BACKGROUND OF THE INVENTION
This application is a non-provisional of Application Ser. No. 63/075,394, filed Sep. 8, 2020, pending, which application is hereby incorporated by this reference in its entirety.
FIELD OF THE INVENTION
The present invention relates to wireless communications, and more particularly, to antennas that incorporate multiple dipole arrangements in several frequency bands.
RELATED ART
The introduction of new spectrum for cellular communications presents challenges for antenna designers. In addition to the traditional low band (LB) and mid band (MB) frequency regimes (617-894 MHz and 1695-2690 MHz, respectively), the introduction of C-Band and CBRS (Citizens Broadband Radio Service) provides additional spectrum of 3.4-4.2 GHz. Further, there is demand for enhanced performance in the C-Band, including 4×4 MIMO (Multiple Input Multiple Output as well as 8T8R (8-port Transmit, 8-port Receive) with beamforming.
The higher frequencies of C-Band allow the implementation of proportionately smaller dipoles within the antenna, and thus creating beamforming arrays within a conventional macro antenna, e.g., four rows of C-Band dipole columns in the case of an 8T8R array. Implementing beamforming and beam steering in the azimuth direction, as is required for 8T8R beamforming, places strenuous performance requirements on the C-Band dipoles themselves. This is because performance deficiencies in a given dipole or radiator assembly multiply when combining radiator assemblies into an 8T8R array. For example, the C-Band dipoles are susceptible to cross polarization, in which the energy radiated by the dipole and/or balun structure of one polarization (e.g., +45 degrees) may cause excitation in the dipole and/or balun structure of the opposite polarization (e.g., −45 degrees) in the same radiator assembly. A cross polarization contamination of 15 dB can severely degrade the gain of a C-Band 8T8R array, affect MIMO performance, and cause leakage between transmit array and the receive array. Further, proper beamforming (e.g., without grating lobes) requires adjacent dipoles be spaced roughly 0.52 apart. With conventional half-λ dipole structures, it becomes difficult to place the dipoles accordingly because the dipole structures either abut or otherwise cannot be spaced close enough without their structures physically interfering with each other or causing coupling between adjacent radiators. Third, as the dipoles get smaller (in the case of C-Band, a problem may arise with the balun structures whereby balun re-radiation may cause dipole arm excitation asymmetry.
Accordingly, what is needed is a dipole structure for high frequencies (e.g., C-Band) that does not suffer from cross polarization interference and dipole arm excitation asymmetry, and is able to be packed together in close proximity to other dipoles to enable beamforming without incurring grating lobes.
SUMMARY OF THE DISCLOSURE
An aspect of the present disclosure involves a radiator assembly configured to radiate two orthogonally polarized radio frequency signals. The radiator assembly comprises a folded dipole having first pair of dipole arms configured to radiate in a first polarization orientation and a second pair of dipole arms configured to radiate in a second polarization orientation, wherein the folded dipole is formed of a single conductive plate; and a balun stem mechanically couled to the folded dipole, the balun stem having a first balun stem plate configured to couple a first radio frequency signal to the first pair of dipole arms and a second balun stem plate configured to couple a second radio frequency signal to the second pair of dipole arms.
BRIEF DESCRIPTION OF THE DRAWINGS
The accompanying figures, which are incorporated herein and form part of the specification, illustrate embodiments of high performance folded dipole for multiband antennas. Together with the description, the figures further serve to explain the principles of the High performance folded dipole for multiband antennas described herein and thereby enable a person skilled in the pertinent art to make and use the high performance folded dipole for multiband antennas
FIG. 1A illustrates an exemplary array face of multiband antenna according to the disclosure.
FIG. 1B illustrates an exemplary smaller array face, or portion of a larger array face, including a C-Band 8T8R beamforming array, according to the disclosure.
FIG. 1C illustrates an exemplary C-Band 8T8R beamforming array according to the disclosure.
FIG. 2A illustrates an exemplary C-Band radiator assembly according to the disclosure.
FIG. 2B is another view of the exemplary C-Band radiator assembly according to the disclosure.
FIG. 3A illustrates an exemplary folded dipole according to the disclosure.
FIG. 3B illustrates an example of current flow through the folded dipole of FIG. 3A.
FIG. 4A illustrates an exemplary first balun trace and ground pattern disposed on a first balun stem plate according to the disclosure.
FIG. 4B illustrates an opposite side of the first balun stem plate.
FIG. 4C illustrates an exemplary second balun trace and ground pattern disposed on a second balun stem plate according to the disclosure.
FIG. 4D illustrates an opposite side of the second balun stem plate.
