The present invention relates generally to antennas for cellular systems and in particular to antennas for cellular basestations
Developments in wireless technology typically require wireless operators to deploy new antenna equipment in their networks. Disadvantageously, towers have become cluttered with multiple antennas while installation and maintenance have become more complicated. Basestation antennas typically covered a single narrow band. This has resulted in a plethora of antennas being installed at a site. Local governments have imposed restrictions and made getting approval for new sites difficult due to the visual pollution of so many antennas. Some antenna designs have attempted to combine two bands and extend bandwidth, but still many antennas are required due to the proliferation of many air-interface standards and bands.
The following definitions are provided as general definitions and should in no way limit the scope of the present invention to those terms alone, but are set forth for a better understanding of the following description.
Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by those of ordinary skill in the art to which the invention belongs. For the purposes of the present invention, the following terms are defined below:
The articles “a” and “an” are used herein to refer to one or to more than one (i.e. to at least one) of the grammatical object of the article. By way of example, “an element” refers to one element or more than one element.
Throughout this specification, unless the context requires otherwise, the words “comprise”, “comprises” and “comprising” will be understood to imply the inclusion of a stated step or element or group of steps or elements, but not the exclusion of any other step or element or group of steps or elements.
In accordance with an aspect of the invention, there is provided a low-band radiator of an ultra-wideband dual-band dual-polarization cellular basestation antenna. The dual bands comprise low and high bands. The low-band radiator comprises a dipole comprising two dipole arms adapted for the low band and for connection to an antenna feed. At least one dipole arm of the dipole comprises at least two dipole segments and at least one radiofrequency (RF) choke. The choke is disposed between the dipole segments. Each choke provides an open circuit or a high impedance separating adjacent dipole segments to minimize induced high band currents in the low-band radiator and consequent disturbance to the high band pattern. The choke is resonant at or near the frequencies of the high band.
Each dipole segment comprises an electrically conducting elongated body; the elongated body is open circuited at one end and short circuited at the other end to a center conductor. The electrically conducting elongated body may be cylindrical or tubular in form, and the center conductor connects the short circuited portions of the dipole segments.
The choke may be a coaxial choke. Each coaxial choke may comprise a protruding portion of center conductor extending between adjacent dipole segments by a gap, and each choke may have a length of a quarter wavelength (λ/4) or less at frequencies in the bandwidth of the high band.
The low and high bands provide wideband coverage.
The choke may contain lumped circuit elements, or be an open sleeve partly or completely enclosing a center conductor.
The at least one dipole arm may comprise three dipole segments separated by two chokes; adjacent dipole segments are spaced apart about so that there is a gap between the adjacent dipole segments.
The center conductor connecting the short circuited may be an elongated cylindrical electrically conducting body. The center conductor may have a thickness adapted to provide immunity from disturbance of the high-band radiation pattern by the low-band radiator over the entire high-band bandwidth.
The space between each cylindrical conducting body and the center conductor may be filled with air, or filled or partly filled with dielectric material.
The conducting body and a center conductor of each dipole segment may have dimensions optimized so that the radiation pattern of the high band is undisturbed by the presence of the low-band radiator.
The low-band radiator may be adapted for the frequency range of 698-960 MHz.
The two dipole arms of the dipole may each comprise at least two dipole segments, and at least one choke disposed between the dipole segments.
The dipole may be an extended dipole and further comprise another dipole comprising two dipole arms. The dipoles may be configured in a cross configuration, each dipole arm being resonant at approximately a quarter-wavelength (λ/4), and adapted for connection to an antenna feed. The extended dipole may anti-resonant dipole arms, each dipole arm being of approximately a half-wavelength (λ/2).
In accordance with another aspect of the invention, there is provided an ultra-wideband dual-band dual-polarization cellular base-station antenna. The dual bands are low and high bands suitable for cellular communications. The dual-band antenna comprises: at least one low-band radiator as set forth in a foregoing aspect of the invention each adapted for dual polarization and providing clear areas on a groundplane of the dual-band antenna for locating high band radiators in the dual-band antenna; and a number of high band radiators each adapted for dual polarization, the high band radiators being configured in at least one array, the low-band radiators being interspersed amongst the high-band radiators at predetermined intervals.
The high-band radiators may be adapted for the frequency range of 1710 to 2690 MHz.
