Let $L$ be the angular momentum, $S$ the spin and $l$ and $s$ the respective quantum numbers.
Then, there are $(2l+1)(2s+1)$ states $|l;m_l;s;m_s\rangle$ for fixed $l$ and $s$.
Let $J = L + S$ be the total angular momentum and $j$ the resprective quantum number.
I know that $|l-s| \leq j \leq l + s$ holds, but how to show that there are as many coupled states $|l;s;j;m_j\rangle$ as uncoupled states?