FIG. 5 illustrates another exemplary folded dipole for providing high performance in both the CBRS bands and the C-Band, according to the disclosure.
FIG. 6 illustrates an exemplary array face, or portion of a larger array face, having a CBRS array and a plurality of mid band radiators according to the disclosure.
DESCRIPTION OF EXEMPLARY EMBODIMENTS
Accordingly, the present invention is directed to high performance folded dipole for multiband antennas that obviates one or more of the problems due to limitations and disadvantages of the related art.
FIG. 1A illustrates an exemplary multiband antenna array face 100a according to the disclosure. Array face 100a has a reflector 102, on which are disposed a plurality of low band radiators 105, mid band radiators 110, and upper band radiators 120, which are disposed in an 8T8R beamforming array 115. In this example, the upper band radiators are C-Band radiators, which may have extended coverage to include CBRS for a total range of 3.4-4.2 GHz. In this case upper band radiators 120 may be referred to as C-Band radiators 120, as a particular example.
Typical deployment of multiband antenna having array face 100a is such that it is mounted vertically, with its elevation axis (illustrated in FIG. 1A) in the vertical direction.
FIG. 1B illustrates exemplary smaller array face 100b, which may be a portion of a larger array face, according to the disclosure. Smaller array face 100b includes a C-Band 8T8R beamforming array 115, which may be similar or identical to the C-Band 8T8R beamforming array 115 of FIG. 1A. Also disposed on the radiator 102 of smaller array face 100b is a plurality of mid band radiators 110 and low band radiator 105 that are in close proximity to C-Band 8T8R beamforming array 115.
FIG. 1C illustrates a C-Band 8T8R beamforming array 115 according to the disclosure. C-Band 8T8R beamforming array 115 has a plurality of C-Band radiators 120, arranged in four columns 125. Each column 125 of C-Band radiators 120 may be coupled to a respective pair of ports (not shown) so that each C-Band radiator 120 may operate independently at two different polarization orientations, e.g., +/−45 degrees. Each C-Band radiator 120 in a given column 125 may radiate the same two signals (one per polarization) and thus may share a single pair of ports. The columns 125 may be oriented vertically along the elevation axis as shown, and each column 125 may be placed side-by-side along the azimuth axis. As illustrated in FIG. 1B, each column 125 may have ten C-Band radiators spaced linearly along the elevation axis. Further, more or fewer C-Band radiators 125 may be present within each of the columns 125.
As mentioned above, in accordance with 8T8R operation, each column 125 is provided two ports, one per +/−45 degree polarization. Accordingly, it is possible to perform beamforming in the azimuth direction (i.e., around the elevation axis) by providing a single RF signal to the four columns 125, but with differential amplitude an phase weighting to each of the columns 125 to provide beamforming and scanning of the formed beam, as is described further below. For beamforming or beamsteering in the elevation direction (i.e., around the azimuth axis), a phase shifter (not shown) may be used to provide differential phasing (and potentially differential amplitude and phase weighting) to each of the C-Band radiators 120 within a given column 120. The phase shifter may provide differential phasing individually to each C-Band radiator 120 along the elevation axis, or may be provided in clusters (e.g., each adjacent pair of C-Band radiators 120 are given the same phasing, etc.). It will be understood that such variations are possible and within the scope of the disclosure.
In order to provide beamforming without the contamination of grating lobes, it is required that the C-Band radiators 120 be spaced apart at a distance equal to a fraction of the center wavelength of the band in which the radiator operates. Illustrated in FIG. 1C are two types of spacing: center-to-center spacing 150, and interdipole gap spacing 155. In the case of the C-Band, a center frequency may be 4 GHz, and the center-to-center spacing 150 between adjacent C-Band radiators 120 may be 0.58λ, where λ is the wavelength corresponding to the 4 GHz center frequency. Given these parameters, the spacing of each C-Band radiator 120 may be 43.5 mm. This requirement presents a challenge in that if the outer edges of dipoles of adjacent C-Band radiators 120 get sufficiently close. In other words, if their interdipole gap spacing 155 becomes too small, it may lead to cross coupling between the neighboring C-Band radiators 120, severely degrading the performance of the C-Band 8T8R beamforming array 115. Accordingly, each C-Band radiator 120 should be designed such that it is as small as possible while maintaining sufficient gain, without incurring cross polarization contamination.
