A Quantum Cryptography Implementation Method Based on Quantum Light Source
A technology of quantum cryptography and implementation method, applied in the application field, can solve the problems of low coincidence rate, unreachable signal state of optimal strength, poor performance, etc., and achieve the effect of eliminating intensity modulation error, excellent practical performance, and avoiding information leakage
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Embodiment 1
[0020] In the scheme of the present invention, a decoy state method and a novel low-loss unequal-arm MZ interferometer are adopted.
[0021] In the QKD system conventionally using HSPS light sources of the present invention, the dual-mode light field state obtained from the parametric down-conversion process can be described as:
[0022]
[0023] Wherein|n>represents an n photon state, and Pn is the corresponding photon number distribution, and in the present invention, Pn obeys Poisson distribution; I and S represent leisure light and signal light respectively, and leisure light (mode I) is usually emitted by Alice Local detection is performed, while the signal light (mode S) is sent to the receiving end Bob.
[0024] The scheme for generating passive HSPS of the present invention is explained below. The main process can be divided into the following steps: the first step, after the parametric down-conversion process, the leisure light is divided into two parts after pass...
Embodiment 2
[0041] For the sake of simplicity in the experiment, only three events such as x, y, z are used to estimate the key extraction rate. The parameters used in the experiment satisfy 010 20 0 1 =tη 10 , η 2 =(1-t)η 20 , with η 1 >0,1-η 2 >0,1-η 1 -η 2 >0. due to d 1 >>1, for any n≥2, we can get:
[0042]
[0043] So for any n≥2 the following inequalities hold:
[0044]
[0045] Using the above formula and considering statistical fluctuations, the lower bound Y of the single photon responsivity can be obtained 1 L and an upper bound on the single-photon bit error rate
[0046]
[0047] where e 0 (=0.5) and Y 0 Respectively represent the qubit bit error rate and dark count at Bob's end in the vacuum state. Q ξ and E ξ (ξ=x, y, z) represent the total responsivity and qubit error in any ξ state, respectively;
[0048]
[0049] γ is the standard deviation of statistical fluctuation analysis, which is assumed to be a constant γ=5.3, and the corresponding...
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