Current developments in the wireless communication and sensor spaces are developing more ways to target an individual user or device. In cellular communications, a system goal is to optimize efficiency and focus energy directly to a user. To achieve this level of performance, systems add additional antennas and complex circuitry that increases their cost and footprint, while incurring latency and delay in processing.
The present application may be more fully appreciated in connection with the following detailed description taken in conjunction with the accompanying drawings, which are not drawn to scale and in which like reference characters refer to like parts throughout, and wherein:
Methods and apparatuses for a frequency-selective antenna are disclosed. The frequency-selective antenna incorporates metastructures that are capable of manipulating electromagnetic (“EM”) waves to provide directed wireless transmission between multiple devices. In various examples, the frequency-selective antenna enables transmission of multiple signals, each having a unique frequency, wherein transmissions at a given frequency are directed to an individual user or group of users. The transmission information for the multiple signals is received as a composite information signal at the user's device, wherein the radiating elements in the metastructures are configured for specific frequencies. Each radiating element has associated electromagnetic properties, including the resonant frequency and the phase of a radiated signal, that are adjustable using a frequency-selective control applied to the radiating element. Such frequency-selective control enables transmission of a user signal from a specific radiating element at a unique frequency and phase, thereby allowing a wireless transmission system to direct specific transmissions to specific users.
It is appreciated that, in the following description, numerous specific details are set forth to provide a thorough understanding of the examples. However, it is appreciated that the examples may be practiced without limitation to these specific details. In other instances, well-known methods and structures may not be described in detail to avoid unnecessarily obscuring the description of the examples. Also, the examples may be used in combination with each other.
Radiating structure 202 is configured on a substrate material, which may be part of system 100 or a separate structure. The antenna controller 204 includes a radiating element control module 216 that controls the radiating elements in radiating structure 202. In various examples and as described below with reference to
Attention is now directed to
A metamaterial is a geometric design of a material, such as a conductor, wherein the shape creates a unique behavior for the device. An MTM cell may be composed of multiple microstrips, gaps, patches, vias, and so forth having a behavior that is the equivalent to a reactance element, such as a combination of series capacitors and shunt inductors. Various configurations, shapes, designs and dimensions are used to implement specific designs and meet specific constraints. In some examples, the number of dimensional degrees of freedom determines the characteristics of a cell, wherein a cell having a number of edges and discontinuities may model a specific-type of electrical circuit and behave in a given manner. In this way, an MTM cell radiates according to its configuration. Changes to the reactance parameters of the MTM cell result in changes to its radiation pattern. Where the radiation pattern is changed to achieve a phase change or phase shift, the resultant structure is a powerful antenna, as small changes to the MTM cell can result in large changes to the beamform. The array of cells 406 is configured so as to form a composite beamform. This may involve subarrays of the cells or the entire array.
The MTM cells 406 may include a variety of conductive structures and patterns, such that a received transmission signal is radiated therefrom. In some examples, each MTM cell may have unique properties. These properties may include a negative permittivity and permeability resulting in a negative refractive index; these structures are commonly referred to as left-handed materials (“LHM”). The use of LHM enables behavior not achieved in classical structures and materials, including interesting effects that may be observed in the propagation of electromagnetic waves, or transmission signals. Metamaterials can be used for several interesting devices in microwave and terahertz engineering such as antennas, sensors, matching networks, and reflectors, such as in telecommunications, automotive and vehicular, robotic, biomedical, satellite and other applications. For antennas, metamaterials may be built at scales much smaller than the wavelengths of transmission signals radiated by the metamaterial. Metamaterial properties come from the engineered and designed structures rather than from the base material forming the structures. Precise shape, dimensions, geometry, size, orientation, arrangement and so forth result in the smart properties capable of manipulating electromagnetic waves by blocking, absorbing, enhancing, or bending waves.
In some examples, at least one of the MTM cells is coupled to a reactance control mechanism, such as a varactor to change the capacitance and/or other parameters of the MTM cell. By changing a parameter of the MTM cell, the resonant frequency is changed, and therefore, the array 406 may be configured and controlled to respond to multiple frequency bands. An example of such a cell is illustrated as MTM cell 408. MTM cell 408 has a conductive outer portion or loop 410 surrounding a conductive area 412 with a space in between. Each MTM cell 406 may be configured on a dielectric layer, with the conductive areas and loops provided around and between different MTM cells. A voltage controlled variable reactance device 414, e.g., a varactor, provides a controlled reactance between the conductive area 412 and the conductive loop 410. Varactor 414 is controlled by MTM cell control 418. The controlled reactance is controlled by an applied voltage, such as an applied reverse bias voltage in the case of a varactor. The change in reactance changes the behavior of the MTM cell 408. The voltage control is performed by MTM cell control 418 in response to identification of a position of the UE with respect to the system 100. The transceiver unit 208 provides this direction information and acts to instruct the MTM cell control 418 as to where to direct the beam.
