The present invention relates to wireless communications, and more particularly, to multiband multiport antennas used in wireless communications.
Several recent trends in cellular communications as put pressure on antenna design and performance. First, new spectrum is being made available, led by the additional licensing of sub-6 GHz frequency bands, as well as the advent of CBRS (Citizens Broadband Radio Service) and licensed use of C-Band, for use by both network operators and private networks. Second, developments such as Carrier Aggregation push for improved performance within and across existing and new bands: e.g., Low Band 617-894 MHz, Mid Band 1695-2690 MHz, and C-Band and CBRS 3.4-4.2 GHz. Third, beamforming and Massive MIMO (Multiple Input Multiple Output) further push demand for multiport operation within a single antenna.
Increase in bands and service providers has led to tower densification, in which more and more antennas as being mounted on existing cell tower infrastructure. This has in turn led to a demand for higher channel capacity (e.g., higher port count) antennas that are capable of operating in numerous frequency bands. This push for increased channel capacity puts additional pressures on antenna design. First, increased channel capacity requires high quality beam patterns for features such as Massive MIMO, 8T8R (Eight Transmit Eight Receive) schemes, and tighter sectorization.
A conventional solution to the design challenges of high channel capacity antennas as described above is to increase the size of the antenna. However, this causes considerable problems in terms of antenna wind loading and weight, with wind loading being a particularly severe problem. Accordingly, designing a high count multiport high channel capacity antenna requires that antenna designers find a way to more densely pack the antenna radiators of each of the different supported frequency bands into a constrained antenna area. This may be referred to as antenna densification or packing density.
Increasing packing density presents considerable challenges, primarily due to mutual coupling of dipoles of different frequency bands and the resulting cross polarization and other interference effects. An example of this is when radiation emitted by a lowband dipole causes excitation within portions of a nearby midband dipole, and the subsequent radiation emitted by the midband dipole couples back into the lowband dipole. The cross-coupled radiation may have a degraded polarization quality that, once coupled back into the lowband dipole, contaminates the isolation between the two radiated polarization states of the lowband dipole. This cross polarization interference can severely degrade beam quality and thus the performance of the antenna. As mentioned above, a conventional approach to preventing cross polarization is to increase the distance between the midband dipoles and the lowband dipoles, but this solution violates the requirement of minimizing antenna wind loading.
Accordingly, what is needed is a dipole design that minimizes cross polarization effects while enabling dipoles of different frequency bands to be packed together as closely as possible.
An aspect of the present invention involves a multiband antenna. The multiband antenna comprises a plurality of first dipoles configured to radiate in a first frequency band; and one or more second dipoles configured to radiate in a second frequency band, wherein each of the first dipoles has a radiator plate and a balun stem, each radiator plate having first side and a second side opposite the first side, a capacitive coupling element disposed on the first side, and a folded dipole element disposed on the second side, wherein the capacitive coupling element has an inductive trace that electrically couples to a radiator inductive trace through a via formed in the radiator plate, the radiator inductive trace coupled to the folded dipole element
Array face 100 may be deployed as part of a multiport antenna, such as a 20-port antenna. In this example, the lowband dipoles 110 may be allocated four ports, one per +/−45 degree polarization of each of the two lowband dipole columns; the midband dipoles 105 may be allocated 8 ports, one per +/−45 degree polarization of each of the four midband dipole columns; and the C-Band/CBRS dipoles 115 may be allocated 8 ports to enable 8T8R operation. It will be understood that this port allocation is exemplary, and that other port allocations are possible and within the scope of the disclosure.
Although the illustrated exemplary array face 100 has four columns of midband dipoles 105 and two interleaved columns of lowband dipoles 110, it will be understood that variations to this configuration are possible and within the scope of the disclosure.
Unit cell 200 may illustrate the challenge of densely packing the midband dipoles 105 with one or more lowband dipoles 110. For example, using conventional dipoles, the center-to-center distance along the x-axis must be at least 4 inches to prevent cross polarization. However, with the exemplary midband dipole 105 according to the disclosure, center-to-center distance between a given midband dipole 105 and a neighboring lowband dipole 110 may be as low as 2.75 inches.
Radiator board 305 has four conductive folded dipole elements 315a and 315b, disposed on its lower surface. Each of the two first polarization folded dipole elements 315a are capacitively and inductively coupled to a corresponding first polarization coupling elements 320a; and each of the two second polarization folded dipole elements 315b are capacitively and inductively coupled to a corresponding second polarization coupling elements 320b.
Folded dipole elements 315a/315b may be configured as disclosed in US Provisional Patent Application HIGH PERFORMANCE FOLDED DIPOLE FOR MULTIBAND ANTENNA, Ser. No. 63/075,394, which is incorporated by reference as if fully disclosed herein.
In an exemplary embodiment, radiator board 305 may be formed of a PCB material such as ZYF300CA-C, having a thickness of 30 mil, and the conductive elements and traces formed on the PCB according to the disclosure may be formed of Copper having a thickness of 1.4 mil. It will be understood that such materials and dimensions are exemplary, and that variations to these are possible and within the scope of the disclosure.
Each inductive trace 345a/b may be disposed on the lower surface of radiator plate 305 such that it follows a path within an open area defined by the geometry of respective folded dipole element 315a/b.
Functionally, a first RF signal provided to the conductive traces of balun plate 325a is coupled through both solder joints 330a to first polarization coupling elements 320a. The first RF signal conducted to first polarization coupling elements 320a are capacitively coupled to respective folded dipole elements 315a. However, additionally, the RF signal is coupled from each folded dipole element 315a through its respective inductive trace 335a, via 340a, and radiator inductive trace 345a. This inductive coupling, in conjunction with the capacitive coupling between first polarization coupling elements 320a respective folded dipole elements 315a, decouples the midband dipole 105 such that it creates an CLC filter, which chokes out any common mode resonance, and making the midband dipole 105 effectively invisible to the lowband dipole 110. Further, the folded dipole structure (as opposed to a cross dipole) of the midband dipole 105 mitigates any subsequent insertion loss due to the decoupling structure according to the disclosure.
The decoupling provided by the disclosed midband dipole 105 renders it effectively invisible to the lowband dipole 110 to where different lowband dipoles may be employed in array face 100 to accommodate different specific licensed and unlicensed frequency bands as may be required for different network operators. Accordingly, different lowband dipoles 110 may be “pugged in” to array face 100 for different customers without the need to redesign the array face 100 or the midband dipoles 105.
Although the above discussion involved the design of a midband dipole that renders it effectively invisible to one or more lowband dipoles located in close proximity, it will be understood that these dipoles may correspond to other frequency bands whereby first dipoles of a first frequency range may have the disclosed dipole design such that it will be rendered effectively invisible to one or more second dipoles of a second frequency range, whereby the first frequencies are sufficiently higher than the second frequencies such that the first frequency band has a 0.4λ relation to the second frequency band. It will be understood that such variations are possible and within the scope of the disclosure.
This application is a continuation of U.S. patent application Ser. No. 17/552,674, filed Dec. 16, 2021, which claims priority to U.S. Provisional Patent Application Ser. No. 63/128,550, filed Dec. 21, 2020, pending, which applications are hereby incorporated by this reference in their entirety as if fully set forth herein.
Number | Date | Country | |
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63128550 | Dec 2020 | US |
Number | Date | Country | |
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Parent | 17552674 | Dec 2021 | US |
Child | 18507428 | US |