
Uniqueness theorem and uniqueness of inverse problems for lossy anisotropic inhomogeneous structures with diagonal material tensors Reza Dehbashi, Konstanty S. Bialkowski, and Amin M. Abbosh Citation: Journal of Applied Physics 121, 203103 (2017); doi: 10.1063/1.4983768 View online: https://doi.org/10.1063/1.4983768 View Table of Contents: http://aip.scitation.org/toc/jap/121/20 Published by the American Institute of Physics Articles you may be interested in Photoconductivity induced by nanoparticle segregated grain-boundary in spark plasma sintered BiFeO3 Journal of Applied Physics 121, 203102 (2017); 10.1063/1.4983764 W/Cu thin film infrared reflector for TiNxOy based selective solar absorber with high thermal stability Journal of Applied Physics 121, 203101 (2017); 10.1063/1.4983763 Dynamic susceptibility of concentric permalloy rings with opposite chirality vortices Journal of Applied Physics 121, 203901 (2017); 10.1063/1.4983759 Practical considerations in the modeling of field emitter arrays with line charge distributions Journal of Applied Physics 121, 203303 (2017); 10.1063/1.4983680 Vertical transport in isotype InAlN/GaN dipole induced diodes grown by molecular beam epitaxy Journal of Applied Physics 121, 205702 (2017); 10.1063/1.4983767 Fluid simulation of species concentrations in capacitively coupled N2/Ar plasmas: Effect of gas proportion Journal of Applied Physics 121, 203302 (2017); 10.1063/1.4983675 JOURNAL OF APPLIED PHYSICS 121, 203103 (2017) Uniqueness theorem and uniqueness of inverse problems for lossy anisotropic inhomogeneous structures with diagonal material tensors Reza Dehbashi,a) Konstanty S. Bialkowski, and Amin M. Abbosh School of Information Technology and Electrical Engineering, University of Queensland, St. Lucia, Brisbane, QLD 4067, Australia (Received 3 February 2017; accepted 7 May 2017; published online 22 May 2017) The uniqueness theorem for lossy anisotropic inhomogeneous structures with diagonal material tensors is proven. For these materials, we prove that all the elements of the constitutive tensors must be lossy. Materials like cloaks and lenses designed based on transformation-optics (TO) could be examples of such materials. The uniqueness theorem is about the uniqueness of Maxwell’s equa- tions solutions for particular sets of boundary conditions. We prove the uniqueness theorem for three cases: Single medium, media composed of two lossy anisotropic inhomogeneous materials with diagonal constitutive parameters, and media composed of two materials, where a material with diagonal material tensors is surrounded by an isotropic material. The latter case can be consid- ered for the TO-based materials like invisibility cloaks or hyper-lenses that usually have diagonal anisotropic inhomogeneous constitutive parameters and also because cloaks or hyper-lenses are usually surrounded by free space and the sources are usually outside. For the sake of our argument in the uniqueness theorem that loss is the main condition for the validity of this theory, for cloaks as an example case of our analysis, it is analytically and numerically proven that the ideal invisibil- ity phenomenon is possible for a simple lossy structure. We also examine the uniqueness of the inverse problem for such structures. We prove that all these materials have the same surface field distribution on a surface enclosing the area of interest, while solutions to Maxwell’s equations inside them are different. The uniqueness of the inverse problem suggests that within the surface, the same medium should exactly be present. However, for lossy anisotropic inhomogeneous struc- tures with diagonal constitutive parameters, this paper illustrates that this might not be true, despite the result of a previous study that shows that uniqueness could be true for some anisotropic inho- mogeneous structures. For the analysis, the transverse electric Z-polarization is used. The simula- tion results are obtained by using a commercial Finite-Element based simulator. Published by AIP Publishing. [http://dx.doi.org/10.1063/1.4983768] I. INTRODUCTION The uniqueness theorem is an important theory in electro- magnetics and is the basis of some other important electro- Transformation optics (TO) was introduced by Pendry magnetics theories like the induction theorem, equivalence et al.1 and later used to design different shapes of invisibility principle, image theory, and conformal mapping theory. The cloaks.1–6 According to that method, an enclosed area can be investigated uniqueness theorem is about the uniqueness of transformed into a shell7–9 that can be used to conceal any the solutions of Maxwell’s equations in a medium with a par- object with any shape and material.1 The method has also been used to design other novel devices like light concentra- ticular boundary condition. Most electromagnetics textbooks 10 11 12,13 have introduced this theorem for lossy isotropic homogeneous tors, lenses, gradient-index