Patent Application
20060022875
The invention relates to antennas, and more particularly to miniature antennas for microwave transmission and reception.
Conventional antennas often have linear dimensions comparable to the wavelength of the radiation being received or transmitted. For example, a typical radio transmitter uses a dipole antenna whose length is about one-half the wavelength of the waves being transmitted. Such an antenna length provides for efficient coupling between the antenna's electrical driver and the radiation field.
However, antennas having linear dimensions comparable to the radiation wavelength are not practical in all situations. In particular, cellular telephones and handheld wireless devices are small. Because such devices provide limited space for antennas, it would be advantageous to equip them with miniaturized antennas. Unfortunately, simply reducing antenna size without deviating from conventional principles leads to small antennas that couple inefficiently to the radiation at the wavelengths typically used in cellular telephones and handheld wireless devices.
U.S. Pat. No. 6,661,392, which issued to Isaacs et al. on Dec. 9, 2003, describes an antenna that resonantly couples to external radiation at communication frequencies even with linear dimensions much smaller than one-half the radiation wavelength. Due to the resonant coupling, the antenna is very sensitive to the radiation.
The antenna includes a resonant object formed of a special material, such as a manmade metamaterial, whose electrical permittivity or magnetic permeability has, in effect, a negative real part at microwave frequencies. One or more sensors located adjacent to or in the object measure an intensity of an electric or a magnetic field therein.
Although antennas based on such special materials have promise, improvements in bandwidth and waveguide coupling efficiency are needed in order for the performance of such antennas to be improved to the fullest possible extent.
An antenna according to the present invention includes a resonant body fabricated of a material whose electrical permittivity or magnetic permeability is negative, or of a manmade metamaterial which emulates such behavior, over a range of communication frequencies. The, e.g., metamaterials are selected to cause the antennas to couple resonantly to external radiation at specified communication frequencies in, e.g., the range 0.1 GHz to 10 THz, and particularly in the range of microwave frequencies between about 1 GHz and about 100 GHz. Due to the resonant coupling, the antennas have high sensitivity to the radiation even though their linear dimensions are much smaller than the wavelength of the radiation.
The resonant coupling results from selecting the metamaterial to have appropriate effective permittivity or permeability values. An appropriate selection of the metamaterial depends on the shape of the object and the frequency range over which a resonant response is desired. Theory shows that for spherical antennas, for example, the permittivity or permeability of an idealized material advantageously has a real part near −2 in a frequency range of interest. For such values, a spherical antenna is very sensitive to external radiation even if its diameter is much smaller than one-half the radiation wavelength.
Accordingly, the invention in one aspect involves an antenna which is meant to operate in a range of frequencies including a resonant frequency fres of the antenna. A vacuum wavelength λres corresponds to electromagnetic radiation at the resonant frequency. The antenna includes a resonator coupled to a transmission line. The resonator comprises a patterned structure, or a shaped material which has negative electric permittivity or magnetic permeability. The maximum spatial extent of the resonator is less than one-half λres. The resonator is effective for supporting a resonance, and for coupling to an external radiation field such that the resonant scattering cross-section of the resonator is greater than or equal to approximately 0.3λres2 for at least one incident polarization and direction of electromagnetic radiation. The transmission line is coupled to the resonator such that when the resonator is driven at fres by a driving signal in the transmission line, there is at least 10 dB of return loss in the transmission line.
Although no naturally occurring materials are known that exhibit negative electrical permittivity or negative magnetic permeability at microwave frequencies, such behavior can be made to occur over a limited frequency range in artificial materials such as so-called structured dielectrics, also referred to as metamaterials. Typical metamaterials are constructed from periodic arrays of wires or metal plates. Negative permittivity has also been observed in plasmas having certain charge densities.
Some such metamaterials having properties which may be useful in the present context are described in R. A. Shelby et al., “Experimental Verification of a Negative Index of Refraction”, Science 292 (2001) 77. Various designs for such metamaterials are provided in D. R. Smith et al., “Composite Medium with Simultaneously Negative Permeability and Permittivity”, Physical Review Letters 84 (2000) 4184 and R. A. Shelby et al., “Microwave transmission through a two-dimensional, isotropic, left-handed metamaterial”, Applied Physics Letters 78 (2001) 489. Exemplary designs produce metamaterials having permittivities, permeabilities, or both, with negative values at frequencies in the ranges of about 4.7-5.2 GHz and about 10.3-11.1 GHz.
