Entanglement of Four-Qubit Rank-22 Mixed States

preprint2015arXivOpen access

Abstract

It is known that there are three maximally entangled states ∣Φ1⟩=(∣0000⟩+∣1111⟩)/2\ket{Φ_1} = (\ket{0000} + \ket{1111}) / \sqrt{2}, ∣Φ2⟩=(2∣1111⟩+∣1000⟩+∣0100⟩+∣0010⟩+∣0001⟩)/6\ket{Φ_2} = (\sqrt{2} \ket{1111} + \ket{1000} + \ket{0100} + \ket{0010} + \ket{0001}) / \sqrt{6}, and ∣Φ3⟩=(∣1111⟩+∣1100⟩+∣0010⟩+∣0001⟩)/2\ket{Φ_3} = (\ket{1111} + \ket{1100} + \ket{0010} + \ket{0001}) / 2 in four-qubit system. It is also known that there are three independent measures Fj(4)(j=1,2,3){\cal F}^{(4)}_j \hspace{.2cm} (j=1,2,3) for true four-way quantum entanglement in the same system. In this paper we compute Fj(4){\cal F}^{(4)}_j and their corresponding linear monotones Gj(4){\cal G}^{(4)}_j for three rank-two mixed states $ρ_j = p \ket{Φ_j}\bra{Φ_j} + (1 - p) \ket{\mbox{W}_4} \bra{\mbox{W}_4}$, where $\ket{\mbox{W}_4} = (\ket{0111} + \ket{1011} + \ket{1101} + \ket{1110}) / 2$. We discuss the possible applications of our results briefly.

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