Metamaterial antenna

This Z antenna tested at the National Institute of Standards and Technology is smaller than a standard antenna with comparable properties. Its high efficiency is derived from the "Z element" inside the square that acts as a metamaterial, greatly boosting the radiated signal. The square is 30 millimeters on a side.

Metamaterial antennas are a class of antennas which use metamaterials to increase performance of miniaturized (electrically small) antenna systems. Their purpose, as with any electromagnetic antenna, is to launch energy into free space. However, this class of antenna incorporates metamaterials, which are materials engineered with novel, often microscopic, structures to produce unusual physical properties. Antenna designs incorporating metamaterials can step-up the antenna's radiated power.

Conventional antennas that are very small compared to the wavelength reflect most of the signal back to the source. A metamaterial antenna behaves as if it were much larger than its actual size, because its novel structure stores and re-radiates energy. Established lithography techniques can be used to print metamaterial elements on a PC board.[1][2][3][4][5]

These novel antennas aid applications such as portable interaction with satellites, wide angle beam steering, emergency communications devices, micro-sensors and portable ground-penetrating radars to search for geophysical features.

Some applications for metamaterial antennas are wireless communication, space communications, GPS, satellites, space vehicle navigation and airplanes.

Antennas designs

Antenna designs incorporating metamaterials can step-up the radiated power of an antenna. The newest metamaterial antennas radiate as much as 95 percent of an input radio signal. Standard antennas need to be at least half the size of the signal wavelength to operate efficiently. At 300 MHz, for instance, an antenna would need to be half a meter long. In contrast, experimental metamaterial antennas are as small as one-fiftieth of a wavelength, and could have further decreases in size.

Metamaterials are a basis for further miniaturization of microwave antennas, with efficient power and acceptable bandwidth. Antennas employing metamaterials offer the possibility of overcoming restrictive efficiency-bandwidth limitations for conventionally constructed, miniature antennas.

Metamaterials permit smaller antenna elements that cover a wider frequency range, thus making better use of available space for space-constrained cases. In these instances, miniature antennas with high gain are significantly relevant because the radiating elements are combined into large antenna arrays. Furthermore, metamaterials' negative refractive index focuses electromagnetic radiation by a flat lens versus being dispersed.[6][7][8]

The DNG shell

The earliest research in metamaterial antennas was an analytical study of a miniature dipole antenna surrounded with a metamaterial. This material is known variously as a negative index metamaterial (NIM) or double negative metamaterial (DNG) among other names.[9]

This configuration analytically and numerically appears to produce an order of magnitude increase in power. At the same time, the reactance appears to offer a corresponding decrease. Furthermore, the DNG shell becomes a natural impedance matching network for this system.[9]

Ground plane applications

Metamaterials employed in the ground planes surrounding antennas offer improved isolation between radio frequency, or microwave channels of (multiple-input multiple-output) (MIMO) antenna arrays. Metamaterial, high-impedance groundplanes can also improve radiation efficiency and axial radio performance of low-profile antennas located close to the ground plane surface. Metamaterials have also been used to increase beam scanning range by using both the forward and backward waves in leaky wave antennas. Various metamaterial antenna systems can be employed to support surveillance sensors, communication links, navigation systems and command and control systems.[6]

Novel configurations

Besides antenna miniaturization, the novel configurations have potential applications ranging from radio frequency devices to optical devices. Other combinations, for other devices in metamaterial antenna subsystems are being researched.[10] Either double negative metamaterial slabs are used exclusively or combinations of double positive (DPS) with DNG slabs, or epsilon-negative (ENG) slabs with mu-negative (MNG) slabs are employed in the subsystems. Antenna subsystems that are currently being researched include cavity resonators, waveguides, scatters and antennas (radiators).[10] Metamaterial antennas were commercially available by 2009.[11][12][13]

History

Pendry et al. were able to show that a three-dimensional array of intersecting, thin wires could be used to create negative values of permittivity (or "ε"), and that a periodic array of copper split ring resonators could produce an effective negative magnetic permeability (or "μ").

In May 2000, a group of researchers, Smith et al. were the first to successfully combine the split-ring resonator (SRR), with thin wire conducting posts and produce a left-handed material that had negative values of ε, μ and refractive index for frequencies in the gigahertz or microwave range.[10][14]

In 2002, a different class of negative refractive index (NRI) metamaterials was introduced that employs periodic reactive loading of a 2-D transmission line as the host medium. This configuration used positive index (DPS) material with negative index material (DNG). It employed a small, planar, negative-refractive-lens interfaced with a positive index, parallel-plate waveguide. This was experimentally verified soon after.[15][16]

Although some SRR inefficiencies were identified, they continued to be employed as of 2009 for research. SRRs have been involved in wide ranging metamaterial research, including research on metamaterial antennas.[3][15][16]

A more recent view is that by using SRRs as building blocks, the electromagnetic response and associated flexibility is practical and desirable.[17]

Phase compensation due to negative refraction

DNG can provide phase compensation due to their negative index of refraction. This is accomplished by combining a slab of conventional lossless DPS material with a slab of lossless DNG metamaterial.

DPS has a conventional positive index of refraction, while the DNG has a negative refractive index. Both slabs are impedance-matched to the outside region (e.g., free space). The desired monochromatic plane wave is radiated on this configuration. As this wave propagates through the first slab of material a phase difference emerges between the exit and entrance faces. As the wave propagates through the second slab the phase difference is significantly decreased and even compensated for. Therefore as the wave exits the second slab the total phase difference is equal to zero.[18]

With this system a phase-compensated, waveguiding system could be produced. By stacking slabs of this configuration, the phase compensation (beam translation effects) would occur throughout the entire system. Furthermore, by changing the index of any of the DPS-DNG pairs, the speed at which the beam enters the front face, and exits the back face of the entire stack-system changes. In this manner, a volumetric, low loss, time delay transmission line could be realized for a given system.[18]

Furthermore, this phase compensation can lead to a set of applications, which are miniaturized, subwavelength, cavity resonators, and waveguides with applications below diffraction limits.[18]

