CN116565533A - A Miniaturized Ultra-Wideband Antenna - Google Patents
A Miniaturized Ultra-Wideband Antenna Download PDFInfo
- Publication number
- CN116565533A CN116565533A CN202310817929.2A CN202310817929A CN116565533A CN 116565533 A CN116565533 A CN 116565533A CN 202310817929 A CN202310817929 A CN 202310817929A CN 116565533 A CN116565533 A CN 116565533A
- Authority
- CN
- China
- Prior art keywords
- antenna
- dielectric substrate
- metasurface
- slots
- wideband
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000005855 radiation Effects 0.000 claims abstract description 37
- 239000000758 substrate Substances 0.000 claims abstract description 35
- 238000010586 diagram Methods 0.000 description 20
- 238000004088 simulation Methods 0.000 description 7
- 238000002955 isolation Methods 0.000 description 5
- 230000008859 change Effects 0.000 description 4
- 238000004891 communication Methods 0.000 description 4
- 238000013461 design Methods 0.000 description 4
- 230000010287 polarization Effects 0.000 description 4
- 238000000605 extraction Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000035945 sensitivity Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 238000004364 calculation method Methods 0.000 description 1
- 230000008094 contradictory effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/36—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
- H01Q1/38—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith formed by a conductive layer on an insulating support
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/36—Structural form of radiating elements, e.g. cone, spiral, umbrella; Particular materials used therewith
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q1/00—Details of, or arrangements associated with, antennas
- H01Q1/50—Structural association of antennas with earthing switches, lead-in devices or lightning protectors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q5/00—Arrangements for simultaneous operation of antennas on two or more different wavebands, e.g. dual-band or multi-band arrangements
- H01Q5/20—Arrangements for simultaneous operation of antennas on two or more different wavebands, e.g. dual-band or multi-band arrangements characterised by the operating wavebands
- H01Q5/25—Ultra-wideband [UWB] systems, e.g. multiple resonance systems; Pulse systems
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q5/00—Arrangements for simultaneous operation of antennas on two or more different wavebands, e.g. dual-band or multi-band arrangements
- H01Q5/50—Feeding or matching arrangements for broad-band or multi-band operation
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02D—CLIMATE CHANGE MITIGATION TECHNOLOGIES IN INFORMATION AND COMMUNICATION TECHNOLOGIES [ICT], I.E. INFORMATION AND COMMUNICATION TECHNOLOGIES AIMING AT THE REDUCTION OF THEIR OWN ENERGY USE
- Y02D30/00—Reducing energy consumption in communication networks
- Y02D30/70—Reducing energy consumption in communication networks in wireless communication networks
Landscapes
- Waveguide Aerials (AREA)
- Aerials With Secondary Devices (AREA)
Abstract
Description
技术领域technical field
本申请涉及天线技术领域,特别是涉及一种小型化超宽带天线。The present application relates to the technical field of antennas, in particular to a miniaturized ultra-wideband antenna.
背景技术Background technique
雷达侦察系统通常采用天线接收各种雷达信号。随着电子信息领域的飞速发展,天线作为无线通信中最重要的组成部分之一,自然也需要不断地推陈出新来适应更加复杂多变的通信系统和环境。近些年来无线通信类应用对天线的综合性能提出了更高要求。通常要求天线具有多个方面的优势,因此综合性能优良的天线越来越受到重视。Radar reconnaissance systems usually use antennas to receive various radar signals. With the rapid development of the electronic information field, antennas, as one of the most important components in wireless communication, naturally need to constantly innovate to adapt to more complex and changeable communication systems and environments. In recent years, wireless communication applications have put forward higher requirements for the comprehensive performance of antennas. Antennas are usually required to have multiple advantages, so antennas with excellent comprehensive performance are receiving more and more attention.
而在这之中,因电磁环境的日益复杂,对雷达侦察设备接受信号的敏感性提出了更高的要求,雷达极化的相关研究愈发深入,对天线小型化与超宽带的要求也日益迫切,相关研究受到瞩目。Among them, due to the increasingly complex electromagnetic environment, higher requirements are put forward for the sensitivity of radar reconnaissance equipment to receive signals. The research on radar polarization is getting more and more in-depth, and the requirements for antenna miniaturization and ultra-wideband are also increasing. It is urgent, and relevant research has attracted attention.
