The present disclosure relates generally to communication antenna systems, and relates more specifically to dual-polarized antenna elements and antenna arrays with parasitic elements having improved port-to-port isolation and broadened impedance bandwidth.
Additional spectrum bands have been released in recent years, and cellular operators have been deploying new radio access technologies to meet subscriber traffic demands. An antenna system at a base station site may support multiple bands operating over a very large bandwidth (e.g. 617-960 MHz, 1427-2690 MHz). The antenna system may also be preferred to have desired radiation properties and diversity performance, with good port-to-port isolation. Dual-polarized antenna elements which have two independent RF ports on the same antenna structure are widely used in mobile communications since the two orthogonal polarized elements are co-located without space penalties and also provide a means for polarization diversity to the radio.
In one example, the present disclosure describes an antenna system that includes at least one dual-polarized antenna element, the at least one dual-polarized antenna element comprising a first dipole and a second dipole which are in a same lateral plane, the first dipole comprising a first dipole arm and a second dipole arm, the second dipole comprising a third dipole arm and a fourth dipole arm, the first dipole being co-located with the second dipole, and the first dipole having an orthogonal polarization to the second dipole. The antenna system may further include a plurality of parasitic elements, each parasitic element comprising at least two branches, the at least two branches including a first branch and a second branch oriented at an angle and forming an apex. In one example, a first branch of a first parasitic element of the plurality of parasitic elements is positioned at a first coupling distance and parallel to the first dipole arm of the first dipole. In addition, a second branch of the first parasitic element may be positioned at a second coupling distance and parallel to the third dipole arm of the second dipole.
In one example, the present disclosure also describes a parasitic element comprising at least two branches, the at least two branches including a first branch and a second branch oriented at an angle and forming an apex. In one example, the parasitic element is for deployment as one of a plurality of parasitic elements for at least one dual-polarized antenna element comprising a first dipole and a second dipole which are in a same lateral plane, the first dipole comprising a first dipole arm and a second dipole arm, the second dipole comprising a third dipole arm and a fourth dipole arm, the first dipole being co-located with the second dipole, and the first dipole being orthogonally polarized to the second dipole. In one example, the first branch of the parasitic element is for positioning at a first coupling distance and parallel to the first dipole arm of the first dipole and the second branch of the parasitic element is for positioning at a second coupling distance and parallel to the third dipole arm of the second dipole.
The teaching of the present disclosure can be readily understood by considering the following detailed description in conjunction with the accompanying drawings, in which:
To facilitate understanding, identical reference numerals have been used, where possible, to designate identical elements that are common to the figures.
Examples of the present disclosure describe a technique to improve the port-to-port isolation and broaden the impedance bandwidth of a dual-polarized antenna element, such as a cross-dipole antenna element. A parasitic element is added between the radiating elements (e.g., the driven dipoles) of a dual-polarized antenna element to provide an orthogonal radio frequency (RF) current cancellation. This results in an improved isolation across a large bandwidth of the dual-polarized antenna element. Concurrently the parasitic element also generates an additional resonance mode, which couples into the main radiating elements to broaden the operating bandwidth.
As used herein, the terms “antenna” and “antenna array” may be used interchangeably. For consistency, and unless otherwise specifically noted, with respect to any of the antenna arrays depicted the real-world horizon is indicated as left-to-right/right-to-left on the page, and the up/vertical direction is in a direction from the bottom of the page to the top of the page consistent with the text/numerals of the figure.
It should also be noted that although the terms, “first,” “second,” “third,” etc., may be used herein, these terms are intended as labels only. Thus, the use of a term such as “third” in one example does not necessarily imply that the example must in every case include a “first” and/or a “second” of a similar item. In other words, the use of the terms “first,” “second,” “third,” and “fourth,” do not imply a particular number of those items corresponding to those numerical values. In addition, the use of the term “third” for example, does not imply a specific sequence or temporal relationship with respect to a “first” and/or a “second” of a particular type of item, unless otherwise indicated.
Additional spectrum bands have been released in recent years, and cellular operators have been deploying new radio access technologies to meet subscriber traffic demands. An antenna system at a base station site may support multiple bands operating over a very large bandwidth (e.g. 617-960 MHz, 1427-2690 MHz). The antenna system may also be preferred to have desired radiation properties and diversity performance, with good port-to-port isolation. Dual-polarized antenna elements which have two independent RF ports on the same antenna structure are widely used in mobile communications since the two orthogonal polarized elements are co-located without space penalties and also provide a means for polarization diversity to the radio.
The LB dual-polarized antenna element 101 may comprise a radiating element 101A such as a dipole which has a slant polarization at +45 degrees and an orthogonally polarized radiating element 101B which has a slant polarization at −45 degrees. Each of the LB dual-polarized antenna elements 1101-110N are distributed along the length of the reflector 102 at a prescribed pitch that is tuned to optimize for directivity, elevation radiation main beam tilt range and elevation radiation pattern sidelobe performance. Each dual-polarized antenna element 103 of the first HB dual-polarized antenna array 107 also comprises +45 degree polarized and −45 degree polarized radiating elements 103A and 103B respectively. Each dual-polarized antenna element 104 of the second HB dual-polarized antenna array 108 also comprises +45 degree polarized and −45 degree polarized radiating elements 104A and 104B, respectively. Due to this arrangement, the reflector width of the antenna may be broadened to accommodate all these elements. However, the proximity of the elements may still create additional mutual coupling effects causing corruption to radiation patterns, poorer port-to-port isolation, and reduced impedance bandwidth.
