CN111444601B - An AI-learning electromagnetic scattering calculation method suitable for any incident field - Google Patents

An AI-learning electromagnetic scattering calculation method suitable for any incident field Download PDF

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CN111444601B
CN111444601B CN202010211086.8A CN202010211086A CN111444601B CN 111444601 B CN111444601 B CN 111444601B CN 202010211086 A CN202010211086 A CN 202010211086A CN 111444601 B CN111444601 B CN 111444601B
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徐魁文
马振超
陈旭东
松仁成
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Hangzhou Dianzi University
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Abstract

The invention discloses an AI learning type electromagnetic scattering calculation method suitable for any incident field, and belongs to the field of electromagnetic scattering. The invention adopts AI learning network to train the learning contrast
Figure DDA0002421709910000011
Incident wave
Figure DDA0002421709910000012
Nonlinear relationship to induced current: sample design: to introduce known information, network input employs
Figure DDA0002421709910000013
As input, calculating forward current data as a real sample of the AI learning network; network design: the AI learning type network is used as a model to complete the training and prediction process, thereby representing the relationship between the input information, namely the scatterer, the incident field and the induced current. Compared with the invention
Figure DDA0002421709910000014
And (3) with
Figure DDA0002421709910000015
As input, the method has wider application range, and under the condition of the same grid division, the method is applied to solve the scattered field, so that the time is faster than that of the traditional algorithm, the precision is improved slightly, and the effectiveness of the method is verified by simulation test.

Description

一种适用于任意入射场的AI学习型电磁散射计算方法An AI learning-type electromagnetic scattering calculation method suitable for any incident field

技术领域technical field

本发明属于电磁散射领域,提出了一种适用于任意入射场的AI学习型电磁散射计算方法。The invention belongs to the field of electromagnetic scattering, and proposes an AI learning type electromagnetic scattering calculation method suitable for any incident field.

背景技术Background technique

自麦克斯韦方程组提出至今,已经有100多年的历史了。在这期间。电磁技术与理论发展迅速,并且得到了广泛的应用,如无线电通信,雷达与天线,地质勘测,生物医学成像等等。电磁波在实际环境中传播十分复杂,因此,研究电磁波特性具有重要的意义,实验和理论分析计算是相辅相成的重要手段。It has been more than 100 years since Maxwell's equations were proposed. During this time. Electromagnetic technology and theory are developing rapidly and have been widely used, such as radio communication, radar and antenna, geological survey, biomedical imaging and so on. The propagation of electromagnetic waves in the actual environment is very complicated. Therefore, it is of great significance to study the characteristics of electromagnetic waves. Experiments and theoretical analysis and calculation are important means that complement each other.

在理论分析计算中,大多数求解电磁学问题都无法直接通过麦克斯韦方程组解析形式来实现,只能依靠数值方法。如发展迅速的计算电磁学方法(CEM),总体可以分为两类:1.积分方程求解;2.偏微分方程求解。基于偏微分方程求解的方法包括有限差分法(FDM),有限元法(FEM),边界元法(BEM)。同时,基于积分方程的电磁计算方法由矩量法(MoM)以及由其衍生的计算方法组成。In theoretical analysis and calculation, most of the electromagnetic problems can not be solved directly through the analytical form of Maxwell's equations, and can only rely on numerical methods. For example, the rapidly developing Computational Electromagnetics Method (CEM) can be divided into two categories: 1. Solving integral equations; 2. Solving partial differential equations. Methods based on partial differential equations include finite difference method (FDM), finite element method (FEM), and boundary element method (BEM). Meanwhile, the electromagnetic calculation method based on the integral equation consists of the method of moments (MoM) and calculation methods derived from it.

虽然以上提到的前向电磁散射问题快速求解已经取得了很大的进步,但是对于大多数全波问题来说,这依然需要大量的时间和内存空间计算成本。因此,在电磁散射问题上,迫切需要一种精确、计算成本低、具备良好鲁棒性的求解方法。Although great progress has been made in the fast solution of the forward electromagnetic scattering problem mentioned above, it still requires a lot of time and memory space computational cost for most full-wave problems. Therefore, there is an urgent need for an accurate, low-cost, and robust solution to the electromagnetic scattering problem.

近年来,人工智能(AI)在实际应用中非常广泛,作为AI领域的深度学习,已应用于计算机视觉、图像处理(分类、分割、恢复)、大数据处理和学习等。虽然基于深度神经网络的电磁技术发展才刚刚开始,但最近已经有很多研究将其应用在逆散射问题,微波成像,雷达和遥感,合成孔径重建(SAR),多输入/多输出(MIMO)系统等等。由于其强大的非线性逼近能力和快速的预测能力,深度学习也逐渐成为一种强大的框架,为计算电磁学领域提供了前所未有的低计算时间消耗和高精度性能。特别是在电磁反演问题中,已有一些结合深度学习技术的优秀成果被报道。DNNs采用卷积神经网络(CNNs)来解决逆散射问题,能够快速生成良好的定量结果。结果表明,基于深度学习的反演方法在图像质量和计算时间上都明显优于传统的迭代反演方法。In recent years, artificial intelligence (AI) has been widely used in practical applications. As deep learning in the field of AI, it has been applied to computer vision, image processing (classification, segmentation, restoration), big data processing and learning, etc. Although the development of electromagnetic technology based on deep neural networks has just begun, many studies have recently applied it to inverse scattering problems, microwave imaging, radar and remote sensing, synthetic aperture reconstruction (SAR), multiple input/multiple output (MIMO) systems etc. Due to its powerful nonlinear approximation capabilities and fast prediction capabilities, deep learning has also emerged as a powerful framework, providing unprecedented low computational time consumption and high-precision performance in the field of computational electromagnetics. Especially in the electromagnetic inversion problem, some excellent results combined with deep learning techniques have been reported. DNNs employ convolutional neural networks (CNNs) to solve the inverse scattering problem, which can quickly generate good quantitative results. The results show that the inversion method based on deep learning significantly outperforms the traditional iterative inversion method in both image quality and computation time.

受到以上工作的启发,设计发明了一种适用于任意入射场的AI学习型电磁散射计算方法来解决电磁散射问题。该方法并没有通过网络直接去获取散射场信息,而是以入射场以及与散射体相关的信息作为输入,通过AI学习型网络来学习得到前向电流,之后才根据电流信息来计算得到散射场。Inspired by the above work, an AI learning electromagnetic scattering calculation method suitable for any incident field is designed and invented to solve the electromagnetic scattering problem. This method does not directly obtain the scattered field information through the network, but takes the incident field and the information related to the scatterer as input, learns the forward current through the AI learning network, and then calculates the scattered field according to the current information .

发明内容Contents of the invention

本发明的目的是针对传统算法在求解散射场的过程中,计算前向电流时需要大量的时间成本和计算空间成本,提出了一种在以对比度

Figure GDA0002475553110000021
与对比度/>
Figure GDA0002475553110000022
和入射场/>
Figure GDA0002475553110000023
乘积的通道数叠加,即/>
Figure GDA0002475553110000024
作为输入,用AI学习型网络来学习预测前向电流,最后计算得到散射场的方法。本发明的技术方案:The purpose of the present invention is to solve the traditional algorithm in the process of solving the scattering field, which requires a lot of time cost and calculation space cost when calculating the forward current, and proposes a method based on contrast
Figure GDA0002475553110000021
with contrast />
Figure GDA0002475553110000022
and incident field />
Figure GDA0002475553110000023
The number of channels of the product is superimposed, i.e. />
Figure GDA0002475553110000024
As input, use the AI learning network to learn to predict the forward current, and finally calculate the method to obtain the scattered field. Technical scheme of the present invention:

本发明设计方法利用AI学习型网络来训练学习对比度

Figure GDA0002475553110000025
入射波/>
Figure GDA0002475553110000026
到感应电流之间的非线性关系,具体方案设计如下:The design method of the present invention utilizes the AI learning network to train and learn contrast
Figure GDA0002475553110000025
incident wave/>
Figure GDA0002475553110000026
The nonlinear relationship between the induced current and the specific scheme is designed as follows:

一种适用于任意入射场的AI学习型电磁散射计算方法,采用AI学习网络来训练学习对比度

Figure GDA0002475553110000027
入射波/>
Figure GDA0002475553110000028
到感应电流之间的非线性关系,其特征在于:An AI learning electromagnetic scattering calculation method suitable for any incident field, using AI learning network to train and learn contrast
Figure GDA0002475553110000027
incident wave/>
Figure GDA0002475553110000028
to the nonlinear relationship between the induced current, characterized by:

样本设计:为了引入已知信息,网络输入采用

Figure GDA0002475553110000029
作为输入,计算得到前向电流数据作为AI学习型网络的真实样本;Sample design: In order to introduce known information, the network input adopts
Figure GDA0002475553110000029
As input, calculate the forward current data as the real sample of the AI learning network;

网络设计:采用AI学习型网络作为模型来完成训练预测过程,从而表征输入信息,也就是散射体,入射场,到感应电流的关系。Network design: AI learning network is used as a model to complete the training and prediction process, so as to represent the relationship between input information, that is, scatterers, incident fields, and induced currents.