Transmission line dispersion compensation

Because of DNG's dispersive nature as a transmission medium, it could be useful as a dispersion compensation device for time-domain applications. The dispersion produces a variance of the group speed of the signals' wave components, as they propagate in the DNG medium. Hence, stacked DNG metamaterials could be useful for modifying signal propagation along a microstrip transmission line. At the same time, dispersion leads to distortion. However, if the dispersion could be compensated for along the microstrip line, RF or microwave signals propagating along them would significantly decrease distortion. Therefore, components for attenuating distortion become less critical, and could lead to simplification of many systems. Metamaterials can eliminate dispersion along the microstrip by correcting for the frequency dependence of the effective permittivity.[19]

The strategy is to design a length of metamaterial-loaded transmission line that can be introduced with the original length of microstrip line to make the paired system dispersionless creating a dispersion-compensating segment of transmission line. This could be accomplished by introducing a metamaterial with a specific localized permittivity and a specific localized magnetic permeability, which then affects the relative permittivity and permeability of the overall microstrip line. It is introduced so that the wave impedance in the metamaterial remains unhanged. The index of refraction in the medium compensates for the dispersion effects associated with the microstrip geometry itself; making the effective refractive index of the pair that of free space.[19]

Part of the design strategy is that the effective permittivity and permeability of such a metamaterial should be negative – requiring a DNG material.[19]

Innovation

Combining left-handed segments with a conventional (right-handed) transmission line results in advantages over conventional designs. Left-handed transmission lines are essentially a high-pass filter with phase advance. Conversely, right-handed transmission lines are a low-pass filter with phase lag. This configuration is designated composite right/left-handed (CRLH) metamaterial.[20][21][22]

The conventional Leaky Wave antenna has had limited commercial success because it lacks complete backfire-to-endfire frequency scanning capability.The CRLH allowed complete backfire-to-endfire frequency scanning, including broadside.

Microwave lens

The metamaterial lens, found in metamaterial antenna systems, is used as an efficient coupler to external radiation, focusing radiation along or from a microstrip transmission line into transmitting and receiving components. Hence, it can be used as an input device. In addition, it can enhance the amplitude of evanescent waves, as well as correct the phase of propagating waves.

Directing radiation

In this instance an SRR uses layers of a metallic mesh of thin wires – with wires in the three directions of space and slices of foam. This material's permittivity above the plasma frequency can be positive and less than one. This means that the refractive index is just above zero. The relevant parameter is often the contrast between the permittivities rather than the overall permittivity value at desired frequencies. This occurs because the equivalent (effective) permittivity has a behavior governed by a plasma frequency in the microwave domain. This low optical index material then is a good candidate for extremely convergent microlenses. Methods that have been developed theoretically using dielectric photonic crystals applied in the microwave domain to realize a directive emitter using metallic grids.[1]

In this instance, arrayed wires in a cubic, crystal lattice structure can be analyzed as an array of aerials (antenna array). As a lattice structure it has a lattice constant. The lattice constant or lattice parameter refers to the constant distance between unit cells in a crystal lattice.[23]

The earlier discovery of plasmons created the view that metal at plasmon frequency fp is a composite material. The effect of plasmons on any metal sample is to create properties in the metal such that it can behave as a dielectric, independent of the wave vector of the EM excitation (radiation) field. Furthermore, a minute-fractionally small amount of plasmon energy is absorbed into the system denoted as γ. For aluminium fp = 15 eV, and γ = 0.1 eV. Perhaps the most important result of the interaction of metal and the plasma frequency is that permittivity is negative below the plasma frequency, all the way to the minute value of γ.[23][24]

These facts ultimately result in the arrayed wire structure as being effectively a homogeneous medium.[23]

This metamaterial allows for control of the direction of emission of an electromagnetic radiation source located inside the material in order to collect all the energy in a small angular domain around the normal.[1] By using a slab of a metamaterial, diverging electromagnetic waves are focused into a narrow cone. Dimensions are small in comparison to the wavelength and thus the slab behaves as a homogeneous material with a low plasma frequency.[1]

Transmission line models

Conventional transmission lines

Variations on the schematic electronic symbol for a transmission line.
Schematic representation of the elementary components of a transmission line.

A transmission line is the material medium or structure that forms all or part of a path from one place to another for directing the transmission of energy, such as electromagnetic waves or electric power transmission. Types of transmission line include wires, coaxial cables, dielectric slabs, striplines, optical fibers, electric power lines and waveguides.[25]

A microstrip is a type of transmission line that can be fabricated using printed circuit board technology and is used to convey microwave-frequency signals. It consists of a conducting strip separated from a ground plane by a dielectric layer known as the substrate. Microwave components such as antennas, couplers, filters and power dividers can be formed from a microstrip.

From the simplified schematics to the right it can be seen that total impedance, conductance, reactance (capacitance and inductance) and the transmission medium (transmission line) can be represented by single components that give the overall value.

With transmission line media it is important to match the load impedance ZL to the characteristic impedance Z0 as closely as possible, because it is usually desirable that the load absorbs as much power as possible.

R is the resistance per unit length,
L is the inductance per unit length,
G is the conductance of the dielectric per unit length,
C is the capacitance per unit length,
j is the imaginary unit, and
\omega is the angular frequency.

Lumped circuit elements

Often, because of the goal that moves physical metamaterial inclusions (or cells) to smaller sizes, discussion and implementation of lumped LC circuits or distributed LC networks are often examined. Lumped circuit elements are actually microscopic elements that effectively approximate their larger component counterparts. For example circuit capacitance and inductance can be created with split rings, which are on the scale of nanometers at optical frequencies. The distributed LC model is related to the lumped LC model, however the distributed element model is more accurate but more complex than the lumped element model.

