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Product States

Canonical treatment: Product States maintains the complete tests, dynamics, examples, exercises, and references.

This bridge is intentionally limited to the factorization criterion and notation needed by the composition postulate.

A bipartite pure state is product across A∣BA|B when

∣Ψ⟩AB=∣ψ⟩A⊗∣ϕ⟩B.\lvert\Psi\rangle_{AB}=\lvert\psi\rangle_A\otimes\lvert\phi\rangle_B.

In a product basis, ∣Ψ⟩=∑ijCij∣i⟩∣j⟩\lvert\Psi\rangle=\sum_{ij}C_{ij}\lvert i\rangle\lvert j\rangle is product exactly when the coefficient matrix CC has rank one. For two qubits this is equivalent to det⁡C=0\det C=0 for a nonzero state.

For local observables,

⟨A⊗B⟩=⟨A⟩ψ⟨B⟩ϕ.\langle A\otimes B\rangle = \langle A\rangle_{\psi}\langle B\rangle_{\phi}.

Local superposition does not imply entanglement: ∣+⟩A⊗∣−⟩B\lvert+\rangle_A\otimes\lvert-\rangle_B remains product. Conversely, a sum of product-basis vectors need not factor.

Always state the subsystem split before calling a vector product. Continue to the canonical page for mixed product states, separability, local dynamics, and multipartite factorization.