2020
DOI: 10.1109/tqe.2020.3044179
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Protocols for Creating and Distilling Multipartite GHZ States With Bell Pairs

Abstract: The distribution of high-quality Greenberger-Horne-Zeilinger (GHZ) states is at the heart of many quantum communication tasks, ranging from extending the baseline of telescopes to secret sharing. They also play an important role in error-correction architectures for distributed quantum computation, where Bell pairs can be leveraged to create an entangled network of quantum computers. We investigate the creation and distillation of GHZ states out of nonperfect Bell pairs over quantum networks. In particular, we… Show more

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Cited by 32 publications
(17 citation statements)
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“…As mentioned in Section 4.2, EPR pairs can be obtained from multipartite states through a proper sequence of local operations assisted by classical communications 19 . But the reverse process -namely, obtaining a multipartite state such as a GHZ by fusing multiple EPR pairs [48,49,50,51] is possible as well. Regardless the particulars of the generation process, entanglement must be distributed among the network nodes through quantum links.…”
Section: Entanglement Generation and Distributionmentioning
confidence: 99%
“…As mentioned in Section 4.2, EPR pairs can be obtained from multipartite states through a proper sequence of local operations assisted by classical communications 19 . But the reverse process -namely, obtaining a multipartite state such as a GHZ by fusing multiple EPR pairs [48,49,50,51] is possible as well. Regardless the particulars of the generation process, entanglement must be distributed among the network nodes through quantum links.…”
Section: Entanglement Generation and Distributionmentioning
confidence: 99%
“…In addition to the physical implementation for entanglement sharing between nodes, a protocol for fault tolerance is required [5,14,54,56].…”
Section: Distributed Quantum Computingmentioning
confidence: 99%
“…• There exists a quantum channel which distills the state into a fixed number of cat-k states which is given by 1 k HP k (A) = 1 α area(m k ) which is strictly less than area(m 2 ). The loss of entanglement can be viewed as the consumption of bell pairs using quantum teleportation to manufacture the necessary correlations [22]. In general a large number of bell pairs are needed for each additional cat-k produced beyond area(t k ) |ψ −→ |k is a codimension-1 Riemannian manifold.…”
Section: S(mentioning
confidence: 99%