Arrangements of low-band radiators of an ultra-wideband dual-band dual-polarization cellular basestation antenna and such dual-band cellular base-station antennas are described hereinafter, by way of an example only, with reference to the accompanying drawings, in which:
Hereinafter, low-band radiators of an ultra-wideband dual-band dual-polarization cellular basestation antenna and such dual-band cellular base-station antennas are disclosed. In the following description, numerous specific details, including particular horizontal beamwidths, air-interface standards, dipole arm shapes and materials, dielectric materials, and the like are set forth. However, from this disclosure, it will be apparent to those skilled in the art that modifications and/or substitutions may be made without departing from the scope and spirit of the invention. In other circumstances, specific details may be omitted so as not to obscure the invention.
As used hereinafter, “low band” refers to a lower frequency band, such as 698-960 MHz, and “high band” refers to a higher frequency band, such as 1710 MHz-2690 MHz. A “low band radiator” refers to a radiator for such a lower frequency band, and a “high band radiator” refers to a radiator for such a higher frequency band. The “dual band” comprises the low and high bands referred to throughout this disclosure. Further, “ultra-wideband” with reference to an antenna connotes that the antenna is capable of operating and maintaining its desired characteristics over a bandwidth of at least 30%. Characteristics of particular interest are the beam width and shape and the return loss, which needs to be maintained at a level of at least 15 dB across this band. In the present instance, the ultra-wideband dual-band antenna covers the bands 698-960 MHz and 1710 MHz-2690 MHz. This covers almost the entire bandwidth assigned for all major cellular systems.
The embodiments of the invention relate generally to low-band radiators of an ultra-wideband dual-band dual-polarization cellular basestation antenna and such dual-band cellular base-station antennas adapted to support emerging network technologies. Such ultra-wideband dual-band dual-polarization antennas enable operators of cellular systems (“wireless operators”) to use a single type of antenna covering a large number of bands, where multiple antennas were previously required. Such antennas are capable of supporting several major air-interface standards in almost all the assigned cellular frequency bands and allow wireless operators to reduce the number of antennas in their networks, lowering tower leasing costs while increasing speed to market capability. Ultra-wideband dual-band dual-polarization cellular basestation antennas support multiple frequency bands and technology standards. For example, wireless operators can deploy using a single antenna Long Term Evolution (LTE) network for wireless communications in 2.6 GHz and 700 MHz, while supporting Wideband Code Division Multiple Access (W-CDMA) network in 2.1 GHz. For ease of description, the antenna array is considered to be aligned vertically.
The embodiments of the invention relate more specifically to ultra-wideband dual-band antennas with interspersed radiators intended for cellular basestation use and in particular to antennas intended for the low-band frequency band of 698 MHz-960 MHz or part thereof and high frequency band of 1710 MHz-2690 MHz or part thereof. In an interspersed design, typically the low-band radiators are located on an equally spaced grid appropriate to the frequency and then the low-band radiators are placed at intervals that are an integral number of high-band radiators intervals—often two such intervals and the low-band radiator occupies gaps between the high-band radiators. The high-band radiators are normally dual-slant polarized and the low-band radiators are normally dual polarized and may be either vertically and horizontally polarized, or dual slant polarized.
The principal challenge in the design of such ultra-wideband dual-band antennas is minimizing the effect of scattering of the signal at one band by the radiating elements of the other band. The embodiments of the invention aim to minimize the effect of the low-band radiator on the radiation from the high-band radiators. This scattering affects the shapes of the high-band beam in both azimuth and elevation cuts and varies greatly with frequency. In azimuth, typically the beamwidth, beam shape, pointing angle gain, and front-to-back ratio are all affected and vary with frequency in an undesirable way. Because of the periodicity in the array introduced by the low-band radiators, a grating lobe (sometimes referred to as a quantization lobe) is introduced into the elevation pattern at angles corresponding to the periodicity. This also varies with frequency and reduces gain. With narrow band antennas, the effects of this scattering can be compensated to some extent in various ways, such as adjusting beamwidth by offsetting the high-band radiators in opposite directions or adding directors to the high-band radiators. Where wideband coverage is required, correcting these effects is significantly difficult.
