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面向ELAA的联合近场信道建模与信道参数估计

陈崇斌,  孙健,  常恒泰,  张文胜,  王承祥

陈崇斌, 孙健, 常恒泰, 张文胜, 王承祥. 面向ELAA的联合近场信道建模与信道参数估计[J]. 电子与信息学报. doi: 10.11999/JEIT260911
引用本文: 陈崇斌, 孙健, 常恒泰, 张文胜, 王承祥. 面向ELAA的联合近场信道建模与信道参数估计[J]. 电子与信息学报. doi: 10.11999/JEIT260911
CHEN Chongbin, SUN Jian, CHANG Hengtai, ZHANG Wensheng, WANG Chengxiang. Unified Near-Field Channel Modeling and Channel Parameter Estimation for ELAA[J]. Journal of Electronics & Information Technology. doi: 10.11999/JEIT260911
Citation: CHEN Chongbin, SUN Jian, CHANG Hengtai, ZHANG Wensheng, WANG Chengxiang. Unified Near-Field Channel Modeling and Channel Parameter Estimation for ELAA[J]. Journal of Electronics & Information Technology. doi: 10.11999/JEIT260911

面向ELAA的联合近场信道建模与信道参数估计

doi: 10.11999/JEIT260911 cstr: 32379.14.JEIT260911
基金项目: 国家自然科学基金(U24A20212),国家重点研发计划(2022YFF0604900, 2022YFF0604903),东南大学国家移动通信研究实验室研究基金(2025A05)
详细信息
    作者简介:

    陈崇斌:男,硕士,研究方向为近场通信与信道建模等,邮箱 chencb@mail.sdu.edu.cn

    孙健:男,副教授,研究方向为无线通信信号处理、无线信道测量与建模、通信感知一体化、软件无线电以及面向无线通信的人工智能技术等,邮箱 sunjian@sdu.edu.cn

    常恒泰:男,副研究员,研究方向为6G信道测量与建模、超高频段近场通信、人工智能驱动的无线通信等。 邮箱 changht@sdu.edu.cn

    张文胜:男,副教授,研究方向为张量计算、随机矩阵理论以及6G无线通信等。 邮箱 zhangwsh@sdu.edu.cn

    王承祥:男,教授,研究方向为无线信道测量与建模、6G无线通信网络以及电磁信息理论等。邮箱 chxwang@seu.edu.cn

    通讯作者:

    孙健 sunjian@sdu.edu.cn

  • 中图分类号: TN929.5

Unified Near-Field Channel Modeling and Channel Parameter Estimation for ELAA

Funds: The National Natural Science Foundation of China (U24A20212), The National Key Research and Development Program of China (2022YFF0604900, 2022YFF0604903), The Research Fund of National Mobile Communications Research Laboratory, Southeast University (2025A05)
  • 摘要: 面向第六代移动通信系统中超大孔径阵列所带来的近场传播特性,针对传统信道模型所采用的远场平面波传播模型失效以及近场信道估计精度受限等挑战,本文提出了一种面向点散射与镜面反射共存的联合近场信道建模框架及相应的参数估计算法。以往近场信道多仅考虑基于第一跳/最后一跳的点散射球面波传播,或者基于几何光学镜像原理将非视距路径等效为虚拟点到阵列的视距路径的端到端球面波传播,本文对两者共存的复杂传播环境进行联合表达,提升了近场信道建模的物理一致性。此外,将针对均匀平面阵列(Uniform Planar Array, UPA)的极域同步迭代无网格加权信道参数估计算法应用于所构建的联合信道模型,并通过球面波半径与传播路径的差异对路径类型进行分类。仿真结果表明,所提方法提升了混合传播环境下的参数估计精度与鲁棒性,在不同传播距离和信噪比条件下,均优于已有算法。
  • 图  1  基于混合预编码的ELAA系统[16]

    图  2  基于UPA的ELAA系统模型

    图  3  几何光学反射原理[16]

    图  4  单元天线的三维方向图

    图  5  目标函数随迭代次数的变化($ R=10\text{m} $)

    图  6  不同阵列规模下单一传播模型的模型失配NMSE

    图  7  不同距离下的NMSE性能($ \text{SNR}=10\text{dB} $)

    图  8  不同SNR下的NMSE性能($ R=10\text{m} $)

    图  9  不同SNR下的NMSE性能($ R=100\text{m} $)

    图  10  不同$ \beta $下的NMSE性能($ R\text{=10m, SNR=10 dB} $)

    图  11  不同Rician因子下的NMSE性能($ R\text{=10m, SNR=10 dB} $)

    图  12  近场中的路径参数估计($ R=10\text{m, SNR=10 dB} $)

    图  13  不同SNR下路径分类的准确率($ R=10\text{m} $)

    图  14  不同天线数量下的NMSE性能($ R=10\text{m, SNR=10 dB} $)