FIGS. 2A and 2B illustrate an exemplary C-Band radiator 120, each from a different angle. Illustrated in both is a folded dipole 205 disposed on a balun stem 210. FIG. 2B further illustrates a balun trace 225a, which has a counterpart balun trace 225b (not shown), each of which provides a signal for its respective polarization; and a pair of mounting tabs 235. Balun stem 210 may suspend folded dipole 205 from reflector 102 by a distance h. In the case of exemplary C-Band radiator 120, the distance h may be 13 mm. The height h may be predetermined by the design of balun trace 225a and 225b, whereby the balun trace may have a meander structure that defines the length of the signal path to control the phases of the signals imparted to the crossed arms folded dipole 205. This is described in further detail below.
FIG. 3A illustrates an exemplary folded dipole 205. Folded dipole 205 may be formed of a single piece of stamped metal that is disposed on a PCB substrate 302. In an exemplary embodiment, folded dipole 205 may be formed of 1.4 mil thick Copper, disposed on an FR4 PCB. Folded dipole 205 may have four dipole arms 305a, 305b, 305c, and 305d. Dipole arms 305a and 305b are disposed diagonally to each other and coupled to the same RF signal via a single balun structure (not shown in FIG. 3); and dipole arms 305c and 305d are disposed diagonally to each other and coupled to the same RF signal (different from the RF signal coupled to dipole arms 305a/b) via a single balun structure (not shown in FIG. 3). Each adjacent pair of dipole arms 305a/b/c/d are coupled by a connecting trace 312 that is spaced from its corresponding coupled dipole arms by a gap 310. Each dipole arm 305a/b/c/d further includes a current channel aperture 335 and a current channel slot 315. Each current channel slot 315 engages its respective dipole arm 305a/b/c/d with its corresponding feed contacts. For example, dipole arm 305a is directly coupled to feed contact 230a; dipole arm 305b is directly coupled to feed contact 232a; dipole arm 305c is directly coupled to feed contact 232b; and dipole arm 305d is directly coupled to feed contact 230b. These connections are described further below with regard to FIGS. 4A-D.
Folded dipole 205 may formed in a 30.2×30.2 mm square. This offers the advantage of close spacing (e.g., at 0.58λ) to enable high quality beamforming with the adjacent folded dipoles 205 being sufficiently spaced apart to prevent coupling between them.
Folded dipole 205 operation may be described as follows. Referring to FIGS. 3B and 3A, a single RF signal is fed, via balun stem plate 210a (not shown) such that the signals present at feed contact 230a and 232a are ideally equal and 180 degrees out of phase from each other. This causes current flow 350a, channeled by corresponding current channel aperture 335, current channel slot 315, and gaps 310, through dipole arm 305a and respective connecting traces 312; and it causes current flow 350b, channeled by corresponding current channel aperture 335, current channel slot 315, and gaps 310, through dipole arm 305b and respective connecting traces 312. The superposition of current flows 350a and 350b results in an electromagnetic propagation along a plane diagonal to dipole 205 and defined by the axis of symmetry formed by the geometries of dipole arms 305a and 305b. The channeling of current imparted by the structure of dipole arms 305a/b, and their respective current channel apertures 335, current channel slots 315, and gaps 310, causes the field components perpendicular to the polarization axis to cancel. This results in an RF signal being radiated along the diagonal axis of symmetry (e.g., +45 degrees) with minimal cross polarized energy. The same but conjugate process occurs with current flows 350b and 350c respectively flowing through dipole arms 305c and 305d, channeled by their respective current channel apertures 335, current channel slots 315, and gaps 310. In this case, a single RF signal is coupled to dipole arms 305c and 305d, respectively by feed contacts 230b and 232b, whereby the signals present at feed contacts 230b and 232b are equal and 180 degrees out of phase.
FIGS. 4A and 4B illustrate opposite sides of exemplary balun stem plate 210a according to the disclosure. As illustrated in both FIGS. 4A and 4B, balun stem plate 210a has the following structural elements: mounting tabs 235 that mechanically engage with the slots 315 of dipole arms 305a and 305b; reflector mounting tabs 410a and 410b that mechanically engage with a base plate or reflector 102; and a coupling slot 405a that mechanically engages with balun stem plate 210b.
