The state is a convex combination of product density operators and is therefore a separable quantum state. Every product density operator has a decomposition into product pure states, so
The Bell state has two nonzero Schmidt coefficients. Since the density operator is pure, every ensemble decomposition uses vectors in the same one-dimensional support, and hence
The four Bell states form an orthonormal basis, so their uniform mixture isIt is a product state and therefore
The linear extension of the stated k-reduction map isIt suffices to consider a pure state of Schmidt rank , because positivity is preserved by sums. WriteThenFor every , the Cauchy-Schwarz inequality givesThus the operator is a positive semidefinite operator. Applying this to every vector in a Schmidt-number- ensemble proves
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