    表  3  仿真参数

    参数 符号 取值或取值范围
    UPA阵列天线数量 $ {N}_{1}\times {N}_{2} $ $ 30\times 30 $
    射频链数量 $ {N}_{\text{RF}} $ $ 8 $
    载波频率 $ {f}_{\text{c}} $ $ 3.5\text{GHz} $
    系统带宽 $ B $ $ 100\text{MHz} $
    导频子载波数量 $ M $ $ 256 $
    传播路径数量 $ L $ $ 8 $
    点散射路径数量 $ {L}_{2} $ $ {L}_{2}\in \left\{1{,}2,3\right\} $
    散射体与UE间距离 $ {R}_{\text{P}} $ $ \mathcal{U}\left(0.3R,0.7R\right) $
    距离门限 $ \Delta {r}_{\text{th}} $ $ 0.2R $
    Rician因子 K 3 dB
    天顶角 $ \theta $ $\sin \left(\dfrac{\pi }{2}-\theta \right)\sim \mathcal{U}\left(-\dfrac{\sqrt{3}}{2},\dfrac{\sqrt{3}}{2}\right)$
    方位角 $ \phi $ $ \sin \phi \sim \mathcal{U}\left(-\frac{\sqrt{3}}{2},\frac{\sqrt{3}}{2}\right) $
    导频长度 $ P $ $ 36 $
    算法迭代次数 $ {N}_{\text{iter}} $ $ 20 $
    实验重复次数 $ {N}_{\text{MC}} $ 100
    下载: 导出CSV

    表  1  不同距离下的最大相位截断误差

    传播距离$ {s}_{l} $最大相位截断误差$ \Delta {\phi }_{\max } $
    6 m0.2776 rad
    10 m0.0982 rad
    30 m0.0107 rad
    77 m(瑞利距离附近)0.0016 rad
    下载: 导出CSV

    1  P-SIGW-UPA算法

     输入:接收信号矩阵$ \boldsymbol{Y} $;合并矩阵$ \boldsymbol{A} $;实际路径数$ L $;最大迭代次数$ {N}_{\text{iter}} $。
     初始化:利用P-SOMP算法获得参数的初始估计,包括天顶角向量$ {\hat{\boldsymbol{\theta }}}^{(0)}=\left[\hat{\theta }_{1}^{(0)},\cdots ,\hat{\theta }_{\hat{L}}^{(0)}\right] $,方位角向量$ {\hat{\boldsymbol{\phi }}}^{(0)}=[\hat{\phi }_{1}^{(0)},\cdots ,\hat{\phi }_{\hat{L}}^{(0)}] $以及距离向
     量$ {\hat{\boldsymbol{r}}}^{(0)}=\left[\hat{r}_{1}^{(0)},\cdots ,\hat{r}_{\hat{L}}^{(0)}\right] $。
     初始优化:对于$ n=1{,}2,\cdots ,{N}_{\text{iter}} $,执行以下步骤:
     1:采用Armijo回溯线搜索方法确定步长参数$ {l}_{1} $、$ {l}_{2} $和$ {l}_{3} $。
     2:根据式(21)更新天顶角和方位角参数。
     3:根据式(22)更新路径距离参数。
     4:根据式(24)更新路径增益矩阵。
     路径剪枝:若估计路径数满足$ \hat{L}> L $,则执行路径剪枝操作:
     1:根据式(25)计算每条路径的能量。
     2:根据式(26)确定被保留路径的索引集合$ \mathcal{I} $。
     3:对参数进行剪枝更新:天顶角$ {\hat{\boldsymbol{\theta }}}^{(n)}\leftarrow{\hat{\boldsymbol{\theta }}}^{(n)}(\mathcal{I}) $,方位角$ {\hat{\boldsymbol{\phi }}}^{(n)}\leftarrow{\hat{\boldsymbol{\phi }}}^{(n)}(\mathcal{I}) $,距离$ {\hat{\boldsymbol{r}}}^{(n)}\leftarrow{\hat{\boldsymbol{r}}}^{(n)}(\mathcal{I}) $,路径增益$ {\hat{\boldsymbol{G}}}^{(n)}\leftarrow{\hat{\boldsymbol{G}}}^{(n)}(\mathcal{I},\colon ) $。
     路径分类:
     1:根据式(27)-(29)计算距离偏差。
     2:根据式(30)进行路径分类,并根据式(28)对点散射路径的距离进行修正。
     输出:根据式(31)构建最终的信道估计矩阵。
    下载: 导出CSV

    表  2  计算复杂度比较

    算法 计算复杂度
    A-SOMP-UPA $ \mathcal{O}(\hat{L}P{N}_{\text{RF}}NM) $
    P-SOMP-UPA $ \mathcal{O}(\hat{L}P{N}_{\text{RF}}NMS) $
    A-SIGW-UPA ${\mathcal{O}}(\hat{L}P{N}_{\text{RF}}NM)+\mathcal{O}({N}_{\text{iter}}({P}^{2}N_{\text{RF}}^{2}M+P{N}_{\text{RF}}{M}^{2}))$
    P-SIGW-UPA $ \mathcal{O}(\hat{L}P{N}_{\text{RF}}NMS)+\mathcal{O}({N}_{\text{iter}}({P}^{2}N_{\text{RF}}^{2}M+P{N}_{\text{RF}}{M}^{2})) $
    下载: 导出CSV
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  • 收稿日期:  2026-07-02
  • 修回日期:  2026-09-04
  • 录用日期:  2026-11-05
  • 网络出版日期:  2026-11-14

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