CN203983456U - A kind of broadband circle polarized omnidirectional antenna based on inclination oscillator - Google Patents
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Abstract
本实用新型公开了一种基于倾斜振子的宽带圆极化全向天线,包括天线辐射部分、柔性介质板、宽带馈电网络和馈电基板,天线辐射部分包括四个倾斜振子,每个倾斜振子由一个主辐射振子和一个寄生振子组成,主辐射振子与寄生振子的长度和倾斜角度都不同,柔性介质板弯曲成空心圆柱状,四个倾斜振子在柔性介质板上呈等分均匀环状排列,宽带馈电网络则印制在馈电基板的正、反面上,其水平放置于介质空心圆柱中心,实现对四个倾斜振子等幅同相馈电。本实用新型具有左、右旋圆极化实现灵活、全向性好和宽带的优点,适用于移动通信基站领域。
The utility model discloses a broadband circularly polarized omnidirectional antenna based on an inclined vibrator, which comprises an antenna radiating part, a flexible dielectric board, a broadband feeding network and a feeding substrate. The antenna radiating part includes four inclined vibrators, each of which is It consists of a main radiation oscillator and a parasitic oscillator. The main radiation oscillator and the parasitic oscillator have different lengths and inclination angles. The flexible dielectric plate is bent into a hollow cylinder, and the four inclined oscillators are arranged in an evenly divided ring on the flexible dielectric plate. , the broadband feed network is printed on the front and back of the feed substrate, and it is placed horizontally in the center of the dielectric hollow cylinder to realize equal-amplitude and in-phase feed to the four inclined oscillators. The utility model has the advantages of flexible realization of left and right circular polarization, good omnidirectionality and broadband, and is suitable for the field of mobile communication base stations.
Description
技术领域technical field
本实用新型涉及一种无线通信领域,具体涉及一种基于倾斜振子的宽带圆极化全向天线。The utility model relates to the field of wireless communication, in particular to a broadband circularly polarized omnidirectional antenna based on an inclined vibrator.
背景技术Background technique
随着社会的不断发展,对天线的性能要求也越来越高,在现代的无线应用系统中,单纯的线极化天线已很难满足人们的需求,圆极化天线越来越受到更为广泛的关注,而全向圆极化天线更是因为其特殊的性能,广泛应用于在通信、遥感遥测、雷达、电子侦察与电子干扰等方面。With the continuous development of society, the performance requirements of antennas are getting higher and higher. In modern wireless application systems, it is difficult to meet people's needs with purely linearly polarized antennas. Circularly polarized antennas are more and more popular Widely concerned, and the omnidirectional circularly polarized antenna is widely used in communication, remote sensing and telemetry, radar, electronic reconnaissance and electronic jamming because of its special performance.
在天线理论中,垂直于地面的电偶极子辐射全向垂直极化波,平行于地面的均匀电流环辐射全向水平极化波,两者辐射的垂直、水平极化电场自然产生90°相位差,当其幅度相等时,两正交极化波在远场叠加可产生全向圆极化波,从而实现全向圆极化辐射。当使用倾斜振子阵实现全向圆极化天线时,每个倾斜振子可以分解为一个水平分量和一个垂直分量,当多个倾斜振子围绕圆周排列时,其水平分量可等效为一个水平均匀电流环,垂直分量等效为一个垂直偶极子,两者在远场产生全向圆极化波。由此方法实现的全向天线可实现较宽的圆极化带宽,但阻抗匹配较难实现。In antenna theory, the electric dipole perpendicular to the ground radiates omnidirectional vertically polarized waves, and the uniform current loop parallel to the ground radiates omnidirectional horizontally polarized waves. The vertical and horizontal polarized electric fields radiated by the two naturally produce 90° Phase difference, when their amplitudes are equal, two orthogonally polarized waves can be superimposed in the far field to generate omnidirectional circularly polarized waves, thereby realizing omnidirectional circularly polarized radiation. When using a tilted dipole array to realize an omnidirectional circularly polarized antenna, each tilted dipole can be decomposed into a horizontal component and a vertical component. When multiple tilted dipoles are arranged around the circumference, its horizontal component can be equivalent to a horizontal uniform current ring, the vertical component is equivalent to a vertical dipole, and the two generate omnidirectional circularly polarized waves in the far field. The omnidirectional antenna realized by this method can achieve a wide circular polarization bandwidth, but the impedance matching is difficult to achieve.
