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具有横向效应的半导体 器的同步传输技术

赵丽娜,魏庆涛

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赵丽娜, 魏庆涛. 具有横向效应的半导体 器的同步传输技术[J]. , 2023, 16(3): 559-566. doi: 10.37188/CO.2022-0031
引用本文: 赵丽娜, 魏庆涛. 具有横向效应的半导体 器的同步传输技术[J]. , 2023, 16(3): 559-566.doi:10.37188/CO.2022-0031
ZHAO Li-na, WEI Qing-tao. Synchronization transmission technology of semiconductor lasers with transverse effect[J]. Chinese Optics, 2023, 16(3): 559-566. doi: 10.37188/CO.2022-0031
Citation: ZHAO Li-na, WEI Qing-tao. Synchronization transmission technology of semiconductor lasers with transverse effect[J].Chinese Optics, 2023, 16(3): 559-566.doi:10.37188/CO.2022-0031

具有横向效应的半导体 器的同步传输技术

doi:10.37188/CO.2022-0031
基金项目:辽宁省教育厅科学研究面上项目(No. LJKMZ20221912,No. LJKZ1354)
详细信息
    作者简介:

    赵丽娜(1982—),女,辽宁大连人,博士,副教授,2008年,2021年于大连交通大学分别获得硕士、博士学位。主要从事非线性光学以及光通信方面的研究。E-mail:68225578@qq.com

  • 中图分类号:O439

Synchronization transmission technology of semiconductor lasers with transverse effect

Funds:Supported by Scientific Research Project of Education Department of Liaoning Province (No. LJKMZ20221912, No.LJKZ1354)
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  • 摘要:

    通过修正描述半导体 器的动力学模型,给出了具有横向效应的半导体 器的动力学方程,并分析了横向效应对半导体 器输出特性的影响。在此基础上,进一步研究了具有横向效应的半导体 器输出信号的同步传输技术。结果表明,考虑横向效应后,半导体 器的输出呈现新的时空混沌态,且对初始值非常敏感。同时,无论是利用半导体 器进行单通道信号的同步传输还是多通道信号的同步传输,其传输性能均十分稳定。该项同步技术十分简单,非常易于实际应用。

  • 图 1方程(2)的Lyapunov指数

    Figure 1.Lyapunov exponent of equation (2)

    图 2混沌吸引子(c=0.73)

    Figure 2.Chaotic attractor (c=0.73)

    图 3 输出随时间的演化(c=0.73)

    Figure 3.Evolution of laser output with time (c=0.73)

    图 4混沌吸引子(c=−2)

    Figure 4.Chaotic attractor (c=−2)

    图 5 输出随时间的演化(c=−2)

    Figure 5.Evolution of laser output with time (c=−2)

    图 6半导体 器输出随时空演化曲线

    Figure 6.Evolution curve of semiconductor laser output with time and space

    图 7耦合系统的最大Lyapunov指数

    Figure 7.Maximum Lyapunov exponent of the coupled system

    图 8两个半导体 器状态变量之间的误差 $ {e_1}(r,t) $

    Figure 8.Error $ {e_1}(r,t) $ between state variables of two semiconductor lasers

    图 9两个半导体 器状态变量之间的误差 $ {e_2}(r,t) $

    Figure 9.Error $ {e_2}(r,t) $ between state variables of two semiconductor lasers

    图 10两个半导体 器状态变量之间的误差 $ {e_3}(r,t) $

    Figure 10.Error $ {e_3}(r,t) $ between state variables of two semiconductor lasers

    图 11多通道信号传输

    Figure 11.Multi-channel signal transmission

    图 12耦合系统的最大Lyapunov指数随耦合强度gi(i=1, 2, 3, 4)的演化

    Figure 12.Evolution of the maximum Lyapunov exponent of coupled system with coupling strengthgi(i=1, 2, 3, 4)

    图 13耦合系统状态变量之间的误差 ${e_{ij}}(r,t)(i = 1,2,3,4\;\;j = 1,2,3)$

    Figure 13.Error ${e_{ij}}(r,t)(i = 1,2,3,4\;\;j = 1,2,3)$ between the state variables of the coupling system

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出版历程
  • 收稿日期:2022-03-03
  • 修回日期:2022-03-23
  • 网络出版日期:2022-06-16

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