At $\mathfrak{su}(2)$, tensor product $3 \otimes 3$ can be decomposed to $3\otimes3=5\oplus3\oplus1$.
In this space, $|1,1\rangle \otimes |1,-1\rangle$ has weight $0$.
So we should be able to write down $$|1,1\rangle \otimes |1,-1\rangle=\alpha|2,0\rangle+\beta|1,0\rangle+\gamma|0,0\rangle.$$
How to calculate $\alpha,\beta,\gamma$?
Apply $\langle 2,0\mid$ on both sides so you get $\alpha$ on the right hand side (assuming standard normalization) and the inner product
$$ \langle 2,0 \mid 1,1 ; 1,-1 \rangle $$
in the
$$ \langle J M \mid j_1 j_2 ; m_1 , m_2 \rangle $$
notation. Now look at the Clebsch-Gordan recurrence relations (the recursion @JyrkiLahtonen refers to).
This is the special case of $j_1=j_2=m_1=-m_2$ in the article. But check that you are using the same normalization convention as the article before using that to check your answer.