实用新型内容Utility model content
为了克服现有技术存在的缺点与不足,本实用新型提供一种低剖面、宽带宽和水平面全向辐射的基于倾斜振子的宽带圆极化全向天线。In order to overcome the shortcomings and deficiencies of the prior art, the utility model provides a broadband circularly polarized omnidirectional antenna with a low profile, wide bandwidth and omnidirectional radiation on a horizontal plane based on an inclined vibrator.
本实用新型采用如下技术方案:The utility model adopts the following technical solutions:
一种基于倾斜振子的宽带圆极化全向天线,包括天线辐射部分、柔性介质板、宽带馈电网络及馈电基板,所述宽带馈电网络印制在馈电基板的正反两面,所述柔性介质板弯曲成空心圆柱,所述馈电基板水平放置于空心圆柱的中心,所述天线辐射部分包括四个倾斜振子,所述四个倾斜振子在空心圆柱外表面呈等分均匀环状排列。A broadband circularly polarized omnidirectional antenna based on a tilted vibrator, including an antenna radiating part, a flexible dielectric board, a broadband feed network and a feed substrate, the broadband feed network is printed on both sides of the feed substrate, and the The flexible dielectric plate is bent into a hollow cylinder, the feed substrate is horizontally placed in the center of the hollow cylinder, and the antenna radiation part includes four inclined vibrators, and the four inclined vibrators are equally divided and evenly ring-shaped on the outer surface of the hollow cylinder arrangement.
所述倾斜振子由主辐射振子和寄生振子构成,主辐射振子与水平面正方向夹角为0<α<180°,所述寄生振子与水平面正方向夹角为0<β<180°。The inclined oscillator is composed of a main radiation oscillator and a parasitic oscillator, the angle between the main radiation oscillator and the positive direction of the horizontal plane is 0<α<180°, and the angle between the parasitic oscillator and the positive direction of the horizontal plane is 0<β<180°.
所述空心圆柱的直径为0.17λ0~0.2λ0,高度为0.4λ0,其中λ0为中心频率2GHz所对应自由空间的波长。The diameter of the hollow cylinder is 0.17λ 0 -0.2λ 0 , and the height is 0.4λ 0 , where λ 0 is the wavelength of free space corresponding to the center frequency of 2GHz.
所述主辐射振子和寄生振子的宽度分别是0.05λ0和0.02λ0,长度分别是0.47λ0和0.31λ0。The main radiation oscillator and the parasitic oscillator have widths of 0.05λ 0 and 0.02λ 0 and lengths of 0.47λ 0 and 0.31λ 0 respectively.
所述主辐射振子和寄生振子无直接连接,其中,主辐射振子最高点与寄生振子最高点垂直方向上距离d1是0.1λ0,水平方向上距离d2是0.05λ0。There is no direct connection between the main radiation oscillator and the parasitic oscillator, wherein the vertical distance d 1 between the highest point of the main radiation oscillator and the highest point of the parasitic oscillator is 0.1λ 0 , and the horizontal distance d 2 is 0.05λ 0 .
所述主辐射振子在长度方向的中间位置断开裂缝,该裂缝通过焊点与宽带馈电网络连接。The main radiation oscillator breaks a crack in the middle of the length direction, and the crack is connected to the broadband feeding network through a welding point.
宽带馈电网络包括四个宽带巴伦及阻抗匹配电路,每个宽带巴伦由在馈电基板背面的缝隙和正面的带45°倒角的L型微带线构成,L型微带线的末端开路,另一端与阻抗匹配电路一端连接,阻抗匹配电路的另一端与空心圆柱的中央馈电点连接。The broadband feed network includes four broadband baluns and impedance matching circuits. Each broadband balun is composed of a slot on the back of the feed substrate and an L-shaped microstrip line with a 45° chamfer on the front. The L-shaped microstrip line The end is open circuit, the other end is connected with one end of the impedance matching circuit, and the other end of the impedance matching circuit is connected with the central feed point of the hollow cylinder.
所述馈电基板背面还印制有带45°倒角的十字型导体贴片。A cross-shaped conductor patch with a 45° chamfer is also printed on the back of the feeder substrate.
所述阻抗匹配网路在馈电基板中央呈十字形交叉连接。The impedance matching network is cross-connected in the center of the feed substrate in a cross shape.
当倾斜振子与水平面正方向的夹角为0<α<90°时,构成右旋圆极化全向天线,当倾斜振子与水平面正方向的夹角为90°<α<180°时,则构成左旋圆极化全向天线。When the angle between the inclined vibrator and the positive direction of the horizontal plane is 0<α<90°, a right-handed circularly polarized omnidirectional antenna is formed; when the angle between the inclined vibrator and the positive direction of the horizontal plane is 90°<α<180°, then Constitutes a left-handed circularly polarized omnidirectional antenna.