进一步的,所述的前向电流数据的计算方法为矩量法MoM、有限元法FEM、时域有限差分发FDTD。Further, the calculation method of the forward current data is method of moments (MoM), finite element method (FEM), and finite difference in time domain (FDTD).

进一步的,所述的前向电流数据的计算方法为矩量法MoM计算步骤如下:Further, the calculation method of the forward current data is the method of moments (MoM) and the calculation steps are as follows:

总场积分方程为:The total field integral equation is:

Figure GDA00024755531100000210
Figure GDA00024755531100000210

其中,

Figure GDA00024755531100000211
和/>
Figure GDA00024755531100000212
分别表示总场和入射场,r与r′分别表示第p次入射的场点与源点;/>
Figure GDA00024755531100000213
为二维自由空间格林公式,表示一个位于空间r处的点源对其周围空间某一点r′所产生的场,其中,/>
Figure GDA00024755531100000214
为第一类零阶汉克尔函数,i表示虚数,k0是弹性波的波数,χ(r′)=(∈(r′)-∈0)/∈0,它为∈r的对比度函数,∈0表示弹性波穿过的介质的某种物理特性。Ω表示计算区域。感应电流J(r′)可以定义为
Figure GDA00024755531100000215
in,
Figure GDA00024755531100000211
and />
Figure GDA00024755531100000212
represent the total field and the incident field respectively, r and r' represent the field point and source point of the pth incident respectively; />
Figure GDA00024755531100000213
is the two-dimensional free space Green's formula, expressing the field generated by a point source located in space r to a point r' in its surrounding space, where, />
Figure GDA00024755531100000214
is the first kind of zero-order Hankel function, i represents an imaginary number, k 0 is the wave number of the elastic wave, χ(r′)=(∈(r′)-∈ 0 )/∈ 0 , it is the contrast function of ∈ r , ∈ 0 represents some physical property of the medium through which the elastic wave passes. Ω denotes the calculation area. The induced current J(r′) can be defined as
Figure GDA00024755531100000215

在观测区域S中,散射场

Figure GDA00024755531100000216
带有电流项J(r′)的电场积分方程可以定义为:In the observation area S, the scattered field
Figure GDA00024755531100000216
The electric field integral equation with the current term J(r′) can be defined as:

Figure GDA0002475553110000031
Figure GDA0002475553110000031

为了便于引入MoM来离散公式(1)和(2),计算区域Ω被离散为M个小方块单元,M=M1×M2,M1,M2分别表示x轴与y轴方向的数量。如果被分离的小单元变长远小于十分之一的波长,每个单元格内的感应电流与总场可以视为相同的。因此,公式(1)可以离散为:In order to facilitate the introduction of MoM to discretize formulas (1) and (2), the calculation area Ω is discretized into M small square units, M=M 1 ×M 2 , M 1 , M 2 represent the quantities in the x-axis and y-axis directions respectively . If the small cells being separated grow much smaller than a tenth of the wavelength, the induced current and the total field within each cell can be considered to be the same. Therefore, formula (1) can be discretized as:

Figure GDA0002475553110000032
Figure GDA0002475553110000032

其中,

Figure GDA0002475553110000033
与/>
Figure GDA0002475553110000034
分别表示在第p次入射时,相应对第m个网格的总场与入射场。Am′表示第m′个网格的面积;/>
Figure GDA0002475553110000035
在第p次入射时,第m′个网格的感应电流。综合计算区域Ω中所有的网格,式子(3)可以写成以下矩阵形式:in,
Figure GDA0002475553110000033
with />
Figure GDA0002475553110000034
Respectively represent the total field and the incident field corresponding to the mth grid at the pth incident. A m' represents the area of the m'th grid; />
Figure GDA0002475553110000035
The induced current of the m′th grid at the pth incident. Comprehensive calculation of all the grids in the area Ω, formula (3) can be written in the following matrix form:

Figure GDA0002475553110000036
Figure GDA0002475553110000036

其中

Figure GDA0002475553110000037
Figure GDA0002475553110000038
表示从感应电流到计算区域Ω中散射场之间的二维自由空间格林公式,其可以表示为:in
Figure GDA0002475553110000037
Figure GDA0002475553110000038
Represents the two-dimensional free-space Green's formula between the induced current and the scattered field in the calculation region Ω, which can be expressed as:

Figure GDA0002475553110000039
Figure GDA0002475553110000039

向量形式的感应电流

Figure GDA00024755531100000310
表示在第p次入射时,所有单元格离散的电流分布,其可以表示为:Induced current in vector form
Figure GDA00024755531100000310
Indicates the discrete current distribution of all cells at the p-th incident, which can be expressed as:

Figure GDA00024755531100000311
Figure GDA00024755531100000311

其中,

Figure GDA00024755531100000312
是一个对角矩阵,对角线上的每个元素对应于每个网格的对比度。将式子(4)代入式子(6),可以得到状态方程,表示如下:in,
Figure GDA00024755531100000312
is a diagonal matrix where each element on the diagonal corresponds to the contrast of each grid. Substituting formula (4) into formula (6), the state equation can be obtained, expressed as follows:

Figure GDA00024755531100000313
Figure GDA00024755531100000313

相同地,位于观测区域S的散射场可以离散为数据方程,表示如下:Similarly, the scattered field located in the observation area S can be discretized into a data equation, expressed as follows:

Figure GDA00024755531100000314
Figure GDA00024755531100000314

其中,

Figure GDA00024755531100000315
表示位于计算区域Ω的感应电流到观测区域S中散射场之间关系的二维格林公式。in,
Figure GDA00024755531100000315
Two-dimensional Green's formula expressing the relationship between the induced current located in the calculation region Ω and the scattered field in the observation region S.

利用传统MoM求解感应电流的状态方程可以表示为:Using traditional MoM to solve the state equation of induced current can be expressed as:

Figure GDA00024755531100000316
Figure GDA00024755531100000316

其中,

Figure GDA0002475553110000041
表示单位矩阵。利用公式(9)求出感应电流后,便可利用公式(8)求出散射场。in,
Figure GDA0002475553110000041
represents the identity matrix. After using the formula (9) to calculate the induced current, the formula (8) can be used to calculate the scattered field.

进一步的,公式(9)计算感应电流的方式替换为采用共轭梯度快速傅立叶变换(CG-FFT)求解感应电流,在复数空间中,共轭梯度法可求解以下线性方程组,Furthermore, the method of calculating the induced current in formula (9) is replaced by using the conjugate gradient fast Fourier transform (CG-FFT) to solve the induced current. In the complex space, the conjugate gradient method can solve the following linear equations,

Figure GDA0002475553110000042
Figure GDA0002475553110000042

等同于求解以下最小化问题:is equivalent to solving the following minimization problem:

Figure GDA0002475553110000043
Figure GDA0002475553110000043

以感应电流

Figure GDA0002475553110000044
作为未知量/>
Figure GDA0002475553110000045
可将公式(9)转为公式(10)的形式,进而利用共轭梯度法求解。induced current
Figure GDA0002475553110000044
as unknown />
Figure GDA0002475553110000045
Formula (9) can be transformed into the form of formula (10), and then solved by the conjugate gradient method.

