I have a slight confusion with the two.
- From what I have understood, state vector describes pure states, which means that with a probability $1$, our state is going to be in that state. However, if we have a superposition state, how do we actually determine that the probability is classical and not the one due to quantum superposition?
- Can we actually use the density matrix to write the state vector? I am confused because say we consider a two level system, where I define the density matrix as the following in $Sz$ basis: \begin{align} \rho = \frac{1}{2}(|0><0| + |1><1|) \end{align} This means that when we use $Tr(P_n\rho)$ to find the probabilities, we get a $\frac{1}{2}$ for both |0>, |1> state. So why can we not write the following state vector: \begin{align} |\psi> = \frac{1}{\sqrt2}(|0> +|1>) \end{align}
- Lastly, can we say that a superposition state is a pure state, if the classical probability for it is $1$ or do we have to ensure the condition $Tr(\rho^2)=1$; are they equivalent?