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Three-dimensional reconstructing of objects buried in spherically multilayered medium using Born Iterative Methods

机译:Born迭代法三维重构球形多层介质中的物体

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In this paper, we applied the Born Iterative Method (BIM) to reconstruct three-dimensional inhomogeneous objects buried in spherically multilayered media. The nonlinear inverse problem is linearized by Born approximations and solved iteratively via the conjugate-gradient approach (CG). The forward scattering problem in the spherically multilayered media is solved by stabilized biconjugate-gradient fast Fourier transform method (BCGS-FFT). The dyadic Greens' functions for spherically multilayered media are constructed using the method of scattering superposition and the recurrence equation system of coefficient matrix. Numerical results showed that these methods are capable of solving the EM scattering problem and inverse problems for inhomogeneous objects of arbitrary shape buried in spherically multilayered media. Figure 1 illustrates the comparison of the electric fields inside the scatter between the simulation results from the commercial software Wavenology and our solutions in spherically three-layered media with the scatter entirely embedded in the second layer. As illustrated in Figure 1(a), an inhomogeneous cuboid is embedded entirely in the second layer in a spherically three-layered medium where r1 = 20m and r2 = 10 m. The three-layered medium is characterized by ∈r1 = 1, σ1 = 0, ∈r2 = 2, σ2 = 0.001 S/m, ∈r3 = 4, σ3 = 0.001 S/m and μr = 1 for all three layers. The electrical parameters of the scatter are ∈rs = 6, σrs = 0.001 S/m and μrs = 1. The center of the scatter is located at (7.25, 7.25.7.25)m and the dimension of the cube is 0.5 × 0.5 × 0.5 m. The electric dipole source is distributed at (15, 15, 15) m. We use Nx = Ny = Nz = 10 for discretization and choose 50MHz to do the calculation. The total electric field of Ez inside the scatter caused by the electric dipole is compared with Wavenology, as is shown in Figures 1(b) and (c).
机译:在本文中,我们应用了Born迭代方法(BIM)重建了埋在球形多层介质中的三维非均匀物体。非线性反问题通过Born近似线性化,并通过共轭梯度法(CG)迭代求解。通过稳定的双共轭梯度快速傅里叶变换方法(BCGS-FFT)解决了球形多层介质中的前向散射问题。利用散射叠加法和系数矩阵递推方程组构造了球形多层介质的二进格林函数。数值结果表明,这些方法能够解决埋在球形多层介质中的任意形状的非均匀物体的电磁散射问题和反问题。图1说明了在商业软件Wavenology的模拟结果与我们在球形三层介质中的解决方案之间的散射内部电场的比较,该解决方案完全分散在第二层中。如图1(a)所示,不均匀的长方体完全埋在球形三层介质的第二层中,其中r1 = 20m,r2 = 10 m。该三层介质的特征是∈r1= 1,σ1= 0,∈r2= 2,σ2= 0.001 S / m,∈r3= 4,σ3= 0.001 S / m和所有三个层的μr= 1。散射的电气参数为εrs= 6,σrs= 0.001 S / m,μrs=1。散射的中心位于(7.25,7.25.7.25)m,立方体的尺寸为0.5×0.5× 0.5米电偶极子源分布在(15、15、15)m。我们使用Nx = Ny = Nz = 10进行离散化,并选择50MHz进行计算。如图1(b)和(c)所示,将由电偶极子引起的散射内的Ez的总电场与Wavenology进行比较。

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