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Overcoming the repeaterless bound in continuous-variable quantum communication without quantum memories

2021/05/08 by Matthew S. Winnel, Joshua J. Guanzon, Winnel, Matthew S. +5 · 7 citations
Computer Science · Mathematics · Physics and Astronomy · #Computer science #FOS: Physical sciences #Mathematics #Physics #Quantum #Quantum Computing Algorithms and Architecture #Quantum Information and Cryptography #Quantum Mechanics and Applications #Quantum Physics (quant-ph) #Quantum mechanics #Variable (mathematics) #quant-ph

paper · pdf · doi:10.48550/arxiv.2105.03586

published in arXiv (Cornell University) (Cornell University) · 12 pages, 7 figures

arxiv created 2021/05/08 · openalex publication_date 2021/05/08 · arxiv updated 2021/05/11 · openalex created_date 2021/05/24 · openalex updated_date 2026/07/28

Abstract

One of the main problems in quantum communications is how to achieve high rates at long distances. Quantum repeaters, i.e., untrusted, intermediate relay stations, are necessary to overcome the repeaterless bound which sets the fundamental rate-distance limit of repeaterless communications. In this work, we introduce a continuous-variable protocol which overcomes the repeaterless bound and scales like the single-repeater bound using just one linear-optical device called a "quantum scissor", combining the entanglement distillation and entanglement swapping elements of previous repeater proposals into a single step, thus, removing the need for quantum memories. Implementing a standard continuous-variable quantum key distribution protocol using our repeater we predict key rates which surpass the repeaterless bound. Our protocol works well for non-ideal single-photon sources and non-ideal single-photon detectors, and can tolerate some level of excess noise, making our protocol implementable with existing technology. We show that our scheme can be extended to longer repeater chains using quantum memories, using less physical resources than previous schemes. Furthermore, for applications beyond key distribution, our scheme generalises to higher order and distils more entanglement at the cost of a reduced probability of success.

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