Composable security analysis of linear optics cloning machine improved discretized polar modulation continuous-variable quantum key distribution

He Ying; Wang Tian-Yi; Li Ying-Ying

doi:10.7498/aps.73.20241094

Abstract

In experimental setups of continuous-variable quantum key distribution (CVQKD) independently modulating the amplitude and phase of coherent states, the ideal Gaussian modulation will be degraded into discretized polar modulation (DPM) due to the finite resolution of the driving voltages of electro-optical modulators. To compensate for the performance degradation induced by the joint effect of amplitude and phase discretization, linear optics cloning machine (LOCM) can be introduced on the receiver side. Implemented by linear optical elements, heterodyne detection and controlled displacement, LOCM introduces extra noise that can be transformed into an advantageous one to combat channel excess noise by dynamically adjusting the relevant parameters into a suitable range. In this paper, the prepare-and-measure version of LOCM DPM-CVQKD is presented, where the incoming signal state enters a tunable LOCM before being measured by the nonideal heterodyne detector. The equivalent entanglement-based model is also established to perform security analysis, where the LOCM is reformulated into combination of the incoming signal state and a thermal state on a beam splitter. The composable secret key rate is derived to investigate the security of LOCM DPM-CVQKD. Simulation results demonstrate that the composable secret key rate and transmission distance are closely related to the tuning gain and the transmittance of LOCM. Once these two parameters are set to appropriate values, LOCM can improve the secret key rate and transmission distance of DPM-CVQKD, as well as its resistance to excess noise. Meanwhile, taking finite-size effect into consideration, the LOCM can also effectively reduce the requirement for the block size of the exchanged signals, which is beneficial to the feasibility and practicability of CVQKD. Owing to the fact that the performance of LOCM DPM-CVQKD is largely reliant on the calibration selection of relevant parameters, further research may concentrate on the optimization of LOCM in experimental implementations, where machine learning related methods may be utilized.

Keywords:

Authors and contacts

College of Big Data and Information Engineering, Guizhou University, Guiyang 550025, China

Corresponding author: Wang Tian-Yi, tywang@gzu.edu.cn

Funds: Project supported by the National Natural Science Foundation of China (Grant No. 62361009) and the Science and Technology Projects of Guizhou Province, China (Grant No. ZK[2021]304).

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References

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Cited By

图 1 LOCM DPM-CVQKD的制备测量方案

Figure 1. The PM scheme of LOCM DPM-CVQKD protocol.

DownLoad: Full-Size Img PowerPoint

图 2 LOCM DPM-CVQKD的纠缠等价方案

Figure 2. The EB scheme of LOCM DPM-CVQKD protocol.

DownLoad: Full-Size Img PowerPoint

图 3 LOCM对DPM-CVQKD可组合安全密钥率的改进

Figure 3. Enhancement of LOCM on the composable secret key rate of DPM-CVQKD.

DownLoad: Full-Size Img PowerPoint

图 4 LOCM对DPM-CVQKD可容忍过量噪声的改进

Figure 4. Enhancement of LOCM on the tolerable excess noise of DPM-CVQKD.

DownLoad: Full-Size Img PowerPoint

图 5 调制方差对最大传输距离的影响, 幅值分辨率和相位分辨率分别设置为${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$

Figure 5. The effect of modulation variance on maximum transmission distance, the amplitude resolution and phase resolution are ${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$, respectively.

DownLoad: Full-Size Img PowerPoint

图 6 LOCM参数对可组合安全密钥率的影响, 幅值分辨率和相位分辨率分别设置为${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$

Figure 6. Effect of LOCM-related parameters on the composable secret key rate, the amplitude resolution and phase resolution are ${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$, respectively.

DownLoad: Full-Size Img PowerPoint

图 7 LOCM参数对最大传输距离的影响, 幅值分辨率和相位分辨率分别设置为${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$　(a)调谐增益$\lambda $与传输损耗的关系; (b)等效透射率$\tau $与传输损耗的关系

Figure 7. Effect of LOCM parameters on maximum transmission distance, the amplitude resolution and phase resolution are set to ${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$, respectively: (a) The tuning gain $\lambda $ versus losses; (b) the equivalent transmittance $\tau $ versus losses.