进一步的,所述的共轭梯度法求解步骤如下:Further, the solution steps of the conjugate gradient method are as follows:

1)设置初值x0,r0=g0=Ax0-b;1) Set the initial value x 0 , r 0 =g 0 =Ax 0 -b;

2)确定第一次梯度搜索方向:P0=-A*r02) Determine the first gradient search direction: P 0 =-A * r 0 ;

3)

Figure GDA0002475553110000046
xk+1=xkkPk,rk+1=rkkAPk;3)
Figure GDA0002475553110000046
x k+1 = x kk P k ,r k+1 =r kk AP k ;

4)

Figure GDA0002475553110000047
Pk+1=-A*rk+1kPk;4)
Figure GDA0002475553110000047
P k+1 =-A * r k+1k P k ;

5)设置迭代终止条件并判断是否满足迭代终止条件,若否,转向步骤3),若是,得到x。5) Set the iteration termination condition and judge whether the iteration termination condition is satisfied, if not, go to step 3), if yes, get x.

其中,变量右上角*表示共轭转置符号;Among them, * in the upper right corner of the variable indicates the conjugate transpose symbol;

在利用共轭梯度法求解时,涉及大量的矩阵运算,考虑到公式(9)进行转换后

Figure GDA0002475553110000048
为Toeplitz矩阵,故可利用快速傅立叶变换(FFT)进行矩阵运算,求解步骤中,形如A*rk,APk都可以利用FFT进行运算,APk的运算可以简化为When using the conjugate gradient method to solve, a large number of matrix operations are involved. Considering the conversion of formula (9)
Figure GDA0002475553110000048
is a Toeplitz matrix, so the fast Fourier transform (FFT) can be used for matrix operations. In the solution step, the shape is A * r k , AP k can be operated by FFT, and the operation of AP k can be simplified as

Figure GDA0002475553110000049
Figure GDA0002475553110000049

其中,a为由矩阵A中第一行与第一列的数据构成的向量,FFT为离散傅立叶变换,.*表示矩阵间的数据两两相乘。Among them, a is a vector composed of the data in the first row and the first column in the matrix A, FFT is the discrete Fourier transform, and .* means that the data between the matrices is multiplied in pairs.

进一步的,所述的AI学习网络采用CNN网络,U-net,生成对抗网络GAN,Pix2pixGAN网络。Further, the AI learning network adopts CNN network, U-net, generated confrontation network GAN, and Pix2pixGAN network.

进一步的,所述的AI学习网络采用Pix2pix GAN网络,Pix2pix GAN网络由两部分网络构成,即生成网络G与对抗网络D。Further, the AI learning network adopts the Pix2pix GAN network, and the Pix2pix GAN network is composed of two parts of the network, that is, the generation network G and the confrontation network D.

进一步的,所述的G网络实际上是一个5层的U-net网络,包括下采样、上采样、跳跃连接层,在G网络最后一层,网络最后直接输出散射体实际值,未使用类似于tanh()之类的激活函数。Further, the G network is actually a 5-layer U-net network, including downsampling, upsampling, and skip connection layers. In the last layer of the G network, the network directly outputs the actual value of the scatterer at the end, without using similar Activation functions like tanh().

进一步的,所述的D网络的输入包含了来源与G网络的预测图像和输入图像作为条件,D网络输出的一组向量。Further, the input of the D network includes the source and the predicted image of the G network and the input image as conditions, and a set of vectors output by the D network.

进一步的,所述的G网络和D网络的损失函数采用最小二乘GAN,定义如下:Further, the loss function of the G network and the D network adopts the least squares GAN, which is defined as follows:

Figure GDA0002475553110000051
Figure GDA0002475553110000051

Figure GDA0002475553110000052
Figure GDA0002475553110000052

其中,x表示网络的输入数据,JMoM表示由MoM算法得到的真实电流数据。λ是一个可调节参数,

Figure GDA0002475553110000054
表示真实电流与预测电流的L1范数,定义为:Among them, x represents the input data of the network, and J MoM represents the real current data obtained by the MoM algorithm. λ is an adjustable parameter,
Figure GDA0002475553110000054
Represents the L1 norm of the real current and the predicted current, defined as:

Figure GDA0002475553110000055
Figure GDA0002475553110000055

实验证明,此发明可解决入射波的入射角度与照射强度不固定的问题,适用范围更广,且在相同网格划分下,应用此方法求解散射场时,不仅在时间上比传统算法快,而且在精度上也有不小的提升。Experiments have proved that this invention can solve the problem that the incident angle and irradiation intensity of the incident wave are not fixed. And there is no small improvement in accuracy.

附图说明Description of drawings

图1是所提出的针对电磁散射问题方案流程图;Figure 1 is a flow chart of the proposed solution for the electromagnetic scattering problem;

图2是所提出的二维电磁散射问题装置结构图;Figure 2 is a structural diagram of the proposed two-dimensional electromagnetic scattering problem device;

图3是本发明采用的网络pix2pix GAN内部结构图;Fig. 3 is the network pix2pix GAN internal structure figure that the present invention adopts;

图4是第一个实例解决入射光照强度变化的网络输入数据;Figure 4 is the network input data for the first example to solve the change of incident light intensity;

图5是第一个实例获得的前向电流结果与传统MoM获得的结果对比图;Fig. 5 is a comparison chart of the forward current result obtained in the first example and the result obtained by traditional MoM;

图6是第二个实例解决入射光照射角度可任意变化的网络输入数据;Fig. 6 is the second example to solve the network input data that the incident light irradiation angle can be changed arbitrarily;

图7是第二个实例获得的前向电流结果与传统MoM获得的结果对比图;Fig. 7 is a comparison diagram of the forward current result obtained in the second example and the result obtained by traditional MoM;

图8是第二个实例重建的散射场结果与传统MoM计算得到的散射场对比图。Fig. 8 is a comparison chart of the scattered field result reconstructed in the second example and the scattered field calculated by the traditional MoM.

具体实施方式Detailed ways

本发明以横向电磁波为例,结合附图对本发明所要解决的电磁散射问题作进一步说明。The present invention takes the transverse electromagnetic wave as an example, and further explains the electromagnetic scattering problem to be solved by the present invention in conjunction with the accompanying drawings.

图1是本发明所提出的AI学习型电磁散射计算方法流程图。即以对比度

Figure GDA0002475553110000053
与对比度
Figure GDA0002475553110000061
和入射场/>
Figure GDA0002475553110000062
乘积的通道数叠加,即/>
Figure GDA0002475553110000063
作为输入,用AI学习型网络来学习预测前向电流,最后计算得到散射场的方法,该方法能有效得到发射天线入射角度任意与照射强度变化的散射场数据。Fig. 1 is a flow chart of the AI learning type electromagnetic scattering calculation method proposed by the present invention. i.e. by contrast
Figure GDA0002475553110000053
and contrast
Figure GDA0002475553110000061
and incident field />
Figure GDA0002475553110000062
The number of channels of the product is superimposed, i.e. />
Figure GDA0002475553110000063
As input, the AI learning network is used to learn and predict the forward current, and finally calculate the scattered field method. This method can effectively obtain the scattered field data with any incident angle of the transmitting antenna and the change of the irradiation intensity.

图2是电磁散射问题装置结构图。该图是一个二维剖面图,正中央是一个剖面计算区域Ω,内部含有已知的散射体分布,外围S域面为发射天线与接收天线排布轨迹。当发射天线照射散射体时,会在散射体内部激起感应电流,该感应电流便会激起一个电磁场,也就是所谓的散射场,可由接收天线接收到。为了模拟仿真散射场数据,本发明提出了一种前向电流学习方法,该方法利用已知散射体和入射场与传统算法得到的感应电流作为样本对,由pix2pix GAN完成复杂学习,最终,训练好的网络可以预测一些样本分布外复杂散射体的散射场分布。Figure 2 is a structural diagram of the electromagnetic scattering problem device. The figure is a two-dimensional cross-sectional view, the center is a cross-sectional calculation area Ω, which contains known scatterers distribution, and the outer S-domain surface is the trajectory of the transmitting antenna and receiving antenna. When the transmitting antenna irradiates the scatterer, an induced current will be induced inside the scatterer, and the induced current will excite an electromagnetic field, the so-called scattered field, which can be received by the receiving antenna. In order to simulate the scattered field data, the present invention proposes a forward current learning method, which uses known scatterers and incident fields and induced currents obtained by traditional algorithms as sample pairs, and completes complex learning by pix2pix GAN. Finally, training A good network can predict the scattered field distribution of complex scatterers outside some sample distributions.