bends and waveguides, 28 black holes,14 and illusion devices.15 Both simulation16 and mediums. However, this theorem has not yet been directly measurement results17 show the effectiveness of transforma- proven for anisotropic inhomogeneous with diagonal tensor tion optics to design invisibility cloaks. The method intro- constitutive parameters. Most TO based materials have such duced in Ref. 1 is not the only way to design invisibility structures, and invisibility cloaking is one of them. Even the cloaks. Cloaking can also be designed using the TO of a newer version of TO, called Quasi-Conformal Transformation curved, non-Euclidean space,18 the transmission-line-method Optics (QCTO), usually creates materials with diagonal con- cloaking,19,20 the external cloaking based on the comple- stitutive tensors in various applications including the antenna 29–31 mentary media concept,21 and the cloaking method to con- applications. The QCTO uses a smoother transformation ceal sub-wavelength objects.22,23 Metamaterials are the key function to limit anisotropy of the structures. There is a con- to implement such methods in reality not only to manipu- cern regarding the validity of the uniqueness theorem for late the electromagnetic waves17,22–26 but also to manipu- structures like invisibility cloaks, as these anisotropic inhomo- late electron and matter waves in the area of quantum geneous media may support sets of distinct solutions having mechanics.27 identical boundary conditions; hence, it might be concluded that the uniqueness theorem may not be valid for such aniso- tropic inhomogeneous media with diagonal constitutive a)E-mail: [email protected]. Telephone: þ61(7)33658316. tensors. However, this notion is a misunderstanding of 0021-8979/2017/121(20)/203103/8/$30.00 121, 203103-1 Published by AIP Publishing. 203103-2 Dehbashi, Bialkowski, and Abbosh J. Appl. Phys. 121, 203103 (2017) uniqueness in an inverse problem.32–34 It is noted that con- with an anisotropic inhomogeneous medium with diagonal cepts of the uniqueness of solutions of Maxwell equations and tensors. The permittivity and permeability tensors for this the uniqueness for inverse scattering problems are different. medium at the position r are eðrÞ and lðrÞ, respectively. The focus of the first part of this paper is on the former one. The current densities J i and Mi are the electric and magnetic Using the procedures used to prove the uniqueness of the solu- sources within this volume, respectively. tions of the Maxwell equations in a lossy homogeneous We assume two distinct solutions of Maxwell’s equa- a a medium,28 we prove the uniqueness theorem for an aniso- tions inside the volume V. These are denoted by ðE ; H Þ b b tropic inhomogeneous medium with diagonal constitutive and ðE ; H Þ. Thus, they satisfy the following: tensors. a a The focus of the second part of this paper is on the r  E ¼ Mi þ jxlðrÞH uniqueness of the inverse problem for TO based materials, a a (1) rH ¼ J þ jxeðrÞE ; like invisibility cloaks which usually have anisotropic inho- i mogeneous constitutive parameters. We show that despite and the validity of the uniqueness theorem for the structure, the uniqueness of the inverse problem for the structure is not b b 30 r  E ¼ Mi þ jxlðrÞH valid, even though it is valid for a particular anisotropic (2) b b inhomogeneous structure. rH ¼ J i þ jxeðrÞE : II. UNIQUENESS THEOREM FOR LOSSY For instance, the electric field Ea can be given by ANISOTROPIC INHOMOGENEOUS STRUCTURES WITH DIAGONAL MATERIAL TENSOR STRUCTURES a a a a E ¼ E1a1 þ E2a2 þ E3a3: (3) For the lossy homogeneous medium, the uniqueness of the solutions of Maxwell’s equations was proven.28 In con- Note that the unit vectors ai appearing in (3) form a trast, this paper focuses on TO based structures with lossy right-handed orthonormal basis at every position specified anisotropic inhomogeneous structures with diagonal material by r. Similarly, other vector fields can be cast in the above tensors. Therefore, the uniqueness is investigated for aniso- form. In our analysis, the eðrÞ and lðrÞ values are assumed tropic inhomogeneous structures with diagonal constitutive to be diagonal, i.e., tensors. It is proven for three cases; one of them (case c) can 2 3 0 00 be considered a cloaking structure. e1 À je1 00 6 0 00 7 eðrÞ¼4 0 e2 À je2 0 5; A. Single medium 00e0 À je00 2 3 3 3 The uniqueness theorem is applied to invisibility cloaks 0 00 l1 À jl1 00 1 6 7 designed through the transformation-optics method. In other lðrÞ¼4 0 l0 À jl00 0 5; words, the uniqueness theorem is presented for anisotropic 2 2 00l0 jl00 inhomogeneous structures with diagonal constitutive tensors. 3 À 3 00 00 Figure 1 depicts a volume V enclosed by surface S and filled ei 6¼ 0; li 6¼ 0; (4) 0 00 0 00 where ðei À jei Þ and ðli À jli Þ are the principal permittivity and permeability along the i–th principal axis, respectively.
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