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Then the results are that afterward: | |
For every value of $\lambda$, there is a probability of $|\langle\Psi|\Psi_\lambda\rangle|^2$ that the system is in state $|\Psi_\lambda\rangle$ | |
This is captured by the density matrix formalism as the transition | |
$|\Psi\rangle\langle\Psi|\Rightarrow\sum_\lambda|\langle\Psi|\Psi_\lambda\rangle|^2|\Psi_\lambda\rangle\langle\Psi_\lambda|$ | |
atyy I guess thinking about it classically, Demystifier's argument must be right. |