Metamaterial – loaded transmission line configurations

Some noted metamaterial antennas employ negative refractive index transmission-line metamaterials (NRI-TLM). These include lenses that can overcome the diffraction limit, small band and broadband phase shifting lines, small antennas, low profile antennas, antenna feed networks, novel power architectures and high directivity couplers. Loading a planar metamaterial network of TLs with series capacitors and shunt inductors produces igher performance. This results in a large operating bandwidth while the refractive index is negative.[10][26]

Because superlenses can overcome the diffraction limit, this allows for a more efficient coupling to external radiation and enables a broader frequency band. For example the superlens can be applied to the TLM architecture. In conventional lenses, imaging is limited by the diffraction limit. With superlenses the details of the near field images are not lost. Growing evanescent waves are supported in the metamaterial (n < 1), which restores the decaying evanescent waves from the source. This results in a diffraction-limited resolution of λ/6, after some small losses. This compares with λ/2, the normal diffraction limit for conventional lenses.[26]

By combining right-handed (RHM) with left-handed materials (LHM) as a composite material (CRLH) construction, both a backward to forward scanning capability is obtained.

Metamaterials were first used for antenna technology around 2005. This type of antenna used the established capability of SNGs to couple with external radiation. Resonant coupling allowed for a wavelength larger than the antenna. At microwave frequencies this allowed for a smaller antenna.[3][26]

A metamaterial-loaded transmission line has significant advantages over conventional or standard delay transmission lines. It is more compact in size, it can achieve positive or negative phase shift while occupying the same short physical length and it exhibits a linear, flatter phase response with frequency, leading to shorter group delays. It can work in lower frequency because of high series distributed-capacitors and has smaller plane dimensions than its equivalent coplanar structure.[26]

Negative refractive index metamaterials supporting 2-D waves

In 2002, rather than using SRR-wire configuration, or other 3-D media, researchers looked at planar configurations that supported backward wave propagation, thus demonstrating negative refractive index and focusing as a consequence.[15]

It has long been known that transmission lines periodically loaded with capacitive and inductive elements in a high-pass configuration support certain types of backward waves. In addition, planar transmission lines are a natural match for 2-D wave propagation. With lumped circuit elements they retain a compact configuration and can still support the lower RF range. With this in mind, high pass and cutoff, periodically loaded, two-dimensional LC transmission line networks were proposed. The LC networks can be designed to support backward waves, without bulky SRR/wire structure. This was the first such proposal which veered away from bulk media for a negative refractive effect. A notable property of this type of network is that there is no reliance on resonance, Instead the ability to support backward waves defines negative refraction.[15]

The principles behind focusing are derived from Veselago and Pendry. Combining a conventional, flat, (planar) DPS slab, M-1, with a left-handed medium, M-2, a propagating electromagnetic wave with a wave vector k1 in M-1, results in a refracted wave with a wave vector k2 in M-2. Since, M-2 supports backward wave propagation k2 is refracted to the opposite side of the normal, while the Poynting vector of M-2 is anti-parallel with k2. Under such conditions, power is refracted through an effectively negative angle, which implies an effectively negative index of refraction.[15]

Electromagnetic waves from a point source located inside a conventional DPS can be focused inside an LHM using a planar interface of the two media. These conditions can be modeled by exciting a single node inside the DPS and observing the magnitude and phase of the voltages to ground at all points in the LHM. A focusing effect should manifest itself as a “spot” distribution of voltage at a predictable location in the LHM.[15]

Negative refraction and focusing can be accomplished without employing resonances or directly synthesizing the permittivity and permeability. In addition, this media can be practically fabricated by appropriately loading a host transmission line medium. Furthermore, the resulting planar topology permits LHM structures to be readily integrated with conventional planar microwave circuits and devices.[15]

When transverse electromagnetic propagation occurs with a transmission line medium, the analogy for permittivity and permeability is ε = L, and μ = C. This analogy was developed with positive values for these parameters. The next logic step was realizing that negative values could be achieved. In order to synthesize a left-handed medium (ε < 0 and μ < 0) the series reactance and shunt susceptibility should become negative, because the material parameters are directly proportional to these circuit quantities.[27]

A transmission line that has lumped circuit elements that synthesize a left-handed medium is referred to as a "dual transmission line" as compared to "conventional transmission line". The dual transmission line structure can be implemented in practice by loading a host transmission line with lumped element series capacitors (C) and shunt inductors (L). In this periodic structure, the loading is strong such that the lumped elements dominate the propagation characteristics.[27]

Left-handed behavior in LC loaded transmission lines

Using SRRs at RF frequencies, as with wireless devices, requires the resonators to be scaled to larger dimensions. This worked against making the devices more compact. In contrast, LC network configurations could be scaled to both microwave and RF frequencies.[28]

LC-loaded transmission lines enabled a new class of metamaterials to produce a negative refractive index. Relying on LC networks to emulate electrical permittivity and magnetic permeability resulted in a substantial increase in operating bandwidths.[28]

Moreover, their unit cells are connected through a transmission-line network and may be equipped with lumped circuit elements, which permit them to be compact at frequencies where an SRR cannot be compact. The flexibility gained through the use of either discrete or printed elements enables planar metamaterials to be scalable from the megahertz to the tens of gigahertz range. In addition, replacing capacitors with varactors allowed the material properties to be dynamically tuned. The proposed media are planar and inherently support two-dimensional (2-D) wave propagation, making them well-suited for RF/microwave device and circuit applications.[28]

Growing evanescent waves in negative-refractive-index transmission-line media

The periodic 2-D LC loaded transmission-line (TL) was shown to exhibit NRI properties over a broad frequency range. This network will be referred to as a dual TL structure since it is of a high-pass configuration, as opposed to the low-pass representation of a conventional TL structure.[29] Dual TL structures have been used to experimentally demonstrate backward-wave radiation and focusing at microwave frequencies.[15][29]

As a negative refractive index medium, a dual TL structure is not simply a phase compensator. It can enhance the amplitude of evanescent waves, as well as correct the phase of propagating waves. Evanescent waves actually grow within the dual TL structure.[29]

Backward wave antenna using an NRI loaded transmission line

Grbic et al. used one-dimensional LC loaded transmission line network, which supports fast backward-wave propagation to demonstrate characteristics analogous to "reversed Cherenkov radiation". Their proposed backward-wave radiating structure was inspired by negative refractive index LC materials. The simulated E-plane pattern at 15 GHz showed radiation towards the backfire direction in the far-field pattern, clearly indicating the excitation of a backward wave. Since the transverse dimension of the array is electrically short, the structure is backed by a long metallic trough. The trough acts as a waveguide below cut-off and recovers the back radiation, resulting in unidirectional far-field patterns.[30]