本发明采用AI学习网络来训练学习对比度

Figure GDA0002475553110000064
入射波/>
Figure GDA0002475553110000065
到感应电流之间的非线性关系。The present invention adopts AI learning network to train and learn contrast
Figure GDA0002475553110000064
incident wave/>
Figure GDA0002475553110000065
to the nonlinear relationship between the induced current.

样本设计:为了引入已知信息,网络输入采用

Figure GDA0002475553110000066
作为输入,并利用传统算法计算得到前向电流数据作为AI学习型网络的真实样本。传统算法如矩量法MoM,有限元法FEM,时域有限差分发FDTD等,都可以应用于此发明,由MoM算法计算感应电流的方法,计算过程如下:Sample design: In order to introduce known information, the network input adopts
Figure GDA0002475553110000066
As input, and use traditional algorithms to calculate the forward current data as the real sample of AI learning network. Traditional algorithms such as method of moments MoM, finite element method FEM, finite difference in time domain FDTD, etc., can be applied to this invention. The method of calculating the induced current by the MoM algorithm is as follows:

总场积分方程为:The total field integral equation is:

Figure GDA0002475553110000067
Figure GDA0002475553110000067

其中,

Figure GDA0002475553110000068
和/>
Figure GDA0002475553110000069
分别表示总场和入射场,r与r′分别表示第p次入射的场点与源点。/>
Figure GDA00024755531100000610
为二维自由空间格林公式,表示一个位于空间r处的点源对其周围空间某一点r′所产生的场,其中,/>
Figure GDA00024755531100000611
为第一类零阶汉克尔函数,i表示虚数,k0是弹性波的波数,χ(r′)=(∈(r′)-∈0)/∈0,它为∈r的对比度函数,∈0表示弹性波穿过的介质的某种物理特性。Ω表示计算区域。感应电流J(r′)可以定义为
Figure GDA00024755531100000612
in,
Figure GDA0002475553110000068
and />
Figure GDA0002475553110000069
represent the total field and the incident field, respectively, and r and r' represent the field point and source point of the pth incident, respectively. />
Figure GDA00024755531100000610
is the two-dimensional free space Green's formula, expressing the field generated by a point source located in space r to a point r' in its surrounding space, where, />
Figure GDA00024755531100000611
is the first kind of zero-order Hankel function, i represents an imaginary number, k 0 is the wave number of the elastic wave, χ(r′)=(∈(r′)-∈ 0 )/∈ 0 , it is the contrast function of ∈ r , ∈ 0 represents some physical property of the medium through which the elastic wave passes. Ω denotes the calculation area. The induced current J(r′) can be defined as
Figure GDA00024755531100000612

在观测区域S中,散射场

Figure GDA00024755531100000613
带有电流项J(r′)的电场积分方程可以定义为:In the observation area S, the scattered field
Figure GDA00024755531100000613
The electric field integral equation with the current term J(r′) can be defined as:

Figure GDA00024755531100000614
Figure GDA00024755531100000614

为了便于引入MoM来离散公式(1)和(2),计算区域Ω被离散为M个小方块单元,M=M1×M2,M1,M2分别表示x轴与y轴方向的数量。如果被分离的小单元变长远小于十分之一的波长,每个单元格内的感应电流与总场可以视为相同的。因此,公式(1)可以离散为:In order to facilitate the introduction of MoM to discretize formulas (1) and (2), the calculation area Ω is discretized into M small square units, M=M 1 ×M 2 , M 1 , M 2 represent the quantities in the x-axis and y-axis directions respectively . If the small cells being separated grow much smaller than a tenth of the wavelength, the induced current and the total field within each cell can be considered to be the same. Therefore, formula (1) can be discretized as:

Figure GDA0002475553110000071
Figure GDA0002475553110000071

其中,

Figure GDA0002475553110000072
与/>
Figure GDA0002475553110000073
分别表示在第p次入射时,相应对第m个网格的总场与入射场。Am′表示第m′个网格的面积;/>
Figure GDA0002475553110000074
在第p次入射时,第m′个网格的感应电流。综合计算区域Ω中所有的网格,式子(3)可以写成以下矩阵形式:in,
Figure GDA0002475553110000072
with />
Figure GDA0002475553110000073
Respectively represent the total field and the incident field corresponding to the mth grid at the pth incident. A m' represents the area of the m'th grid; />
Figure GDA0002475553110000074
The induced current of the m′th grid at the pth incident. Comprehensive calculation of all the grids in the area Ω, formula (3) can be written in the following matrix form:

Figure GDA0002475553110000075
Figure GDA0002475553110000075

其中

Figure GDA0002475553110000076
Figure GDA0002475553110000077
表示从感应电流到计算区域Ω中散射场之间的二维自由空间格林公式,其可以表示为:in
Figure GDA0002475553110000076
Figure GDA0002475553110000077
Represents the two-dimensional free-space Green's formula between the induced current and the scattered field in the calculation region Ω, which can be expressed as:

Figure GDA0002475553110000078
Figure GDA0002475553110000078

向量形式的感应电流

Figure GDA0002475553110000079
表示在第p次入射时,所有单元格离散的电流分布,其可以表示为:Induced current in vector form
Figure GDA0002475553110000079
Indicates the discrete current distribution of all cells at the p-th incident, which can be expressed as:

Figure GDA00024755531100000710
Figure GDA00024755531100000710

其中,

Figure GDA00024755531100000711
是一个对角矩阵,对角线上的每个元素对应于每个网格的对比度。将式子(4)代入式子(6),可以得到状态方程,表示如下:in,
Figure GDA00024755531100000711
is a diagonal matrix where each element on the diagonal corresponds to the contrast of each grid. Substituting formula (4) into formula (6), the state equation can be obtained, expressed as follows:

Figure GDA00024755531100000712
Figure GDA00024755531100000712

相同地,位于观测区域S的散射场可以离散为数据方程,表示如下:Similarly, the scattered field located in the observation area S can be discretized into a data equation, expressed as follows:

Figure GDA00024755531100000713
Figure GDA00024755531100000713

其中,

Figure GDA00024755531100000714
表示位于计算区域Ω的感应电流到观测区域S中散射场之间关系的二维格林公式。in,
Figure GDA00024755531100000714
Two-dimensional Green's formula expressing the relationship between the induced current located in the calculation region Ω and the scattered field in the observation region S.

利用传统MoM求解感应电流的状态方程可以表示为:Using traditional MoM to solve the state equation of induced current can be expressed as:

Figure GDA00024755531100000715
Figure GDA00024755531100000715

其中,

Figure GDA00024755531100000716
表示单位矩阵。利用公式(9)求出感应电流后,便可利用公式(8)求出散射场。in,
Figure GDA00024755531100000716
represents the identity matrix. After using the formula (9) to calculate the induced current, the formula (8) can be used to calculate the scattered field.

可以看到,在利用公式(9)求感应电流时,当计算区域Ω较大时,计算复杂度高,计算量非常大,故本例采用共轭梯度快速傅立叶变换(CG-FFT)来求解感应电流,大大提高了计算效率。It can be seen that when using formula (9) to find the induced current, when the calculation area Ω is large, the calculation complexity is high and the calculation amount is very large, so this example uses the conjugate gradient fast Fourier transform (CG-FFT) to solve The induction current greatly improves the calculation efficiency.

共轭梯度(CG)法是一种数值求解无约束优化问题的数学方法,该算法的特点是使用的迭代方向是共轭方向而不是局部梯度方向,通常比最速下降法收敛得更快。The conjugate gradient (CG) method is a mathematical method for numerically solving unconstrained optimization problems. The characteristic of this algorithm is that the iterative direction used is the conjugate direction instead of the local gradient direction, and it usually converges faster than the steepest descent method.

