For a normalized pure state of two qubits with coefficient matrix , the concurrence is . It ranges from zero for a product state to one for a maximally entangled state.
For a normalized two-qubit pure state with coefficient matrix , concurrence is . The displayed convex roof extension defines its mixed-state version. Combining decompositions proves convexity: . Every separable quantum state has a decomposition into product vectors, each with zero determinant, so its concurrence is zero.
For , with invertible , a pure coefficient matrix transforms as . Its unnormalized determinant is multiplied by . The invertible filter bijects pure decompositions before and after conditioning, with branch weights rescaled by their success probabilities. Taking both infima in the convex roof extension gives the displayed exact scaling. If either filter has rank one, the retained state is separable across that party.
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