2014
DOI: 10.1103/physreva.90.042334
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Measurement-device-independent quantum key distribution with a passive decoy-state method

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Cited by 17 publications
(11 citation statements)
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“…According to ref. 29 , the lower bound of can be given where λ = X or Z and the coefficients of the total gain in each mode are and The upper bound of can be obtained with The subscripts c 0 and c 1 denote Alice or Bob prepare a signal state and a decoy state, respectively. If a subscript 0 appears, then Alice or Bob prepares a vacuum state.…”
Section: Resultsmentioning
confidence: 99%
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“…According to ref. 29 , the lower bound of can be given where λ = X or Z and the coefficients of the total gain in each mode are and The upper bound of can be obtained with The subscripts c 0 and c 1 denote Alice or Bob prepare a signal state and a decoy state, respectively. If a subscript 0 appears, then Alice or Bob prepares a vacuum state.…”
Section: Resultsmentioning
confidence: 99%
“…we choose σ α = 5, which means the failure probability is 5.73 × 10 7 . These parameters used in our method are the same as those in the refs 12 and 29 . is the length of data in the situation that Alice has the c i mode and Bob has the c j mode, where i , j = 0 or 1.…”
Section: Resultsmentioning
confidence: 99%
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“…Among the proposals on how to implement the decoy-state MDI-QKD, most of them use three intensities [29][30][31][32][33] or one intensity [34], and show poorer performance compared with that using an infinite number of decoy-states. Recently, a four-intensity decoy-state method has been proposed [35], which largely improves the key generation rate and transmission distance.…”
Section: Introductionmentioning
confidence: 98%