The present invention relates to wireless communications, and more particularly to cellular antennas that provide beam forming and MIMO (Multi Input-Multi Output) in higher frequency bands.
The advent of new high frequency bands for use in cellular communications brings both opportunities and technical challenges. 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. The smaller sizes of individual radiators (corresponding to higher frequencies) of CBRS and the C-Band enables the construction of array faces within traditional cellular macro antennas that facilitate features such as 4×4 MIMO (Multiple Input Multiple Output) and 8T8R (8-port Transmit, 8-port Receive) with beamforming.
A challenge arises in implementing 8T8R beamforming and 4×4 MIMO within an antenna in that the performance of these featured depends greatly on phase coherence between the signals on the ports. Any phase mismatch can seriously degrade the performance of the antenna. For example, a phase mismatch is introduced to one of the port signals can impart an insertion loss to the signals provided to the antenna radiators. This not only decreases the efficiency of the antenna but also degrades the quality of the gain pattern intended by the beamforming weights applied to the different columns of radiators. This challenge becomes exacerbated with higher frequencies in that minor phase mismatches due to cable length differences within the antenna. For example, in the C-Band, a 1 mm difference in cable length can impart a 10 degree phase mismatch between signals. Further, these phase errors due to cable length mismatches are cumulative with each set of cables introduced into the signal paths. Given that the precision of typical cable cutting machines is around +/−0.5 mm, these errors can compound. Further, for conventional antennas, the cables for each given port may be of different length, which not only complicates the manufacturing process and increases manufacturing costs, but also introduces more risk in phase mismatches from improper cable allocation that can lead to lack of performance consistencies.
Accordingly, what is needed is an integrated antenna calibration and phase shifter board that compensates for phase differences, that reduces the number of cables required in the signal path of each signal port, and simplifies manufacturing by enabling cables of identical length across multiple ports' signal paths.
An aspect of the present disclosure involves an antenna. The antenna comprises a plurality of radiator columns, each radiator column having a plurality of radiator clusters; a phase shifter/calibration board having a plurality input ports and a plurality of phase shifters, each of the plurality of phase shifters is coupled to a corresponding input port via an input trace, each input trace is capacitively coupled to provide a representative power signal to one of a plurality of power dividers, wherein each phase shifter has a plurality of phase shifter output traces having an output port, each of the output ports is coupled to a corresponding radiator cluster of a corresponding radiator column, wherein a subset of the plurality of phase shifter output traces have a designated meander pattern that collectively provides phase matching between the output ports, wherein the plurality of power dividers sums the plurality of representative power signals into a single calibration signal; and a plurality of RF cables, each of the plurality of RF cables couples a given phase shifter output port to its corresponding radiator cluster of its corresponding radiator column, wherein the plurality of RF cables have the same length.
In this example, each radiator column 105w-z has ten crossed radiator pairs 102 that are divided into five clusters of two radiator pairs. Each cluster of two radiator pairs 102 has two signal feeds, one per polarization. Each cluster of two radiator pairs 102 may have, for each polarization, a signal splitter (not shown) that splits the RF signal from each of the two signal feeds to two balun circuits (not shown) for each polarization. Each balun circuit is disposed on a balun stem (not shown) that supports the dipoles 110 of the corresponding radiator pair 102. The signal feeds to each cluster of two radiator pairs 102 are coupled to outputs of phase shifters, as described below.
Phase/calibration board 135 has a plurality of phase shifters PS1-PS8, each of which correspond to a single set of dipoles 110a-h corresponding to a given polarization within a given radiator column 105w-z. For example, phase shifter PS1 has a signal input port 120a. Phase shifter PS1 may further have five output signal feeds: feed 115a that corresponds to the reference port (no phase shift imparted by phase shifter PS1) to the dipoles 110a of the center cluster of two radiator pairs 102 within radiator column 105w; feed 116a that corresponds to a first output of phase shifter PS1 that imparts a first phase shift to the signal from input port 120a that gets fed to the dipoles 110a of the cluster of two radiator pairs 102 distal and adjacent to the center cluster; feed 117a that corresponds to a second output of phase shifter PS1 that imparts a second phase shift to the signal from input port 120a that gets fed to the dipoles 110a of the cluster of two radiator pairs 102 at the distal end of radiator column 105w; feed 118a that corresponds to a third output of phase shifter PS1 that imparts a third phase shift to the signal from input port 120a that gets fed to the dipoles 110a of the cluster of two radiator pairs 102 proximal and adjacent to the center cluster; and feed 119a that corresponds to a fourth output of phase shifter PS1 that imparts a fourth phase shift to the signal from input port 120a that gets fed to the dipoles 110a of the cluster of two radiator pairs 102 at the proximal end of radiator column 105w.
