The present disclosure relates to antennas. In particular, the present disclosure relates to a liquid-crystal tunable metasurface for beam steering antennas.
Signal strength in an antenna system is dependent on a number of factors, such as distance from the receiver to the transmitter, obstacles between the transmitter and receiver, signal fading, multipath reception, line of sight interference, Fresnel zone interference, radio frequency (RF) interference, weather conditions, noise, etc. Any one, or a combination, of these factors may result in poor connections, dropped connections, low data rates, high latency, etc. In order to mitigate these factors, a lobe of a radiation pattern for the transmitter antenna and/or the receiver antenna may be adjusted to direct the lobe between the receiver and the transmitter. Adaptive beam formers or beam steering automatically adapts the antenna response (of the transmitter, receiver, or both) to compensate for signal loss. In beam formers, interfering and constructing patterns may be used to change the shape and direction of the signal beam from multiple antennas using antenna spacing and the phase of signal emission from each antenna in an antenna array. Beam steering may change the directionality of the main lobe by controlling the phase and relative amplitude of the signal at each transmitter.
A metasurface, which is an artificial sheet material having electromagnetic properties that can varied on demand, may control reflection and transmission characteristics of EM wave. For example, a metasurface can be a two-dimensional periodical structure that contains electrically small scatterers with periodicity relatively small compared to an operating wavelength. A metasurface for purposes of beam steering system is described in “Two-Dimensional Beam Steering Using an Electrically Tunable Impedance Surface” by Sievenpiper et al. (IEEE Trans. On Antennas and Prop., Vol. 51, No. 10, pp 2713-2721, October, 2003). Sievenpiper discloses a two-dimensioning beam steering using an electrically tunable impedance surface loaded using varactor diodes. The use of varactor diode loading becomes impractical for high frequencies with a large surface where over hundreds of diodes are required. For communications applications, use of varactor diodes may be undesirable due to its nonlinearity which can induce undesirable noise due to passive intermodulation (PIM).
Example embodiments are described of an electronically tunable metasurface whose reflective phase can be electronically reconfigured to allow effective antenna beam steering.
According to one example aspect is a metasurface for reflecting an incident wave to effect beam steering. The metasurface includes first and second double sided substrates defining an intermediate region between them containing liquid crystal in a nematic phase. The first substrate has a first microstrip patch array formed on a side thereof that faces the second substrate, the first microstrip patch array comprising a two-dimensional array of microstrip patches each being electrically connected to a common potential. The second double sided substrate has a second microstrip patch array formed on a side thereof that faces the first substrate, the second microstrip patch array comprising a two-dimensional array of microstrip patches each having a respective conductive terminal. The first microstrip patch array and the second microstrip patch array are aligned to form a two dimensional array of cells, each cell comprising a microstrip patch of the first microstrip patch array arranged in spaced apart opposition to a microstrip patch of the second microstrip patch array with a volume of the liquid crystal located therebetween. The conductive terminal to the microstrip patch of the microstrip patch second array permitting a control voltage to be applied to the cell to control a dielectric value of the volume of the liquid crystal, thereby permitting a reflection phase of the cell to be selectively tuned.
The metasurface may include a gridded wire mesh on the first substrate, each of the microstrip patches of the first microstrip patch array being electrically connected to a respective point of the gridded wire mesh to provide the common potential. The gridded wire mesh may be formed on a side of the first substrate that is opposite the side on which the first microstrip patch array is formed, each of the microstrip patches of the first microstrip patch array being electrically connected to the gridded wire mesh by a respective plated through hole that extends through the first substrate. The respective conductive terminals that extend through the second substrate may also each be plated through holes.
In some configurations, a thickness of the first substrate and a thickness of the intermediate region containing the liquid crystal are each less than ¼ of an intended minimum operating wavelength of the incident wave.