在复数空间中,共轭梯度法可求解以下线性方程组,In the space of complex numbers, the conjugate gradient method solves the following system of linear equations,

Figure GDA0002475553110000081
Figure GDA0002475553110000081

等同于求解以下最小化问题:is equivalent to solving the following minimization problem:

Figure GDA0002475553110000082
Figure GDA0002475553110000082

以感应电流

Figure GDA0002475553110000083
作为未知量/>
Figure GDA0002475553110000084
可将公式(9)转为公式(10)的形式,进而利用共轭梯度法求解。induced current
Figure GDA0002475553110000083
as unknown />
Figure GDA0002475553110000084
Formula (9) can be transformed into the form of formula (10), and then solved by the conjugate gradient method.

共轭梯度法求解步骤如下:The solution steps of the conjugate gradient method are as follows:

1)设置初值x0,r0=g0=Ax0-b;1) Set the initial value x 0 , r 0 =g 0 =Ax 0 -b;

2)确定第一次梯度搜索方向:P0=-A*r02) Determine the first gradient search direction: P 0 =-A * r 0 ;

3)

Figure GDA0002475553110000085
xk+1=xkkPk,rk+1=rkkAPk;3)
Figure GDA0002475553110000085
x k+1 = x kk P k ,r k+1 =r kk AP k ;

4)

Figure GDA0002475553110000086
Pk+1=-A*rk+1kPk;4)
Figure GDA0002475553110000086
P k+1 =-A * r k+1k P k ;

5)设置迭代终止条件并判断是否满足迭代终止条件,若否,转向步骤3),若是,得到x。5) Set the iteration termination condition and judge whether the iteration termination condition is satisfied, if not, go to step 3), if yes, get x.

其中,变量右上角*表示共轭转置符号。Among them, * in the upper right corner of the variable indicates the conjugate transpose symbol.

在利用共轭梯度法求解时,涉及大量的矩阵运算,考虑到公式(9)进行转换后

Figure GDA0002475553110000088
为Toeplitz矩阵,故可利用快速傅立叶变换(FFT)进行矩阵运算,该变换大大降低了计算复杂度。求解步骤中,形如A*rk,APk都可以利用FFT进行运算,以APk为例,该运算可以简化为When using the conjugate gradient method to solve, a large number of matrix operations are involved. Considering the conversion of formula (9)
Figure GDA0002475553110000088
It is a Toeplitz matrix, so the fast Fourier transform (FFT) can be used for matrix operation, which greatly reduces the computational complexity. In the solution step, both A * r k and AP k can be operated by FFT. Taking AP k as an example, the operation can be simplified as

Figure GDA0002475553110000087
Figure GDA0002475553110000087

其中,a为由矩阵A中第一行与第一列的数据构成的向量,FFT为离散傅立叶变换,.*表示矩阵间的数据两两相乘。从以上可以看出,矩阵计算量大大降低。Among them, a is a vector composed of the data in the first row and the first column in the matrix A, FFT is the discrete Fourier transform, and .* means that the data between the matrices is multiplied in pairs. It can be seen from the above that the amount of matrix calculation is greatly reduced.

通过以上方法,便求出了样本中的感应电流。Through the above method, the induced current in the sample is obtained.

网络设计:Network design:

本发明设计采用AI学习型网络作为模型来完成训练预测过程,在得到样本对后,将其输入到AI学习型网络中完成训练,从而表征输入信息,也就是散射体,入射场,到感应电流的关系。AI可采用CNN网络,U-net,生成对抗网络GAN等,此处以pix2pix GAN网络为例,pix2pix GAN网络内部结构图如图3所示。The design of the present invention uses the AI learning network as a model to complete the training and prediction process. After obtaining the sample pair, it is input into the AI learning network to complete the training, so as to represent the input information, that is, the scatterer, the incident field, and the induced current. Relationship. AI can use CNN network, U-net, generated confrontation network GAN, etc. Here, the pix2pix GAN network is taken as an example. The internal structure diagram of the pix2pix GAN network is shown in Figure 3.

此处以Pix2pix GAN网络由两部分网络构成,即生成网络G与对抗网络D。本发明中,G网络实际上是一个5层的U-net网络,可以分为三部分,下采样、上采样、跳跃连接层。在G网络最后一层,本发明删去了类似于tanh()之类的激活函数,这样一来,网络最后输出的便是散射体实际值。Here, the Pix2pix GAN network is composed of two parts of the network, namely the generation network G and the confrontation network D. In the present invention, the G network is actually a 5-layer U-net network, which can be divided into three parts, down-sampling, up-sampling, and skip connection layers. In the last layer of the G network, the present invention deletes activation functions similar to tanh(), so that the final output of the network is the actual value of the scatterer.

D网络的目的是为了判别预测图像与真实图像。Pix2pix GAN网络是以条件GAN(CGAN)作为基础的,故D的输入不仅包含了来源与G网络的预测图像,还包含了输入图像作为条件。在pix2pix GAN网络中,D网络输出的一组向量而不是一个标量,这使得D能在图像上子区域块上做出更细微的鉴别,实际上,向量上的每一个元素都对应图像上的一个感受野,也就是所谓的patchGAN操作。The purpose of the D network is to distinguish the predicted image from the real image. The Pix2pix GAN network is based on the conditional GAN (CGAN), so the input of D not only includes the source and the predicted image of the G network, but also includes the input image as the condition. In the pix2pix GAN network, the D network outputs a set of vectors instead of a scalar, which enables D to make more subtle discrimination on the sub-region blocks on the image. In fact, each element on the vector corresponds to the image on the A receptive field, the so-called patchGAN operation.

G和D的损失函数采用最小二乘GAN,定义如下:The loss function of G and D adopts the least squares GAN, which is defined as follows:

Figure GDA0002475553110000091
Figure GDA0002475553110000091

Figure GDA0002475553110000092
Figure GDA0002475553110000092

其中,x表示网络的输入数据,JMoM表示由MoM算法得到的真实电流数据。λ是一个可调节参数,

Figure GDA0002475553110000093
表示真实电流与预测电流的L1范数,定义为:Among them, x represents the input data of the network, and J MoM represents the real current data obtained by the MoM algorithm. λ is an adjustable parameter,
Figure GDA0002475553110000093
Represents the L1 norm of the real current and the predicted current, defined as:

Figure GDA0002475553110000094
Figure GDA0002475553110000094

实施例1Example 1

本发明设计采用的实验装置结构图如图2所示,矩形框与S域面的中心都位于(0,0)处。矩形框大小为2×2m,发射天线与接收天线距离圆心处3m。共有32个接收天线等间距地排布在S域,在设置样本时,发射天线角度选在180°(S域最左侧),入射光波长设定为0.75m。入射场

Figure GDA0002475553110000095
的强度设定为/>
Figure GDA0002475553110000096
Figure GDA0002475553110000097
The structure diagram of the experimental device designed and adopted by the present invention is shown in Fig. 2, and the centers of the rectangular frame and the S domain plane are located at (0, 0). The size of the rectangular frame is 2×2m, and the distance between the transmitting antenna and the receiving antenna is 3m from the center of the circle. A total of 32 receiving antennas are arranged at equal intervals in the S domain. When setting the sample, the transmitting antenna angle is selected at 180° (the leftmost side of the S domain), and the incident light wavelength is set to 0.75m. incident field
Figure GDA0002475553110000095
The intensity is set to />
Figure GDA0002475553110000096
Figure GDA0002475553110000097

