Double-scanning 4-intensity MDI-QKD method and system based on corrected coherent state light source
A dual-scan, light source technology, applied in key distribution, can solve the problems of code rate limitation and low single-photon rate, and achieve a wide range of effects.
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Embodiment 1
[0057] Such as figure 1 As shown, a dual-scan 4-intensity MDI-QKD system based on a modified coherent state light source includes three parts: Alice, Bob, and Charlie. Alice and Bob, as the sender, have exactly the same structure, and emit light to the third party Charlie at the same time pulse. Charlie, as the measurement party, measures the received light pulse pairs, and Charlie can also be an untrustworthy eavesdropper (Eve). This scheme is suitable for phase encoding system.
[0058] The workflow of this system includes:
[0059] (1) When the MCS light sources of Alice and Bob emit photons, it is necessary to ensure that the single photons on both sides have the same frequency, so that the two photons arriving at Charlie will interfere. In this embodiment, it can be implemented by using the frequency locking technology of the lasers on both sides.
[0060] (2) The MCS light sources of Alice and Bob respectively modulate and send N light pulses, and the light pulses at...
Embodiment 2
[0081] The difference between this embodiment and embodiment one is:
[0082] Such as figure 2 As shown, for the polarization encoding system, after the two-photon interference occurs at the beam splitter BS of the measurement party Charlie, Charlie performs the Bell state measurement, and uses two polarization beam splitters PBS and four single-photon detectors after the beam splitter BS The device SPD performs interferometry on the four polarization states.
Embodiment 3
[0084] A dual-scan 4-intensity MDI-QKD method based on a modified coherent state light source, from the perspective of the sender, includes the following steps:
[0085] Use the modified coherent state light source to modulate and send multiple light pulses. When sending light pulses, they are randomly modulated into different quantum states with a certain probability, and the parameters of the vacuum state and decoy state are numerically limited, and the parameters of the signal state are not limited. ;
[0086] Receive published measurements and screen your own bits;
[0087] The final key is obtained by post-processing the filtered bit string.
[0088] Specifically, there are two senders, and the optical pulses sent by each have the same photon frequency.
[0089] Specifically, the quantum state includes the vacuum state of the corresponding sender, the first decoy state and the second decoy state under the X basis vector, and the signal state under the Z basis vector.
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