A normalized state vector in a complex HH is a vector ψ∈H\psi\in H with ∥ψ∥=1\lVert\psi\rVert=1. It lies on the .

In quantum mechanics, ψ\psi and eiθψe^{i\theta}\psi represent the same pure state, because all transition probabilities depend only on squared inner-product magnitudes. The phase-independent state is equivalently represented by the ∣ψ⟩⟨ψ∣|\psi\rangle\langle\psi|.