训练所用散射体截面为MNIST手写数据集,同时为了使样本多样化,在每个数据截面中随机加了一个圆,圆的半径范围设定为0.15m-0.5m。手写数据与圆的对比度为在

Figure GDA0002475553110000101
Figure GDA0002475553110000102
数值在0.01-0.50之间随机变化,两者相互独立。样本总数为10000,其中,9500个用于训练,500个用于测试。输入样本如图4所示,/>
Figure GDA0002475553110000103
对应输入方案/>
Figure GDA0002475553110000104
The scatterer section used for training is the MNIST handwritten data set. At the same time, in order to diversify the samples, a circle is randomly added to each data section, and the radius of the circle is set to 0.15m-0.5m. The contrast between the handwritten data and the circle is at
Figure GDA0002475553110000101
Figure GDA0002475553110000102
Values vary randomly between 0.01-0.50, independent of each other. The total number of samples is 10000, of which 9500 are used for training and 500 are used for testing. The input sample is shown in Figure 4, />
Figure GDA0002475553110000103
Corresponding input scheme />
Figure GDA0002475553110000104

为了让本发明的实验结果与传统MoM算法进行精度对比,先将网格离散为64×64,在利用传统MoM算法得到感应电流(记为J64)后,等间距采样为32×32,记为J64to32。同时,传统MoM算法在网格划分为32×32情况下,计算出的感应电流记为J32。J64to32便是输入网络的电流数据,同时也是评估网络预测出的电流与J32的标准。Jpix2pix表示网络预测得到的电流。In order to compare the accuracy of the experimental results of the present invention with the traditional MoM algorithm, the grid is discretized to 64×64 first, and after using the traditional MoM algorithm to obtain the induced current (denoted as J 64 ), the equidistant sampling is 32×32, denoted for J 64to32 . At the same time, the induced current calculated by the traditional MoM algorithm is denoted as J 32 when the grid is divided into 32×32. J 64to32 is the current data input into the network, and it is also the standard for evaluating the current predicted by the network and J 32 . J pix2pix represents the current predicted by the network.

Pix2pix GAN网络中的patchGAN设定为15×15,图3中网络通道数N设定为64。G网络与D网络的初始学习率为0.0002,且每经过100个循环降低一半,总循环为300。Batchsize设定为64,公式(14)中参数λ设定为100。The patchGAN in the Pix2pix GAN network is set to 15×15, and the number of network channels N in Figure 3 is set to 64. The initial learning rate of G network and D network is 0.0002, and it is reduced by half every 100 cycles, and the total cycle is 300. Batchsize is set to 64, and the parameter λ in formula (14) is set to 100.

图5是2个网络预测出的电流与传统MoM算法计算得出的电流对比图。该实验第一个测试的对比度为0.2,入射光照强度为

Figure GDA0002475553110000105
第二个测试的对比度为0.4,入射光照强度为/>
Figure GDA0002475553110000106
两个例子具有相同的/>
Figure GDA0002475553110000107
同时,实验增加了/>
Figure GDA0002475553110000108
与/>
Figure GDA0002475553110000109
两个输入方案作为对比。图中(a)表示计算区域真实截面;(b)表示J64;(c)表示J64to32;(d)表示J32;(e)分别J32与J64to32的绝对误差;(f)-(h)分别表示/>
Figure GDA00024755531100001010
三种作为网络输入所预测的电流与J64to32的绝对误差图。表1包含了2个例子的散射体介电常数信息以及平均绝对误差数据。Figure 5 is a comparison chart of the current predicted by the two networks and the current calculated by the traditional MoM algorithm. The contrast of the first test of this experiment is 0.2, and the incident light intensity is
Figure GDA0002475553110000105
The second test has a contrast ratio of 0.4 and an incident light intensity of />
Figure GDA0002475553110000106
Both examples have the same />
Figure GDA0002475553110000107
At the same time, the experiment added />
Figure GDA0002475553110000108
with />
Figure GDA0002475553110000109
Two input schemes are used for comparison. In the figure (a) represents the real section of the calculation area; (b) represents J 64 ; (c) represents J 64to32 ; (d) represents J 32 ; (e) the absolute error of J 32 and J 64to32 respectively; (f)-( h) represent respectively />
Figure GDA00024755531100001010
Absolute error plot of J 64to32 for the three currents predicted as input to the network. Table 1 contains the scatterer permittivity information and mean absolute error data for the two examples.

可以看出,在入射天线的照射强度不固定时,在相同的网格划分下,本发明所采用的前向电流学习方法,

Figure GDA00024755531100001011
作为输入的方案比其他两种方案(即/>
Figure GDA00024755531100001012
作为输入)效果好很多,且比传统MoM算法精度高,且能够模拟出样本之外复杂散射体的散射场数据分布,在计算速度上也比传统算法快得多。It can be seen that when the irradiation intensity of the incident antenna is not fixed, under the same grid division, the forward current learning method adopted in the present invention,
Figure GDA00024755531100001011
The scheme as input is more efficient than the other two schemes (ie />
Figure GDA00024755531100001012
As the input), the effect is much better, and the accuracy is higher than the traditional MoM algorithm, and it can simulate the scattering field data distribution of the complex scatterer outside the sample, and the calculation speed is much faster than the traditional algorithm.

Figure GDA0002475553110000111
Figure GDA0002475553110000111

表1实施例1获得的前向电流结果与传统MoM获得的电流平均绝对误差数据Table 1 The forward current result obtained in Example 1 and the current mean absolute error data obtained by traditional MoM

实施例2Example 2

本发明设计采用的实验装置结构图如图2所示,矩形框与S域面的中心都位于(0,0)处。矩形框大小为2×2m,发射天线与接收天线距离圆心处3m。共有32个接收天线等间距地排布在S域,在设置样本时,发射天线的位置不唯一,每10°设置一个入射点位,入射点位分布在0°-360°之间。入射光波长设定为0.75m。The structure diagram of the experimental device designed and adopted by the present invention is shown in Fig. 2, and the centers of the rectangular frame and the S domain plane are located at (0, 0). The size of the rectangular frame is 2×2m, and the distance between the transmitting antenna and the receiving antenna is 3m from the center of the circle. A total of 32 receiving antennas are arranged at equal intervals in the S domain. When setting samples, the position of the transmitting antenna is not unique. An incident point is set every 10°, and the incident points are distributed between 0°-360°. The incident light wavelength was set to 0.75m.

训练所用散射体截面为MNIST手写数据集,同时为了使样本多样化,我们在每个数据截面中随机加了一个圆,圆的半径范围设定为0.15m-0.5m。手写数据与圆的对比度在0.01-0.50之间随机变化,两者相互独立。样本总数为20000,其中,19000个用于训练,1000个用于测试。输入样本如图6所示,

Figure GDA0002475553110000112
对应输入方案/>
Figure GDA0002475553110000113
图中三个样本发射天线的采样点分别位于310°,10°,80°。The scatterer section used for training is the MNIST handwritten data set. At the same time, in order to diversify the samples, we randomly added a circle to each data section, and the radius of the circle was set to 0.15m-0.5m. The contrast between the handwritten data and the circle was randomly varied from 0.01 to 0.50, independent of each other. The total number of samples is 20,000, of which 19,000 are used for training and 1,000 are used for testing. The input sample is shown in Figure 6,
Figure GDA0002475553110000112
Corresponding input scheme />
Figure GDA0002475553110000113
The sampling points of the three sample transmitting antennas in the figure are respectively located at 310°, 10°, and 80°.

为了让本发明的实验结果与传统MoM算法形成对照,首次将网格离散为64×64,在利用传统MoM算法得到感应电流(记为J64)后,等间距采样为32×32,记为J64to32。同时,传统MoM算法在网格划分为32×32情况下,计算出的感应电流记为J32。J64to32便是输入网络的电流数据,同时也是评估网络预测出的电流与J32的标准。Jpxi2pix表示网络预测得到的电流。In order to compare the experimental results of the present invention with the traditional MoM algorithm, the grid is discretized to 64×64 for the first time. After using the traditional MoM algorithm to obtain the induced current (denoted as J 64 ), the equidistant sampling is 32×32, denoted as J 64to32 . At the same time, the induced current calculated by the traditional MoM algorithm is denoted as J 32 when the grid is divided into 32×32. J 64to32 is the current data input into the network, and it is also the standard for evaluating the current predicted by the network and J 32 . J pxi2pix represents the current predicted by the network.

