At the proposed boundary , the identity from part (iv) yieldsBoth and are convex combinations of product states, so is a separable quantum state. For , the state is a convex combination of and the maximally mixed product state , and is therefore separable.
For the converse, the partial transpose of the maximally entangled projector is , where is the swap operator. ThereforeOn the antisymmetric subspace, has eigenvalue , so the corresponding eigenvalue of iswhich is negative exactly when . The positive partial transpose criterion then proves that is entangled. Thus
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