Consider one normalized measurement vector on C. The unnormalized partial inner product on AB isIts tensor-product coefficient matrix and determinant areThe two-qubit product-state determinant criterion therefore says that this branch is entangled whenever . Its probability is , so such a branch is physically possible and can be normalized without changing whether its determinant vanishes.
For an orthonormal basis , completeness gives . At least one vector has . Hence at least one nonzero-probability outcome leaves AB entangled, proving conditional entanglement of the three-qubit W state. Some bases give two entangled branches; the computational basis gives one entangled and one product branch. The claim is not that every outcome must entangle AB.
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