2009
DOI: 10.1103/physreva.79.022319
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Differential-quadrature-phase-shift quantum key distribution

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Cited by 20 publications
(11 citation statements)
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“…The former simplifies the estimation of Eve's information, but requires an overly complicated QKD receiver setup [13][14][15][16] , making it impractical. The latter separates the signal from the differential phase shift protocol into blocks, each having a global phase that varies randomly, ensuring the protocol is immune against coherent attacks 17,18 . It does, however, stray from the main goal of DPR protocols to provide simpler QKD implementations, due to the phase randomization requirement that would ordinarily require extra system components.…”
mentioning
confidence: 99%
“…The former simplifies the estimation of Eve's information, but requires an overly complicated QKD receiver setup [13][14][15][16] , making it impractical. The latter separates the signal from the differential phase shift protocol into blocks, each having a global phase that varies randomly, ensuring the protocol is immune against coherent attacks 17,18 . It does, however, stray from the main goal of DPR protocols to provide simpler QKD implementations, due to the phase randomization requirement that would ordinarily require extra system components.…”
mentioning
confidence: 99%
“…We performed the phase-encode BB84 and DQPS-QKD [2] protocols, wherein sequential pulses with phase differences of {0, π} {π/2, 3π/2} were transmitted and received with the setup shown in the dashed box, indicated by "Bob" in Fig. 1.…”
Section: Polarization-insensitive Active Basis Selectionmentioning
confidence: 99%
“…In phase-encoding BB84-based QKD protocols that transmit sequential pulses with phase differences of {0, π} {π/2, 3π/2}, the basis selection is performed by {0, π/2} phase modulation (PM) onto one arm of a delay Mach-Zehnder interferometer (MZI), i.e., active basis selection occurs, which requires phase stabilization for the MZI and polarization control for the phase modulation in practical implementation [1] . Alternatively, a combination of a beam splitter and two MZIs with path phase differences of 0 and π/2, respectively, followed by four single-photon detectors (SPDs), can also be used for passive basis selection [2] . This method is free from the phase-and polarization-control issues, but the receiver is massive and expensive.…”
Section: Introductionmentioning
confidence: 99%
“…Here we introduce a DQPS protocol considered in this work, which is slightly modified from the one [23] proposed by Inoue and Iwai (See Fig. 1).…”
Section: Protocolmentioning
confidence: 99%