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具有横向效应的半导体激光器的同步传输技术

赵丽娜 魏庆涛

赵丽娜, 魏庆涛. 具有横向效应的半导体激光器的同步传输技术[J]. 中国光学(中英文), 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激光器的同步传输技术[J]. 中国光学(中英文), 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激光器的同步传输技术

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)
More Information
  • 摘要:

    通过修正描述半导体激光器的动力学模型,给出了具有横向效应的半导体激光器的动力学方程,并分析了横向效应对半导体激光器输出特性的影响。在此基础上,进一步研究了具有横向效应的半导体激光器输出信号的同步传输技术。结果表明,考虑横向效应后,半导体激光器的输出呈现新的时空混沌态,且对初始值非常敏感。同时,无论是利用半导体激光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  激光输出随时间的演化(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  激光输出随时间的演化(c=−2)

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

    图 6  半导体激光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  两个半导体激光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  两个半导体激光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  两个半导体激光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 strength gi (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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