本实用新型的有益效果:The beneficial effects of the utility model:
(1)本实用新型采用的四个倾斜振子围绕空心圆柱等分均匀环状排列实现了全向圆极化辐射,利用寄生振子和宽带馈电网络,实现了宽带圆极化;(1) The four inclined oscillators adopted in the utility model are arranged in a uniform ring around the hollow cylinder to realize omnidirectional circular polarization radiation, and the broadband circular polarization is realized by using the parasitic oscillator and the broadband feed network;
(2)圆极化全向天线的极化旋向由倾斜振子与水平面正方向的倾斜角度α决定,当倾斜振子与水平面正方向的夹角为0<α<90°时,构成右旋圆极化全向天线,而倾斜振子与水平面正方向的夹角为90°<α<180°时,则构成左旋圆极化全向天线,转换方式灵活;(2) The polarization rotation of the circularly polarized omnidirectional antenna is determined by the tilt angle α between the tilted oscillator and the positive direction of the horizontal plane. When the angle between the tilted oscillator and the positive direction of the horizontal plane is 0<α<90°, a right-handed circle is formed Polarized omnidirectional antenna, and when the angle between the inclined vibrator and the positive direction of the horizontal plane is 90°<α<180°, it constitutes a left-handed circularly polarized omnidirectional antenna with flexible conversion methods;
(3)每个倾斜振子包括一个主辐射振子和一个寄生振子,它们都围绕空心圆柱等分均匀环状排列,主辐射振子倾斜角度和圆柱半径是实现全向圆极化辐射的关键,利用寄生振子与主辐射振子之间耦合展宽了天线带宽,从而实现宽带圆极化特性;(3) Each tilted oscillator includes a main radiation oscillator and a parasitic oscillator, which are uniformly arranged in a ring around the hollow cylinder. The tilt angle of the main radiation oscillator and the radius of the cylinder are the keys to realize omnidirectional circularly polarized radiation. Using the parasitic The coupling between the oscillator and the main radiation oscillator broadens the bandwidth of the antenna, thereby realizing the broadband circular polarization characteristics;
(4)宽带馈电网络仅影响天线阻抗性能,对天线圆极化和全向特性几乎无影响;宽带馈电网络对四个倾斜振子等幅同相馈电,实现了宽带阻抗匹配,此圆极化全向天线的10dB的回波损耗带宽可达到61%(1.35-2.54GHz),3dB轴比带宽为44%(1.69-2.64GHz),在1.7-2.4GHz频段内,水平面方向图不圆度小于1.5dB,交叉极化小于-15dB,容易实现双圆极化功能。(4) The broadband feed network only affects the antenna impedance performance, and has almost no effect on the circular polarization and omnidirectional characteristics of the antenna; the broadband feed network feeds the four inclined oscillators with equal amplitude and phase, realizing broadband impedance matching. The 10dB return loss bandwidth of the optimized omnidirectional antenna can reach 61% (1.35-2.54GHz), and the 3dB axial ratio bandwidth is 44% (1.69-2.64GHz). In the 1.7-2.4GHz frequency band, the horizontal plane pattern is not round Less than 1.5dB, cross polarization less than -15dB, easy to achieve dual circular polarization function.
附图说明Description of drawings
图1是本实用新型一种基于倾斜振子的宽带圆极化全向天线结构示意图;Fig. 1 is a schematic structural diagram of a broadband circularly polarized omnidirectional antenna based on a tilted vibrator of the present invention;
图2是图1中的倾斜振子结构示意图;Fig. 2 is a schematic diagram of the structure of the inclined vibrator in Fig. 1;
图3是图1中宽带馈电网络结构示意图;Fig. 3 is a schematic structural diagram of the broadband feed network in Fig. 1;
图4(a)是本实用新型实施例回波损耗的仿真结果与测试结果对比图,图4(b)是本实用新型实施例轴比的仿真结果与测试结果对比图。Figure 4(a) is a comparison chart of the simulation results and test results of the return loss of the embodiment of the utility model, and Figure 4(b) is a comparison chart of the simulation results and test results of the axial ratio of the embodiment of the utility model.
