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城市街道下场景IRS辅助D2D通信系统波束成形设计

张祖凡 刘建 张晨璐

张祖凡, 刘建, 张晨璐. 城市街道下场景IRS辅助D2D通信系统波束成形设计[J]. 电子与信息学报, 2024, 46(9): 3571-3582. doi: 10.11999/JEIT240112
引用本文: 张祖凡, 刘建, 张晨璐. 城市街道下场景IRS辅助D2D通信系统波束成形设计[J]. 电子与信息学报, 2024, 46(9): 3571-3582. doi: 10.11999/JEIT240112
ZHANG Zufan, LIU Jian, ZHANG Chenlu. Beamforming Design for IRS-assisted D2D Communication System Under Urban Street Scenarios[J]. Journal of Electronics & Information Technology, 2024, 46(9): 3571-3582. doi: 10.11999/JEIT240112
Citation: ZHANG Zufan, LIU Jian, ZHANG Chenlu. Beamforming Design for IRS-assisted D2D Communication System Under Urban Street Scenarios[J]. Journal of Electronics & Information Technology, 2024, 46(9): 3571-3582. doi: 10.11999/JEIT240112

城市街道下场景IRS辅助D2D通信系统波束成形设计

doi: 10.11999/JEIT240112
基金项目: 国家自然科学基金(62202077),重庆市教育委员会科学技术研究计划青年项目(KJQN0202200609)
详细信息
    作者简介:

    张祖凡:男,教授,博士生导师,研究方向为无线通信、移动社交网络、机器学习等

    刘建:男,硕士生,研究方向为智能反射面、无线通信等

    张晨璐:男,硕士,研究方向为5G、6G国际标准化研究等

    通讯作者:

    刘建 S210131130@stu.cqupt.edu.cn

  • 中图分类号: TN929.5

Beamforming Design for IRS-assisted D2D Communication System Under Urban Street Scenarios

Funds: The National Natural Science Foundation of China (62202077), The Youth Project of Science and Technology Research Program of Chongqing Municipal Education Commission, China (KJQN0202200609)
  • 摘要: 针对城市街道场景下蜂窝用户和D2D通信用户共享频谱以及城市街道下无线信道特性,该文提出一种IRS辅助的联合波束成形设计方法。在D2D链路信号与干扰加噪声比的约束下,以最大化蜂窝用户容量为目标,设计了最优的波束形成向量、相移矩阵和D2D链路发射功率。引入松弛变量将非凸且变量耦合的优化问题转换为解耦后的凸优化问题和二分法搜索功率分配,采用黎曼共轭梯度算法对反射相移矩阵进行优化。仿真结果表明,所提算法收敛性较好,且与基准方案相比能有效地提升用户信道容量。
  • 图  1  系统模型

    图  2  十字路口形状分布

    图  3  城市街道场景下IRS辅助多D2D用户对和蜂窝用户通信系统

    图  4  D2D对与复用候选集合二部图

    图  5  仿真场景

    图  6  不同IRS反射单元数下蜂窝用户信道容量与算法迭代次数的关系

    图  7  不同算法下蜂窝用户信道容量与IRS反射单元的关系

    图  8  不同算法下蜂窝用户信道容量与算法迭代次数的关系

    图  9  不同算法下蜂窝用户信道容量与街道宽度的关系

    图  10  城市和郊区部署IRS和无IRS下蜂窝用户信道容量与迭代次数的关系

    图  11  不同信干噪比下中断概率变化

    1  二分法搜索功率算法

     给定基站波束形成向量${\boldsymbol{w}}$和反射相移矩阵$ {\boldsymbol{\varTheta }} $,初始化功率$ {P_{\text{t}}}^{\left( 0 \right)} $,右边界${r^{\left( 0 \right)}} = {P_{{\text{max}}}}$,左边界${l^{\left( 0 \right)}} = 0$,$i = 0$和迭代更新精度${\varepsilon _1} > 0$;
     (1) 循环
     (2) 计算${P_{{\text{mid}}}}^{\left( i \right)} = \dfrac{{{l^{\left( i \right)}} + {r^i}}}{2}$,其中${P_{{\text{mid}}}}^{\left( i \right)}$是搜索范围的中间值;
     (3) 计算目标函数的值${\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( i \right)}} \right)$,如果$\left| {{\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( i \right)}} \right) - {\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( {i - 1} \right)}} \right)} \right| < {\varepsilon _1}$,则${P_{{\text{mid}}}}^{\left( i \right)}$是最优解的一部分,搜索结束;
     (4) 判断目标函数的值${\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( i \right)}} \right)$分母是否为 0。如果分母为0,说明${P_{\text{t}}} = 0$是最优解,直接返回目标值为0;
     (5) 如果${\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( i \right)}} \right)$大于目标值,则${P_{{\text{mid}}}}^{\left( i \right)}$说明可能是最优解的一部分,将${P_{{\text{mid}}}}^{\left( i \right)}$作为新的右边界,返回步骤 2。如果${\gamma _{\text{c}}}\left( {{P_{{\text{mid}}}}^{\left( i \right)}} \right)$小于
     目标值,则说明${P_{{\text{mid}}}}^{\left( i \right)}$不可能是最优解的一部分,将${P_{{\text{mid}}}}^{\left( i \right)}$作为新的左边界,返回步骤2。
    下载: 导出CSV

