MDI-QKD system and MDI-QKD method
A public measurement and laser technology, applied in the field of quantum communication, can solve problems such as complex system structure, high-speed coding application limitations, and limited device performance levels, and achieve the effect of reducing usage and simplifying structure
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Embodiment 1
[0061] The present invention is based on the theory of injection-locked semiconductor lasers. The concept of injection-locked was first proposed by R. Adler in 1946, and then K. Kurokawa explained the physical model and mathematical theory of injection-locked. When an oscillator is injected with a reference signal, when certain conditions are met between the power and frequency of the injected reference signal and the intrinsic frequency of the oscillator, the injected reference signal causes the oscillator to undergo stimulated radiation, and the stimulated radiation consumes The carriers in the resonant cavity of the oscillator saturate the optical gain in the resonant cavity, the intrinsic lasing of the oscillator is suppressed, and the frequency of the outgoing light becomes the frequency of the stimulated radiation light, that is, the frequency of the oscillator is due to the injection of the reference signal And re-stabilize on the frequency of the injected signal, and th...
Embodiment 2
[0100] Embodiment 1 adopts the three-state MDI-QKD protocol, and in this embodiment, the four-state phase-time coding is applied to the MDI-QKD protocol, as follows:
[0101] The MDI-QKD system structure of the present embodiment (as Figure 5 shown) is basically the same as Embodiment 1, the difference is that a phase modulator PM is added between the slave laser LD1 / LD2 and the adjustable optical attenuator VOA at the user end for the preparation of the phase-encoded quantum state. The functions realized by other devices are the same as those in Embodiment 1.
[0102]The four quantum states prepared by the MDI-QKD system in this embodiment include two short pulse pair intensity distribution states of |01> and |10> in Example 1, and their corresponding relationship with bit values 0 and 1 are the same as in Example 1 The same, the preparation process is also the same as that of Example 1; it also includes |0>, |π> quantum states of the internal phase difference of two shor...
Embodiment 3
[0114] In embodiment 1, the system passes through the synchronization module ( figure 2 Not shown in ) to control two short pulses excited from the lasers LD1 and LD2 can arrive at the beam splitter 3 for interference at the same time. This embodiment provides an example of this synchronization module, as Figure 7 shown. Because the synchronization of the two optical signals of Alice and Bob is mainly affected by the difference between the two long-distance separated quantum channels 1 and 2, the circular path is constructed to make the optical signal of Alice at the user end pass through the quantum channel 1 and quantum channel 2. 2. The optical signal of Bob at the user end also passes through quantum channel 1 and quantum channel 2, so the influence of the path difference on synchronization can be avoided.
[0115] Such as Figure 7 As shown, path selection module A and path selection module B are respectively added in user end Alice and Bob to connect the walking path...
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