图中示出:The figure shows:
1-天线辐射部分;2-柔性介质板;3-宽带馈电网络;4-馈电基板;5-主辐射振子;6-寄生振子;7-焊点;8-中央馈电点;9-缝隙;10-L型微带线;11-阻抗匹配电路;12-十字型导体贴片。1-antenna radiation part; 2-flexible dielectric board; 3-broadband feed network; 4-feed substrate; 5-main radiation oscillator; 6-parasitic oscillator; Gap; 10-L-type microstrip line; 11-impedance matching circuit; 12-cross-shaped conductor patch.
具体实施方式Detailed ways
下面结合实施例及附图,对本实用新型作进一步地详细说明,但本实用新型的实施方式不限于此。The utility model will be described in further detail below in conjunction with the embodiments and accompanying drawings, but the implementation of the utility model is not limited thereto.
实施例Example
如图1所示,一种基于倾斜振子的宽带圆极化全向天线,包括天线辐射部分1、柔性介质板2、宽带馈电网络3及馈电基板4,所述宽带馈电网络3印制在馈电基板4的正、反两面,所述柔性介质板2弯曲成空心圆柱,所述空心圆柱的直径为0.17λ0~0.2λ0,高度为0.4λ0,其中λ0为中心频率2GHz所对应自由空间的波长,所述馈电基板4水平放置于空心圆柱的中心,且馈电基板的直径与空心圆柱直径相等,所述天线辐射部分1包括四个倾斜振子,所述四个倾斜振子在空心圆柱外表面呈等分均匀环状排列。As shown in Figure 1, a broadband circularly polarized omnidirectional antenna based on a tilted vibrator includes an antenna radiating part 1, a flexible dielectric board 2, a broadband feed network 3 and a feed substrate 4, and the broadband feed network 3 prints Made on the front and back sides of the feeder substrate 4, the flexible dielectric plate 2 is bent into a hollow cylinder, the diameter of the hollow cylinder is 0.17λ 0 ~0.2λ 0 , and the height is 0.4λ 0 , where λ 0 is the center frequency The wavelength of free space corresponding to 2GHz, the feed substrate 4 is horizontally placed in the center of the hollow cylinder, and the diameter of the feed substrate is equal to the diameter of the hollow cylinder, the antenna radiation part 1 includes four inclined oscillators, the four The inclined vibrator is arranged in an evenly divided ring on the outer surface of the hollow cylinder.
如图2所示,每个倾斜振子由一个主辐射振子5和一个寄生振子6构成,本实施例中主辐射振子的长度k1为73mm,宽度h1是7.5mm,与水平面正方向夹角α为35°,寄生振子的长度k2为47mm,宽度h2是3mm,与水平面正方向夹角β为40°。所述主辐射振子和寄生振子无直接连接,其中,主辐射振子最高点与寄生振子最高点垂直方向上距离d1是14.8mm,水平方向上距离d2是7.3mm。主辐射振子在长度方向的中间位置断开裂缝,所述裂缝宽度为1.2mm,该裂缝通过焊点7与宽带馈电网络3连接。As shown in Figure 2, each inclined oscillator is composed of a main radiation oscillator 5 and a parasitic oscillator 6. In this embodiment, the length k1 of the main radiation oscillator is 73mm, the width h1 is 7.5mm, and the angle between the positive direction of the horizontal plane α is 35°, the length k 2 of the parasitic oscillator is 47 mm, the width h 2 is 3 mm, and the angle β with the positive direction of the horizontal plane is 40°. There is no direct connection between the main radiating oscillator and the parasitic oscillator, wherein the vertical distance d 1 between the highest point of the main radiating oscillator and the highest point of the parasitic oscillator is 14.8 mm, and the horizontal distance d 2 is 7.3 mm. The main radiation oscillator breaks a crack at the middle position in the length direction, and the crack width is 1.2mm, and the crack is connected to the broadband feed network 3 through the welding point 7 .
本实施例的柔性介质板厚度为0.05mm高频板Panasonic R-F775板材,相对介电常数3.2,损耗角正切是0.0015,直径为0.185λ0,高度为0.4λ0,其中λ0为中心频率2GHz所对应自由空间的波长。The thickness of the flexible dielectric plate in this embodiment is 0.05mm high-frequency plate Panasonic R-F775 plate, the relative dielectric constant is 3.2, the loss tangent is 0.0015, the diameter is 0.185λ 0 , and the height is 0.4λ 0 , where λ 0 is the center frequency 2GHz corresponds to the wavelength in free space.