Various designs for 2- and 3-dimensional manmade objects of metamaterials include 2- and 3-dimensional arrays of conducting objects. Various embodiments of the objects include single and multiple wire loops, split-ring resonators, conducting strips, and combinations of these objects. The exemplary objects made of single or multiple wire loops have resonant frequencies that depend in known ways on the parameters defining the objects. The effective electrical permittivities and magnetic permeabilities of the metamaterials depend on both the physical traits of the objects therein and the layout of the arrays of objects. For wire loop objects, the resonant frequencies depend on the wire thickness, the loop radii, the multiplicity of loops, and the spacing of the wires making up the loops. See e.g.,; “Loop-wire medium for investigating plasmons at microwave frequencies”, D. R. Smith et al., Applied Physics Letters 75 (1999) 1425.
It has been found that localized plasma resonances in negative permittivity materials can couple strongly to radiating electromagnetic fields even when the resonating structures are smaller in spatial extent than one vacuum wavelength of the radiating field. (Such structures are referred to here as “subwavelength” structures.)
At the frequencies of interest, the permittivity in the materials of interest is dependent on the frequency of the electromagnetic field. For example, at least some negative permittivity materials are modeled by an expression of the form
in which ε(ω) is the permittivity as a function of frequency ω, ωp is the plasma frequency of the material, and γ represents loss. We refer to this expression as a “permittivity dispersion relation.” In at least certain structures, strong plasma resonances are predicted at those frequencies for which the permittivity lies near −2. For example, resonance is predicted for subwavelength spheres near frequencies ω for which ε(ω)=−2, and for cylinders of infinite length and subwavelength radius near frequencies ω for which ε(ω)=−1.
Importantly, theoretical studies predict that at resonance, the electromagnetic scattering cross section of a lossless negative permittivity sphere whose diameter is much smaller than one wavelength will be fixed at
even when the sphere is vanishingly small. Thus, anomalously strong coupling to radiative fields is predicted for small bodies behaving as antennas. We believe that a range of subwavelength structures having non-spherical geometries and moderate amounts of loss will also exhibit such anomalous coupling behavior if there is negative permittivity. Detailed calculations have confirmed this belief for at least one such structure, as will be explained below.
One feature that is important for characterizing the performance of an antenna is the bandwidth or the Q factor of the antenna. (The bandwidth, expressed as a percentage of the resonant frequency, is
If the bandwidth is too small (Q is too high), the antenna may be ineffective for transmitting or receiving in more than a portion of a desired communication band. It is well known from conventional antenna theory that, for antennas much smaller than the wavelength, the minimum achievable Q of the antenna varies inversely with the cube of the radius of the smallest sphere enclosing the entire antenna; thus, as the radius decreases, the resonance bandwidth also decreases. Furthermore, most conventional antenna designs are not optimized to achieve this minimum value of Q, and tend to perform substantially worse than this fundamental limit. However, for radii much less than one wavelength, the theoretical Q of a lossless negative permittivity sphere is only a factor of 3/2 greater than the fundamental lower limit. This suggests that negative permittivity spheres will have particularly good bandwidth performance (relative to the fundamental limit) when utilized as small antennas, and furthermore that, for resonant geometries other than a sphere, the use of negative permittivity structures as resonators will provide improved bandwidth performance relative to conventional antenna designs of the same size.
Material loss, i.e., dissipation of electromagnetic energy within the antenna material, is another feature that should be considered in antenna design. In general, the permittivity is a complex number, i.e., ε=εr+iεi, wherein εr and εi are real numbers denoting, respectively, the real and imaginary parts of the permittivity. When the permittivity is said to be “negative,” what is meant is that εr is negative. Material loss is characterized by εi. Although some loss may lead to a beneficial broadening of the resonance bandwidth of the antenna, there is a tradeoff because loss also decreases the scattering efficiency of the antenna.
The scattering efficiency η is defined as the ratio of the scattering cross section to the sum of the scattering and absorption cross sections. Although the specific scattering efficiency needed for an antenna to be useful depends on the specific application and may in some cases be quite low, it is generally desirable for the scattering efficiency to be at least 50%.
For a resonant subwavelength sphere as described above, the theoretical scattering efficiency is given by
in which r is the radius of the sphere and λ is the vacuum wavelength corresponding to frequency ω. It will be seen that as the radius of the sphere is reduced, the scattering efficiency decreases, and that for very small radii, the theoretical scattering efficiency varies as r3.
According to the model described above, to maintain a scattering efficiency above 50%, a resonant sphere with r/λ=0.1 would need εi<0.5 and a resonant sphere with r/λ=0.05 would need εi<0.06.
