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Metamaterial Electromagnetic Cloak at Microwave Frequencies

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Science  10 Nov 2006:
Vol. 314, Issue 5801, pp. 977-980
DOI: 10.1126/science.1133628

Abstract

A recently published theory has suggested that a cloak of invisibility is in principle possible, at least over a narrow frequency band. We describe here the first practical realization of such a cloak; in our demonstration, a copper cylinder was “hidden” inside a cloak constructed according to the previous theoretical prescription. The cloak was constructed with the use of artificially structured metamaterials, designed for operation over a band of microwave frequencies. The cloak decreased scattering from the hidden object while at the same time reducing its shadow, so that the cloak and object combined began to resemble empty space.

A new approach to the design of electromagnetic structures has recently been proposed, in which the paths of electromagnetic waves are controlled within a material by introducing a prescribed spatial variation in the constitutive parameters (1, 2). The recipe for determining this variation, based on coordinate transformations (3), enables us to arrive at structures that would be otherwise difficult to conceive, opening up the new field of transformation optics (4, 5).

One possible application of transformation optics and media is that of electromagnetic cloaking, in which a material is used to render a volume effectively invisible to incident radiation. The design process for the cloak involves a coordinate transformation that squeezes space from a volume into a shell surrounding the concealment volume. Maxwell's equations are form-invariant to coordinate transformations, so that only the components of the permittivity tensor ϵ and the permeability tensor μ are affected by the transformation (5), becoming both spatially varying and anisotropic. By implementing these complex material properties, the concealed volume plus the cloak appear to have the properties of free space when viewed externally. The cloak thus neither scatters waves nor imparts a shadow in the transmitted field, either of which would enable the cloak to be detected. Other approaches to invisibility either rely on the reduction of backscatter or make use of a resonance in which the properties of the cloaked object and the cloak itself must be carefully matched (6, 7).

It might be of concern that we are able to achieve two different solutions to Maxwell's equations that both have, in principle, the exact same field distributions on a surface enclosing the region of interest. Indeed, the uniqueness theorem would suggest that these two solutions would be required to have the exact same medium within the surface. The uniqueness theorem, however, applies only to isotropic media (8, 9); the required media that result from our coordinate transformations are generally anisotropic. Such media have been shown to support sets of distinct solutions having identical boundary conditions (10, 11).

The effectiveness of a transformation-based cloak design was first confirmed computationally in the geometric optic limit (1, 5) and then in full-wave finite-element simulations (12). Advances in the development of metamaterials (13), especially with respect to gradient index lenses (14, 15), have made the physical realization of the specified complex material properties feasible. We implemented a two-dimensional (2D) cloak because its fabrication and measurement requirements were simpler than those of a 3D cloak. Recently, we have demonstrated the capability of obtaining detailed spatial maps of the amplitude and phase of the electric field distribution internal to 2D negative-index metamaterial samples at microwave frequencies (16). Using this measurement technique, we confirmed the performance of our cloak by comparing our measured field maps to simulations.

In both the cloaking simulations and the measurements presented here, the object being cloaked is a conducting cylinder at the inner radius of the cloak; this is the largest and most strongly scattering object that can be concealed in a cloak of cylindrical geometry.

For the cloak design, we start with a coordinate transformation that compresses space from the cylindrical region 0 < r < b into the annular region a < r′ < b, where r and r′ are the radial coordinates in the original and transformed system, respectively, a is the cloak inner radius, and b is the cloak outer radius. A simple transformation that accomplishes this goal is Embedded Image(1) where θ and z are the angular and vertical coordinates in the original system, and θ′ and z′ are the angular and vertical coordinates in the transformed system. This transformation leads to the following expression for the permittivity and permeability tensor components Embedded Image(2) Embedded Image Equation 2 shows that all of the tensor components have gradients as a function of radius, implying a very complicated metamaterial design. However, because of the nature of the experimental apparatus, in which the electric field is polarized along the z axis (cylinder axis), we benefit from a substantial simplification in that only ϵz, μr, and μθ are relevant. Moreover, if we wish to primarily demonstrate the wave trajectory inside the cloak, which is solely determined by the dispersion relation, we gain even more flexibility in choosing the functional forms for the electromagnetic material parameters. In particular, the following material properties Embedded Image(3) have the same dispersion as those of Eq. 2, implying that waves will have the same dynamics in the medium. In the geometric limit, for example, rays will follow the same paths in media defined by Eqs. 2 or 3, and refraction angles into or out of the media will also be the same (12). The only penalty for using the reduced set of material properties (Eq. 3) is a nonzero reflectance.