DownLoad: Full-Size Img PowerPoint

图 8 不同传输距离下码长对可组合安全密钥率的影响, 幅值分辨率和相位分辨率分别设置为${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$

Figure 8. Effect of block length on the composable secret key rate under different transmission distances, the amplitude resolution and phase resolution are set to ${\delta _{\text{a}}} = 0.25$, ${\delta _{\text{p}}} = 0.02$, respectively.

DownLoad: Full-Size Img PowerPoint

[1]	Portmann C, Renner R 2022 Rev. Mod. Phys. 94 025008 Google Scholar
[2]	Pirandola S, Andersen U L, Banchi L, Berta M, Bunandar D, Colbeck R, Englund D, Gehring T, Lupo C, Ottaviani C, Pereira J L, Razavi M, Shaari J S, Tomamichel M, Usenko V C, Vallone G, Villoresi P, Wallden P 2020 Adv. Opt. Photonics 12 1012 Google Scholar
[3]	Zhang C X, Wu D, Cui P W, Ma J C, Wang Y, An J M 2023 Chin. Phys. B 32 124207 Google Scholar
[4]	Zapatero V, Navarrete A, Curty M 2024 Adv. Quantum Technol. 202300380
[5]	Diamanti E, Leverrier A 2015 Entropy 17 6072 Google Scholar
[6]	Laudenbach F, Pacher C, Fung C H F, Poppe A, Peev M, Schrenk B, Hentschel M, Walther P, Hubel H 2018 Adv. Quantum Technol. 1 1800011 Google Scholar
[7]	Guo H, Li Z, Yu S, Zhang Y C 2021 Fundam. Res. 1 96 Google Scholar
[8]	Zhang Y C, Bian Y M, Li Z Y, Yu S 2024 Appl. Phys. Rev. 11 011318 Google Scholar
[9]	Leverrier A 2015 Phys. Rev. Lett. 114 070501 Google Scholar
[10]	Leverrier A 2017 Phys. Rev. Lett. 118 200501 Google Scholar
[11]	Zhang Y C, Li Z Y, Chen Z Y, Weedbrook C; Zhao Y J, Wang X Y, Huang Y D, Xu C C, Zhang X X, Wang Z Y, Li M, Zhang X Y, Zheng Z Y, Chu B J, Gao X Y, Meng N, Cai W W, Wang Z, Wang G, Yu S, Guo H 2019 Quantum Sci. Technol. 4 035006 Google Scholar
[12]	Zhang Y C, Chen Z Y, Pirandola S, Wang X Y, Zhou C, Chu B J, Zhao Y J, Xu B J, Yu S, Guo H 2020 Phys. Rev. Lett. 125 010502 Google Scholar
[13]	Jain N, Chin H M, Mani H, Lupo C, Nikolic D S, Kordts A, Pirandola S, Pedersen T B, Kolb M, Omer B, Pacher C, Gehring T, Andersen U L 2022 Nat. Commun. 13 4740 Google Scholar
[14]	Hajomer A A E, Derkach I, Jain N, Chin H M, Andersen U L, Gehring T 2024 Sci. Adv. 10 eadi9474 Google Scholar
[15]	Wang T, Huang P, Li L, Zhou Y M, Zeng G H 2024 New J. Phys. 26 023002 Google Scholar
[16]	廖骎, 柳海杰, 王铮, 朱凌瑾 2023 物理学报 72 040301 Google Scholar Liao Q, Liu H J, Wang Z, Zhu L J 2023 Acta Phys. Sin. 72 040301 Google Scholar
[17]	Chen Z Y, Wang X Y, Yu S, Li Z Y, Guo H 2023 npj Quantum Inf. 9 28 Google Scholar