The embodiments of the invention reduce the induced current at the high band on the low-band radiating elements by introducing one or more RF chokes that are resonant at or near the frequencies of the high band. Thus, the use of one or more chokes is advantageous in the dipole arms, as described hereinafter. As shown in the drawings, the RF chokes are coaxial chokes, being gaps about a center conductor between cylindrical or tubular conducting bodies. However, the chokes may be practiced otherwise. For example, the chokes may contain lumped circuit elements or be an open sleeve partly or completely enclosing the center conductor. The important point is that the choke presents an open circuit or high impedance across each of the gaps. The embodiments of the invention are particularly effective when applied to a low-band long dipole, which has arms that are anti-resonant approaching half a wavelength (λ/2). For example, adding two high-band chokes to these elements has been found to reduce undesirable effects caused by scattering described above, in particular the grating lobe or quantization lobe is reduced to below −17 dB relative to the main beam in a ten element antenna. Perhaps more important are the reduction in variation of pointing, improvement in front-to back ratio, and stability of azimuth beamwidth.
Ultra-Wideband Dual-Band Dual-Polarization Cellular Basestation Antenna
In
The center feed 130 suspends the extended dipole 120 above a metal groundplane 110, by preferably a quarter wavelength. A pair of auxiliary radiating elements 150A and 150B, such as tuned parasitic elements or dipoles, or driven dipoles, is located in parallel with the conventional dipole 140 at opposite ends of the extended dipole 120. The tuned parasitic elements may each be a dipole formed on a PCB with metallization formed on the PCB, an inductive element formed between arms of that dipole on the PCB. An inductive element may be formed between the metal arms of the parasitic dipoles 150A, 150B to adjust the phase of the currents in the dipole arms to bring these currents into the optimum relationship to the current in the driven dipole 140. Alternatively, the auxiliary radiating elements may comprise driven dipole elements. The dipole 140 and the pair of auxiliary radiating elements 150 together produce a desired narrower beamwidth.
The dipole 140 is a vertical dipole with dipole arms 140A, 140B that are approximately a quarter wavelength (λ/4), and the extended dipole 120 is a horizontal dipole with dipole arms 120A, 120B that are approximately a half wavelength (λ/2) each. The auxiliary radiating elements 150A and 150B, together with the dipole 140, modify or narrow the horizontal beamwidth in vertical polarization.
The antenna architecture depicted in
The dipole 120 has anti-resonant dipole arms 120A, 120B of length of approximately .lamda./2 with a capacitively coupled feed with an 18 dB impedance bandwidth >32% and providing a beamwidth of approximately 65 degrees. This is one component of a dual polarized element in a dual polar wideband antenna. The single halfwave dipole 140 with the two parallel auxiliary radiating elements 150A, 150B provides the orthogonal polarization to signal radiated by extended dipole 120. The low-band radiator 100 of the ultra-wideband dual-band cellular basestation antenna is well suited for use in the 698-960 MHz cellular band. A particular advantage of this configuration is that this low band radiator 100 leaves unobstructed regions or clear areas of the groundplane where the high-band radiators of the ultra-wideband dual-band antenna can be located with minimum interaction between the low band and high band radiators.
The low-band radiators 100 of the antenna 400 as described radiate vertical and horizontal polarizations. For cellular basestation antennas, dual slant polarizations (linear polarizations inclined at +45.degree. and −45.degree. to vertical) are conventionally used. This can be accomplished by feeding the vertical and horizontal dipoles of the low-band radiator from a wideband 180.degree. hybrid (i.e., an equal-split coupler) well known to those skilled in the art.
The crossed-dipoles 120 and 140 define four quadrants, where the high-band radiators 420 and 410 are located in the lower-left and lower-right quadrants, and the high-band radiators 440 and 430 are Located in the upper-left and upper-right quadrants. The low-band radiator 100 is adapted for dual polarization and provides clear areas on a groundplane 110 of the dual-band antenna 400 for locating the high band radiators 4W, 420, 430, 440 in the dual-band antenna 400. Ellipsis points indicate that a basestation antenna may be formed by repeating portions 400 shown in
For example, each high-band radiator 410, 420, 430, 440 may comprise a pair of crossed dipoles each located in a square metal enclosure. In this case the crossed dipoles are inclined at 45.degree. so as to radiate slant polarization. The dipoles may be implemented as bow-tie dipoles or other wideband dipoles. While specific configurations of dipoles are shown, other dipoles may be implemented using tubes or cylinders or as metallized tracks on a printed circuit board, for example.
