PPLN-waveguide-based polarization entangled QKD simulator
dc.contributor.author | Gariano, John | |
dc.contributor.author | Djordjevic, Ivan B. | |
dc.date.accessioned | 2018-01-31T19:05:20Z | |
dc.date.available | 2018-01-31T19:05:20Z | |
dc.date.issued | 2017-08-30 | |
dc.identifier.citation | John Gariano, Ivan B. Djordjevic, "PPLN-waveguide-based polarization entangled QKD simulator", Proc. SPIE 10409, Quantum Communications and Quantum Imaging XV, 104090A (30 August 2017); doi: 10.1117/12.2272449; http://dx.doi.org/10.1117/12.2272449 | en |
dc.identifier.issn | 0277-786X | |
dc.identifier.doi | 10.1117/12.2272449 | |
dc.identifier.uri | http://hdl.handle.net/10150/626494 | |
dc.description.abstract | We have developed a comprehensive simulator to study the polarization entangled quantum key distribution (QKD) system, which takes various imperfections into account. We assume that a type-II SPDC source using a PPLN-based nonlinear optical waveguide is used to generate entangled photon pairs and implements the BB84 protocol, using two mutually unbiased basis with two orthogonal polarizations in each basis. The entangled photon pairs are then simulated to be transmitted to both parties; Alice and Bob, through the optical channel, imperfect optical elements and onto the imperfect detector. It is assumed that Eve has no control over the detectors, and can only gain information from the public channel and the intercept resend attack. The secure key rate (SKR) is calculated using an upper bound and by using actual code rates of LDPC codes implementable in FPGA hardware. After the verification of the simulation results, such as the pair generation rate and the number of error due to multiple pairs, for the ideal scenario, available in the literature, we then introduce various imperfections. Then, the results are compared to previously reported experimental results where a BBO nonlinear crystal is used, and the improvements in SKRs are determined for when a PPLN-waveguide is used instead. | |
dc.description.sponsorship | ONR MURI program [N00014-13-1-0627] | en |
dc.language.iso | en | en |
dc.publisher | SPIE-INT SOC OPTICAL ENGINEERING | en |
dc.relation.url | https://www.spiedigitallibrary.org/conference-proceedings-of-spie/10409/2272449/PPLN-waveguide-based-polarization-entangled-QKD-simulator/10.1117/12.2272449.full | en |
dc.rights | © (2017) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). | en |
dc.subject | Quantum Key Distribution | en |
dc.subject | Quantum cryptography | en |
dc.subject | Polarization entanglement | en |
dc.title | PPLN-waveguide-based polarization entangled QKD simulator | en |
dc.type | Article | en |
dc.identifier.eissn | 1996-756X | |
dc.contributor.department | Univ Arizona | en |
dc.identifier.journal | QUANTUM COMMUNICATIONS AND QUANTUM IMAGING XV | en |
dc.description.collectioninformation | This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu. | en |
dc.eprint.version | Final published version | en |
refterms.dateFOA | 2018-09-12T01:11:30Z | |
html.description.abstract | We have developed a comprehensive simulator to study the polarization entangled quantum key distribution (QKD) system, which takes various imperfections into account. We assume that a type-II SPDC source using a PPLN-based nonlinear optical waveguide is used to generate entangled photon pairs and implements the BB84 protocol, using two mutually unbiased basis with two orthogonal polarizations in each basis. The entangled photon pairs are then simulated to be transmitted to both parties; Alice and Bob, through the optical channel, imperfect optical elements and onto the imperfect detector. It is assumed that Eve has no control over the detectors, and can only gain information from the public channel and the intercept resend attack. The secure key rate (SKR) is calculated using an upper bound and by using actual code rates of LDPC codes implementable in FPGA hardware. After the verification of the simulation results, such as the pair generation rate and the number of error due to multiple pairs, for the ideal scenario, available in the literature, we then introduce various imperfections. Then, the results are compared to previously reported experimental results where a BBO nonlinear crystal is used, and the improvements in SKRs are determined for when a PPLN-waveguide is used instead. |