BACKGROUND OF THE INVENTION
Field of the Invention
The present invention relates to wireless communications, and more particularly, to compact multi-band antennas.
Related Art
The introduction of additional spectrum for cellular communications, such as the Citizens Broadband Radio Service (CBRS), opens up vast resources of additional capacity for existing cellular customers as well as new User Equipment (UE) types. New UE types include Internet of Things (IoT) devices, drones, and self-driving vehicles. Further, the advent of CBRS enables a whole new cellular communication paradigm in private networks.
Accommodating CBRS in existing LTE and 5G cellular networks requires enhancing antennas to operate in 3550-3700 MHz, in addition to LTE low band and (now mid) bands in the range of 700 MHz and 2.3 GHz, respectively. A challenge arises in integrating CBRS radiators into antennas designed to operate in the existing lower bands in that energy radiated by the CBRS radiators may cause resonances in the lower band radiators. A particular problem may arise in the low band radiators that are in close proximity to the CBRS radiators whereby the low band radiators may significantly degrade the performance of the antenna in the CBRS band. A conventional solution to this problem is to increase the area of the antenna array face to accommodate the new CBRS radiators. However, this may be impractical due to space constraints on the antennas.
Accordingly, what is needed is an array face configuration and low band radiator design that mitigates the low band interference problem while not increasing the area of the array face of the antenna.
SUMMARY OF THE INVENTION
An aspect of the present invention involves a multiband antenna. The multiband antenna comprises an array of high band radiators arranged in at least one column, the array of high band radiators having an outer high band radiator at each end of the array; a plurality of low band radiators, the low band radiators having at least one inward dipole arm and at least one outer dipole arm, wherein the at least one inward dipole arm has a structure that is different from an at least one outer dipole arm structure, and wherein an adjacent outer high band radiator is partly obstructed by the at least one inward dipole arm; and a plurality of mid band radiators, each of the mid band radiators having a mid band parasitic disk having a plurality of cloaking slots.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 illustrates an exemplary array face incorporating low band, mid band, and CBRS radiators in which standard low band radiators are deployed.
FIG. 2 illustrates the exemplary array face of FIG. 1, but with exemplary low band radiators and mid band radiators according to the disclosure.
FIG. 3A is a top-down view of an exemplary asymmetric low band radiator according to the disclosure.
FIG. 3B is another view of an exemplary asymmetric low band radiator according to the disclosure.
FIG. 4 is an alternate view of an exemplary array face incorporating an exemplary asymmetric low band radiator according to the disclosure as well as an exemplary mid band parasitic disk radiator according to the disclosure.
FIGS. 5A-D illustrate a first embodiment of a low-interference dipole arm of an exemplary asymmetric low band radiator according to the disclosure.
FIGS. 6A-D illustrate a second embodiment of a low-interference dipole arm of an exemplary asymmetric low band radiator according to the disclosure.
FIGS. 7A-D illustrate a third embodiment of a low-interference dipole arm of an exemplary asymmetric low band radiator according to the disclosure.
FIG. 8 illustrates a mid band radiator having an exemplary mid band parasitic disk according to the disclosure.
FIG. 9 illustrates a mid band parasitic disk according to the disclosure.
DESCRIPTION OF EXEMPLARY EMBODIMENTS
FIG. 1 illustrates an exemplary array face 100 incorporating low band radiators 105, mid band radiators 110, and CBRS or high band radiators 115. As illustrated, the CBRS radiators 115 are integrated into array face 100 to provide optimal performance in the CBRS bands, although the outer CBRS radiators of the cluster are partly obstructed by the inward-directed dipole arms of the low band radiators 105. This obstruction, or shadowing, effects the performance of the outer CBRS radiators 115, thereby corrupting the antenna's gain pattern in the CBRS bands.
FIG. 2 illustrates the exemplary array face 200 according to the disclosure. As illustrated, the placement of the radiators remains unchanged. Further illustrated are two asymmetric low band radiator 205 according to the disclosure. Each asymmetric low band radiator 205 has inward-directed dipole arms that mitigate obstruction or shadowing with the outer CBRS radiators 115. Further illustrated are exemplary mid band radiators 210 according to the disclosure.
