1. 阜阳师范学院物理与电子工程学院,安徽,阜阳,236037
2. 阜阳师范学院数学与统计学院,安徽,阜阳,236037
3. 阜阳师范学院物理与电子工程学院,安徽,阜阳,236037
4. 阜阳师范学院数学与统计学院,安徽,阜阳,236037
网络出版:2016-02-25,
纸质出版:2016
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刘广东, 葛新同. 时域反演德鲁色散媒质的电磁逆散射技术[J]. 电子学报, 2016,44(2):385-391.
LIU Guang-dong, GE Xin-tong. An Electromagnetic Inverse Scattering Technique in Time Domain for Drude Dispersive Media[J]. Acta Electronica Sinica, 2016, 44(2): 385-391.
刘广东, 葛新同. 时域反演德鲁色散媒质的电磁逆散射技术[J]. 电子学报, 2016,44(2):385-391. DOI: 10.3969/j.issn.0372-2112.2016.02.020.
LIU Guang-dong, GE Xin-tong. An Electromagnetic Inverse Scattering Technique in Time Domain for Drude Dispersive Media[J]. Acta Electronica Sinica, 2016, 44(2): 385-391. DOI: 10.3969/j.issn.0372-2112.2016.02.020.
德鲁(Drude)经验模型常用于描述等离子体、金属等媒质的电色散特性.利用宽带的时域测量数据直接反演电参数
相比单频(频域)技术而言
具有信息量大、成像分辨率高的优势.时域直接反演色散媒质电参数的主要困难在于它们是频率相关的.为了克服该困难
本文提出了一种时域电磁(EM)逆散射新技术:转而同时反演德鲁模型的4类频率无关的模型参数.该技术的主要环节为:(1)描述为含正则化项的约束最小化问题;(2)转化为无约束最小化问题;(3)解析导出梯度;(4)分别利用时域有限差分(FDTD)法、共轭梯度(CG)法迭代求解正演、反演子问题.在一维(1-D)、二维(2-D)两个数值算例中
所需的测量数据也由FDTD仿真值代替
并加入了加性高斯白噪声(AWGN).反演结果初步证实了该技术的性能.
Drude empirical models are frequently used for description of dispersion characteristics of many media
such as plasmas
and metals.Reconstructed electrical properties by directly using wide-band measured data in time domain
are better than those by application of any single-frequency technique
in amount of information
and resolution of generated images.One of difficulties in time-domain reconstruction of dispersive characteristics is their frequency correlation.In order to overcome this difficulty
an electromagnetic (EM) inverse scattering technique in time domain is proposed
in which four kinds of frequency-independence parameters from a Drude model are estimated simultaneously.Main segments for the technology are:(1) formulating the inverse scattering problem as a constrained minimization problem with a term of regularization;(2) transforming resulting problem into an unconstrained minimization one;(3) deriving a set of closed gradients of its cost functional;(4) solving iteratively resulting forward and backward sub-problems by a finite-difference time-domain (FDTD) method and any conjugate gradient (CG) algorithm
respectively.In one-dimensional (1-D) and two-dimensional (2-D) numerical examples
necessary measurements are replaced by simulated fields based on the FDTD method
and it is assumed that they are corrupted by an additive white Gaussian noise (AWGN).Numerical results preliminarily confirm performance of the inversion methodology.
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