[18]	Zheng Y, Wang Y L, Fang C L, Shi H B, Pan W 2024 Phys. Rev. A 109 022424 Google Scholar
[19]	张光伟, 白建东, 颉琦, 靳晶晶, 张永梅, 刘文元 2024 物理学报 73 060301 Google Scholar Zhang G W, Bai J D, Jie Q, Jin J J, Zhang Y M, Liu W Y 2024 Acta Phys. Sin. 73 060301 Google Scholar
[20]	Jouguet P, Kunz-Jacques S, Diamanti E, Leverrier A 2012 Phys. Rev. A 86 032309 Google Scholar
[21]	吴晓东, 黄端, 黄鹏, 郭迎 2022 物理学报 71 240304.Google Scholar Wu X D, Huang D, Huang P, Guo Y, 2022 Acta Phys. Sin. 71 240304 Google Scholar
[22]	张云杰, 王旭阳, 张瑜, 王宁, 贾雁翔, 史玉琪, 卢振国, 邹俊, 李永民 2024 物理学报 73 060302 Google Scholar Zhang Y J, Wang X Y, Zhang Y, Wang N, Jia Y X, Shi Y Q, Lu Z G, Zou J, Li Y M 2024 Acta Phys. Sin. 73 060302 Google Scholar
[23]	Lupo C 2020 Phys. Rev. A 102 022623 Google Scholar
[24]	Wang T Y, Li M, Wang X 2022 Opt. Express 30 36122 Google Scholar
[25]	Wang T Y, Li M, Wang X, Hou L 2023 Opt. Express 31 21014 Google Scholar
[26]	Guo Y, Lv G, Zeng G H 2015 Quantum Inf. Process. 14 4323 Google Scholar
[27]	Wu X D, Liao Q, Huang D, Wu X H, Guo Y 2017 Chin. Phys. B 26 110304 Google Scholar
[28]	Zhang H, Mao Y, Huang D, Guo Y, Wu X D, Zhang L 2018 Chin. Phys. B 27 090307 Google Scholar
[29]	Yang F L, Qiu D W 2020 Quantum Inf. Process. 19 99 Google Scholar
[30]	He Y, Wang T Y 2024 Quantum Inf Process. 23 135 Google Scholar
[31]	Mao Y Y, Wang Y J, Guo Y, Mao Y H, Huang W T 2021 Acta Phys. Sin. 70 110302 [毛宜钰, 王一军, 郭迎, 毛堉昊, 黄文体 2021 物理学报 70 110302]Google Scholar Mao Y Y, Wang Y J, Guo Y, Mao Y H, Huang W T 2021 Acta Phys. Sin. 70 110302 Google Scholar
[32]	吴晓东, 黄端 2023 物理学报 72 050303 Google Scholar Wu X D, Huang D 2023 Acta Phys. Sin. 72 050303 Google Scholar
[33]	Stefano P 2021 Phys. Rev. Res. 3 013279 Google Scholar
[34]	Pirandola S 2021 Phys. Rev. Res. 3 043014 Google Scholar
[35]	Mountogiannakis A G, Papanastasiou P, Pirandola S 2022 Phys. Rev. A 106 042606 Google Scholar
[36]	Liu J Y, Ding H J, Zhang C M, Xie S P, Wang Q 2019 Phys. Rev. Appl. 12 014059 Google Scholar
[37]	Liu J Y, Jiang Q Q, Ding H J, Ma X, Sun M S, Xu J X, Zhang C H, Xie S P, Li J, Zeng G H, Zhou X Y, Wang Q 2023 Sci. China Inf. Sci. 66 189402 Google Scholar
[38]	Zhang Z K, Liu W Q, Qi J, He C, Huang P 2023 Phys. Rev. A 107 062614 Google Scholar
[39]	Chin H M, Jain N, Zibar D, Andersen U L, Gehring T 2021 npj Quantum Inf. 7 20 Google Scholar
[40]	Xu J X, Ma X, Liu J Y, Zhang C H, Li H W, Zhou X Y, Wang Q 2024 Sci. China Inf. Sci. 67 202501 Google Scholar

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