To implement the material specification in Eq. 3 with a metamaterial, we must choose the overall dimensions, design the appropriate unit cells, and specify their layout, which for our implementation represents a pattern that is neither cubic nor even periodic. All three of these design elements share parameters, making it advantageous and necessary to optimize them all at once. Equation 3 shows that the desired cloak will have constant ϵz and μθ, with μr varying radially throughout the structure. This parameter set can be achieved in a metamaterial in which split-ring resonators (SRRs), known to provide a magnetic response that can be tailored (17), are positioned with their axes along the radial direction (Fig. 1).

Fig. 1.

2D microwave cloaking structure (background image) with a plot of the material parameters that are implemented. μr (red line) is multiplied by a factor of 10 for clarity. μθ (green line) has the constant value 1. ϵz (blue line) has the constant value 3.423. The SRRs of cylinder 1 (inner) and cylinder 10 (outer) are shown in expanded schematic form (transparent square insets).

As can be seen from Eq. 3, the transformed material properties depend strongly on the choice of a and b. Because of constraints from the unit cell design and layout requirements, we chose the seemingly arbitrary values a = 27.1 mm and b = 58.9 mm. The resulting material properties are plotted in Fig. 1.

All metamaterials reported to date have consisted of elements repeated in cubic or other standard lattice configurations and are usually diagonal in the Cartesian basis. The layout of our cylindrical cloak, however, uses cells that are diagonal in a cylindrical basis and has “unit cells” that are curved sectors with varied electromagnetic environments. The correct retrieval procedure that would obtain the effective medium properties from such irregular unit cells is not yet available. Given that the curvature is not extreme in this cloak design, however, we modeled the unit cells as right-rectangular prisms in a periodic array of like cells, with the assumption that the actual cells will produce minor corrections in the effective medium properties.

Because of constraints of the layout, we chose a rectangular unit cell with dimensions aθ = az = 10/3 mm and ar = 10/π mm. We were able to obtain both the desired ϵz and μr(r) from an SRR by tuning two of its geometric parameters: the length of the split s and the radius of the corners r (Fig. 2). The parameters r and s shift the frequency of the electric and magnetic resonance, respectively, though there is some cross-coupling that must be compensated for.

Fig. 2.

SRR design. The in-plane lattice parameters are aθ = az = 10/3 mm. The ring is square, with edge length l =3mmandtracewidth w = 0.2 mm. The substrate is 381-μm-thick Duroid 5870 (ϵ = 2.33, td = 0.0012 at 10 GHz, where td is the loss tangent). The Cu film, from which the SRRs are patterned, is 17 μm thick. The parameters r and s are given in the table together with the associated value of μr. The extractions gave roughly constant values for the imaginary parts of the material parameters, yielding 0.002 and 0.006 for the imaginary part of ϵz and μr, respectively. The inner cylinder (cyl.) is 1 and the outer cylinder is 10.

Using commercial, full-wave, finite-element simulation software (Microwave Studio, Computer Simulation Technology), we performed a series of scattering (S) parameter simulations for the SRR unit cells over a discrete set of the parameters r and s covering the range of interest. A standard retrieval procedure (18, 19) was then performed to obtain the effective material properties ϵz and μr from the S parameters. The discrete set of simulations and extractions was interpolated to obtain the particular values of the geometric parameters that yielded the desired material properties. We chose an operating frequency of 8.5 GHz, which yields a reasonable effective medium parameter λ/aθ > 10, where λ is the wavelength in free space.

The layout consisted of 10 concentric cylinders, each of which was three unit cells tall. The evenly spaced set of cylinder radii was chosen so that an integral number of unit cells fit exactly around the circumference of each cylinder, necessitating a particular ratio of radial-to-circumferential unit cell size. We chose to increase the number of unit cells in each successive cylinder by six, enabling us to use six supporting radial spokes that can intersect each of the cylinders in the spaces between the SRRs. This led to the requirement ar/aθ = 3/π. Additionally, to minimize the magnetoelectric coupling inherent in single-split SRRs (20), we alternated their orientation along the z direction (Fig. 1).

The overall scale of the cloak is such that a complete field mapping of the cloak and its immediate environment is feasible (Fig. 3). By the same reasoning, numerical simulations of the cloak are also feasible, so long as the cloak is approximated by continuous materials. A complete simulation of the actual cloak structure, including the details of the thousands of SRRs, would be impractical for general optimization studies.

Fig. 3.

Cutaway view of the planar waveguide apparatus. Microwaves (red and yellow patterns) are introduced by means of a coaxial-to-waveguide transition (not shown) attached to the lower plate (lined with a circular sawtooth-shaped microwave absorber). An antenna mounted in the fixed upper plate measures the phase and amplitude of the electric field. To perform field maps, we stepped the lower plate in the lateral directions (black arrows).