Similarly, phase shifter PS2 has a signal input port 120b and five signal feeds 115b-119b, which provide signals to the dipoles 110b of the corresponding clusters of radiator pairs according to a signal connection similar to that of phase shifter 120a but for the orthogonal polarization within the same radiator column 105w. It will be understood that signal input ports 120a and 120b may corresponding to distinct and independent signals. It will also be understood that the connections of signal feeds 115b-119b, with their corresponding phases imparted by corresponding phase shifter PS2, may be similar as described above with respect to phase shifter PS1 and dipoles 110a.
Phase shifters PS3 and PS4 may be coupled to respective dipoles 110c and 110d of radiator column 105x in a manner similar to that described with respect to phase shifters PS1 and PS2 and radiator column 105w; phase shifters PS5 and PS6 may be coupled to respective dipoles 110e and 110f of radiator column 105y in a manner similar to that described with respect to phase shifters PS1 and PS2 and radiator column 105w; and phase shifters PS7 and PS8 may be coupled to respective dipoles 110g and 110h of radiator column 105z in a similar corresponding manner.
Having different clusters of dipoles 110a-h within a given radiator column 105w-z fed with signals such that each cluster's signal has a different phase shift imparted by corresponding phase shifter PS1-8 enables independent beam pointing of each signal input 120a-h along an axis parallel to the axis of radiator columns 105w-z according to conventional Remote Electrical Tilt methods.
Each of the phase shifters PS1-8 are coupled to the calibration segment 130 of phase/calibration board 135. Calibration segment 130, in addition to being coupled to each of the input signal ports 120a-h, provides a calibration output port 140 and a Bias-T port 145, which are described in further detail below.
Accordingly, each coupling point 220a-h provides the Wilkinson power divider 210 a copy of the signal present at input traces 215a-h with a 26 dB drop. In doing so, each signal at the input signal ports 120a-h are tapped (uniformly attenuated by 26 dB) in such a way that minimal signal power is extracted from the signals to be fed to radiator columns 105w-z. As illustrated, each successive Wilkinson power divider 210 sums the detected signal power tapped from input traces 215a-h, and the arrangement of cascaded Wilkinson power dividers 210 sums the power of tapped signals from input traces 215a-h according to the following combination: (((215a+215b)+(215c+215d))+((215e+215f)+(215g+215h))). The output of the apex Wilkinson Power Divider 210, which is coupled to calibration output port 140, is the summed signal power according to this relation.
In keeping with Wilkinson power divider theory, the signal of calibration trace 309 corresponding to input trace 215a (for example) is summed with the signal of calibration trace 309 corresponding to input trace 215b. Both calibration traces 309 are input to corresponding Wilkinson power divider 210 with a loss of −3 dB (half power) at each input port. Accordingly, given that the two signals are summed at the output of the Wilkinson power divider 210, the half-power losses at the input ports are restored by the summing of the two signals into a single output. This lossless operation, however, depends on the two signals at calibration traces 309 (and thus at input traces 215a and 215b) are equal in magnitude and phase. The lossless nature of operation of the Wilkinson power divider 210 applies for each level of their cascading topology. Accordingly, signal at calibration port 140 is a lossless combination of a 26 dB dropped representation of the signals at input traces 215a-h (and thus input ports 120a-h), assuming that all of the signals at input ports 120a-h are of equal magnitude and phase. However, if one or more of the signals at input ports 120a-h experiences a phase mismatch to the others, the cascaded Wilkinson power dividers in the summation path of the cascade topology are no longer lossless, and the signal level at calibration output port 140 will drop. Accordingly, a signal drop beyond 2 dB below the expected 26 dB drop may indicate a phase mismatch at one or more input port 120a-h.
Any phase mismatch between the signals at input ports 120a-h will result in a beamforming error. For example, a phase mismatch might be due to an RF cable carrying one of the input signals 120a-h being replaced by one having a different length. Regardless of how imparted, a phase mismatch leads to an increase in insertion loss at the relevant input trace 215a-h, which in turn leads to a drop in power at calibration output port 140. Another example might be the failure of one of the phase shifters PS1-8. This also would result in a drop in signal at the corresponding input trace 215a-h, which would in turn lead to a reduction of signal power at calibration output port 140.
A network operator or neutral host may deploy equipment that monitors signal power at calibration output port 140. If the signal power at calibration output port 140 drops below a predetermined threshold (indicating a phase mismatch or malfunction in the RF path of one of the input signals 120a-h) the operator or neutral host may either increase the power at a suspect mismatched input signal 120a-h or change the phase of a suspect mismatched input signal 120a-h. Either actions compensates for insertion loss.
