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Measurement-device-independent quantum secret sharing with hyper-encoding |
| Xing-Xing Ju(居星星)1,3, Wei Zhong(钟伟)3, Yu-Bo Sheng(盛宇波)2,3, and Lan Zhou(周澜)1,† |
1. College of Science, Nanjing University of Posts and Telecommunications, Nanjing 210023, China;
2. College of Electronic and Optical Engineering & College of Flexible Electronics (Future Technology), Nanjing University of Posts and Telecommunications, Nanjing 210023, China;
3. Institute of Quantum Information and Technology, Nanjing University of Posts and Telecommunications, Nanjing 210003, China |
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Abstract Quantum secret sharing (QSS) is a typical multi-party quantum communication mode, in which the key sender splits a key into several parts and the participants can obtain the key by cooperation. Measurement-device-independent quantum secret sharing (MDI-QSS) is immune to all possible attacks from measurement devices and can greatly enhance QSS's security in practical applications. However, previous MDI-QSS's key generation rate is relatively low. Here, we adopt the polarization-spatial-mode hyper-encoding technology in the MDI-QSS, which can increase single photon's channel capacity. Meanwhile, we use the cross-Kerr nonlinearity to realize the complete hyper-entangled Greenberger—Horne—Zeilinger state analysis. Both above factors can increase MDI-QSS's key generation rate by about 103. The proposed hyper-encoded MDI-QSS protocol may be useful for future multiparity quantum communication applications.
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Received: 25 March 2022
Revised: 10 May 2022
Accepted manuscript online:
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PACS:
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03.67.Pp
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(Quantum error correction and other methods for protection against decoherence)
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03.67.Hk
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(Quantum communication)
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03.65.Ud
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(Entanglement and quantum nonlocality)
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| Fund: Project supported by the National Natural Science Foundation of China (Grant Nos. 11974189 and 12175106). |
Corresponding Authors:
Lan Zhou
E-mail: zhoul@njupt.edu.cn
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Cite this article:
Xing-Xing Ju(居星星), Wei Zhong(钟伟), Yu-Bo Sheng(盛宇波), and Lan Zhou(周澜) Measurement-device-independent quantum secret sharing with hyper-encoding 2022 Chin. Phys. B 31 100302
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