Planar NIMs with periodic loaded transmission lines

Planar media can be implemented with an effective negative refractive index. The underlying concept is based on appropriately loading a printed network of transmission lines periodically with inductors and capacitors. This technique results in effective permittivity and permeability material parameters that are both inherently and simultaneously negative, obviating the need to employ separate means. The proposed media possess other desirable features including very wide bandwidth over which the refractive index remains negative, the ability to guide 2-D TM waves, scalability from RF to millimeter-wave frequencies and low transmission losses, as well as the potential for tunability by inserting varactors and/or switches in the unit cell. The concept has been verified with circuit and full-wave simulations. A prototype focusing device has been tested experimentally. The experimental results demonstrated focusing of an incident cylindrical wave within an octave bandwidth and over an electrically short area; suggestive of near-field focusing.[31]

RF/microwave devices can be implemented based on these proposed media for applications in wireless communications, surveillance and radars.[31]

Larger transmission lines

According to some researchers SRR/wire-configured metamaterials are bulky 3-D constructions that are difficult to adapt for RF/microwave device and circuit applications. These structures can achieve a negative index of refraction only within a narrow bandwidth. When applied to wireless devices at RF frequencies the split ring-resonators have to be scaled to larger dimensions, which, in turn forces a larger device size.[31]

The proposed structures go beyond the wire/SRR composites in that they do not rely on SRRs to synthesize the material parameters, thus leading to dramatically increased operating bandwidths. Moreover, their unit cells are connected through a transmission-line network and they may, therefore, be equipped with lumped elements, which permit them to be compact at frequencies where the SRR cannot be compact. The flexibility gained through the use of either discrete or printed elements enables planar metamaterials to be scalable from the megahertz to the tens of gigahertz range. In addition, by utilizing varactors instead of capacitors, the effective material properties can be dynamically tuned. Furthermore, the proposed media are planar and inherently support two-dimensional (2-D) wave propagation. Therefore, these new metamaterials are well suited for RF/microwave device and circuit applications.[31]

In the long-wavelength regime, the permittivity and permeability of conventional materials can be artificially synthesized using periodic LC networks arranged in a low-pass configuration. In the dual (high-pass) configuration, these equivalent material parameters assume simultaneously negative values, and may therefore be used to synthesize a negative refractive index.[32]

Configurations

Main article: Antenna (radio)

Antenna theory is based on classical electromagnetic theory as described by Maxwell's equations.[33] Physically, an antenna is an arrangement of one or more conductors, usually called elements. An alternating current is created in the elements by applying a voltage at the antenna terminals, causing the elements to radiate an electromagnetic field. In reception, the reverse occurs: an electromagnetic field from another source induces an alternating current in the elements and a corresponding voltage at the antenna's terminals. Some receiving antennas (such as parabolic and horn types) incorporate shaped reflective surfaces to collect EM waves from free space and direct or focus them onto the actual conductive elements.

An antenna creates sufficiently strong electromagnetic fields at large distances. Reciprocally, it is sensitive to the electromagnetic fields impressed upon it externally. The actual coupling between a transmitting and receiving antenna is so small that amplifier circuits are required at both the transmitting and receiving stations. Antennas are usually created by modifying ordinary circuitry into transmission line configurations.[33]

The required antenna for any given application is dependent on the bandwidth employed, and range (power) requirements. In the microwave to millimeter-wave range – wavelengths from a few meters to millimeters – the following antennas are usually employed:[33]

Dipole antennas, short antennas, parabolic and other reflector antennas, horn antennas, periscope antennas, helical antennas, spiral antennas, surface-wave and leaky wave antennas. Leaky wave antennas include dielectric and dielectric loaded antennas, and the variety of microstrip antennas.[33]

Radiation properties with SRRs

The SRR was introduced by Pendry in 1999, and is one of the most common elements of metamaterials.[34] As a nonmagnetic conducting unit, it comprises an array of units that yield an enhanced negative effective magnetic permeability, when the frequency of the incident electromagnetic field is close to the SRR resonance frequency. The resonant frequency of the SRR depends on its shape and physical design. In addition, resonance can occur at wavelengths much larger than its size.[35][36]

Double negative metamaterials

Through the application of double negative metamaterials (DNG), the power radiated by electrically small dipole antennas can be notably increased. This could be accomplished by surrounding an antenna with a shell of double negative (DNG) material. When the electric dipole is embedded in a homogeneous DNG medium, the antenna acts inductively rather than capacitively, as it would in free space without the interaction of the DNG material. In addition, the dipole-DNG shell combination increases the real power radiated by more than an order of magnitude over a free space antenna. A notable decrease in the reactance of the dipole antenna corresponds to the increase in radiated power.[9]

The reactive power indicates that the DNG shell acts as a natural matching network for the dipole. The DNG material matches the intrinsic reactance of this antenna system to free space, hence the impedance of DNG material matches free space. It provides a natural matching circuit to the antenna.[9]

Single negative SRR and monopole composite

The addition of an SRR-DNG metamaterial increased the radiated power by more than an order of magnitude over a comparable free space antenna. Electrically small antennas, high directivity and tunable operational frequency are produced with negative magnetic permeability. When combining a right-handed material (RHM) with a Veselago-left-handed material (LHM) other novel properties are obtained. A single negative material resonator, obtained with an SRR, can produce an electrically small antenna when operating at microwave frequencies, as follows:[3]

The configuration of an SRR assessed was two concentric annular rings with relative opposite gaps in the inner and outer ring. Its geometrical parameters were R = 3.6 mm, r = 2.5 mm, w = 0.2 mm, t = 0.9 mm. R and r are used in annular parameters, w is the spacing between the rings and t = the width of the outer ring. The material had a thickness of 1.6 mm. Permittivity was 3.85 at 4 GHz. The SRR was fabricated with an etching technique onto a 30 μm thick copper substrate. The SRR was excited by using a monopole antenna. The monopole antenna was composed of a coaxial cable, ground plane and radiating components. The ground plane material was aluminium. The operation frequency of the antenna was 3.52 GHz, which was determined by considering the geometrical parameters of SRR. An 8.32 mm length of wire was placed above the ground plane, connected to the antenna, which was one quarter of the operation wavelength. The antenna worked with a feed wavelength of 3.28 mm and feed frequency of 7.8 GHz. The SRR's resonant frequency was smaller than the monopole operation frequency.[3]