Phase/calibration board 135 further includes a Bias-T circuit 225 with Bias-T output port 145. Bias-T circuit 225 filters out the sinusoidal components of the signal present at calibration output port 140 to provide a DC voltage output at Bias-T output port 145. This DC voltage may be used by components within the antenna in which array face 100 is integrated. For example, the DC voltage from Bias-T output port 145 may be used to power the Remote Electrical Tilt (RET) motors that drive the phase shifter wiper arms 207.
In addition to reference port trace 315, phase shifter/calibration signal path 300 has four output traces, each corresponding to signal outputs 116/117/118/119. For example, proximal end radiator cluster signal output 119 is coupled to output trace 319; and distal end radiator signal output 117 is coupled to output trace 317. Although output traces 319 and 317 may be formed of a single contiguous conductive trace, output trace 319 may be defined as beginning at the capacitive couple at phase shifter wiper arm 207 and extending in one direction; and output trace 317 may also be defined as beginning at the capacitive couple at phase shifter wiper arm 207 and extending in the opposite direction. Similarly, proximal inner radiator cluster signal output 118 is coupled to output trace 318; and distal inner radiator cluster signal output 116 is coupled to output trace 316. Further, although output traces 318 and 316 may be formed of a single contiguous conductive trace, output trace 318 may be defined as beginning at the capacitive couple at phase shifter wiper arm 207 and extending in one direction; and output trace 316 may also be defined as beginning at the capacitive couple at phase shifter wiper arm 207 and extending in the opposite direction.
Each output trace 315/316/317/318/319 may have a respective designated meander pattern that provides individual phase deltas. The individual phase deltas provide phase matching between signal outputs 115/116/117/118/119 to compensate for individual systemic phase mismatches. This enables the internal RF cables (not shown) between the phase shifters PS1-8 and radiator columns 105w-z to be formed of a single length, greatly simplifying the manufacture of the antenna. However, complications arise in providing meander patterns for output traces 315/316/317/318/319 due to possible coupling between meander features of a single output trace, as well as cross coupling between adjacent output traces.
For each output trace 315/316/317/318/319, phase matching control that minimizes internal coupling as well as cross coupling may involve tailored use of the following trace design features: number of meander turns 335; spacing of meander turns 322; width of meander turns 324, staggering of meander turns 335 for adjacent output traces; and length of chamfer 330. In the example illustrated in
The spacing of meander turns 322 should be sufficiently long to prevent coupling between parallel segments of the given individual output trace 315/316/317/318/319. If more phase delay is required, the width of meander turn 324 can be increased, but this may place the given output trace in sufficient proximity to an adjacent output trace to cause cross coupling. To mitigate this, the meander turns 335 of adjacent output traces may be staggered to reduce proximity. To further reduce the risk of cross coupling, chamfers 330 may be added at the corners of meander turns 335 to help maintain distance between adjacent output traces.
Each of the output traces 315/316/317/318/319 may be formed of 1.4 mil Copper on a printed circuit board. Given that trace etching precision may be +/−3 mil, this offers considerable precision in adjusting the differential phases of each output trace to mitigate phase mismatch, relative to the +/−0.5 mm precision in RF cable length. With the systemic phase mismatches compensated as described herein, each of the RF cables (not shown) between signal outputs 115/116/117/118/119 and their respective radiator pair clusters may be of the same length. This may significantly reduce the complexity and cost of manufacture of the antenna in which exemplary array face 100 is deployed while mitigating phase mismatches that lead to beamforming errors.
Accordingly, an antenna with exemplary array face 100 provides the following capabilities and advantages. First, phase alignment is critical in 8T8R scenarios in which all radiator columns are used to form a broadcast beam (one per polarization) that can be tilted, to form a service beam that can be scanned as well as tilted. It enables an operator to identify failure of one or more phase shifters as well as to identify and compensate for externally-induced phase mismatch (change in cable with one of a different length). Additionally, uniformity in phase is built into the antenna by the combination of higher integration and phase alignment via designated meander patterns, eliminating the need for certain cables between the phase shifter and the calibration board as well as enabling the use of RF cables of a single length to couple the phase shifters to the corresponding radiator clusters, thereby reducing cost as well as eliminating another source of potential detrimental phase deltas.
Filing Document | Filing Date | Country | Kind |
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PCT/US2021/051878 | 9/24/2021 | WO |
Number | Date | Country | |
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63084889 | Sep 2020 | US |