Some similar questions have been ask before, but I still don't really get the definition of seperable states in quantum mechanics.
Consider a bell state of a two qubit system. \begin{align} \left|\Psi\right> = \frac{1}{\sqrt{2}}(\left|0 \right>_A\otimes \left|0\right>_B + \left|1 \right>_A\otimes \left|1\right>_B) \end{align} where the indices A and B denote the one qubit subsystems. I see, that this is not a product state and is therefore called an entangled state. So this means that the corresponding density matrix can not be seperable. So let's check this. The density matrix corresponding to the Bell state above is \begin{align} \rho &= \left|\Psi \right>\left<\Psi\right| \\ &= \frac{1}{2}(\left|0\right>_A\left<0\right|_A\otimes \left|0\right>_B\left<0\right|_B + \left|0\right>_A\left<1\right|_A\otimes \left|0\right>_B\left<1\right|_B + \left|1\right>_A\left<0\right|_A\otimes \left|1\right>_B\left<0\right|_B + \left|1\right>_A\left<1\right|_A\otimes \left|1\right>_B\left<1\right|_B ) \end{align}
Now a density matrix is called seperable, if it can be written as a convex combination of tensor products of the subsystem \begin{align} \rho_{sep} = \sum_ip_i (\rho^i_A\otimes \rho^i_B) \end{align} But if we take all the $p_i=\frac{1}{2}$ and take \begin{align} \rho^1_A &= \left|0\right>_A\left<0\right|_A \\ \rho^1_B &= \left|0\right>_B\left<0\right|_B \\ \\ \rho^2_A &= \left|0\right>_A\left<1\right|_A \\ \rho_B^2 &= \left|0\right>_B\left<1\right|_B \end{align} and so on we see that the density matrix corresponding to the Bell state can be written as a convex combination and therefore is seperable.
There must be a conceptual misunderstanding and I would be really thankful if one could help me cure this.