    2  基于迭代的黎曼共轭梯度算法

     给定基站波束形成向量${\boldsymbol{w}}$,DS发射功率${P_{\text{t}}}$。初始化${{\boldsymbol{\theta }}_0}$,$ {{\boldsymbol{\eta }}_0} = - {{\mathrm{grad}}} {\gamma _{\text{c}}}({{\boldsymbol{\theta }}_0}) $,$i = 0$和迭代更新精度${\varepsilon _2} > 0$;
     (1) 循环
     (2) 选择Armijo回溯线搜索步长$\alpha $;
     (3) 根据(30)更新${\boldsymbol{\theta }}$;
     (4) 计算新的${\gamma _{\text{d}}}$,如果${\gamma _{\text{d}}} \ge {\gamma ^{{\text{req}}}}$,则保持当前的优化变量不变;否则,将优化变量投影到约束空间${C}$中,即${{\boldsymbol{\theta }}_i} = {\text{Pro}}{{\text{j}}_{C}}({{\boldsymbol{\theta }}_i})$;
     (5) 根据(24)更新黎曼梯度;
     (6) 根据(28)更新搜索方向;
     (7) $i \leftarrow i + 1$;
     (8) until $ \Vert \mathrm{grad}{\gamma }_{\text{c}}({{\boldsymbol{\theta}} }_{i}){\Vert }_{2}\le {\varepsilon}_{2} $。
    下载: 导出CSV

    3  问题P1的交替优化算法

     初始化${{\boldsymbol{w}}^{(0)}}$, $P_t^{(0)}$和${{\boldsymbol{\varTheta }}^{(0)}}$和迭代更新精度${\varepsilon _3} > 0$;
     (1) 循环
     (2) 给定${{\boldsymbol{\varTheta }}^{(k)}}$,$P_t^{(k)}$,使用CVX工具求解子问题P1.3,更新${{\boldsymbol{w}}^{(k + 1)}}$;
     (3) 给定${{\boldsymbol{\varTheta }}^{(k)}}$,${{\boldsymbol{w}}^{(k + 1)}}$,基于算法1,更新$P_t^{(k + 1)}$;
     (4) 给定${{\boldsymbol{w}}^{(k + 1)}}$,$P_t^{(k + 1)}$,基于算法2,更新${{\boldsymbol{\theta }}^{k + 1}}$,${{\boldsymbol{\varTheta }}^{(k + 1)}} = {{\mathrm{diag}}} \left( {{{\boldsymbol{\theta}}^{k + 1}}} \right)$;
     (5) 根据迭代结果${{\boldsymbol{w}}^{(k + 1)}}$,$P_t^{(k + 1)}$和${{\boldsymbol{\varTheta }}^{(k + 1)}}$,计算CU用户容量$ {\gamma _{\text{c}}}^{\left( {k + 1} \right)} $;
     (6) until $ \left| {{{\log }_2}\left(\dfrac{{1 + {\gamma _{\text{c}}}^{\left( {k + 1} \right)}}}{{1 + {\gamma _{\text{c}}}^{\left( k \right)}}}\right)} \right| < {\varepsilon _3} $。
    下载: 导出CSV

    表  1  仿真参数设置

    仿真参数设置取值仿真参数设置取值
    拐角损耗$ {L_{{\text{corner}}}} $(dB)20IRS单元间隔与电磁波波长比值0.5
    街道宽度${w_1}$, ${w_2}$(m)20与IRS相关的路径损耗指数(dB)2
    IRS反射单元数100BS到D2D路径损耗指数(dB)3.5
    基站天线数4D2D用户之间路径损耗指数(dB)3
    D2D用户和蜂窝用户天线数1莱斯衰落因子${\varepsilon _x}$(dB)3
    D2D链路最小SINR需求$ {\gamma ^{{\text{req}}}} $(dBm)1单位路径损耗(dB)30
    基站最大发射功率$P$(dBm)20噪声功率谱密度(dBm·Hz–1)–170
    D2D链路最大发射功率${P_{\max }}$(dBm)5误差精度0.001
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-02-28
  • 修回日期:  2024-08-23
  • 网络出版日期:  2024-08-31
  • 刊出日期:  2024-09-26

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