Pix2pix GAN网络中的patchGAN设定为15×15,图3中网络通道数N设定为64。G网络与D网络的初始学习率为0.0002,且每经过100个循环降低一半,总循环为300。Batchsize设定为64,公式(14)中参数λ设定为100。The patchGAN in the Pix2pix GAN network is set to 15×15, and the number of network channels N in Figure 3 is set to 64. The initial learning rate of G network and D network is 0.0002, and it is reduced by half every 100 cycles, and the total cycle is 300. Batchsize is set to 64, and the parameter λ in formula (14) is set to 100.

图7是4个网络预测出的电流与传统MoM算法计算得出的电流对比图。图中(a)表示计算区域真实截面;(b)表示J64;(c)表示J64to32;(d)表示J32;(e)分别J32与J64to32的绝对误差;(f)-(h)分别表示

Figure GDA0002475553110000121
三种作为网络输入所预测的电流与J64to32的绝对误差图。表2包含了4个例子的散射体介电常数信息,发射天线所处位置,以及平均绝对误差数据。图8是4个例子重建的散射场结果与传统MoM计算得到的散射场对比图。可以看出,后面两个例子发射天线的入射角度在样本选取点之外,预测得到的电流数据依旧准确,故实现了天线任意发射位置散射场数据的预测。同时,在相同的网格划分下,本发明所采用的前向电流学习方法,/>
Figure GDA0002475553110000122
作为输入的方案比传统MoM算法精度高,且能够模拟出样本之外复杂散射体的散射场数据分布,在计算速度上也比传统算法快得多。Figure 7 is a comparison chart of the current predicted by the four networks and the current calculated by the traditional MoM algorithm. In the figure (a) represents the real section of the calculation area; (b) represents J 64 ; (c) represents J 64to32 ; (d) represents J 32 ; (e) the absolute error of J 32 and J 64to32 respectively; (f)-( h) represent respectively
Figure GDA0002475553110000121
Absolute error plot of J 64to32 for the three currents predicted as input to the network. Table 2 contains information on the permittivity of the scatterers, the location of the transmitting antenna, and the mean absolute error data for the four examples. Figure 8 is a comparison of the scattered field results reconstructed in four examples and the scattered field calculated by traditional MoM. It can be seen that the incident angle of the transmitting antenna in the latter two examples is outside the sample selection point, and the predicted current data is still accurate, so the prediction of the scattered field data at any transmitting position of the antenna is realized. At the same time, under the same grid division, the forward current learning method adopted by the present invention, />
Figure GDA0002475553110000122
The input scheme has higher accuracy than the traditional MoM algorithm, and can simulate the distribution of scattering field data of complex scatterers outside the sample, and its calculation speed is much faster than the traditional algorithm.

Figure GDA0002475553110000123
Figure GDA0002475553110000123

表2实施例2获得的前向电流结果与传统MoM获得的电流平均绝对误差数据The forward current result obtained in Table 2 Example 2 and the current mean absolute error data obtained by traditional MoM

上述两个实例仅仅只是例证本发明方法,并非是对于本发明的限制,本发明也并非仅限于上述两个实例,只要符合本发明方法的要求,均属于本发明方法的保护范围。Above-mentioned two examples just illustrate the method of the present invention, are not for restriction of the present invention, and the present invention is not limited to above-mentioned two examples, as long as meet the requirement of the method of the present invention, all belong to the protection domain of the method of the present invention.

Claims (10)

