论文标题

从实验反向散射数据中同时重建电介质常数和电导率的逆问题

An inverse problem of a simultaneous reconstruction of the dielectric constant and conductivity from experimental backscattering data

论文作者

Khoa, Vo Anh, Bidney, Grant W., Klibanov, Michael V., Nguyen, Loc H., Nguyen, Lam H., Sullivan, Anders J., Astratov, Vasily N.

论文摘要

该报告扩展了我们最近在解决由Helmholtz方程式控制的具有挑战性的3D反向散射问题方面的进展。我们的目标应用是重建非常紧密地埋在地下的物体的前表面的介电常数,电导率和形状。这些物体模仿爆炸物,例如,例如反某人地雷和简易的爆炸装置。我们解决了一个系数的反问题,其中移动源以固定频率生成的反向散射数据。到目前为止,通过我们新开发的凸化方法对这种情况进行了研究,该方法包括对耦合的准椭圆系统的边界值问题的新推导。但是,在我们以前的工作中,仅计算了对象的未知介电常数和前表面的形状。与此不同,在当前的数值凸化算法的工作性能中,对于介电常数,电导率和对象的形状尚不清楚的情况。通过通过实验收集的反向散射数据进行多个测试,我们发现我们可以准确地对介电常数和兴趣目标的介电常数和形状进行成像,包括具有空隙的目标的具有挑战性的情况。计算的电导率可可靠地区分导电物体和非导电物体。不久将重新审视我们的数值程序的全球融合。

This report extends our recent progress in tackling a challenging 3D inverse scattering problem governed by the Helmholtz equation. Our target application is to reconstruct dielectric constants, electric conductivities and shapes of front surfaces of objects buried very closely under the ground. These objects mimic explosives, like, e.g., antipersonnel land mines and improvised explosive devices. We solve a coefficient inverse problem with the backscattering data generated by a moving source at a fixed frequency. This scenario has been studied so far by our newly developed convexification method that consists in a new derivation of a boundary value problem for a coupled quasilinear elliptic system. However, in our previous work only the unknown dielectric constants of objects and shapes of their front surfaces were calculated. Unlike this, in the current work performance of our numerical convexification algorithm is verified for the case when the dielectric constants, the electric conductivities and those shapes of objects are unknown. By running several tests with experimentally collected backscattering data, we find that we can accurately image both the dielectric constants and shapes of targets of interests including a challenging case of targets with voids. The computed electrical conductivity serves for reliably distinguishing conductive and non-conductive objects. The global convergence of our numerical procedure is shortly revisited.

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