Author Affiliations
1School of Communication Engineering, Xidian University, Xi'an, Shaanxi 710071, China2Department of Applied Physics, School of Physics and Optoelectronic Engineering, Xidian University, Xi'an, Shaanxi 710071, Chinashow less
Fig. 1. Phase and intensity of Laguerre-Gaussian beams with p=1 and m=3. (a) Phase; (b) intensity
Fig. 2. Light intensity produced by the coherent superposition of U0,10 and U0,3. (a) Theoretical result; (b) experimental result
Fig. 3. Structure diagram of multiband multiband vortex optical communication system
Fig. 4. Dual-channel multiband modulation signal. (a) First signal; (b) second signal
Fig. 5. Encoding method
Fig. 6. 16 kinds of superimposed light intensity correlations. (a) Beam groups {U0,4,U0,6,U0,8,U0,10} and {U0,2,U0,3,U1,2,U1,3}; (b) beam groups {U0,4,U0,6,U0,8,U0,10} and {U0,-2,U0,-3,U1,2,U1,3}
Fig. 7. Phase distribution diagrams corresponding to 16 symbols. The left side represents the phase diagrams, the middle represents the theoretical simulation diagrams at z=0 m, and the right side is the light intensity diagrams recorded by the CCD camera at z=1 m
Fig. 8. Atmospheric turbulence phase simulation diagram at =1×10-14 m-2/3. (a) 3D simulation; (b) phase screen
Fig. 9. Light intensity diagrams under different atmospheric turbulence conditions. (a) =1×10-17 m-2/3; (b) =1×10-14 m-2/3
Fig. 10. Structure diagram of VGG16 model
Fig. 11. Training data set
Fig. 12. Test accuracy and test loss during training process
Symbol encoding | Selected beam | Light intensity shape description |
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0000 | U0,2+U0,4 | 2 petals | 0001 | U0,2+U0,6 | 4 petals | 0010 | U0,2+U0,8 | 6 petals | 0011 | U0,2+U0,10 | 8 petals | 0100 | U0,3+U0,4 | 1 petal | 0101 | U0,3+U0,6 | 3 petals | 0110 | U0,3+U0,8 | 5 petals | 0111 | U0,3+U0,10 | 7 petals | 1000 | U1,2+U0,4 | Two layers, 2 petals on the outer layer | 1001 | U1,2+U0,6 | Two layers, 4 petals on the outer layer | 1010 | U1,2+U0,8 | Two layers, 6 petals on the outer layer | 1011 | U1,2+U0,10 | Two layers, 8 petals on the outer layer | 1100 | U1,3+U0,4 | Two layers, 1 petal on the outer layer | 1101 | U1,3+U0,6 | Two layers, 3 petals on the outer layer | 1110 | U1,3+U0,8 | Two layers, 5 petals on the outer layer | 1111 | U1,3+U0,10 | Two layers, 7 petals on the outer layer | 编码理论和方法如下。①双通道,每一个信道可选择的光束集为四种LG光束,比如选择{U0,2,U0,3,U1,2,U1,3}和 {U0,4,U0,6,U0,8,U0,10}两组光束,记录下不同的花瓣数和光强信息。②为了提高识别的效果,使用阶数为1和0的两种LG光束,叠加后产生的光强将会被分成两层和单层两个种类。③涡旋光束的拓扑荷值选择4,6,8,10,叠加后将产生不同的花瓣,为了提高识别效果,尽可能大地增加叠加光强的差异性,因此使用的1阶和0阶涡旋光束的拓扑荷值有两种2和3,那么第二组光束中拓扑荷值的下标至少应该相差2。④如果不满足两组光束之间的拓扑荷值和阶数之间的关系,那么导致的结果仅仅是只增加了光强图案的大小,并不能改变形状。 |
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Table 1. Coding results of 16 kinds of symbols in beam sets {U0,4,U0,6,U0,8,U0,10} and {U0,2,U0,3,