The monopole-SRR antenna operated efficiently at (λ/10) using the SRR-wire configuration. It demonstrated good coupling efficiency and sufficient radiation efficiency. Its operation was comparable to a conventional antenna at λ/2, which is a conventional antenna size for efficient coupling and radiation. Therefore, the monopole-SRR antenna becomes an acceptable electrically small antenna at the SRR's resonance frequency.[3]

When the SRR is made part of this configuration, characteristics such as the antenna's radiation pattern are entirely changed in comparison to a conventional monopole antenna. With modifications to the SRR structure the antenna size could reach (λ/40). Coupling 2, 3, and 4 SRRs side by side slightly shifts radiation patterns.[3]

Patch antennas

In 2005 a patch antenna with a metamaterial cover was proposed that enhanced directivity. According to the numerical results, the antenna showed significant improvement in directivity, compared to conventional patch antennae. This was cited in 2007 for an efficient design of directive patch antennas in mobile communications using metamaterials. This design was based on the left-handed material (LHM) transmission line model, with the circuit elements L and C of the LHM equivalent circuit model. This study developed formulae to determine the L and C values of the LHM equivalent circuit model for desirable characteristics of directive patch antennas. Design examples derived from actual frequency bands in mobile communications were performed, which illustrates the efficiency of this approach.[37][38][39]

Flat lens horn antenna

This configuration uses a flat aperture constructed of zero-index metamaterial. This has advantages over ordinary (conventional) curved lenses, which results in a much improved directivity. These investigations have provided capabilities for the miniaturization of microwave source and non-source devices, circuits, antennas and the improvement of electromagnetic performance.[40]

Improvements in design

Research and applications of metamaterial based antennas. Related components are also researched.[41][42]

Subwavelength cavities and waveguides

When the interface between a pair of materials that function as optical transmission media interact as a result of opposing permittivity and / or permeability values that are either ordinary (positive) or extraordinary (negative), notable anomalous behaviors may occur. The pair would be a DNG metamaterial (layer), paired with a DPS, ENG or MNG layer. Wave propagation behavior and properties may occur that would otherwise not happen if only DNG layers are paired together.[43]

At the interface between two media, the concept of the continuity of the tangential electric and magnetic field components can be applied. If either the permeability or permittivity of two media has opposite signs then the normal components of the tangential field, on both sides of the interface, will be discontinuous at the boundary. This implies a concentrated resonant phenomenon at the interface. This appears to be similar to the current and voltage distributions at the junction between an inductor and capacitor, at the resonance of an L-C circuit. This "interface resonance" is essentially independent of the total thickness of the paired layers, because it occurs along the discontinuity between two such conjugate materials.[43][44]

Parallel-plate waveguiding structures

The geometry consists of two parallel plates as perfect conductors (PEC), an idealized structure, filled by two stacked planar slabs of homogeneous and isotropic materials with their respective constitutive parameters ε1, ε2, u1, u2. Each slab has thickness = d, slab 1 = d1, and slab 2 = d2. Choosing which combination of parameters to employ involves pairing DPS and DNG or ENG and MNG materials. As mentioned previously, this is one pair of oppositely-signed constitutive parameters, combined.[45]

Thin subwavelength cavity resonators

Phase compensation

The real component values for negative permittivity and permeability results in real component values for negative refraction n. In a lossless medium, all that would exist are real values. This concept can be used to map out phase compensation when a conventional lossless material, DPS, is matched with a lossless NIM (DNG).[44]

In phase compensation, the DPS of thickness d1 has ε > 0 and µ > 0. Conversely, the NIM of thickness d2 has ε < 0 and µ < 0. Assume that the intrinsic impedance of the DPS dielectric material (d1) is the same as that of the outside region and responding to a normally incident planar wave. The wave travels through the medium without any reflection because the DPS impedance and the outside impedance are equal. However, the plane wave at the end of DPS slab is out of phase with the plane wave at the beginning of the material.[44]

The plane wave then enters the lossless NIM (d2). At certain frequencies ε < 0 and µ < 0 and n < 0. Like the DPS, the NIM has intrinsic impedance that is equal to the outside, and, therefore, is also lossless. The direction of power flow (i.e., the Poynting vector) in the first slab should be the same as that in the second one, because the power of the incident wave enters the first slab (without any reflection at the first interface), traverses the first slab, exits the second interface, enters the second slab and traverses it, and finally leaves the second slab. However, as stated earlier, the direction of power is anti-parallel to the direction of phase velocity. Therefore, the wave vector k2 is in the opposite direction of k1. Furthermore, whatever phase difference is developed by traversing the first slab can be decreased and even cancelled by traversing the second slab. If the ratio of the two thicknesses is d1 / d 2 = n2 / n1, then the total phase difference between the front and back faces is zero.[44] This demonstrates how the NIM slab at chosen frequencies acts as a phase compensator. It is important to note that this phase compensation process is only on the ratio of d1 / d 2 rather than the thickness of d1 + d1. Therefore, d1 + d1 can be any value, as long as this ratio satisfies the above condition. Finally, even though this two-layer structure is present, the wave traversing this structure would not experience the phase difference.

