frac{H_{n}^{(2)}H_{n}}{n^{3}} = - \frac{31}{6} \zeta(6) + \frac{17}{4} \zeta(2) \zeta(4) + \frac{5}{2} \zeta^{2}(3) - \zeta^{3}(2) \approx 1.4716926365,$$
which is equivalent to your answer.
$ $
$(1)$ Generalized Euler sum $\sum_{n=1}^\infty \frac{H_n}{n^q}$
$(2)$ Intruiging Symmetric harmonic sum $\sum_{n\geq 1} \frac{H^{(k)}_n}{n^k}\, = \frac{\zeta{(2k)}+\zeta^{2}(k)}{2}$