We can write a Singlet state of two $\frac{1}{2}$ spin particles like this:
$$|S\rangle = \frac{1}{\sqrt{2}}\left( |+ \rangle ⊗ |-\rangle - |-\rangle ⊗|+\rangle \right) $$
is this the same as writing this:
$$|S\rangle = \frac{1}{\sqrt{2}}\left( |+ \rangle |-\rangle - |-\rangle |+\rangle \right) $$ ?
Another example(from the Clebsch-Gordan Coeffiecients):
We have two particles one with spin $\frac{3}{2}$ and the other with spin $\frac{1}{2}$, we can then write the state $|2,1 \rangle$ the following way:
$$|2,1 \rangle = \frac{1}{2}\left|\frac{3}{2},\frac{3}{2} \right\rangle\left|\frac{3}{2},-\frac{1}{2} \right\rangle +\sqrt{\frac{3}{4}}\left|\frac{3}{2},\frac{1}{2} \right\rangle\left|\frac{3}{2},\frac{1}{2} \right\rangle$$
Is this as well to be meant as a tensor product? otherwise I dont see how to mulitply those kets.