馈电基板4是厚度为0.8mm介质板Taconic TLY-5板材,相对介电常数2.2,损耗角正切是0.0009,直径为27.95mm。The feed substrate 4 is a Taconic TLY-5 plate with a thickness of 0.8 mm, a relative dielectric constant of 2.2, a loss tangent of 0.0009, and a diameter of 27.95 mm.
同轴线采用柔性同轴线Johnson/Emerson RG-178,直径为2.5mm,特征阻抗为50Ω。The coaxial cable adopts flexible coaxial cable Johnson/Emerson RG-178 with a diameter of 2.5mm and a characteristic impedance of 50Ω.
如图3所示,所述馈电基板水平放置于柔性介质板弯曲的空心圆柱的中心,宽带馈电网络3印制在基板的正、反两面上,宽带馈电网络包括四个宽带巴伦及阻抗匹配电路11,宽带巴伦由在馈电基板背面的缝隙9和正面的带45度倒角的L型微带线10构成,L型微带线的末端开路,另一端与阻抗匹配电路11相连,阻抗匹配电路的另一端则连接到圆柱的中央馈电点8上,接到馈电所用50Ω同轴线上,馈电基板背面还印制有带倒角的十字型导体贴片12,导体贴片的倒角角度是45°,倒角的第一段部分长度l8为2mm,倒角的第二部分长度l9也为2mm,贴片上蚀刻了缝隙,贴片宽度wg是12mm。As shown in Figure 3, the feeder substrate is horizontally placed in the center of the curved hollow cylinder of the flexible dielectric plate, and the broadband feeder network 3 is printed on the front and back sides of the substrate, and the broadband feeder network includes four broadband baluns And the impedance matching circuit 11, the broadband balun is composed of the slit 9 on the back of the feed substrate and the L-shaped microstrip line 10 with a 45-degree chamfer on the front, the end of the L-shaped microstrip line is open, and the other end is connected to the impedance matching circuit 11, the other end of the impedance matching circuit is connected to the central feeding point 8 of the cylinder, and connected to the 50Ω coaxial line used for feeding, and a cross-shaped conductor patch 12 with chamfers is also printed on the back of the feeding substrate , the chamfering angle of the conductor patch is 45°, the length l 8 of the first part of the chamfer is 2 mm, the length l 9 of the second part of the chamfer is also 2 mm, the patch is etched with a gap, and the patch width w g It is 12mm.
宽带馈电网络可以实现对四个倾斜振子等幅同相馈电,其中参数说明如下:ls是缝隙长度为19mm,ws是缝隙宽度为1.2mm,l1是阻抗匹配网络第一段的长度为4mm,l2是阻抗匹配网络第二段部分的长度为23.5mm,l3是阻抗匹配网络第三段部分长度为3mm,w1是阻抗匹配网络第一、二和三段的宽度均为0.4mm,l4是带倒角的微带线长度为4mm,倒角角度也是45°,l5是微带线倒角第一段部分长度为1.5mm,l6是微带线倒角第二段部分长度为1.5mm,l7是带倒角的微带线的弯折部分长度为15.5mm,w2是带倒角微带线宽度为1.5mm。The broadband feed network can feed the four inclined oscillators with equal amplitude and same phase. The parameters are described as follows: l s is the slot length of 19mm, w s is the slot width of 1.2mm, l 1 is the length of the first section of the impedance matching network is 4mm, l 2 is the length of the second section of the impedance matching network is 23.5mm, l 3 is the length of the third section of the impedance matching network is 3mm, w 1 is the width of the first, second and third sections of the impedance matching network 0.4mm, l 4 is the length of the chamfered microstrip line is 4mm, and the chamfer angle is also 45°, l 5 is the length of the first section of the microstrip line chamfer is 1.5mm, l 6 is the second section of the microstrip line chamfer The length of the second section is 1.5 mm, l 7 is the length of the bending part of the microstrip line with chamfering is 15.5 mm, and w 2 is the width of the microstrip line with chamfering is 1.5 mm.
倾斜振子与宽带馈电网络相连的焊点长度wf是1.5mm,焊点7与十字型导体贴片12连接的距离长度hf是2.5mm。The length w f of the welding point connecting the inclined vibrator to the broadband feed network is 1.5 mm, and the distance h f connecting the welding point 7 to the cross-shaped conductor patch 12 is 2.5 mm.