A transmission signal 416 is provided to the antenna feed 402, wherein the transmission signal includes communication information for multiple UEs. Antenna feed 402 has a plurality of transmission lines for distributing the signal 416 to the metastructure antenna 404. The transmission signal for each UE has a corresponding frequency at which certain MTM cells 406 resonate. For example, the top row of MTM cells 406 are at a first frequency f1, and they resonate or radiate at frequency f1, but do not radiate EM signals at other frequencies. Similarly, the other rows of MTM cells 406 are each resonant at specific frequencies, and not respond to other frequencies. In this way, the MTM cells 406 act as specific band-pass filters.
In another example, each cell may have an hexagonal shape as in cell 508 to provide design flexibility for a densely packed array. Each cell 508 has an outer geometric shape, referred to herein as a hexagonal conductive loop, e.g., loop 510, and an inner geometric shape that is referred to as a hexagonal conductive patch, e.g., patch 512. The hexagonal shape provides the flexibility of design for a densely packed array, e.g., arrays 514-516, and the parametric shape enables computational design that can be easily scaled and modified while maintaining the basic shape of the hexagon. In this example, the dimensions of the shapes are geometrically similar and their relationship is proportionally maintained.
As illustrated, the sides of the hexagonal loop 510 are designated by reference letter “a” and the sides of the hexagonal patch 512 are designated by reference letter “b”. The hexagonal patch 512 is centered within the hexagonal loop 510. Corresponding points on the perimeters of the loop and patch are equidistant from each other, specifically in this example, at a distance designated by “d”. This configuration is repeated to form a densely packed lattice.
In
In some examples, each portion of the cells, or subarray of cells, is responsive to a first frequency. The subarray of cells are configured to operate together and thus to direct communications to a given user or in a specific direction. This may be used in a cellular communication system to direct a communication stream to a given user and maximize available transmission energy to that user, and thus increase the throughput to that user. This is a consideration in many applications, such as in video streaming to a mobile device. In a congested environment, it helps the transmission to each user, and allows the system to adjust the energy used for each transmission. For example, the system 100 of
The examples of
In the illustrated example, a first user receives signals at frequency f1, and the antenna controller adjusts the EM parameters of the subarray of cells that respond to the frequency f1. The adjustment changes the phase of individual cells such that their combined radiation forms a beam directed at the user. The beam direction concentrates energy to that user. In some situations, the beam is a pencil beam, or very thin beam, and in other situations, such as a multi-cast to multiple users, the beam may be sized to reach multiple users with a same transmission. As the subarrays responsive to frequency f1 are not responsive to the other frequencies, they do not radiate these frequencies of the composite signal, which includes all the frequencies. Each subarray responds to its frequency, while the other frequencies have little to no effect on that subarray. This concurrent transmission to multiple users with a frequency-selective directed antenna enables increases in throughput of a wireless system.
In some systems, the subarrays may be used for different functions, such as one subarray for cellular communications and another for functions using the Industrial, Scientific, Medical (“ISM”) band. The ability for a single metastructure antenna array to provide multiple frequency transmissions is a great improvement over other wireless systems. The metastructure antenna described above is particularly applicable for directed beam generation in a wireless transmission device. This directivity may be used to improve the capabilities of a communication system, such as to enable 5th Generation (“5G”) communications.
It is appreciated that the previous description of the disclosed examples is provided to enable any person skilled in the art to make or use the present disclosure. Various modifications to these examples will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other examples without departing from the spirit or scope of the disclosure. Thus, the present disclosure is not intended to be limited to the examples shown herein but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.
This application claims priority to U.S. Non-Provisional application Ser. No. 16/195,792, entitled “Method And Apparatus For A Frequency-Selective Antenna,” filed on Nov. 19, 2018, and incorporated herein by reference; which claims priority to U.S. Provisional Application No. 62/587,618, filed on Nov. 17, 2017, and incorporated herein by reference.
