Invisibility Cloaks in Electromagnetic Theory Marco A. Ribeiro †, Carlos R. Paiva ¥ † Instituto de Telecomunicações, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal Phone: +351-218418457, Fax: +351-218418472, e-mail: [email protected] ¥ Instituto de Telecomunicações, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal Phone: +351-218418479, Fax: +351-218418472, e-mail: [email protected]

Abstract 1— In this communication, using a previously derived for electromagnetics and show how it can be used to design framework that we have called the equivalence principle for invisibility devices. electromagnetics, we analyze invisibility cloaking devices. These In section II we address the technical details regarding the devices compress and drag the electromagnetic , without design of cylindrical invisibility devices. We present two disturbing their functionality, to render an object invisible examples cloakings: first, a cloak in which we can control within the concealment region. To assess the accuracy of our how the electromagnetic field is compressed inside it; second, geometric modeling full-wave numerical simulations are also a cloaking which is capable of dragging the electromagnetic provided. field inside it. Finally, in section III we provide full-wave numerical simulations, using the FDTD method, for the invisibility I. INTRODUCTION devices introduced in section II. The unprecedented control over the material properties that can offer [1] has prompted a new and powerful II. THEORETICAL FORMULATION strategy for designing electromagnetic devices. This strategy stems from an equivalence principle for electromagnetics [2]: A. Electrodynamics in general relativity a given geometry creates an effective medium in the same way as a given electromagnetic medium creates an effective In general relativity, and using analysis, the free- geometry [3, 4]. This interplay between geometry and space Maxwell equations are written as [8] F Fαβ j α , (1) electromagnetic media can be explored for designing []αβ; γ =0, ;β = invisibility devices. In fact, cloaking devices that aim the where the semi-colon means covariant differentiation and the concealment of a given object have been the subject of some square brackets indicate anti-symmetrization. It is possible to recent research in electromagnetics [5, 6]. They belong to a cast the information in these equations in the form of two family of extraordinary new devices – called transformation generally covariant Maxwell equations (homogeneous and media – which have many promising applications, e.g., inhomogeneous) and address all the geometric aspects of the shielding from mobile phone and radar , new optical underlying pseudo-Riemannian manifold (M,g ) into a devices and medical imaging. The physical origin for this equivalence principle can be separate spacetime relation. By performing this separation tracked down to Fermat’s principle: rays follow the between the two Maxwell equations and the metric structure stationary optical path in media. That is why especially of spacetime, we get a framework called pre-metric electrodynamics [9]. Using the coordinate-free approach tailored inhomogeneous metamaterials – the up mentioned 2 transformation media – can achieve active transformations by presented in [2] these pre-metric equations are written as dF = 0,( homogeneous equation ) deviating electromagnetic radiation along a prescribed (2) trajectory, thereby obnubilating the object covered with a δ G= J,() inhomogeneous equation cloaking device. 0 123 where F= E ∧ e + ce B is the EM (electromagnetic In this communication we show how the metric-free (and coordinate-free) mathematical setup introduced in [2] - which field) strength untwisted 2-form, G=e123 Hc − D ∧ e 0 is the is based simultaneously on the grammar of Clifford’s EM field excitation bivector density, J is the -current geometric algebras and the language of differential forms - vector density whereas d and δ are the exterior and can be used to design several cylindrical invisibility devices contraction derivatives respectively (see [2] for details). in light of the equivalence principle for electromagnetics. The spacetime relation corresponding to free-space, without This communication is organized as follows. In section I we which the set (2) would not be complete, is given by present a brief description of the theoretical formulation * G= y0 − gg ( F ) , (3) introduced in [2] which was employed - as a unifying approach - to design invisibility devices and study moving media in [7]. We also introduce the principle of equivalence

2 The notation is the same as in [2]: we use italic fonts for forms defined over the cotangent bundle (e.g. F ) and regular fonts for vectors defined over the tangent bundle (e.g. G and J ). where g is a Lorentz metric, g * its inverse bundle map, The parameters ε , ξ , µ and ζ in (4) relate to the metric of spacetime in the following way: g= det (g ) and y0= ε 0 µ 0 . −g The particularly distinctive feature of this approach is that ∗ ε ()E= − g⊥ () E , the two Maxwell equations belong to different bundles of M g00 (see Fig. 1): the homogeneous equation belongs to forms 1 ∗ ξ ()H=e123() H ∧ g ⊥ () e 0 , bundle ( ∧T M ) whereas the in-homogeneous equation g 00 (5) M belongs to exterior algebra bundle ( ∧T ). By using this −g µ ()H= − g∗ () H , strategy, we are able to write our spacetime relation (3) g ⊥ completely free of indices. It seams that this is not easily done 00 with an approach based solely on differential forms [9]. 1 ζ ()E= −e123() E ∧ g ⊥ () e 0 . g00

