A normalized bipartite pure state is entangled when it cannot be written as a product state . Equivalently, its Schmidt rank exceeds one. This definition concerns the specified partition into systems A and B; the mixed-state definition of separability requires a different convex-mixture condition.
A bipartite unitary operator is an entangling gate if it maps at least one product state to an entangled state. It need not entangle every product input. For example, the controlled-NOT gate entangles but leaves as a product. A gate that preserves every product input is not entangling, even if it exchanges the two subsystems.

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