The coefficient matrix in the computational orthonormal bases, with Alice's index labelling rows, is
Since the entries are real, the reduced density matrices are
Both have trace one and determinant . Their characteristic polynomial is , so the nonzero eigenvalues are
Both are positive. Thus the Schmidt rank, or the Schmidt number of this pure state, is
If “Schmidt numbers” denotes the individual positive Schmidt coefficients instead, those are
Their squares are ; giving both the Schmidt rank and the Schmidt coefficients removes this terminology ambiguity. The pure state is entangled because its Schmidt rank exceeds one.

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