Following this, the next step is the subwavelength cavity resonator.[44]

Compact subwavelength 1-D cavity resonators using metamaterials

The phase compensator described above can be used to conceptualize the possibility of designing a compact 1-D cavity resonator. The above two-layer structure is applied as two perfect reflectors, or in other words, two perfect conducting plates. Conceptually, what is constrained in the resonator is d1 / d2, not d1 + d2. Therefore, in principle, one can have a thin subwavelength cavity resonator for a given frequency, if at this frequency the second layer acts a metamaterial with negative permittivity and permeability and the ratio correlates to the correct values.[44]

The cavity can conceptually be thin while still resonant, as long as the ratio of thicknesses is satisfied. This can, in principle, provide possibility for subwavelength, thin, compact cavity resonators.[44]

Miniature cavity resonator utilizing FSS

Frequency selective surface (FSS) based metamaterials utilize equivalent LC circuitry configurations. Using FSS in a cavity allows for miniaturization, decrease of the resonant frequency, lowers the cut-off frequency and smooth transition from a fast-wave to a slow-wave in a waveguide configuration.[46]

Composite metamaterial based cavities

As an LHM application four different cavities operating in the microwave regime were fabricated and experimentally observed and described.[47]

Metamaterial ground plane

Leaky mode propagation with metamaterial ground plane

A magnetic dipole was placed on metamaterial (slab) ground plane. The metamaterials have either constituent parameters that are both negative, or negative permittivity or negative permeability. The dispersion and radiation properties of leaky waves supported by these metamaterial slabs, respectively, were investigated.[48]

Patented systems

Microstrip line (400) for a phased array metamaterial antenna system. 401 represents unit-cell circuits composed periodically along the microstrip. 402 series capacitors. 403 are T-junctions between capacitors, which connect (404) spiral inductor delay lines to 401. 404 are also connected to ground vias 405.

Multiple systems have patents.

Phased array systems and antennas for use in such systems are well known in areas such as telecommunications and radar applications. In general phased array systems work by coherently reassembling signals over the entire array by using circuit elements to compensate for relative phase differences and time delays.[49]

Phased array antenna

Patented in 2004, one phased array antenna system is useful in automotive radar applications. By using NIMs as a biconcave lens to focus microwaves, the antenna's sidelobes are reduced in size. This equates to a reduction in radiated energy loss, and a relatively wider useful bandwidth. The system is an efficient, dynamically-ranged phased array radar system.[49]

In addition, signal amplitude is increased across the microstrip transmission lines by suspending them above the ground plane at a predetermined distance. In other words, they are not in contact with a solid substrate. Dielectric signal loss is reduced significantly, reducing signal attenuation.[49]

This system was designed to boost the performance of the Monolithic microwave integrated circuit (MMIC), among other benefits. A transmission line is created with photolithography. A metamaterial lens, consisting of a thin wire array focuses the transmitted or received signals between the line and the emitter / receiver elements.[49]

The lens also functions as an input device and consists of a number of periodic unit-cells disposed along the line. The lens consists of multiple lines of the same make up; a plurality of periodic unit-cells. The periodic unit-cells are constructed of a plurality of electrical components; capacitors and inductors as components of multiple distributed circuits.[49]

The metamaterial incorporates a conducting transmission element, a substrate comprising at least a first ground plane for grounding the transmission element, a plurality of unit-cell circuits composed periodically along the transmission element and at least one via for electrically connecting the transmission element to at least the first ground plane. It also includes a means for suspending this transmission element a predetermined distance from the substrate in a way such that the transmission element is located at a second predetermined distance from the ground plane.[49]

ENG and MNG waveguides and scattering devices

This structure was designed for use in waveguiding or scattering of waves. It employs two adjacent layers. The first layer is an epsilon-negative (ENG) material or a mu-negative (MNG) material. The second layer is either a double-positive (DPS) material or a double-negative (DNG) material. Alternatively, the second layer can be an ENG material when the first layer is an MNG material or the reverse.[50]

Reducing interference

A keyless entry system key fob

Metamaterials can reduce interference across multiple devices with smaller and simpler shielding. While conventional absorbers can be three inches thick, metamaterials can be in the millimeter range—2 mm (0.078 in) thick.[51]

See also

General references

Ziolkowski, R. W.; Lin, Chia-Ching; Nielsen, Jean A.; Tanielian, Minas H.; Holloway, Christopher L. (August–September 2009). "Design and Experimental Verification of.." (PDF). Antennas and Wireless Propagation Letters, IEEE 8: 989–993. Bibcode:2009IAWPL...8..989Z. doi:10.1109/LAWP.2009.2029708. Retrieved 2010-12-22.

