Optical Fiber Communication Mynbaev Pdf 117 !!BETTER!! 🠶

warrod/ Dezembro 26, 2022/ Uncategorized/ 0 comments

Optical Fiber Communication Mynbaev Pdf 117 !!BETTER!! 🠶

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Optical Fiber Communication Mynbaev Pdf 117

To that end, we have analysed the theoretically most secure QKD protocols, the quantum twirling (QT) protocols,13,14,15,16 and compared their implementation with another previously published QT protocol, the practical cryptographic tunable universal two-photon source, PTunU2.17 We have shown that PTunU2 allows us to generate a lower-photon-number state than QT, which makes our protocol more suitable for boosting key generation rates. We have also formulated a general resource-efficient protocol, the generalized LT (GLT) protocol, that is mathematically equivalent to PTunU2 and is basically the same as QT protocol, but with some differences in the importance of the involved experimental parameters.

Specifically, we have shown that the protocols share some commonalities, but differ significantly in other important parameters. For example, we have calculated that MDI-QKD in the THA with the single-photon source requires a qubit assumption to guarantee the key generation rate, while PTunU2 works without any qubit assumption. We have shown that the performance of MDI-QKD depends on detector dark counts and accordingly we have formulated two different dark-count-based attack strategies. We have also found that the difference in performance between these two protocols can be attributed to the interaction between individual photons in the single-photon source. Specifically, the increased effect of noise in PTunU2 allows Eve to efficiently extract the key through photon-number splitting and the need for two-flip detection in MDI-QKD implies that they can sabotage the key generation process. For each of these attacks we have proposed counter-measures that can protect the key generation process, such as decoy-state21,22 or the counter-measure against photon-number splitting can be improved using some of QKD components, such as phase modulators.

All these different aspects have highlighted the importance of the source characterisation for QKD demonstrations. Namely, while any characterisation of the source is still sufficient if it only covers the parameters that are used to implement the protocol, complete characterisation is the only way to ensure the implementation security of the QKD protocol.

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