While the low-band radiator (crossed dipoles with auxiliary radiating elements) 100 can be used for the 698-960 MHz band, the high-band radiators 410, 420, 430, 440 can be used for the 1.7 GHz to 2.7 GHz (1710-2690 MHz) band. The low-band radiator 100 provides a 65 degree beamwidth with dual polarization (horizontal and vertical polarizations). Such dual polarization is required for basestation antennas. The conventional dipole 140 is connected to an antenna feed, while the extended dipole 120 is coupled to the antenna feed by a series inductor and capacitor. The low-band auxiliary radiating elements (e.g., parasitic dipoles) 150 and the vertical dipole 140 make the horizontal beamwidth of the vertical dipole 140 together with the auxiliary radiating elements 150 the same as that of the horizontal dipole 120. The antenna 400 implements a multi-band antenna in a single antenna. Beamwidths of approximately 65 degrees are preferred, but may be in the range of 60 degrees to 70 degrees on a single degree basis (e.g., 60, 61, or 62 degrees). This ultra-wideband, dual-band cellular basestation antenna can be implemented in a limited physical space.
To minimize interaction between low and high band radiators in a dual-polarization, dual-band cellular basestation antenna, the low band radiators are desirably in the form of vertical and horizontal radiating components to leave an unobstructed space for placing the high-band radiators. To radiate dual-slant linear polarization using radiator components that radiate horizontal and vertical polarizations, an ultra-wideband 180.degree. hybrid may be used to feed the horizontal and vertical components of a radiator of one band of an ultra-wideband dual-band dual-polarization cellular basestation antenna, e.g., the low band.
As shown in
As shown in
The dipole arm 200 may comprise at least two dipole segments 210, 220. Adjacent dipole segments 210 and 220 on the one hand and 220 and 230 on the other hand are spaced apart about the center conductor 250 so that there is a gap between the adjacent dipole segments 210, 220. The dimensions of the components of the coaxial chokes are such as to place the resonance of the coaxial choke 240A, 240B in the high band. The center conductor 250 may be an elongated cylindrical conducting body. The thickness or diameter C of the center conductor influences the bandwidth of the choke and may be adapted to minimize the high-band current over the whole of the high band thereby providing immunity from disturbance of the high-band radiation pattern by the low-band radiator 100 over the entire high-band bandwidth.
The space between the cylindrical conducting body 260, 270, 280 and the center conductor 250 may be filled with air, as depicted in
The cylindrical conducting body 260, 270, 280 and the center conductor 250 of each dipole segment 210, 220, 230 have dimensions optimized so that the radiation pattern of the high band is largely undisturbed by the presence of the low-band radiator 100. The radiator 100 is adapted for the frequency range of 698-960 MHz.
The dipole may be an extended dipole 120 and the radiator 100 may further comprise another dipole 140 comprising two dipole arms. The dipoles 120, 140 are configured hi a cross configuration. Each dipole arm is resonant at approximately a quarter-wavelength (λ/4) and is adapted for connection to an antenna feed. The extended dipole 120 has anti-resonant dipole arms. Each dipole arm is of approximately a half-wavelength (λ/2).
In accordance with another embodiment of the invention, an ultra-wideband dual-band dual-polarization cellular base-station antenna 400 is provided comprising at least one low-band radiator 100 and a number of high-band radiators 410, 420, 430, 440. The dual bands are low and high bands suitable for cellular communications. Each low-band radiator 100 is adapted for dual polarization and provides clear areas on a groundplane 110 of the dual-band antenna 400 for locating high band radiators 410, 420, 430, 440 in the dual-band antenna 400. The high band radiators 410, 420, 430, 440 are each adapted for dual polarization. The high-band radiators 410, 420, 430, 440 are configured in at least one array. The low-band radiator 100 is interspersed amongst the high-band radiators 410, 420, 430, 440 at predetermined intervals. The high-band radiators 410, 420, 430, 440 are adapted for the frequency range of 1710 to 2690 MHz.
Thus, low-band radiators of an ultra-wideband dual-band dual-polarization cellular basestation antenna and such dual-band cellular base-station antennas described herein and/or shown in the drawings are presented by way of example only and are not limiting as to the scope of the invention. Unless otherwise specifically stated, individual aspects and components of the hybrids may be modified, or may have been substituted therefore known equivalents, or as yet unknown substitutes such as may be developed in the future or such as may be found to be acceptable substitutes in the future.
This U.S. non-provisional patent application claims priority as a continuation application of U.S. Patent Application Ser. No. 14/358,763, filed May 16, 2014, which in turn is a national stage application under 35 U.S.C. 371 of PCT/CN2012/087300; Filed Dec. 24, 2012.
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Number | Date | Country | |
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Parent | 14358763 | US | |
Child | 17212346 | US |
Number | Date | Country | |
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Parent | 15393333 | Dec 2016 | US |
Child | 17212346 | US |