阻抗匹配电路在馈电基板中央呈十字形交叉连接。当倾斜振子与水平面正方向的夹角为0<α<90°时,构成右旋圆极化全向天线,而倾斜振子与水平面正方向的夹角为90°<α<180°时,则构成左旋圆极化全向天线,转换方法简单、灵活。The impedance matching circuit is cross-connected in the center of the feed substrate in a cross shape. When the angle between the inclined vibrator and the positive direction of the horizontal plane is 0<α<90°, a right-handed circularly polarized omnidirectional antenna is formed, and when the angle between the inclined vibrator and the positive direction of the horizontal plane is 90°<α<180°, then A left-handed circularly polarized omnidirectional antenna is formed, and the conversion method is simple and flexible.
如图4(a),图4(b)所示本实施例的天线通过宽带馈电网络对四个倾斜振子等幅同相馈电,实现了宽带阻抗匹配,此圆极化全向天线的10dB的回波损耗带宽可达到61%(1.35-2.54GHz),3dB轴比带宽为44%(1.69-2.64GHz),在1.7-2.4GHz频段内,水平面方向图不圆度小于1.5dB,交叉极化小于-15dB,容易实现双圆极化功能。As shown in Fig. 4 (a), the antenna of this embodiment shown in Fig. 4 (b) feeds four inclined oscillators with equal amplitude and in-phase feed through a broadband feed network, and realizes broadband impedance matching. The 10dB of this circularly polarized omnidirectional antenna The return loss bandwidth can reach 61% (1.35-2.54GHz), the 3dB axial ratio bandwidth is 44% (1.69-2.64GHz), in the 1.7-2.4GHz frequency band, the horizontal plane pattern is less than 1.5dB, and the cross pole Polarization is less than -15dB, easy to achieve dual circular polarization function.
本实用新型提供一种利用多个倾斜振子进行排列组合的方式,通过将同样四单元的倾斜振子共形于空心圆柱表面,使得每个天线单元在远场叠加产生了全向圆极化波原理,再通过寄生单元和宽带馈电网络的设计,最终实现宽带圆极化全向辐射。The utility model provides a way to arrange and combine multiple inclined oscillators. By making the same four-unit inclined oscillators conform to the surface of a hollow cylinder, each antenna unit superimposes in the far field to produce an omnidirectional circularly polarized wave principle. , and then through the design of the parasitic unit and the broadband feed network, the broadband circular polarization omnidirectional radiation is finally realized.
利用该实用新型还可进行天线组阵,形成多单元水平极化全向天线阵列,提高天线增益,从而满足移动通信基站天线高增益的需求。The utility model can also be used to form an antenna array to form a multi-unit horizontally polarized omnidirectional antenna array to improve antenna gain, thereby meeting the high-gain requirement of mobile communication base station antennas.
上述实施例为本实用新型较佳的实施方式,但本实用新型的实施方式并不受所述实施例的限制,其他的任何未背离本实用新型的精神实质与原理下所作的改变、修饰、替代、组合、简化,均应为等效的置换方式,都包含在本实用新型的保护范围之内。The above-mentioned embodiment is a preferred implementation mode of the present utility model, but the implementation mode of the present utility model is not limited by the described embodiment, and any other changes, modifications, modifications, Substitution, combination, and simplification should all be equivalent replacement methods, and are all included in the protection scope of the present utility model.
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
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CN104092007A (en) * | 2014-06-27 | 2014-10-08 | 华南理工大学 | A Broadband Circularly Polarized Omnidirectional Antenna Based on Inclined Vibrator |
CN110637392A (en) * | 2017-02-28 | 2019-12-31 | 株式会社Kmw | Dual-polarized omnidirectional antenna and base station comprising same |
CN111029737A (en) * | 2019-11-22 | 2020-04-17 | 深圳市鼎耀科技有限公司 | Compact circularly polarized omnidirectional antenna |
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Publication number | Priority date | Publication date | Assignee | Title |
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CN104092007A (en) * | 2014-06-27 | 2014-10-08 | 华南理工大学 | A Broadband Circularly Polarized Omnidirectional Antenna Based on Inclined Vibrator |
CN110637392A (en) * | 2017-02-28 | 2019-12-31 | 株式会社Kmw | Dual-polarized omnidirectional antenna and base station comprising same |
US11114772B2 (en) | 2017-02-28 | 2021-09-07 | Kmw Inc. | Dual polarized omni-directional antenna and base station including same |
CN110637392B (en) * | 2017-02-28 | 2022-11-15 | 株式会社Kmw | Dual-polarized omnidirectional antenna and base station comprising same |
CN111029737A (en) * | 2019-11-22 | 2020-04-17 | 深圳市鼎耀科技有限公司 | Compact circularly polarized omnidirectional antenna |
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