According to another aspect is a metasurface for reflecting an incident wave to effect beam steering. The metasurface includes a wire mesh layer; a ground plane layer generally parallel to the wire mesh layer; and a plurality of cells between the wire mesh layer and the ground plane, each cell comprising a pair of microstrip patches having layer of nematic liquid crystal therebetween.
According to another aspect is a method of beam steering. The method includes providing a metasurface to reflect an incident wave from an antenna, the metasurface comprising a two dimensional array of cells each including a volume of liquid crystal; applying voltages to control terminals associated with a plurality of the cells of the metasurface, the voltage orienting molecules of a liquid crystal within each cell; and adjusting the phase of the incident wave by adjusting a resonant frequency of each cell by varying the orientation of the molecules.
Providing a metasurface can include: providing a first printed circuit board (PCB) having an intermediate substrate layer with a first two dimensional array of microstrip patches formed on one side of the substrate layer and a gridded wire mesh formed on an opposite side of the substrate layer, each of the microstrip patches of the first two dimensional array be electrically connected to a respective point on the wire mesh by a conductor extending through the intermediate substrate layer; providing a second PCB having an intermediate substrate layer with a second two dimensional array of microstrip patches formed on one side of the substrate layer, each of the microstrip patches of the second two dimensional array having a respective conductive control terminal that extends through the second substrate; and arranging the first PCB and the second PCB with a layer of nematic state liquid crystal therebetween such that the microstrip patches of the first two dimensional array each align with a respective microstrip patch of the second two dimensional array to form the two dimensional array of cells.
Reference will now be made, by way of example, to the accompanying drawings which show example embodiments of the present application, and in which:
Similar reference numerals may have been used in different figures to denote similar components.
An electronically tunable metasurface 100 is shown in
A physical implementation of metasurface 100 will now be described according to example embodiments.
Upper PCB 120 has a central non-conductive substrate layer (shown in cross-hatch in
Lower PCB 122 has a central non-conductive substrate layer (shown in cross-hatch in
In the example embodiment described above, control voltages are provided to the lower microstrip patches 142 through PTH vias 114 that are accessible through the ground plane 130. Other embodiments could have different configurations, including a control line layer that could be integrated into substrate 122 to provide conductive control terminals to each of the microstrip patches 142.
As described above, the upper and lower PCBs 120, 122 are located in spaced opposition to each other with an intermediate layer of liquid crystal 146 located between them. The upper PCB microstrip patches 140 and the lower PCB microstrip patches 142 align with each other to from an array of cell regions 144, each of which contains a volume of liquid crystal 146, thus providing an array of individually controllable, LC cell regions 144.
Accordingly, as can be appreciated from
The metasurface 100 has a resonant frequency that can depend on the geometry of the cells 106 and dielectric properties of the materials used in the PCBs 120, 122. In example embodiments, the microstrip patches 140, 142 have rectangular surfaces (for example square) having a maximum normal dimension that is less than ¼ of the minimum intended operating wavelength, however other microstrip patch configurations could be used. In example embodiments, the microstrip patches 140, 142 may have dimensions that are less than quarter of a wavelength of the intended operating wavelength of the metasurface 100. In an example embodiment, wire mesh 118 has a periodicity and grid dimensions that correspond to those of microstrip patches 140, with a grid intersection point occurring over a center point of each microstrip patch 140.
As noted above, in at least some examples, the metasurface 100 illustrated in
In example embodiments, the liquid crystal 146 is a nematic liquid crystal that has an intermediate nematic gel-like state between solid crystalline and liquid phase at the intended operating temperature range of the metasurface 100. Examples of liquid crystal include, for example, GT3-23001 liquid crystal and BL038 liquid crystal from the Merck group. Liquid crystal 146 in a nematic state possesses dielectric anisotropy characteristics at microwave frequencies, whose effective dielectric constant may be adjusted by setting different orientations of the molecules of liquid crystal 146 relative to its reference axis.
