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智能反射表面辅助的全双工通信系统的物理层安全设计

齐本胜 饶星楠 邓志祥 苗红霞

齐本胜, 饶星楠, 邓志祥, 苗红霞. 智能反射表面辅助的全双工通信系统的物理层安全设计[J]. 电子与信息学报, 2023, 45(6): 1990-1998. doi: 10.11999/JEIT220547
引用本文: 齐本胜, 饶星楠, 邓志祥, 苗红霞. 智能反射表面辅助的全双工通信系统的物理层安全设计[J]. 电子与信息学报, 2023, 45(6): 1990-1998. doi: 10.11999/JEIT220547
QI Bensheng, RAO Xingnan, DENG Zhixiang, MIAO Hongxia. Physical Layer Security For Intelligent Reflecting Surface Assisted Full-duplex Communication[J]. Journal of Electronics & Information Technology, 2023, 45(6): 1990-1998. doi: 10.11999/JEIT220547
Citation: QI Bensheng, RAO Xingnan, DENG Zhixiang, MIAO Hongxia. Physical Layer Security For Intelligent Reflecting Surface Assisted Full-duplex Communication[J]. Journal of Electronics & Information Technology, 2023, 45(6): 1990-1998. doi: 10.11999/JEIT220547

智能反射表面辅助的全双工通信系统的物理层安全设计

doi: 10.11999/JEIT220547
基金项目: 江苏省输配电装备技术重点实验室开放课题(2021JSSPD05)
详细信息
    作者简介:

    齐本胜:男,副教授,研究方向为超宽带通信技术

    饶星楠:男,硕士生,研究方向为智能反射表面

    邓志祥:男,副教授,研究方向为无线物理层安全

    苗红霞:女,副教授,研究方向为输配电设备故障诊断技术

    通讯作者:

    邓志祥 dengzhixiang@hhu.edu.cn

  • 中图分类号: TN92

Physical Layer Security For Intelligent Reflecting Surface Assisted Full-duplex Communication

Funds: The Jiangsu Key Laboratory Open Subject of Power Transmission&Distribution Equipment Technology of Jiangsu Province (2021JSSPD05)
  • 摘要: 带内全双工技术可以缓解无线通信系统中频谱资源紧张的问题。为有效保障全双工通信系统的信息安全,针对全双工接入点(FD-AP)与上行用户、下行用户同时同频通信的系统模型,该文提出一种智能反射表面(IRS)辅助的物理层安全方案。考虑以最大化下行用户的安全速率为目标,在满足AP发射功率、AP信干噪比(SINR)以及IRS反射相移单位模的约束下,构建一个AP发射波束赋型和IRS反射相移联合优化问题。针对该变量耦合的非凸优化问题,该文采用交替优化(AO)算法迭代优化AP发射波束赋型和IRS反射相移,并提出一种基于精确罚函数法的黎曼流形优化算法,将反射相移优化子问题转换成黎曼流形上的无约束最小化问题进行求解。仿真结果表明,所提方案可以明显提升全双工通信系统的安全性能;并且相较于当前常用的半正定松弛(SDR)算法,所提算法有更低的计算复杂度。
  • 图  1  IRS辅助的全双工通信系统模型

    图  2  仿真系统模型坐标图

    图  3  收敛性能

    图  4  安全速率与IRS反射单元数目的关系

    图  5  安全速率与AP最大发射功率的关系(N=60)

    图  6  安全速率与上行用户最大发射功率的关系(N=60)

    图  7  安全速率与IRS部署位置的关系(N=60)

    图  8  计算时间

    算法1 基于光滑精确罚函数的黎曼流形优化算法
     初始化,给定可行初始点$ {{\boldsymbol{p}}_0} $,设置迭代次数$ t = 0 $、收敛精度$ \delta $、初始惩罚因子$ \rho $、惩罚增长系数$ c $
     (1) While $ g({{\boldsymbol{p}}_t}) > \delta $
     (2) 使用惩罚因子$ \rho $将AP信干噪比约束$ {\text{C1}} $并入目标函数中,并根据式(17)进行光滑处理
     (3) 构建复环流形${\rm{CCM}}$,令$ {\boldsymbol{p}}_0^m = {{\boldsymbol{p}}_t} $,设置迭代次数$ k = 0 $、收敛精度$ \varepsilon $
     (4) 根据式(21),计算得到初始搜索方向$ {{\xi }_0} = - {\text{Rgra}}{{\text{d}}_{{\boldsymbol{p}}_0^m}}f $
     (5) While $ {\left\| {{\text{Rgra}}{{\text{d}}_{{\boldsymbol{p}}_k^m}}f} \right\|_2} > \varepsilon $
     (6) 使用Armijo非精确搜索得到搜索步长$ {\mu _k} $,根据式(23),计算得到切空间$ {T_{{\boldsymbol{p}}_k^m}}\mathcal{M} $上的更新结果${\boldsymbol{p} }_{k + 1}^{m'}$
     (7) 根据式(24),收缩映射得到$ {\boldsymbol{p}}_{k + 1}^m $
     (8) 根据式(22),计算得到新的搜索方向$ {{\xi }_{k + 1}} $
     (9) $ k = k + 1 $
     (10) End While, $ {{\boldsymbol{p}}_{t + 1}} = {\boldsymbol{p}}_k^m $
     (11) $ \rho = c\rho ,{\text{ }}t = t + 1 $
     (12) End While, $ {{\boldsymbol{p}}^ * } = {{\boldsymbol{p}}_t} $
     (13) 根据式(25),从$ {{\boldsymbol{p}}^ * } $中恢复$ {{\boldsymbol{q}}^ * } $
    下载: 导出CSV
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出版历程
  • 收稿日期:  2022-05-05
  • 修回日期:  2022-06-14
  • 网络出版日期:  2022-06-20
  • 刊出日期:  2023-06-10

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