2018
DOI: 10.1103/physreva.98.062335
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Entanglement robustness against particle loss in multiqubit systems

Abstract: When some of the parties of a multipartite entangled pure state are lost, the question arises whether the residual mixed state is also entangled, in which case the initial entangled pure state is said to be robust against particle loss. In this paper, we investigate this entanglement robustness for N -qubit pure states. We identify exhaustively all entangled states that are fragile, i.e., not robust, with respect to the loss of any single qubit of the system. We also study the entanglement robustness propertie… Show more

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Cited by 26 publications
(17 citation statements)
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“…The first example are states that possess a Schmidt decomposition [ 28 ], i.e., with . For qubits, these are exactly the states that become separable as soon as one particle is ignored [ 29 ]. A famous example is the m -partite Greenberger–Horne–Zeilinger (GHZ) state for which the local projective measurements on and are optimal, since the conditional state of all systems is a pure product state independently of the outcome and its energy can thus be minimised using local unitaries.…”
Section: Multipartite Daemonic Ergotropymentioning
confidence: 99%
“…The first example are states that possess a Schmidt decomposition [ 28 ], i.e., with . For qubits, these are exactly the states that become separable as soon as one particle is ignored [ 29 ]. A famous example is the m -partite Greenberger–Horne–Zeilinger (GHZ) state for which the local projective measurements on and are optimal, since the conditional state of all systems is a pure product state independently of the outcome and its energy can thus be minimised using local unitaries.…”
Section: Multipartite Daemonic Ergotropymentioning
confidence: 99%
“…Let us consider a possibility of non-invertible intermediate transformations of Lqubit states, i.e., non-invertible gates, which are described by the 2 L × 2 L matrices U(r) of (possibly) less than full rank 1 ≤ r ≤ 2 L . This can be related to the production of "degenerate" states (see, e.g., [43]), "particle loss" [53][54][55], and the role of ranks in multiparticle entanglement [56,57].…”
Section: Invertible and Noninvertible Quantum Gatesmentioning
confidence: 99%
“…Permutation symmetric N -qubit states draw attention due to their experimental feasibility and for the mathematical simplicity offered by them [49][50][51][52][53][54][55][56][57][58][59][60]. This class of states belong to the d = 2j + 1 = N + 1 dimensional subspace of the 2 N dimensional Hilbert space, which corresponds to the maximum value j = N/2 of angular momentum of N -qubit system.…”
Section: Violation Of Lsur By Permutation Symmetric N -Qubit Statesmentioning
confidence: 99%