Number | Name | Date | Kind |
---|---|---|---|
4368469 | Ott | Jan 1983 | A |
4743914 | Schuss | May 1988 | A |
6043790 | Derneryd | Mar 2000 | A |
6687492 | Sugar | Feb 2004 | B1 |
6871081 | Llewellyn | Mar 2005 | B1 |
7405698 | de Rochemont | Jul 2008 | B2 |
7847739 | Achour et al. | Dec 2010 | B2 |
7889129 | Fox | Feb 2011 | B2 |
8178457 | de Rochemont | May 2012 | B2 |
8487832 | Lam | Jul 2013 | B2 |
8493281 | Lam | Jul 2013 | B2 |
8593819 | de Rochemont | Nov 2013 | B2 |
8633866 | Sarabandi | Jan 2014 | B2 |
8715839 | de Rochemont | May 2014 | B2 |
8803739 | Rajgopal | Aug 2014 | B2 |
8922347 | de Rochemont | Dec 2014 | B1 |
8952858 | de Rochemont | Feb 2015 | B2 |
9094102 | Corman | Jul 2015 | B2 |
9184496 | Duwel | Nov 2015 | B2 |
9190738 | Alexopoulos | Nov 2015 | B2 |
9236892 | Dupuy | Jan 2016 | B2 |
9293821 | Duwel | Mar 2016 | B2 |
9425890 | Corman | Aug 2016 | B2 |
9520649 | de Rochemont | Dec 2016 | B2 |
9711866 | Doane | Jul 2017 | B1 |
9786986 | Johnson | Oct 2017 | B2 |
9882274 | de Rochemont | Jan 2018 | B2 |
9905928 | de Rochemont | Feb 2018 | B2 |
10566683 | Campbell | Feb 2020 | B1 |
11451944 | Achour | Sep 2022 | B2 |
20080048917 | Achour | Feb 2008 | A1 |
20090135087 | Gummalla | May 2009 | A1 |
20100060544 | Penev | Mar 2010 | A1 |
20100123635 | Lopez | May 2010 | A1 |
20110175789 | Lee | Jul 2011 | A1 |
20110194551 | Lee | Aug 2011 | A1 |
20120039242 | Alexiou | Feb 2012 | A1 |
20140203969 | Maltsev | Jul 2014 | A1 |
20140210666 | Maltsev | Jul 2014 | A1 |
20140375525 | Shi | Dec 2014 | A1 |
20150022407 | Piazza | Jan 2015 | A1 |
20150022421 | Vigano | Jan 2015 | A1 |
20150229028 | Bily | Aug 2015 | A1 |
20160087349 | Lee | Mar 2016 | A1 |
20160141754 | Leyh | May 2016 | A1 |
20160345189 | Miyagawa | Nov 2016 | A1 |
20180152235 | Smoot | May 2018 | A1 |
20220247074 | Zamanifekri | Aug 2022 | A1 |
Entry |
---|
G. Mumcu, et al., “Metamaterial Antennas,” in Frontiers in Antennas Next Generation Design & Engineering, New York, NY, McGraw Hill, 2011, ch. 5, pp. 203-239. |
Y.J. Guo, et al., “Reconfigurable Antennas for Wireless Communications,” European Conference on Antennas and Propagation (EuCAP), Gothenburg, Sweden, Jun. 2013, pp. 165-168. |
Y.J. Cheng, “Substrate Integrated Waveguide Frequency-Agile Slot Antenna and its Multibeam Application,” Progress In Electromagnetics Research, vol. 130, pp. 153-168, Aug. 2012. |
G.H. Huff, et al. ,“Reconfigurable Antennas,” in Frontiers in Antennas Next Generation Design & Engineering, New York, NY, McGraw Hill, 2011, ch. 7, pp. 271-303. |
H. Lee, “A Compact Single Radiator CRLH-Inspired Circularly Polarized Leaky-Wave Antenna Based on Substrate- Integrated Waveguide,” IEEE Transactions on Antennas and Propagation, vol. 63, No. 10, pp. 4566-4572, Oct. 2015. |
M. Salarkaleji, et al., “Two-Dimensional Full-Hemisphere Frequency Scanning Array Based on Metamaterial Leaky Wave Antennas and Feed Networks,” IEEE MTT-S International Microwave Symposium (IMS), San Francisco, CA, May 2016. |
D. Patron, “Compact Reconfigurable Antennas for Wireless Systems and Wearable Applications,” Ph.D. dissertation, Dept. of Electrical and Computer Eng., Drexel University, Philadelphia, PA, May 2015. |
J. Reis, et al., “Two-Dimensional Antenna Beamsteering Using Metamaterial Transmitarray,” European Conference on Antennas and Propagation (EuCAP), Lisbon, Portugal, Aug. 2015. |
M.C. Johnson, “Self-Optimizing Metamaterial Antennas,” Ph.D. dissertation, Dept. of Applied Mathematics, Univ. of Washington, Seattle, WA, 2014. |
S. Gupta, “Analysis and Design of Substrate Integrated Waveguide-Based Antennas for Millimeter Wave Applications,” M.S. thesis, Dept. of Electrical and Computer Eng., Concordia Univ., Montreal, Quebec, Canada, May 2016. |
C. Tripon-Canseliet, et al., “Contribution of MetaMaterials to Improvement of Scan Performance and Reconfigurability of Phased Array Antennas,” International Radar Conference, Lille, France, Oct. 2014, pp. 1-3. |
Number | Date | Country | |
---|---|---|---|
20220109459 A1 | Apr 2022 | US |
Number | Date | Country | |
---|---|---|---|
62587618 | Nov 2017 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 16195792 | Nov 2018 | US |
Child | 17551088 | US |