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Local vs. Joint Measurements for the Entanglement of Assistance

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arxiv quant-ph/0206192 v2 pith:NSWIMPJL submitted 2002-06-27 quant-ph

classification quant-ph
keywords entanglementmeasurementspartiesstatesassistanceassistantassistantsconsider
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We consider a variant of the entanglement of assistance, as independently introduced by D.P. DiVincenzo {\em et al.} ({\tt quant-ph/9803033}) and O. Cohen (Phys. Rev. Lett. {\bf 80}, 2493 (1998)). Instead of considering three-party states in which one of the parties, the assistant, performs a measurement such that the remaining two parties are left with on average as much entanglement as possible, we consider four-party states where two parties play the role of assistants. We answer several questions that arise naturally in this scenario, such as (i) how much more entanglement can be produced when the assistants are allowed to perform joint measurements, (ii) for what type of states are local measurements sufficient, (iii) is it necessary for the second assistant to know the measurement outcome of the first, and (iv) are projective measurements sufficient or are more general POVMs needed?

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  1. Error exponents for tripartite-to-bipartite entanglement transformations

    quant-ph 2025-07 accept novelty 7.0 of 10

    For pure tripartite states, the optimal deterministic rate is the minimum of two min-entropies of entanglement, and the direct and strong converse error exponents are given by explicit rate formulas.

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