III. PERMEABILITY AND PERMITIVITY FUNCTIONS OF CLOAKING DEVICES Cloaking devices do not exhibit magneto-electric coupling

( g⊥ (e0 ) = 0 ). Therefore, in (5) we make ξ= ζ = 0 . On the other hand, there is some freedom associated with g and 00 Fig. 1. The generally covariant Maxwell equations are written in we chose g00 = − 1 for commodity. Hence from (5) we find different bundles of M . the compact expression − 1 2 B. The equivalence principle for electromagnetics ε= µ = (g∗ ) g* . (6) According to the equivalence principle [2], there are two A. Cylindrical cloak – compression transformation alternative interpretations for (3): the topological and the materials interpretation. The equivalence principle states that Cylindrical cloaks are devices mapping the space in a 3- dimensional cylindrical volume (radius r ) into a cylindrical the topological interpretation (M,g ) is, from the 2 shell of inner radius and outer radius (Fig. 2). electromagnetic point of view, entirely equivalent to the r1 r2 materials interpretation: it corresponds to a trivial manifold (M, I ) filled with a medium described by a CR (constitutive relation) that caries the information contained in g : M M ()()(),g ⇔,I + CR g վ վ վ

topological interpretation equivalence principle materials interpretation The strength of these interpretations relies in the fact that the generally covariant Maxwell equations are preserved by any diffeomorphism over the four-dimensional spacetime M : we can pull and stretch spacetime, thereby modifying its metric, without any effect on the form of Maxwell equations. Actually, only the spacetime relation, which characterizes free-space from the electromagnetic point of view, will change. One should stress that the information about the flexible metric in (M,g ) cannot be transferred into the realm of (M, I ) : it is now ingrained in the texture of the CR Fig. 2. A light ray passing through a cloak with inner radius characterizing the medium that permeates the trivial and rigid r= 0.1 m and outer radius r= 0.2 m for two values of the M 1 2 ( , I ) ; the flexible metric g gives place, in the materials compression factor n . a) materials interpretation; b) topological interpretation, to a medium – that we call a simple medium - interpretation for n = 1 ; c) topological interpretation for n = 0.4 ; characterized by a CR that corresponds in three-dimensional d) profile of the transformation. space to an inhomogeneous bianisotropic medium [2] D=εε()E + εµξ () H , We consider a transformation r֏ f( r ) which is 0 0 0 (4) characterized by the compression function B=µµ0()H + εµζ 0 0 () E . r2− r 1 n r r r− r 1 fr() =n rr +1, 0 << rr 2 , (7) ε()()e= µ en = er + φ () re θ , r2 r whose profile is illustrated in Fig. 2a for compression factors 1+φ 2 ()r r εeereθ= µ θ = φ + e , (10) n = 1 and n = 0.4 . The effect of the compression factor is ()() () r θ n r− r 1 revealed in Fig. 2b: as we decrease n light rays will pass 2 2 n−1 closer to the outer shell. The transformed space, z z 1 r2 ()r− r 1 ε()()e= µ e = 2 e z . corresponding to the topological interpretation, is also shown n()r− r n r in Fig. 2c and Fig. 2d for n = 1 and n = 0.4 respectively. 2 1 where, Here we can see clearly the intrinsic relation between the ray rθ 1 trajectory and the structure of space which is revealed in the 0 n φ ()r= −1 () r − r 1 (11) topological interpretation. ()r− r n Using the methodology described in [2,7] we can easily 2 1 derive the medium parameters for this cloaking: IV. NUMERICAL SIMULATIONS r r r− r 1 ε()()e= µ en = e r , r Finally, we present full-wave numerical simulations of the devices that have been analyzed in this communication. All θ θ 1 r ε()()e= µ e = e θ , (8) the simulations are preformed at the working of n r− r 1 2GHz using the FDTD method. The visualization window is a 2 −1 1 r 2 ()r− r n rectangular grid of 1.2m (8 wave-lengths) by 0.8m (2.67 εez= µ e z = 2 1 e . ()() 2 z wave-lengths) and we have used material average nr− r n r ()2 1 optimization (nine subcells) in all devices in order to reduce B. Cylindrical cloak – rotation transformation the effect of abrupt transitions in the material parameters. The cell size and time step are respectively 3mm and 0,5ps in We now analyze the compression effect introduced in the all simulations. The domain is bounded with PML’s (backed last section combined with a transformation θ֏ θ + h( r ) with PEC walls) in the sides and corners to reduce scattering which is capable of dragging the rays inside the cloaking. The into the simulation domain, [10]. All the devices have inner profile function corresponding to the dragging effect is radius r1 = 0.1 m and outer radius r2 = 0.2 m . r− r In Fig. 4 we describe the of a 2 GHz TM time- hr() =2 θ , 0 < rr < . (9) 0 2 harmonic uniform plane wave striking a PMC cylinder r2 This dragging transformation must necessarily be applied enclosed by the cloaking material obtained from (8) with n = 1 . As can be seen, the wave does not interact with the before the compression function. Here, θ is the maximum 0 PMC shell at all: it is deflected and dragged around the angle by which the inner shell of the device is rotated. The object, causing it to be invisible. transformed space corresponding to this transformation (we use (7) with n = 1 for commodity) is shown in Fig. 3 for

