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Exact monogamy constraints on entanglement of four-qubit pure states

S. Shelly Sharma

Published Feb 3, 2020• 0 citations
OpenAlex

Abstract

We report a set of monogamy constraints on one-tangle, two-tangles, three-tangles and four-way correlations of a general four-qubit pure state. It is found that given a two-qubit marginal $\rho$ of an $N$ qubit pure state $\left\vert \Psi_{N}\right\rangle $, the non-Hermitian matrix $\rho \widetilde{\rho}$ where $\widetilde{\rho}$ $=\left( \sigma_{y}\otimes \sigma_{y}\right) \rho^{\ast}\left( \sigma_{y}\otimes\sigma_{y}\right) $, contains information not only about the entanglement properties of the two-qubits in that state but also about the correlations of the pair of qubits with $\left( N-2\right) $ qubits in $\left\vert \Psi_{N}\right\rangle $. To extract information about tangles of a four-qubit state $\left\vert \Psi_{4}\right\rangle $, the coefficients in the characteristic polynomial of matrix $\rho\widetilde{\rho}$ are analytically expressed in terms of $2\times2$ matrices of state coefficients. A general monogamy relation satisfied by one-tangle, two-tangles, three-tangles, and residual correlations in a multiqubit state $\left\vert \Psi_{N}\right\rangle $ is also given.

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We report a set of monogamy constraints on one-tangle, two-tangles, three-tangles and four-way correlations of a general four-qubit pure state. It is found that given a two-qubit marginal ρ\rhoρ of an NNN qubit pure state ∣ΨN⟩\left\vert \Psi_{N}\right\rangle ∣ΨN​⟩, the non-Hermitian matrix ρρ~\rho \widetilde{\rho}ρρ​ where ρ~\widetilde{\rho}ρ​ =(σy⊗σy)ρ∗(σy⊗σy)=\left( \sigma_{y}\otimes \sigma_{y}\right) \rho^{\ast}\left( \sigma_{y}\otimes\sigma_{y}\right) =(σy​⊗σy​)ρ∗(σy​⊗σy​), contains information not only about the entanglement properties of the two-qubits in that state but also about the correlations of the pair of qubits with (N−2)\left( N-2\right) (N−2) qubits in ∣ΨN⟩\left\vert \Psi_{N}\right\rangle ∣ΨN​⟩. To extract information about tangles of a four-qubit state ∣Ψ4⟩\left\vert \Psi_{4}\right\rangle ∣Ψ4​⟩, the coefficients in the characteristic polynomial of matrix ρρ~\rho\widetilde{\rho}ρρ​ are analytically expressed in terms of 2×22\times22×2 matrices of state coefficients. A general monogamy relation satisfied by one-tangle, two-tangles, three-tangles, and residual correlations in a multiqubit state ∣ΨN⟩\left\vert \Psi_{N}\right\rangle ∣ΨN​⟩ is also given.
Given a multipartite quantum system that consists of two-level particles (qubits), one may or may not have access to all the subsystems. What can we know about the entanglement of the multiqubit system and residual correlations beyond two-tangle if we have access only to two-qubits at a time? Algebraic analysis of two-qubit states yields monogamy constraints on distribution of entanglement between sub-systems of an N-qubit state and criterion to determine if the state has multipartite entanglement. Monogamy constraints, reported in this letter, are relations between well known entanglement measures such as one-tangle, two-tangles and three-tangles of an N-qubit pure state.
We discuss the possibility to interpret the residual entanglement for more than three qubits in terms of distributed multipartite entanglement or, in other words, possible extensions of the Coffman-Kundu-Wootters monogamy equality to higher qubit numbers. Existing knowledge on entanglement in multipartite systems puts narrow constraints on the form of such extensions. We study various examples for families of pure four-qubit states for which the characterization of three-qubit and four-qubit entanglement in terms of polynomial invariants is known. These examples indicate that, although families with such extensions do exist, a generalized monogamy equality cannot be found along those lines.
We investigate the monogamy relations related to the concurrence and the entanglement of formation. General monogamy inequalities given by the $\ensuremath{\alpha}\text{th}$ power of concurrence and entanglement of formation are presented for NNN-qubit states. The monogamy relation for entanglement of assistance is also established. Based on these general monogamy relations, the residual entanglement of concurrence and entanglement of formation are studied. Some relations among the residual entanglement, entanglement of assistance, and three tangle are also presented.