References

  1. ↑ 1.0 1.1 1.2 1.3 Enoch, Stefan; Tayeb, G; Sabouroux, P; Guérin, N; Vincent, P (2002-11-04). "A Metamaterial for Directive Emission" (PDF). Phys. Rev. Lett. (2nd free PDF download: A Metamaterial for Directive Emission) 89 (21): 213902. Bibcode:2002PhRvL..89u3902E. doi:10.1103/PhysRevLett.89.213902. PMID 12443413. Retrieved 2009-09-16.
  2. ↑ Omar F., Siddiqui; Mo Mojahedi, and George V. Eleftheriades (2003-10-14). "Periodically LTL With Effective NRI and Negative Group Velocity". IEEE Transactions on Antennas and Propagation (Univ. of Toronto, Ont., Canada: IEEE) 51 (10): 2619–2625. Bibcode:2003ITAP...51.2619S. doi:10.1109/TAP.2003.817556.
  3. ↑ 3.0 3.1 3.2 3.3 3.4 3.5 3.6 Kamil, Boratay Alici; Ekmel Özbay (2007-03-22). "Radiation properties of a split ring resonator and monopole composite" (PDF). Physica Status Solidi (b) 244 (4): 1192–1196. Bibcode:2007PSSBR.244.1192A. doi:10.1002/pssb.200674505. Retrieved 2009-09-17.
  4. ↑ Wu, B.-I.; W. Wang, J. Pacheco, X. Chen, T. Grzegorczyk and J. A. Kong (2005). "A Study of Using Metamaterials as Antenna Substrate to Enhance Gain" (PDF). Progress in Electromagnetics Research (MIT,Cambridge,MA,USA: EMW Publishing) 51: 295–328 (34 pages). doi:10.2528/PIER04070701. Retrieved 2009-09-21.
  5. ↑ Some content is reproduced from Public Domain material available from the National Institute of Standards and Technology (NIST).
  6. ↑ 6.0 6.1 Bukva, Ms. Erica; Navy-Unmanned Combat Air Systems (N-UCAS) (August 20 – September 19, 2007). "Metamaterial-Based Electrically Small Antenna". Acquisition Program: Advanced Development Prgm Office for N-UCAS. Navy SBIR 2007.3 – Topic N07-184. Retrieved 2010-03-19.
  7. ↑  This article incorporates public domain material from the United States Navy document "Metamaterial-Based Electrically Small Antenna" (retrieved on 2011-02).
  8. ↑ Metamaterials 2009 Bilotti, Filiberto; Vegni, Lucio. "Metamaterial-inspired electrically small radiators: it is time to draw preliminary conclusions and depict the future challenges". Proceedings of the 3rd International Congress on Advanced Electromagnetic Materials in Microwaves and Optics, London, UK, August 30th-September 4th, 2009. METAMORPHOSE VI AISBL. ISBN 978-0-9551179-6-1.
  9. ↑ 9.0 9.1 9.2 9.3 Ziolkowski, Richard Wly; Allison D. Kipple (2003-10-14). "Application of Double Negative Materials to Increase the Power Radiated by Electrically Small Antennas" (PDF). IEEE Transactions on Antennas and Propagation 51 (10): 2626. Bibcode:2003ITAP...51.2626Z. doi:10.1109/TAP.2003.817561. Retrieved 2009-11-30.
  10. ↑ 10.0 10.1 10.2 10.3 Engheta, Nader; Richard W. Ziolkowski (June 2006). Metamaterials: physics and engineering explorations. Wiley & Sons. pp. 43–85. ISBN 978-0-471-76102-0.
  11. ↑ "NETGEAR Ships 'The Ultimate Networking Machine' for Gamers, Media Enthusiasts and Small Businesses" ("...EIGHT ULTRA-SENSITIVE, INTERNAL, METAMATERIAL ANTENNAS..."). The New York Times. 2009-10-20. Retrieved 2009-10-20.
  12. ↑ Hurst, Brian (2009-09-28). "RAYSPAN Ships 20 Millionth Metamaterial Antenna". Reuters. Retrieved 2009-10-20.
  13. ↑ Das, Saswato R. (October 2009). "Metamaterials Arrive in Cellphones" (ONLINE MAGAZINE ARTICLE). Metamterial antennas. IEEE Spectrum. Retrieved 2011-03-09. LG Chocolate BL40 is first cellphone to use a metamaterials antenna
  14. ↑ Shelby, R. A.; Smith, D. R.; Schultz, S. (2001). "Experimental Verification of a Negative Index of Refraction". Science 292 (5514): 77–79. Bibcode:2001Sci...292...77S. doi:10.1126/science.1058847. PMID 11292865.
  15. ↑ 15.0 15.1 15.2 15.3 15.4 15.5 15.6 15.7 Iyer, Ashwin K.; George V. Eleftheriades (2002-06-07). "Negative Refractive Index Metamaterials Supporting 2-D Waves" (PDF). IEEE MTT-S International Microwave Symposium Digest 2: 1067. doi:10.1109/MWSYM.2002.1011823. ISBN 0-7803-7239-5. Retrieved 2009-11-08.
  16. ↑ 16.0 16.1 Iyer, Ashwin K.; Kremer, Peter; Eleftheriades, George (2003-04-07). "Experimental and theoretical verification of focusing in a large, periodically loaded transmission line negative refractive index metamaterial" (PDF). Optics Express 11 (7): 696–708. Bibcode:2003OExpr..11..696I. doi:10.1364/OE.11.000696. PMID 19461781. Retrieved 2009-11-08.
  17. ↑ Chen, Hou-Tong et al. (2008-09-04). "Hybrid metamaterials enable fast electrical modulation of freely propagating terahertz waves" (PDF). Applied Physics Letters 93 (9): 091117 (2008). Bibcode:2008ApPhL..93i1117C. doi:10.1063/1.2978071. Retrieved 2009-11-12.
  18. ↑ 18.0 18.1 18.2
  19. ↑ 19.0 19.1 19.2 Ziolkowski, Richard W. and; Ching-Ying Cheng (2004-01-07). "Tailoring double negative metamaterial responses to achieve anomalous propagation effects along microstrip transmission lines". Microwave Theory and Techniques, IEEE Transactions on 51 (12): 203–206. Bibcode:2003ITMTT..51.2306C. doi:10.1109/TMTT.2003.819193.
  20. ↑ UCLA Technology. Backfire to Endfire Leaky wave antenna. 2003.
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  22. ↑ URSI Commission B website (2007). "URSI Commission B EMT-Symposium 2007" (CONFERENCE DIGEST AVAILABLE HERE). All Symposium papers available here (PDF). Retrieved 2010-04-24.
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  24. ↑ Bube, Richard H. (1992-09). Electrons in solids: an introductory survey. San Diego, CA: Elsevier Science. pp. 155, 156. ISBN 978-0-12-138553-8. Retrieved 2009-09-27. Check date values in: |date= (help)
  25. ↑ Federal Standard 1037C
  26. ↑ 26.0 26.1 26.2 26.3 Sanada, Atsushi; Caloz, C.; Itoh, T. (2004-02-26). "Characteristics of the Composite Right/Left-Handed Transmission Lines" (PDF). IEEE Microwave and Wireless Components Letters. Vol. 14, no. 2, pp.. February 2004 14 (2): 68–70. doi:10.1109/LMWC.2003.822563. Retrieved 2009-12-28.