Continuous medium simulations of cloaking structures were performed by means of the COMSOL Multiphysics finite-element–based electromagnetics solver (12). The simulation result of the ideal case is shown in Fig. 4A, with material properties as in Eq. 2, and no absorption loss. Several real-world effects were incorporated into another simulation (Fig. 4B) to match experimental conditions as much as possible. In the latter simulation, the reduced material properties of Eq. 3 were used, and μr(r) was approximated by a 10-step piecewise constant to mimic the concentric rings of the fabricated cloak. Additionally, absorption loss was added corresponding to that found in the unit cell simulations (and given in Fig. 2).

Fig. 4.

Snapshots of time-dependent, steady-state electric field patterns, with stream lines [black lines in (A to C)] indicating the direction of power flow (i.e., the Poynting vector). The cloak lies in the annular region between the black circles and surrounds a conducting Cu cylinder at the inner radius. The fields shown are (A) the simulation of the cloak with the exact material properties, (B) the simulation of the cloak with the reduced material properties, (C) the experimental measurement of the bare conducting cylinder, and (D) the experimental measurement of the cloaked conducting cylinder. Animations of the simulations and the measurements (movies S1 to S5) show details of the field propagation characteristics within the cloak that cannot be inferred from these static frames. The right-hand scale indicates the instantaneous value of the field.

For the experimental confirmation, we measured the metamaterial cloak in a parallel-plate waveguide comprising two flat conducting (Al) plates spaced 11 mm apart (Fig. 3). Microwaves were introduced through an X-band (8 to 12 GHz) coax-to-waveguide adapter that was attached to the lower plate and were incident on the cloak, which rested on the lower plate and was nearly of the same height (10 mm) as the plate separation.

A field-sensing antenna was formed from a coaxial fixture inserted into a hole drilled through the upper plate. The center conduc tor and dielectric of the coaxial connector extended to a position flush with the lower surface of the upper plate and did not protrude into the chamber volume. The lower plate was mounted on two orthogonal linear translation stages, so that the lower plate (including the cloak, waveguide feed, and absorber) could be translated with respect to the upper plate and to the detector. By stepping the lower plate in small increments and recording the field amplitude and phase at every step, a full 2D spatial field map of the microwave scattering pattern could be acquired both inside the cloak and in the surrounding free-space region. Further experimental details can be found in (16) and in the supporting online material.

Both the cloak surrounding a 25-mm-radius Cu cylinder (Fig. 4D) and the bare Cu cylinder (Fig. 4C) were measured. The samples were placed on the lower plate in the center of the mapping region and illuminated with microwaves over a discrete set of frequencies that included the expected operating frequency of the cloak. At each frequency, the complex electric field was acquired, and the process was repeated for all x and y positions in the scan range. After reviewing the field maps at all frequencies, the optimal frequency for the cloak sample was determined to be 8.5 GHz, in near-exact agreement with the design target. The optimal frequency was selected as that which best matched the simulated field plots. The acquired real part of the electric field distribution is shown (Fig. 4, C and D).

Comparison of Fig. 4, C and D, shows that the cloak reduces both backscatter (reflection) and forward scatter (shadow). The backscatter is particularly evident in movie S3 as a strong standing-wave component. Comparison of Fig. 4, B and D, shows that the field plots found through full-wave simulations are in marked agreement with the experimental data. The underlying physics of the cloaking mechanism can be studied even further by viewing the field animations (movies S1 to S5). As the waves propagate through the cloak, the center section of the wavefront begins to lag as it approaches the inner radius, exhibiting a compression in wavelength and a reduction in intensity. The wavefront then separates to pass around the cloak hole and reforms on the opposite side, where its center section initially leads the wavefront. The wavefronts at the boundary of the cloak match the wavefronts outside the cloak, which essentially correspond to those of empty space. The scattering is thus minimized, though not perfectly, as a result of the reduced parameter implementation. The fields on the exit side are noticeably attenuated because of the absorption of the cloak material.

The agreement between the simulation and the experiment is evidence that metamaterials canindeedbedesignedtodetailedandexacting specifications, including gradients and nonrectangular geometry. Though the invisibility is imperfect because of the approximations used and material absorption, our results do provide an experimental display of the electromagnetic cloaking mechanism and demonstrate the feasibility of implementing media specified by the transformation optics method with metamaterial technology.

Supporting Online Material

www.sciencemag.org/cgi/content/full/1133628/DC1

SOM Text

Figs. S1 to S3

Movies S1 to S5

References and Notes

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