• Chinese Optics Letters
  • Vol. 18, Issue 7, 070601 (2020)
Mi Li*, Yuan Chen, Yuejiang Song, Cheng Zeng, and Xuping Zhang
Author Affiliations
  • Key Laboratory of Intelligent Optical Sensing and Manipulation, College of Engineering and Applied Sciences, Nanjing University, Nanjing 210093, China
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    DOI: 10.3788/COL202018.070601 Cite this Article Set citation alerts
    Mi Li, Yuan Chen, Yuejiang Song, Cheng Zeng, Xuping Zhang. DOE effect on BER performance in MSK space uplink chaotic optical communication[J]. Chinese Optics Letters, 2020, 18(7): 070601 Copy Citation Text show less

    Abstract

    With the increasing demand for space optical communication security, space chaotic optical communication has attracted a great amount of attention. Compared with traditional space optical communication, a chaotic optical communication system has a higher bit error rate (BER) for its complex system design. In order to decrease the BER of space chaotic optical communication systems, we introduce two diffractive optical elements (DOEs) at a transmitting terminal (Tx). That is because the commonly used reflective optical antenna at Tx blocks the central part of the transmission beam, which leads to a great amount of power consumption. Introducing the DOEs into the optical subsystem at Tx can reshape the transmission beam from a Gaussian distribution to a hollow Gaussian distribution so that the block of the secondary mirror in the reflective optical antenna can be avoided. In terms of the DOE influence on communication quality, we give a BER model based on a minimum-shift-key (MSK) space uplink chaotic optical communication system to describe the DOE function. Based on the model, we further investigate the effect of the DOEs through analyzing the BER relationship versus basic system parameters based on the BER model. Both different mismatch conditions of chaotic systems and different atmospheric turbulence conditions are considered. These results will be helpful for the scheme design of space uplink chaotic optical communication systems.
    A30={er32w032r30<|r3|<r3m0otherwise,(1)

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    A31={α·E0E30·er32w032r30<|r3|<r3m0otherwise,(2)

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    I4(x4,y4)={(1λL)2·|F{A30(x30,y30)}|2without DOE(1λL)2·|F{A31(x31,y31)}|2with DOE,(3)

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    PI(r,I)=12πσI2(r,L)1I·exp{[lnI12RRRRI4(x4,y4)dx4dy4+2r2W2+σI2(r,L)2]22σI2(r,L)},(4)

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    P(r)=rσr2exp(r22σr2),(5)

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    σ12=σd12+σd12+σn2,(6)

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    σ02=σd02+σd02+σn2,(7)

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    m1=Ge(Kb+Ks)+2IdcTs,(8)

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    m0=GeKb+2IdcTs,(9)

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    BERDCD=14[erfc(m0+a22σ1)+erfc(m0a22σ1)],(10)

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    BER=00BERDCD·12πσI2(r,L)·1Irσr2exp(r22σr2)·exp{[ln2IRRRRI4(x4,y4)dx4dy4+2r2W2+σI2(r,L)2]22σI2(r,L)}drdI.(11)

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    rlarge=m1σd12+σd12+1/2K2σmlarge2,(12)

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    rsmall=m1σd12+σd12+0.1·(1/2K2σmlarge2),(13)

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    Δσn2=12K2·0.112K2·0.01=0.09·12K2,(14)

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    Mi Li, Yuan Chen, Yuejiang Song, Cheng Zeng, Xuping Zhang. DOE effect on BER performance in MSK space uplink chaotic optical communication[J]. Chinese Optics Letters, 2020, 18(7): 070601
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