For the radiant structure to function as a useful antenna, it should be able to convert, with relatively high efficiency, between guided waves in a transmission line or other waveguiding structure, and radiating waves in free space. It should be noted in this regard that both operation in transmission and operation in reception are envisaged. In transmission, conversion is from the guided wave to the wave radiating in free space, and conversely for reception.
Stub 60 is a short straight portion of center conductor 30 that extends above plate 50 (as seen in the figure) in the direction perpendicular thereto. Stub 60 is electrically insulated from plate 50.
The symmetry axis of torus 20 is collinear with that of stub 60. The distance of closest approach between torus 20 and plate 50 is 1.5 mm, and the distance of closest approach between the torus and stub 60 is also 1.5 mm.
In a series of numerical simulations which are described in more detail below, we varied the length of stub 60 to find that length which gave optimum coupling between the transmission line and the antenna structure. We found an optimum stub length of about 10 mm, which was approximately one-fourteenth the vacuum wavelength of radiation at the resonant frequency.
For our numerical simulations, we chose resonator 20 to be toric in shape for two reasons: the torus provides good modal overlap between the transmission line and the resonator, and the axial symmetery of the torus simplifies the numerical modeling calculations. Therefore, it should be noted that effective resonators are likely to be found in other configurations, including those that lack axial symmetry, so long as good modal overlap is provided. One configuration of interest, for example, is a spherical resonator offset a small distance from the stub.
In at least some cases, it will also be advantageous to configure a resonator as a collection of two or more separate but electromagnetically coupled bodies.
In regard to modal overlap, reference is made to
In our numerical simulations, we assumed that the permittivity of the resonator varied with frequency according to the permittivity dispersion relation specified above. As noted, the toric structure was adopted partly to afford good modal overlap with the stub. The amount of modal overlap was estimated by well-known quasi-static techniques of electric field analysis. It should be noted in this regard that localized plasmon resonances, such as are expected in our resonator structures, have electric field profiles that are uniform across the resonating structure.
In our numerical simulations, we considered two hypothetical values for the loss coefficient γ: γ=0 and γ=0.02 ωp, in which ωp is the plasma frequency of the resonator. In each case, we launched an incident wave into the transmission line and measured (through simulations) the return loss in the transmission line. A large negative value of the return loss in decibels signifies that power has been efficiently coupled from the transmission line to the resonator, and from the resonant plasmon mode to radiating modes in free space.
The results shown in
Our simulations also showed that a stub of optimal length extends about halfway into the toric resonator. Our simulations also showed that varying the distance of closest approach of the torus to the stub and ground plate shifts the resonant frequency to lower values as the distance decreases.
Our simulations showed that when operated in transmission, the antenna structure of
The return loss of an antenna fed by a transmission line is readily measured by connecting a network analyzer to the transmission line and using the network analyzer to measure, versus frequency, the relative amount of power incident on the antenna that is reflected back into the transmission line.
In general, an antenna according to the principles described herein will be useful for at least some applications if it exhibits a return loss of magnitude greater than about 10 dB. If the return loss is substantially less than 10 dB, too little microwave power will be coupled into the antenna (for transmission) or out of the antenna (for reception) to be useful for any applications other than some specialized applications. From our numerical modeling, we believe that, surprisingly, return losses of 10 dB and more can be realized in antenna structures of subwavelength dimensions.
Turning back to
In one embodiment, a resonator of the kind discussed here is implemented using an actual plasma with a plasma frequency determined by the charge density n of the plasma according to the well-known equation
where e and m are the electric charge and mass of the individual charge elements of the plasma. This can be achieved, for example, using a conventional gas-discharge tube, or alternatively, using semiconductors where the individual charge elements are introduced by doping or carrier injection (electrical or optical).
Because of the strict dependence of the plasma frequency on charge density, not all frequency ranges of interest may be available using an actual plasma as described above. For example, achievable dopant levels in semiconductors result in plasma frequencies that are at minimum several hundred gigahertz. However, as noted above, other embodiments can utilize the ability of structured dielectrics to emulate the behavior of negative permittivity materials.
The scattering spectra of
even though the radii of these structures range from 0.15 to 0.057 times the exciting wavelength at resonance. These resonators therefore emulate the electromagnetic response of negative permittivity resonators, and can be used in lieu of actual negative permittivity materials to achieve the desired behavior at the frequencies of interest. It should be noted that although the exemplary resonators shown in
We have described exemplary embodiments of the invention in which the resonator is made from a material that exhibits negative effective electrical permittivity. As noted, other embodiments can be made which instead rely upon material exhibiting negative magnetic permeability. Such embodiments are also considered to lie within the scope and spirit of the present invention.
