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利用双载频方向图相乘的稀疏均匀阵栅瓣抑制方法

王旭 黄冬平 魏国华 白嘉豪 朱沁源

王旭, 黄冬平, 魏国华, 白嘉豪, 朱沁源. 利用双载频方向图相乘的稀疏均匀阵栅瓣抑制方法[J]. 电子与信息学报, 2023, 45(2): 534-541. doi: 10.11999/JEIT211492
引用本文: 王旭, 黄冬平, 魏国华, 白嘉豪, 朱沁源. 利用双载频方向图相乘的稀疏均匀阵栅瓣抑制方法[J]. 电子与信息学报, 2023, 45(2): 534-541. doi: 10.11999/JEIT211492
WANG Xu, HUANG Dongping, WEI Guohua, BAI Jiahao, ZHU Qinyuan. Sparse Uniform Array Grating Lobe Suppression Using Dual-carrier Frequency Pattern Multiplication[J]. Journal of Electronics & Information Technology, 2023, 45(2): 534-541. doi: 10.11999/JEIT211492
Citation: WANG Xu, HUANG Dongping, WEI Guohua, BAI Jiahao, ZHU Qinyuan. Sparse Uniform Array Grating Lobe Suppression Using Dual-carrier Frequency Pattern Multiplication[J]. Journal of Electronics & Information Technology, 2023, 45(2): 534-541. doi: 10.11999/JEIT211492

利用双载频方向图相乘的稀疏均匀阵栅瓣抑制方法

doi: 10.11999/JEIT211492
基金项目: 国家自然科学基金(61671059)
详细信息
    作者简介:

    王旭:男,副研究员,研究方向为高速实时数字信号处理

    黄冬平:男,硕士生,研究方向为雷达信号处理

    魏国华:男,研究员,研究方向为雷达系统及其信号处理

    白嘉豪:男,博士生,研究方向为雷达信号处理

    朱沁源:男,硕士生,研究方向为雷达信号处理

    通讯作者:

    魏国华 ghwei@bit.edu.cn

  • 中图分类号: TN958

Sparse Uniform Array Grating Lobe Suppression Using Dual-carrier Frequency Pattern Multiplication

Funds: The National Natural Science Foundation of China (61671059)
  • 摘要: 针对稀疏阵列天线间距远大于信号波长导致阵列方向图出现大量栅瓣的问题,该文基于不同载频阵列方向图主瓣与栅瓣相对位置关系存在差异的特性提出一种新型的栅瓣抑制算法。该算法充分利用不同载频回波信息,避免了大规模搜索,有效降低了计算量。首先根据算法原理确定了影响该栅瓣抑制算法性能的因素,然后进一步对影响栅瓣抑制性能的关键参数进行了定量分析,推导得出了栅瓣抑制后峰值旁瓣比(PSLR)与频率差的关系表达式。该表达式为栅瓣抑制快速选择最优频率差提供了理论依据。最后,通过计算机仿真验证了该算法对栅瓣抑制的有效性以及该文所推导的峰值旁瓣比与频率差关系表达式的正确性。
  • 图  1  稀疏阵列天线分布示意图

    图  2  栅瓣抑制算法实现流程

    图  3  相乘后方向图(波束最大值指向0°)

    图  4  相乘后方向图(波束最大值指向20°)

    图  5  峰值旁瓣对应角度与频率差关系图

    图  6  峰值旁瓣比与频率差关系图

    算法1 栅瓣抑制算法
     发射与接收端:
     (1) 发射双载频信号$ {\boldsymbol{z}}\left( t \right) $;
     (2) 接收回波信号$ {\boldsymbol{x}}\left( t \right) $。
     信号处理端:
     (1) 利用式(7)和式(8)对$ {\boldsymbol{x}}\left( t \right) $进行下变频和频域滤波分离出$ {{\boldsymbol{x}}_0}\left( t \right) $
       和$ {{\boldsymbol{x}}_1}\left( t \right) $两路信号;
     (2) 利用式(9)和式(10)分别对$ {{\boldsymbol{x}}_0}\left( t \right) $和$ {{\boldsymbol{x}}_1}\left( t \right) $进行匹配滤波得到
       $ {{\boldsymbol{v}}_0}\left( t \right) $和$ {{\boldsymbol{v}}_1}\left( t \right) $;
     (3) 使用式(11)和式(12)对$ {{\boldsymbol{v}}_0}\left( t \right) $和$ {{\boldsymbol{v}}_1}\left( t \right) $信号分别进行波束形成
       得到$ {y_0}\left( t \right) $和$ {y_1}\left( t \right) $;
     (4) 对$ {y_0}\left( t \right) $和$ {y_1}\left( t \right) $进行归一化得到$ {\widetilde y_0}\left( t \right) $和$ {\widetilde y_1}\left( t \right) $;
     (5) 将$ {\widetilde y_0}\left( t \right) $,$ {\widetilde y_1}\left( t \right) $进行相乘处理到$ \widetilde y\left( t \right) $;
     (6) 从$ \widetilde y\left( t \right) $选取检测单元,从$ {\widetilde y_0}\left( t \right) $或$ {\widetilde y_1}\left( t \right) $选取该检测单元对应
       的参考单元进行恒虚警检测;
     (7) 调整波束指向转到步骤(3),完成空域的搜索,退出。
    下载: 导出CSV

    表  1  仿真实验的详细参数

    发射天线
    数量M
    接收天线
    数量N
    发射天线
    间距系数${\gamma _{{\rm{T}}}}$
    接收天线
    间距系数${\gamma _{{\rm{R}}}}$
    天线间距
    公约系数q
    基准信号
    频率${f_0}$
    10102025510 GHz
    下载: 导出CSV
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出版历程
  • 收稿日期:  2021-12-13
  • 修回日期:  2022-05-19
  • 网络出版日期:  2022-05-24
  • 刊出日期:  2023-02-07

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