利用ACA驱动的测量矩阵插值加速目标宽带电磁散射特性分析

王仲根; 吴承钢; 聂文艳; 孙玉发

doi:10.11999/JEIT260392

利用ACA驱动的测量矩阵插值加速目标宽带电磁散射特性分析

doi: 10.11999/JEIT260392 cstr: 32379.14.JEIT260392

1.
安徽理工大学电气与信息学院淮南 232001
2.
淮南师范学院机械与电气工程学院淮南 232001
3.
安徽大学电子信息工程学院合肥 230601

基金项目: 国家自然科学基金(62071004)，安徽省教育厅科学研究重点项目(2025AHGXZK31006)

详细信息

作者简介:
王仲根：男，教授，研究方向为计算电磁学、阵列信号处理

吴承钢：男，硕士生，研究方向为计算电磁学、电磁散射等

聂文艳：女，教授，研究方向为计算电磁学、电磁散射等

孙玉发：男，教授，研究方向为计算电磁学、天线理论及设计等

通讯作者:
王仲根　zgwang@ahu.edu.cn

中图分类号: TN011
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出版历程
- 收稿日期: 2026-04-07
- 修回日期: 2026-06-29
- 录用日期: 2026-07-03
- 网络出版日期: 2026-07-13

Accelerated Broadband Electromagnetic Scattering Analysis via ACA-Driven Measurement Matrix Interpolation

1.
College of Electrical and Information Engineering, Anhui University of Science and Technology, Huainan, Anhui 232001, China
2.
College of Mechanical and Electrical Engineering, Huainan Normal University, Huainan 232001, China
3.
College of Electronics and Information Engineering, Anhui University, Hefei 230061, China

Funds: The National Natural Science Foundation of China (62071004), The Natural Science Research Project of Anhui Educational Committee (2025AHGXZK31006)