1.一种适用于任意入射场的AI学习型电磁散射计算方法,采用AI学习网络来训练学习对比度
Figure FDA0004143099830000011
入射波/>
Figure FDA0004143099830000012
到感应电流之间的非线性关系,其特征在于:
1. An AI learning electromagnetic scattering calculation method suitable for any incident field, using AI learning network to train and learn contrast
Figure FDA0004143099830000011
incident wave/>
Figure FDA0004143099830000012
to the nonlinear relationship between the induced current, characterized by:
样本设计:为了引入已知信息,网络输入采用
Figure FDA0004143099830000013
作为输入,计算得到前向电流数据作为AI学习型网络的真实样本;
Sample design: In order to introduce known information, the network input adopts
Figure FDA0004143099830000013
As input, calculate the forward current data as the real sample of the AI learning network;
网络设计:采用AI学习型网络作为模型来完成训练预测过程,从而表征输入信息,也就是散射体,入射场,到感应电流的关系。Network design: AI learning network is used as a model to complete the training and prediction process, so as to represent the relationship between input information, that is, scatterers, incident fields, and induced currents.
2.根据权利要求1所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的前向电流数据的计算方法为矩量法MoM、有限元法FEM、时域有限差分法FDTD。2. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 1, characterized in that the calculation method of the forward current data is method of moments MoM, finite element method FEM, time Finite Difference Domain Method FDTD. 3.根据权利要求1所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的前向电流数据的计算方法为矩量法MoM计算步骤如下:3. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 1, characterized in that the calculation method of the forward current data is the method of moments (MoM) calculation steps are as follows: 总场积分方程为:The total field integral equation is:
Figure FDA0004143099830000014
Figure FDA0004143099830000014
其中,
Figure FDA0004143099830000015
和/>
Figure FDA0004143099830000016
分别表示总场和入射场,r与r分别表示第p次入射的场点与源点;/>
Figure FDA0004143099830000017
为二维自由空间格林公式,表示一个位于空间r处的点源对其周围空间某一点r所产生的场,其中,/>
Figure FDA0004143099830000018
为第一类零阶汉克尔函数,i表示虚数,k0是弹性波的波数,χ(r)=(ε(r)-∈0)/∈0,它为∈r的对比度函数,∈0表示弹性波穿过的介质的某种物理特性;Ω表示计算区域,感应电流J(r)可以定义为
Figure FDA0004143099830000019
在观测区域S中,散射场/>
Figure FDA00041430998300000110
带有电流项J(r)的电场积分方程可以定义为:
in,
Figure FDA0004143099830000015
and />
Figure FDA0004143099830000016
represent the total field and the incident field respectively, r and r ' represent the field point and the source point of the pth incident respectively; />
Figure FDA0004143099830000017
is the two-dimensional free space Green's formula, expressing the field produced by a point source located at space r to a certain point r ' in its surrounding space, where, />
Figure FDA0004143099830000018
is the first kind of zero-order Hankel function, i represents an imaginary number, k 0 is the wave number of elastic wave, χ(r )=(ε(r )-∈ 0 )/∈ 0 , it is the contrast function of ∈ r , ∈ 0 represents a certain physical property of the medium through which the elastic wave passes; Ω represents the calculation area, and the induced current J(r ) can be defined as
Figure FDA0004143099830000019
In the observation area S, the scattered field />
Figure FDA00041430998300000110
The electric field integral equation with the current term J(r ) can be defined as:
Figure FDA00041430998300000111
Figure FDA00041430998300000111
为了便于引入MoM来离散公式(1)和(2),计算区域Ω被离散为M个小方块单元,M=M1×M2,M1,M2分别表示x轴与y轴方向的数量,如果被分离的小单元变长远小于十分之一的波长,每个单元格内的感应电流与总场可以视为相同的,因此,公式(1)可以离散为:In order to facilitate the introduction of MoM to discretize formulas (1) and (2), the calculation area Ω is discretized into M small square units, M=M 1 ×M 2 , M 1 , M 2 represent the quantities in the x-axis and y-axis directions respectively , if the length of the separated small unit becomes much smaller than one-tenth of the wavelength, the induced current and the total field in each unit can be regarded as the same, therefore, formula (1) can be discretized as:
Figure FDA00041430998300000112
Figure FDA00041430998300000112
其中,
Figure FDA0004143099830000021
与/>
Figure FDA0004143099830000022
分别表示在第p次入射时,相应对第m个网格的总场与入射场,Am′表示第m个网格的面积;/>
Figure FDA0004143099830000023
在第p次入射时,第m个网格的感应电流,综合计算区域Ω中所有的网格,式子(3)可以写成以下矩阵形式:
in,
Figure FDA0004143099830000021
with />
Figure FDA0004143099830000022
Respectively represent the total field and the incident field corresponding to the mth grid at the pth incident, and A m' represents the area of the m ' th grid; />
Figure FDA0004143099830000023
When the p-th incident occurs, the induced current of the m ' th grid is comprehensively calculated for all the grids in the area Ω, and the formula (3) can be written in the following matrix form:
Figure FDA0004143099830000024
Figure FDA0004143099830000024
其中
Figure FDA0004143099830000025
Figure FDA0004143099830000026
表示从感应电流到计算区域Ω中散射场之间的二维自由空间格林公式,其可以表示为:
in
Figure FDA0004143099830000025
Figure FDA0004143099830000026
Represents the two-dimensional free-space Green's formula between the induced current and the scattered field in the calculation region Ω, which can be expressed as:
Figure FDA0004143099830000027
Figure FDA0004143099830000027
向量形式的感应电流
Figure FDA0004143099830000028
表示在第p次入射时,所有单元格离散的电流分布,其可以表示为:
Induced current in vector form
Figure FDA0004143099830000028
Indicates the discrete current distribution of all cells at the p-th incident, which can be expressed as:
Figure FDA0004143099830000029
Figure FDA0004143099830000029
其中,
Figure FDA00041430998300000210
是一个对角矩阵,对角线上的每个元素对应于每个网格的对比度,将式子(4)代入式子(6),可以得到状态方程,表示如下:
in,
Figure FDA00041430998300000210
is a diagonal matrix, and each element on the diagonal corresponds to the contrast of each grid. Substituting equation (4) into equation (6), the state equation can be obtained, expressed as follows:
Figure FDA00041430998300000211
Figure FDA00041430998300000211
相同地,位于观测区域S的散射场可以离散为数据方程,表示如下:Similarly, the scattered field located in the observation area S can be discretized into a data equation, expressed as follows:
Figure FDA00041430998300000212
Figure FDA00041430998300000212
其中,
Figure FDA00041430998300000213
表示位于计算区域Ω的感应电流到观测区域S中散射场之间关系的二维格林公式;
in,
Figure FDA00041430998300000213
Two-dimensional Green's formula expressing the relationship between the induced current located in the calculation area Ω and the scattered field in the observation area S;
利用传统MoM求解感应电流的状态方程可以表示为:Using traditional MoM to solve the state equation of induced current can be expressed as:
Figure FDA00041430998300000214
Figure FDA00041430998300000214
其中,
Figure FDA00041430998300000215
表示单位矩阵,利用公式(9)求出感应电流后,便可利用公式(8)求出散射场。
in,
Figure FDA00041430998300000215
Represents the unit matrix, and after using the formula (9) to calculate the induced current, the formula (8) can be used to calculate the scattering field.
4.根据权利要求3所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于公式(9)计算感应电流的方式替换为采用共轭梯度快速傅立叶变换(CG-FFT)求解感应电流,在复数空间中,共轭梯度法可求解以下线性方程组,4. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 3, it is characterized in that formula (9) calculates the mode of induced current to be replaced by using conjugate gradient fast Fourier transform (CG-FFT ) to solve the induced current, in the complex space, the conjugate gradient method can solve the following linear equations,
Figure FDA00041430998300000216
Figure FDA00041430998300000216
等同于求解以下最小化问题:is equivalent to solving the following minimization problem:
Figure FDA0004143099830000031
Figure FDA0004143099830000031
以感应电流
Figure FDA0004143099830000032
作为未知量/>
Figure FDA0004143099830000033
可将公式(9)转为公式(10)的形式,进而利用共轭梯度法求解。
induced current
Figure FDA0004143099830000032
as unknown />
Figure FDA0004143099830000033
Formula (9) can be transformed into the form of formula (10), and then solved by the conjugate gradient method.
5.根据权利要求4所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的共轭梯度法求解步骤如下:5. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 4, characterized in that said conjugate gradient method solution steps are as follows: 1)设置初值x0,r0=g0=Ax0-b;1) Set the initial value x 0 , r 0 =g 0 =Ax 0 -b; 2)确定第一次梯度搜索方向:P0=-A*r02) Determine the first gradient search direction: P 0 =-A * r 0 ; 3)
Figure FDA0004143099830000034
xk+1=xkkPk,rk+1=rkkAPk
3)
Figure FDA0004143099830000034
x k+1 = x kk P k ,r k+1 =r kk AP k ;
4)
Figure FDA0004143099830000035
Pk+1=-A*rk+1kPk
4)
Figure FDA0004143099830000035
P k+1 =-A * r k+1k P k ;
5)设置迭代终止条件并判断是否满足迭代终止条件,若否,转向步骤3),5) Set the iteration termination condition and judge whether the iteration termination condition is satisfied, if not, turn to step 3), 若是,得到x;If so, get x; 其中,变量右上角*表示共轭转置符号;Among them, * in the upper right corner of the variable indicates the conjugate transpose symbol; 在利用共轭梯度法求解时,涉及大量的矩阵运算,考虑到公式(9)进行转换后
Figure FDA0004143099830000036
为Toeplitz矩阵,故可利用快速傅立叶变换(FFT)进行矩阵运算,求解步骤中,形如A*rk,APk都可以利用FFT进行运算,APk的运算可以简化为
When using the conjugate gradient method to solve, a large number of matrix operations are involved. Considering the conversion of formula (9)
Figure FDA0004143099830000036
is a Toeplitz matrix, so the fast Fourier transform (FFT) can be used for matrix operations. In the solution step, the shape is A * r k , AP k can be operated by FFT, and the operation of AP k can be simplified as
Figure FDA0004143099830000037
Figure FDA0004143099830000037
其中,a为由矩阵A中第一行与第一列的数据构成的向量,FFT为离散傅立叶变换,.*表示矩阵间的数据两两相乘。Among them, a is a vector composed of the data in the first row and the first column in the matrix A, FFT is the discrete Fourier transform, and .* means that the data between the matrices is multiplied in pairs.
6.根据权利要求1所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的AI学习网络采用CNN网络,U-net,生成对抗网络GAN,Pix2pix GAN网络。6. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 1, characterized in that said AI learning network adopts CNN network, U-net, generating confrontation network GAN, Pix2pix GAN network . 7.根据权利要求1所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的AI学习网络采用Pix2pix GAN网络,Pix2pix GAN网络由两部分网络构成,即生成网络G与对抗网络D。7. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 1, characterized in that said AI learning network adopts Pix2pix GAN network, and Pix2pix GAN network is composed of two parts of the network, namely generating Network G and confrontation network D. 8.根据权利要求7所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于生成网络G实际上是一个5层的U-net网络,包括下采样、上采样、跳跃连接层,在生成网络G最后一层,网络最后直接输出散射体实际值,未使用类似于tanh()之类的激活函数。8. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 7, characterized in that the generation network G is actually a 5-layer U-net network, including downsampling, upsampling, The skip connection layer is the last layer of the generation network G, and the network directly outputs the actual value of the scatterer at the end, without using an activation function similar to tanh(). 9.根据权利要求7所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的对抗网络D的输入包含了来源与生成网络G的预测图像和输入图像作为条件,对抗网络D输出的一组向量。9. An AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 7, characterized in that the input of the confrontation network D includes the source and generation network G's predicted image and input image as condition, a set of vectors output by the adversarial network D. 10.根据权利要求7所述的一种适用于任意入射场的AI学习型电磁散射计算方法,其特征在于所述的生成网络G和对抗网络D的损失函数采用最小二乘GAN,定义如下:10. A kind of AI learning type electromagnetic scattering calculation method applicable to any incident field according to claim 7, characterized in that the loss function of the generation network G and the confrontation network D adopts the least squares GAN, which is defined as follows:
Figure FDA0004143099830000041
Figure FDA0004143099830000041
Figure FDA0004143099830000042
Figure FDA0004143099830000042
其中,x表示网络的输入数据,JMoM表示由MoM算法得到的真实电流数据;λ是一个可调节参数,
Figure FDA0004143099830000043
表示真实电流与预测电流的L1范数,定义为:
Among them, x represents the input data of the network, J MoM represents the real current data obtained by the MoM algorithm; λ is an adjustable parameter,
Figure FDA0004143099830000043
Represents the L1 norm of the real current and the predicted current, defined as:
Figure FDA0004143099830000044
Figure FDA0004143099830000044
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