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I have a slight confusion with the two.

  1. 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?
  2. 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}
  3. 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?

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