A first dipole 203 (or “dipole antenna”) as shown in
Additionally, each dipole 203 and 205 only resonates at a single frequency F1 due to its physical length generating a single current path, e.g., current path 207 as shown in
Dual-polarized antenna elements can be designed for optimal (i.e., low to zero) radiated cross-polar components or for optimal (i.e., large) bandwidth. These two design goals are often in conflict with one another. A wideband dual-polarized antenna element using bow-tie dipoles may generate larger radiated cross-polar components, whereas a dual-polarized antenna element using dipoles may provide small radiated cross-polar components but may remain relatively narrowband. This is because the physical dimensions of the feeds and dipoles/radiating elements do not scale with frequency to provide consistent optimal radiated behaviour.
In order to achieve good port-to-port isolation and improved cross polarization level while maintaining wider bandwidths, antenna designs may use aperture-coupled feeds or a feed capacitive coupling method to minimize parasitic inductive effects of an antenna launch probe (e.g., a physical feed line coupled to a radiating element via a solder joint or the like, or a parasitic coupling without physical contact) to give larger bandwidth. In another example, multiple feed ports may be used to drive the same antenna element with inverted phase to cancel out the parasitic current magnitude that contributes to radiated cross-polar power. Reducing the number of feed ports and complexity of the feed network may improve port-to-port isolation. However, it may require specific phasing techniques to ensure that all elements are radiating coherently.
Examples of the present disclosure enhance the impedance bandwidth of the single resonance dipole (or dipole antenna), and also generate an orthogonal current path that allows a vector cancelation of cross-polar power in a dual-polarized antenna element deployment, providing improved radiation pattern performance, port-to-port isolation (e.g., between RF ports feeding orthogonal polarization radiating elements of a dual-polarized antenna element and/or antenna array), and simplified implementation without the complication of multiple feeds.
In
The four parasitic elements 302A, 302B, 302C, 302D as shown in
The unit cell configuration 507i is a complex RF environment where in-band isolation of the LB and HB dual-polarized antenna elements can be degraded due to mutual coupling of the antenna elements. In one example, isolation may be maximized by arranging the HB dual-polarized antenna elements 503, 504, 505 and 506 at equal distances from a respective LB dual-polarized antenna element 301 as defined by the distance D591 along the length 508 of the reflector 510, and distance D592 along the width 509 of the reflector 510. This implies that distances D591 and D592 are equal, from the center of the LB dual-polarized antenna element 301 to the center of each of the HB dual-polarized antenna elements 503, 504, 505, and 506.
However, in many base station antennas which have a unit cell configuration of one LB and four HB dual-polarized antenna elements as described above, the separation distances D591 and D592 are not equal. In general, when D591 is larger than D592, grating lobes in the elevation radiation plane appear at shallower elevation beam tilt angles. The distance for D592 may be limited to the reflector width size that is available for the HB dual-polarized antenna elements 503, 504, 505, and 506 placed on the left and right side of the LB dual-polarized antenna element 301. The HB dual-polarized antenna elements 503, 504, 505, and 506 may be placed as far away as possible from the LB dual-polarized antenna element 301 to reduce shadowing effects from the larger LB component dipoles and to minimize mutual interactions. Unequal separation distances D591 and D592 may therefore cause an unbalanced RF environment, resulting in less port-to-port isolation and/or cross-polar isolation in the LB dual-polarized antenna element 301. To recover a symmetric RF environment, the parasitic elements 302A, 302B, 302C, 302D shown on the LB dual-polarized antenna element 301 in unit cell 507N can be adjusted independently to the best position. For example, parasitic elements 302B and 302D can be separated at a distance 314B which is not equal to the separation of the parasitic elements 302A and 302C at a distance of 314A. The imbalanced separation distances of the parasitic elements 302A and/or 302C, and 302B and/or 302D around the LB dual-polarized antenna element 301 may offset the imbalance of the HB dual-polarized antenna element separation distances D591 and D592. This results in improved antenna performance. It should also be noted that in various examples, separation distances 314A and 314C can be also be different, and likewise for D591 and D592.
It should be noted that examples of the present disclosure describe the use of +45/−45 degree slant linear polarizations. However, although linear polarization is typical, and examples are given using linear polarizations, other embodiments of the present disclosure can be readily arrived at, for example including dual-orthogonal elliptical polarization, or left hand circular and right hand circular polarizations, as will be appreciated by those skilled in the art.
While the foregoing describes various examples in accordance with one or more aspects of the present disclosure, other and further example(s) in accordance with the one or more aspects of the present disclosure may be devised without departing from the scope thereof, which is determined by the claim(s) that follow and equivalents thereof.
This application claims priority to U.S. Provisional Patent Application Ser. No. 62/714,421, filed Aug. 3, 2018, which is herein incorporated by reference in its entirety.
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62714421 | Aug 2018 | US |