In particular, with reference to
In summary, the resonant frequency of each unit cell 106 may be tuned individually and electronically by adjusting DC voltage at each cell 106. Because reflection phase is determined by the frequency of the incoming wave with respect to the resonance frequency, the metasurface 100 can be tuned to form a distributed 2D phase shifter. Therefore, an incoming wave may be redirected by adjusting DC voltages of unit cells 106 to give proper phase distribution for the desired direction of reflected wave.
In example embodiments the metasurface 100 has a relatively high density/small periodicity of cells 106 and can be analyzed as an effective medium with its surface impedance defined by effective lumped-element circuit parameters. In an example embodiment, where A represents an minimum intended operating frequency, top PCB 120 is relatively thin, having a thickness h1<λ/20 and the liquid crystal 146 in cell region 144 has a thickness of h2<λ/20 (i.e. the gap between the opposed microstrip patches 140 and 142). The thicknesses h1 and h2 can be different from each other. In example embodiments the bottom PCB 122 has a finite thickness h3<λ/4. The narrow gap between the opposed microstrip patches 120 and 122 of each cell 106 and small spacing gaps 148 between neighboring cells 106 that results from the small periodicity provides metasurface 100 with an equivalent sheet capacitance C, and permits each cell 106 to be modeled as a parallel resonant circuit 700, 800 as shown in
Parallel resonant circuit 800 has a surface impedance Zs given by
which has a typical resonance frequency at:
Where Cv is the input capacitance of cell 106.
In the case of fixed values of L and Cv, the metasurface 100 reflects an incident wave with a phase shift of 180 degrees for frequency below the resonance frequency, and 0 degrees at the resonance frequency, and approaches −180 degrees for frequencies above the resonance frequency. Since the reflection phase may be determined by the frequency of the incoming wave with respect to the resonance frequency of the metasurface 100, the phase shift of the incoming wave can be adjusted for each individual cell 106 by varying the equivalent input capacitance Cv of the unit cell 106, which is a function of the geometry of the microstrip patches 120 and 122, and thickness and dielectric constant of the liquid crystal layer 146.
Therefore, the effective dielectric constant of a unit cell 106 may be independently tuned by changing electrostatic voltage between microstrip patches 120 and 122 of the unit cell 106. This change in effective dielectric constant of a unit cell 106 leads to the change in the input capacitance, Cv, of the cell 106. As a result, a phase differential at various locations of the metasurface 100 may be changed individually. The structure of the unit cell 106 is simulated in
It will thus be appreciated that the reflection phase of an incident wave at the surface of the metasurface 100 can be controlled by varying the DC voltages applied to unit cells 106 such that continuous beam steering of an EM wave can be achieved by regulating DC voltage distribution to unit cells 106 across the metasurface 100.
The present disclosure may be embodied in other specific forms without departing from the subject matter of the claims. The described example embodiments are to be considered in all respects as being only illustrative and not restrictive. Selected features from one or more of the above-described embodiments may be combined to create alternative embodiments not explicitly described, features suitable for such combinations being understood within the scope of this disclosure. For examples, although specific sizes and shapes of cells 106 are disclosed herein, other sizes and shapes may be used.
Although the example embodiments disclose individually addressable cells, other embodiments may have cells that may be addressable by row or column or in a multiplexed manner.
Although the example embodiments are described with reference to a particular orientation (e.g. upper and lower), this was simply used as a matter of convenience and ease of understanding in describing the reference figures. The metasurface may have any arbitrary orientation.
All values and sub-ranges within disclosed ranges are also disclosed. Also, while the systems, devices and processes disclosed and shown herein may comprise a specific number of elements/components, the systems, devices and assemblies could be modified to include additional or fewer of such elements/components. For example, while any of the elements/components disclosed may be referenced as being singular, the embodiments disclosed herein could be modified to include a plurality of such elements/components. The subject matter described herein intends to cover and embrace all suitable changes in technology.
This application claims priority to and benefit of U.S. Provisional Patent Application No. 62/398,141, filed Sep. 22, 2016, the contents of which are incorporated herein by reference.
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