摘要

摘要: 针对目标宽带电磁散射特性分析中待求频点阻抗矩阵重复计算、矩阵方程重复求解的问题，本文提出一种基于压缩感知框架的自适应交叉近似(ACA)驱动测量矩阵插值(MMI)的高效计算方法。该方法首先在最高频率点通过ACA提取主导行索引并全频段复用，实现测量矩阵确定性构建；其次采用MMI技术，通过少量采样频点的低维测量矩阵插值避免完整阻抗矩阵冗余计算；最后对插值后矩阵的远场组再次进行ACA分解，进一步加速矩阵向量积运算，实现传感矩阵的快速构建，将电流系数求解转换成压缩感知模型下超定方程的求解，实现待求频点电流快速求解。研究结果表明，该方法在保证计算精度的前提下，有效提高了测量矩阵的构造效率，显著降低插值的矩阵维数，大幅提升了目标宽带散射分析的效率。
- 宽带散射 /
- 压缩感知 /
- 自适应交叉近似 /
- 测量矩阵插值
Abstract: Objective Broadband electromagnetic scattering is essential in modern fields such as radar target recognition, stealth technologies, and microwave imaging. While the Method of Moments (MoM) provides high accuracy, it incurs substantial computational costs for electrically large or complex targets due to the construction and solution of large-scale impedance matrices. Although acceleration techniques like the Multilevel Fast Multipole Method (MLFMM) and Adaptive Cross Approximation (ACA) have been developed, they still require costly per-frequency recomputations during wideband sweeps. To mitigate this redundancy, techniques such as Asymptotic Waveform Evaluation (AWE), Model-Based Parameter Estimation (MBPE), and impedance matrix interpolation have been introduced. However, AWE suffers from error accumulation in wideband scenarios, MBPE entails high initial sampling costs, and traditional matrix interpolation remains burdened by the need to compute full high-dimensional matrices at sampling points. Recently, Compressive Sensing MoM (CS-MoM) and its derivative, CS-HBFM, have offered promising wideband solutions by utilizing Hyper-Basis Functions (HBFs). By calculating Characteristic Mode Basis Functions (CMBFs) only once at the highest frequency, CS-HBFM eliminates the redundant generation of basis functions. Nevertheless, existing CS-HBFM frameworks rely on non-deterministic random or uniform sampling strategies. Furthermore, they are hindered by large-scale matrix-vector products and the persistent need to reconstruct and solve impedance equations at every frequency step. Methods With CS as the basic framework, this study proposes the CS-ACA-MMI accelerated analysis method for broadband electromagnetic scattering, which achieves efficient calculation of broadband scattering through the collaborative acceleration of dual ACA decomposition and low-dimensional measurement matrix interpolation. The specific implementation steps are as follows: First, CMBFs are constructed at the highest frequency point, and the dominant HBFs are selecting significant modes based on the Modal Significance (MS) criterion. ACA low-rank decomposition is performed on the complete impedance matrix at this frequency point to extract deterministic row indices representing the dominant Rao–Wilton–Glisson (RWG) basis functions, which are maintained throughout the frequency sweep to avoid the problem of non-deterministic sampling. Second, Chebyshev-Lobatto nodes are selected to determine four key sampling frequency points, and the low-dimensional measurement matrix of each sampling point is directly filled based on the pre-extracted row indices, circumventing the calculation of the complete high-dimensional impedance matrix, thereby significantly reducing the computational overhead of filling the matrix element-by-element at each frequency point. The measurement impedance elements of the sampling points are corrected by geometric distance, and then the corrected measurement impedance of the target frequency point is obtained via interpolation and further restored to the real measurement impedance, eliminating the redundancy of constructing measurement matrices at each frequency point. Third, a second ACA decomposition is carried out on the far-field impedance component of the interpolated measurement matrix, converting the large-scale far-field matrix-vector product into a low-dimensional matrix product. The near-field part is directly obtained by multiplying the measurement matrix with the basis function, and finally the complete sensing matrix is rapidly assembled. Fourth, the solution of the traditional dense matrix equation is transformed into the solution of an overdetermined equation under the CS framework, and the least square method is adopted to reconstruct the current coefficient, thereby calculating the broadband Radar Cross Section (RCS) of the target, with the Root Mean Square Error (RMSE) used to measure the computational accuracy. Fifth, three typical targets (including simple regular, complex slotted, and electrically large irregular structures) such as a cylinder, a slotted cone, and an almond are selected, with different broadband analysis frequency bands and subdivision parameters set. The broadband RCS is calculated by MoM, CS-HBFM, and CS-ACA-MMI respectively, and the computational accuracy, total calculation time, and memory occupation of the single-frequency point measurement matrix of the three methods are compared and analyzed to verify the effectiveness of the proposed method. Results and Discussions Three typical numerical examples, a PEC cylinder, a cone-sphere with a gap and a almond, are used to verify the performance of the CS-ACA-MMI method. The spatial distribution of ACA-extracted row indices shows obvious hotspot clustering at geometric boundaries and structural junctions, which confirms the physical rationality and effectiveness of the deterministic sampling strategy (Fig.2). Parametric studies demonstrate that appropriate ACA thresholds and four sampling points achieve the best balance between computational accuracy and efficiency (Fig.3, Fig.4, Fig.5). The wideband RCS results calculated by the proposed method are in excellent agreement with those from the traditional MoM over the entire frequency band (Fig.6, Fig.7, Fig8). The root-mean-square errors (RMSE) remain very low, verifying the high numerical accuracy of the method. Compared with the conventional CS-HBFM method, the CS-ACA-MMI framework reduces the total computation time by 93.4% for the cylinder, 96.7% for the cone-sphere with a gap and 81% for the almond, respectively (Table 2). The significant improvement in efficiency benefits from deterministic index reuse, low-dimensional measurement matrix interpolation, and dual ACA acceleration, which effectively alleviate the heavy computational burden in wideband frequency-sweeping analysis. Conclusions This study successfully develops a CS acceleration framework, CS-ACA-MMI, which integrates ACA with MMI. This framework effectively addresses the bottlenecks of repetitive matrix construction and equation solving in broadband electromagnetic scattering analysis, while overcoming the non-deterministic sampling and high computational/storage overhead inherent in traditional CS-HBFM. The core advantages of CS-ACA-MMI are three-fold: First, by extracting dominant row indices via ACA at the highest frequency and reusing them across the entire band, it ensures a deterministic construction of the measurement matrix and provides a stable physical benchmark for broadband interpolation. Second, the interpolation process is shifted from high-dimensional full impedance matrices to low-dimensional measurement matrices. Combined with Chebyshev-Lobatto node technology, this eliminates the redundant matrix filling at each frequency point. Third, by applying a second ACA decomposition to the far-field components, large-scale matrix-vector products are converted into low-dimensional matrix multiplications, significantly accelerating the sensing matrix construction. Numerical results for various structures (cylinder, cone-sphere with a gap, and almond) demonstrate that CS-ACA-MMI maintains high computational accuracy consistent with the conventional MoM. Meanwhile, the proposed method reduces total computation time by over 81% and cuts single-frequency memory requirements by up to 65%. By only requiring the storage of measurement matrices at a few sampling points, it markedly reduces the overall storage overhead.
- broadband scattering /
- compressive sensing /
- adaptive cross approximation /
- measurement matrix interpolation

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图 1 ACA测量矩阵构建示意图

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图 2 ACA全局行索引的高亮图

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图 3 行索引获取中不同ACA阈值下的时间和RMSE

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图 4 传感矩阵构建中不同ACA阈值下的时间和RMSE

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图 5 不同采样点数下的时间和RMSE

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图 6 圆柱体的宽带RCS

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图 7 带缝圆锥的宽带RCS

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图 8 杏仁体的宽带RCS

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表 1 两种方法的计算复杂度对比

方法	测量矩阵构建	近场传感矩阵构建	远场传感矩阵构建
CS-HBFM	$ O({N}_{f}MN) $	$ O((1-\eta ){N}_{f}MNK) $	$ O(\eta {N}_{f}MNK) $
CS-ACA-MMI	$ O(4SN) $	$ O((1-\eta ){N}_{f}SNK) $	$ O(\eta {N}_{f}RNK) $

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表 2 两种方法的计算时间对比

目标	方法	抽取行数	总时间(s)	RMSE(dBsm)	单频点测量矩阵的内存(GB)
圆柱体	CS-HBFM	3001	5285.27	0.46	0.46
圆柱体	CS-ACA-MMI	1104	349.33	0.4	0.16
带缝圆锥	CS-HBFM	4082	34991.7	0.04	0.83
带缝圆锥	CS-ACA-MMI	2839	1154.52	0.05	0.58
杏仁体	CS-HBFM	17633	180182.5	0.07	15.44
杏仁体	CS-ACA-MMI	13292	34316.2	0.05	11.64

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