FIGS. 3A and 3B are different views of an exemplary asymmetric low band radiator 205 according to the disclosure. Asymmetric low band radiator 205 has two outward-directed standard dipole arms 305 and two inward-directed dipole arms 310 that are designed to minimize interference with the CBRS radiators 115. Each inward-directed dipole arms 310 has a plurality of radiative segments 315 coupled by linking inductive segments 320. The inductive segments 320 both mechanically and electrically couple the radiative segments 315 together. The inductive segments 320 may point “downward”, orthogonally to the plane defined by the inward-directed dipole arms 310 and standard dipole arms 305 (hereinafter “radiator plane”). The radiative segments 315 and inductive segments 320 may be formed of a single piece of aluminum, although other materials may be used given sufficient conductivity and mechanical strength.
FIG. 4 is an alternate view of an exemplary array face 200 incorporating two exemplary asymmetric low band radiators 205 according to the disclosure and exemplary mid band radiators 210. As illustrated, the asymmetric low band radiators 205 are mounted to balun stems 107, and the inductive segments 320 of the inward-directed dipole arms 310 point toward the array face 200.
FIGS. 5A-D illustrate a first exemplary embodiment of an inward-directed dipole arm 310 of an exemplary asymmetric low band radiator 205 according to the disclosure. FIG. 5A is a transparent line drawing of inward-directed dipole arm 310 from a position below it relative to the array face 200, and FIG. 5B is a solid figure drawing of the inward-directed dipole arm 310 from the same perspective. FIG. 5C is a transparent line drawing of inward-directed dipole arm 310 from a position above it relative to the array face 200, and FIG. 5D is a solid figure drawing of the inward-directed dipole arm 310 from the same perspective. Illustrated are radiative segments 315 and inductive segments 320.
FIGS. 6A-D illustrate a second exemplary embodiment of an inward-directed dipole arm 610 according to the disclosure. FIG. 6A is a transparent line drawing of inward-directed dipole arm 610 from a position below it relative to the array face 200, and FIG. 6B is a solid figure drawing of the inward-directed dipole arm 610 from the same perspective. FIG. 6C is a transparent line drawing of inward-directed dipole arm 610 from a position above it relative to the array face 200, and FIG. 6D is a solid figure drawing of the inward-directed dipole arm 610 from the same perspective. Illustrated are radiative segments 615 and inductive segments 620.
FIGS. 7A-D illustrate a third exemplary embodiment of an inward-directed dipole arm 710 according to the disclosure. FIG. 7A is a transparent line drawing of inward-directed dipole arm 710 from a position below it relative to the array face 200, and FIG. 7B is a solid figure drawing of the inward-directed dipole arm 710 from the same perspective. FIG. 7C is a transparent line drawing of inward-directed dipole arm 710 from a position above it relative to the array face 200, and FIG. 7D is a solid figure drawing of the inward-directed dipole arm 710 from the same perspective. Illustrated are radiative segments 715 and inductive segments 720.
The differences between embodiments 310, 610, and 710 include the following. Inward-directed dipole arm 310 has radiative segments 315 that are mechanically coupled solely by inductive segments 320. Having the inductive segments 315 as the sole electrical coupling between radiative segments 315 provides for maximum cloaking and thus interference mitigation. However, having the inductive segments 315 as the sole mechanical coupling between radiative segments 315 may make this embodiment of inward-directed dipole arm 315 susceptible to vibration and mechanical deformation relative to dipole arms 610 and 710. Inward-directed dipole arm 610 has radiative segments 615 that are electrically and mechanically by inductive segments 620 as well as an in-plane coupling element 617, which couple adjacent radiative segments 615 on alternating sides. The presence of in-plane coupling elements 617 provides for improved mechanical rigidity but at the expense of performance in the CBRS gain pattern. Similarly, inward-directed dipole arm 710 has radiative segments 715 that are electrically and mechanically by inductive segments 720 as well as an in-plane coupling element 717, which couple adjacent radiative segments 715 on both sides. The presence of in-plane coupling elements 717 provide for improved mechanical rigidity—more so than inward-directed dipole arm 610—but further at the expense of performance in the CBRS gain pattern. It will be understood that such variations are possible and within the scope of the disclosure.
FIG. 8 illustrates an exemplary mid band radiator 210 according to the disclosure. Mid band radiator 210 includes an exemplary parasitic disk 810 having cloaking slots 815 formed therein to prevent the mid band radiator 210 from coupling with emissions from the high band radiators 115. A conventional mid band parasitic radiator within mid band radiator 110 of FIG. 1 suffers the deficiency of resonating with the high band radiators 115. The presence of cloaking slots 815 in exemplary mid band parasitic radiator 810 substantially prevents this resonance, thereby improving the gain pattern of the array of CBRS (high band) radiators 115 in antenna array face 200.