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  30. ↑ Grbic, Anthony; George V. Eleftheriades (2002-08-07). "A backward-wave antenna based on negative refractive index L-C networks" (PDF). Antennas and Propagation Society International Symposium, 2002. IEEE 4: 340–343. doi:10.1109/APS.2002.1016992. ISBN 0-7803-7330-8.
  31. ↑ 31.0 31.1 31.2 31.3 Eleftheriades, G.V.; Iyer, A.K. Kremer, P.C. Edward S. Rogers Sr (2002-12-16). "Planar negative refractive index media using periodically L-C loaded transmission lines" (PDF). IEEE Transactions on Microwave Theory and Techniques 50 (12): 2702–2712. Bibcode:2002ITMTT..50.2702E. doi:10.1109/TMTT.2002.805197.
  32. ↑ Iyer, Ashwin; Peter Kremer; George Eleftheriades (2003). "Experimental and theoretical verification of focusing in a large, periodically loaded transmission line negative refractive index metamaterial". Optics Express 11 (7): 696–708. Bibcode:2003OExpr..11..696I. doi:10.1364/OE.11.000696. PMID 19461781.
  33. ↑ 33.0 33.1 33.2 33.3 Chatterjee, Rajeswari (1996). Antenna theory and practice. New Delhi: New Age International. pp. 1, 2. ISBN 0-470-20957-7.
  34. ↑ Pendry, J.B. et al. (1999). "Magnetism from conductors and enhanced nonlinear phenomena". IEEE Trans. Microw. Theory Tech. 47 (11): 2075. Bibcode:1999ITMTT..47.2075P. doi:10.1109/22.798002.
  35. ↑ Hsu, Yi-Jang; Huang, Yen-Chun; Lih, Jiann-Shing; Chern, Jyh-Long (2004). "Electromagnetic resonance in deformed split ring resonators of left-handed meta-materials". Journal of Applied Physics 96 (4): 1979. Bibcode:2004JAP....96.1979H. doi:10.1063/1.1767290.
  36. ↑ Aydin, Koray; Bulu, Irfan; Guven, Kaan; Kafesaki, Maria; Soukoulis, Costas M; Ozbay, Ekmel (2005). "Investigation of magnetic resonances for different split-ring resonator parameters and designs". New Journal of Physics 7: 168. Bibcode:2005NJPh....7..168A. doi:10.1088/1367-2630/7/1/168.
  37. ↑ Fangming Zhu; Qingchun Lin; Jun Hu (2005). "2005 Asia-Pacific Microwave Conference Proceedings" 3. p. 1. doi:10.1109/APMC.2005.1606717. ISBN 0-7803-9433-X. |chapter= ignored (help)
  38. ↑ Wang, Rui; Yuan, Bo; Wang, Gaofeng; Yi, Fan (2007). "Efficient Design of Directive Patch Antennas in Mobile Communications Using Metamaterials". International Journal of Infrared and Millimeter Waves 28 (8): 639. Bibcode:2007IJIMW..28..639W. doi:10.1007/s10762-007-9249-1.
  39. ↑ Alu, Andrea; Bilotti, Filiberto; Engheta, Nader; Vegni, Lucio (2007). "Subwavelength, Compact, Resonant Patch Antennas Loaded With Metamaterials". IEEE Transactions on Antennas and Propagation 55: 13. Bibcode:2007ITAP...55...13A. doi:10.1109/TAP.2006.888401.
  40. ↑ WU, Q.; Pan, P.; Meng, F.-Y.; Li, L.-W.; Wu, J. (2007-01-31). "A novel flat lens horn antenna designed based on zero refraction principle of metamaterials". Appl. Phys. A 87 (2): 151–156. Bibcode:2007ApPhA..87..151W. doi:10.1007/s00339-006-3820-9.
  41. ↑ Metamaterial-Engineered Antennas. University of Arizona. Accessed 2011-03-12.
  42. ↑ AFRL-Demonstrated Metamaterials Technology Transforms Antenna Radiation Pattern. U.S. Air Force research.Accessed 2011-03-12
  43. ↑ 43.0 43.1 Alu, A.; Engheta, N. (2003). "Pairing an epsilon-negative slab with a mu-negative slab: Resonance, tunneling and transparency". IEEE Transactions on Antennas and Propagation 51 (10): 2558. Bibcode:2003ITAP...51.2558A. doi:10.1109/TAP.2003.817553.
  44. ↑ 44.0 44.1 44.2 44.3 44.4 44.5 44.6 Engheta, Nader (2002). "An Idea for Thin Subwavelength Cavity Resonators Using Metamaterials With Negative Permittivity and Permeability". Antennas and Wireless Propagation Letters (University of Pennsylvania: IEEE) 1 (1): 10–13. Bibcode:2002IAWPL...1...10E. doi:10.1109/LAWP.2002.802576. Retrieved 2009-10-08.
  45. ↑ Alù, Andrea and; Nader Engheta (January 2004). "Guided Modes in a Waveguide Filled With a Pair of Single-Negative (SNG), Double-Negative (DNG), and/or Double-Positive (DPS) Layers". IEEE Transactions on Microwave Theory and Techniques 52 (1): 199. Bibcode:2004ITMTT..52..199A. doi:10.1109/TMTT.2003.821274. Retrieved 2010-01-03.
  46. ↑ Caiazzo, Marco; Maci, S.; Engheta, N. (2004). "A Metamaterial Surface for Compact Cavity Resonators". IEEE Antennas and wireless propagation letters 3: 261. Bibcode:2004IAWPL...3..261C. doi:10.1109/LAWP.2004.836576.
  47. ↑ Caglayan, Humeyra; Bulu, I; Loncar, M; Ozbay, E (2008-07-21). "Experimental observation of cavity formation in composite metamaterials" (PDF). Optics Express 16 (15): 11132–40. Bibcode:2008OExpr..1611132C. doi:10.1364/OE.16.011132. PMID 18648427. Retrieved 2009-11-30.
  48. ↑ Baccarelli, Paolo; Burghignoli, P.; Frezza, F.; Galli, A.; Lampariello, P.; Lovat, G.; Paulotto, S. (2005-01-17). "Effects of Leaky-Wave Propagation in Metamaterial Grounded Slabs Excited by a Dipole Source". IEEE Transactions on microwave theory and techniques 53: 32. Bibcode:2005ITMTT..53...32B. doi:10.1109/TMTT.2004.839346.
  49. ↑ 49.0 49.1 49.2 49.3 49.4 49.5 US 6958729 patent
  50. ↑ Engheta, Nader; Alù, Andrea "Waveguides and scattering devices incorporating epsilon-negative and/or mu-negative slabs" U.S. Patent 7,218,190 publication date May 15, 2007
  51. ↑ Matthew, Finnegan (December 10, 2010). "Metamaterials to revolutionize wireless infrastructure". TechEye (JAM IT Media Ltd). Retrieved 2010-12-30. With the increasing proliferation of wireless devices inside and out of the home and workplace there are concerns over how interference from the external electromagnetic environment can cause problems for the connectivity of devices in the future.

External links