Continuous variable quantum key distribution variable transmittance and data bit frame synchronization method
A quantum key distribution and data synchronization technology, applied in the field of computer information, can solve problems such as synchronization difficulties and low signal-to-noise ratio, and achieve the effects of improving operating efficiency, facilitating integration, and resisting random phase drift.
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Embodiment 1
[0051] A continuous-variable quantum key distribution (CVQKD) variable transmittance and data bit frame synchronization method. This method is mainly applicable to CVQKD systems such as free space CVQKD or underwater CVQKD where the channel transmittance is variable. In contrast, the channel transmittance of traditional optical fiber CVQKD systems can usually be regarded as a constant. In the optical fiber CVQKD system, it is only necessary to synchronize the data of Alice and Bob, and then estimate the channel transmittance through the parameter estimation step. In CVQKD systems such as free space or underwater, we need to separate a part of the light to monitor in real time to obtain the channel transmittance of each pulse, and also need to synchronize the Alice-side data, Bob-side data and channel transmittance data. , this scheme proposes a method for synchronizing Bob's data and channel transmittance data. The main steps of the method are as follows: Step A: constructing...
Embodiment 2
[0069] In the continuous variable quantum key distribution system, the quantum state sent by Alice (the sender) is subject to Gaussian modulation, that is, the position and momentum of the quantum state are subject to Gaussian distribution. The sending end makes the transmitted data obey the Gaussian distribution by loading a signal that obeys Rayleigh distribution on the amplitude modulator AM and loading a uniformly distributed signal on the phase modulator PM. For the convenience of discussion, the following analysis takes the position component X of the quantum state as an example, and has the same result for the momentum component P. For the X component and P component that obey the Gaussian distribution, when modulated at the sending end, the purpose of encoding the X component and P component in the light field is achieved by modulating the amplitude and phase of the optical signal. The modulation amplitude is The phase is θ=angle(X+iP). Such as figure 1 As shown, ...
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