The state of a particle moving along x is described by a complex wave function ψ(x,t) such that
dP=∣ψ(x,t)∣2dx
is the probability of finding the particle between x and x+dx at the time t (Born’s rule); hence the normalisation ∫−∞∞∣ψ∣2dx=1, and the expectation values ⟨x⟩=∫x∣ψ∣2dx, Δx2=⟨x2⟩−⟨x⟩2. Wave functions obey the superposition principle: if ψ1 and ψ2 are possible states, so is αψ1+βψ2 (normalised), and the probabilities then contain the interference term 2Re(α∗βψ1∗ψ2). A global phase factor eiθ changes nothing; a relative phase between two superposed components changes the interference.