FIG. 4A illustrates the side of balun stem plate 210a having balun trace 225a, which directly couples to ground element 227a. Ground element 227a includes feed contact 230a, which couples to dipole arm 305a, and ground contact 240a, which couples to a ground plane (not shown) of reflector 102. Unlike conventional balun stem configurations, which have a “J-hook” balun trace that capacitively couples to a ground plane on the opposite side of the balun stem plate, balun trace 225a directly couples to the ground element 227a that is disposed on the same side of balun stem plate 210a. The shape and length of balun trace 225a may be designed so that the phase difference between the signal imparted to dipole arm 305a and 305b. Further, balun trace 225 may be designed with a meander structure to maintain phase length and enable the shortening the balun stem plate 210a (and thus balun stem 210). A shorter balun stem 210 (illustrated by height h in FIG. 2B) enables dipole 205 to be disposed closer to reflector 102. In an exemplary embodiment, height h may be 13 mm Having an appropriate low height h, such as 13 mm, prevents re-radiation of energy from mid band radiators 110, effectively cloaking the conductors in balun stem 210 from the mid band radiators 110. Further, an appropriately low height h, given its proximity to reflector 102, enables each C-Band radiator 120 to project energy in a gain pattern that approximates a 90 degree lobe. This offers considerable performance improvement, because having a baseline 90 degree lobe gain pattern for individual radiator assemblies 120 enables better beamforming for creating 45 degree broadcast beam; 65 degree broadcast beam; a scanned service beam; or operating in a “soft split” mode, in which one 65 degree beam can be split into two 33 degree beams for increasing network capacity.
FIG. 4B illustrates the opposite side of balun stem plate 210a. Disposed on this side of balun stem plate 210a is a second ground element 229a, which is disposed on balun stem plate 210a opposite balun trace 225a. Second ground element 229a has a feed contact 232a, which couples to dipole arm 305b. Feed contact 232a is disposed on the mounting tab 235 that mechanically couples with dipole arm 305b via its corresponding slot 330.
The design and arrangement of balun trace 225a, the direct coupling of balun trace 225a to ground element 227a on the same side of balun stem plate 210a, and capacitive coupling of balun trace 225a to second ground element 220a, combine to provide more linear coupling of the RF signal fed to balun trace 225a to dipole arms 305a and 305b. A further advantage is that this design provides for a more precise 180 degree phase differentiation between the signals imparted to the two dipole arms 305a and 305b. Improving the phase between dipole arms 305a and 305b further mitigates cross polarization between the signals radiated by dipole arms 305a/b and 305c/d. These advantages of this design apply across the C-Band frequencies.
FIG. 4C illustrates the side of balun stem plate 210b having balun trace 225b, which directly couples to ground element 227b. Ground element 227b includes feed contact 230b, which couples to dipole arm 305c, and ground contact 240b, which couples to a ground plane (not shown) of reflector 102. Balun trace 225b and its direct connection to ground element 227b, both of which are disposed on the same side of balun stem plate 210b, are substantially similar to the counterpart components on balun stem plate 225a. A difference between balun stem plate 210b and 210a is that the coupling slot 405b is disposed on the side of balun stem plate 210b that faces the folded dipole 205. This enables balun stem plate 210a to mechanically engage balun stem plate 210b via their respective coupling slots 405a/b, forming a balun stem 210 having a cruciform shape. The location of coupling slot 405b in balun stem plate 210b requires balun trace 225b to take a different path to accommodate it. The modified design of balun trace 225b and ground element 227b may be done, as illustrated in FIG. 4C, so that the same advantages in phase precision, linearity, and reduced cross polarization apply to dipole arms 305b/c as they do for dipole arms 305a/b.
FIG. 5 illustrates another exemplary folded dipole 500, which has improved performance in the CBRS range (3.55-3.7 GHz) of the C-Band (3.4-4.2 GHz). Folded dipole 500 has four dipole arms 505a-d, wherein adjacent dipole arms are coupled by a connecting trace 512, which is separated from the body of each corresponding dipole arm 505a-d by a gap 510. Each dipole arm 505a-d has a current channel aperture 530, which may direct current densities within the dipole arm 505a-d in a manner similar to the combination of current channel aperture 335 and current channel slot 315 of dipole arms 305a-d. Folded dipole 500 may have a square shape with dimensions of 29.39 mm×29.39 mm and may operate with a conventional J-hook balun.
FIG. 6 illustrates an exemplary array face 600, which may be a portion of a larger array face, according to the disclosure. Array face 600 has a plurality of CBRS radiator assemblies 605, each of which having exemplar While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. It will be apparent to persons skilled in the relevant art that various changes in form and detail can be made therein without departing from the spirit and scope of the present invention. Thus, the breadth and scope of the present invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
y folded dipole 500. The CBRS radiator assemblies 605 may be arranged so that the center-to-center spacing of folded dipoles 500 is 50 mm, which offers good isolation. Array face 600 may also have a plurality of mid band radiators 110, which may be substantially similar to the mid band radiators 110 of exemplary array face 100a.
While various embodiments of the present invention have been described above, it should be understood that they have been presented by way of example only, and not limitation. It will be apparent to persons skilled in the relevant art that various changes in form and detail can be made therein without departing from the spirit and scope of the present invention. Thus, the breadth and scope of the present invention should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
Patent Grant
11581660