θ0 = − π 4 . Note that a negative value of θ0 corresponds to a clockwise dragging effect.

Fig. 4. Cylindrical cloak with trivial compression profile ( n = 1 ).

Fig. 3. The topological interpretation of a cylindrical cloak of inner Light does not interact with the PMC shell: it is deflected and radius r = 0.1 and outer radius r = 0.2 . Inside the cloak space is dragged around the object, causing it to be invisible. 1 2 dragged by a maximum amount of θ= − π 4 . 0 In Fig. 5 we show what happens if we use the material obtained from (8) with n = 0.4 . In fact, as we decrease the The medium parameters for this cloaking are given by compression factor n the electromagnetic field concentrates closer to the outer shell of the cloak. This is in accordance with the prediction of the topological interpretation given before.

Fig. 5. Cylindrical cloak with non-trivial compression profile π Fig. 8. Cylindrical cloak with drag effect ( θ = ). ( n = 0.4 ). 0 2

Note that spurious reflections are observed in Fig. 5 which V. CONCLUSIONS we believe to be originated in the sharp variations of the constitutive parameters when n = 0.4 . Nevertheless, the We have shown, in this communication, how the cloaking performance is acceptable. This fact becomes clear equivalence principle for electromagnetics can be used to when we compare it with the situation in Fig. 6 where the design several invisibility cloaking devices. We have wave interacts directly with the PMC shell. illustrated this strategy with cylindrical cloaks which have the ability to compress and drag the electromagnetic field inside them. The numerical simulations, using the FDTD method, clearly demonstrate the accuracy of our geometric design and that all the devices herein presented will render an object – placed inside the concealment region – actually invisible.

REFERENCES [1] A. Shivola, “Metamaterials in electromagnetics,” Metamaterials , vol. 1, no. 1, pp. 2-11, 2007. [2] M. A. Ribeiro and C. R. Paiva, “An equivalence principle for electromagnetics through Clifford’s geometric algebra,” Metamaterials , vol. 2, pp. 77-91, 2008. Fig. 6. Without cloaking – the 2GHz TM time-harmonic uniform [3] D. Schurig, J. B. Pendry and D. R. Smith, “Calculation of plane wave interacts with the PMC elliptic cylinder ( e = 0.7 ) material properties and ray tracing in transformation media,” causing it to be visible. Opt. Express , vol. 14, pp. 9794-9804, 2006. [4] U. Leonhardt and T. G. Philbin, “General relativity in electrical In Fig. 7 and Fig. 8 we show two more simulations engineering,” New J. Phys. , vol. 8, no. 247, pp. 1-18, 2006. illustrating the drag effect for θ0 = − π 4 and θ0 = π 2 [5] U. Leonhardt, “Optical conformal mapping,” Science , vol. 312, respectively. pp. 1777-1780, 2006. [6] J. B. Pendry, D. Schurig and D. R. Smith, “Controlling electromagnetic fields,” Science , vol. 312, pp. 1780-1782, 2006. [7] M. A. Ribeiro and C. R. Paiva, “Transformation and Moving Media: A Unified Approach Using Geometric Algebra,” pp. 63-74, in: S. Zoudhi, et al. , Eds., Metamaterials and Plasmonics: Fundamentals, Modelling and Applications . Dordrecht: Springer, 2009. [8] C. W. Misner, K. S. Thorne and J. A. Wheeler, Gravitation , San Francisco: Freeman, 1973. [9] F. W. Hehl and Y. N. Obukhov, Foundations of Classical

π Electrodynamics: Charge, Flux, and Metric . Boston: Fig. 7. Cylindrical cloak with drag effect ( θ = − ). Birkhäuser, 2003. 0 4 [10] J. Berenger, “A perfectly matched layer for the absorption of electromagnetic waves,” J. Comp. Phys ., vol. 114, pp. 185- 200, 1994.