现有技术中,很少有天线能够同时实现小型化和超宽带,或者,能够同时实现小型化和超宽带,但是以牺牲天线增益为代价,使得天线的应用范围变窄,或是天线结构复杂,不易于设计和加工,成本造价高。In the prior art, there are few antennas that can achieve miniaturization and ultra-wideband at the same time, or can achieve miniaturization and ultra-wideband at the same time, but at the expense of antenna gain, the application range of the antenna is narrowed, or the antenna structure is complicated , is not easy to design and process, and the cost is high.
发明内容Contents of the invention
基于此,有必要针对上述技术问题,提供一种小型化超宽带天线,能够实现小型化超宽带天线,而不牺牲天线增益。Based on this, it is necessary to address the above technical problems and provide a miniaturized ultra-wideband antenna, which can realize a miniaturized ultra-wideband antenna without sacrificing antenna gain.
一种小型化超宽带天线,包括:天线单元;A miniaturized ultra-wideband antenna, comprising: an antenna unit;
所述天线单元包括:介质基板以及两个辐射贴片;两个所述辐射贴片均设在所述介质基板的正面;The antenna unit includes: a dielectric substrate and two radiation patches; the two radiation patches are both arranged on the front side of the dielectric substrate;
所述辐射贴片上设有多个槽缝;所述辐射贴片与所述槽缝关于所述介质基板的同一中心线呈轴对称分布;The radiation patch is provided with a plurality of slots; the radiation patch and the slots are distributed axially symmetrically with respect to the same center line of the dielectric substrate;
所述槽缝按照天线频点处表面电流最小或表面电流小于0.1A/m的电流路径分布。The slots are distributed according to the current path where the surface current at the frequency point of the antenna is the smallest or the surface current is less than 0.1A/m.
在一个实施例中,所述电流路径通过三次多项式拟合。In one embodiment, the current path is fitted by a cubic polynomial.
在一个实施例中,所述天线单元为Vivaldi天线。In one embodiment, the antenna unit is a Vivaldi antenna.
在一个实施例中,所述天线单元还包括:设在所述介质基板的正面的超表面透镜;In one embodiment, the antenna unit further includes: a metasurface lens disposed on the front surface of the dielectric substrate;
所述超表面透镜与两个所述辐射贴片间隔设置,且所述超表面透镜关于所述介质基板的一条中心线呈轴对称分布。The metasurface lens is spaced apart from the two radiation patches, and the metasurface lens is distributed axially symmetrically with respect to a central line of the dielectric substrate.
在一个实施例中,所述超表面透镜的折射率大于空气的折射率。In one embodiment, the refractive index of the metasurface lens is greater than that of air.
在一个实施例中,所述超表面透镜包括:多个阵列分布的超表面子镜;In one embodiment, the metasurface lens includes: a plurality of metasurface mirrors distributed in an array;
多个所述超表面子镜的数量沿着从介质基板边缘朝向介质基板中心线的方向呈斐波那契数列递增。The number of the plurality of metasurface mirrors increases along the direction from the edge of the dielectric substrate to the centerline of the dielectric substrate in a Fibonacci sequence.
在一个实施例中,所述超表面子镜包括:一个第一部分以及四个第二部分;In one embodiment, the metasurface mirror comprises: a first part and four second parts;
所述第一部分为正方环形结构;The first part is a square ring structure;
所述第二部分为条形结构;四个所述第二部分的一个对应端分别与所述正方环形结构的一边中点垂直相连,另一个对应端向远离所述第一部分的方向延伸。The second part is a bar-shaped structure; one corresponding end of the four second parts is vertically connected to the midpoint of one side of the square ring structure, and the other corresponding end extends away from the first part.
在一个实施例中,所述天线单元的数量为两个;In one embodiment, the number of the antenna units is two;
两个所述天线单元十字交叉相连。The two antenna units are cross-connected.
在一个实施例中,以沿着介质基板长度方向的中心线为对称轴,所述天线单元上还设有:沿着所述对称轴分布的插槽;In one embodiment, taking the centerline along the length direction of the dielectric substrate as the axis of symmetry, the antenna unit is further provided with: slots distributed along the axis of symmetry;
两个天线单元上插槽的方向相反,且两个天线单元上插槽的槽底相对抵接。The directions of the slots on the two antenna units are opposite, and the bottoms of the slots on the two antenna units are relatively abutted against each other.
在一个实施例中,所述天线单元还包括:设在所述介质基板的背面的馈电结构;In one embodiment, the antenna unit further includes: a feeding structure provided on the back of the dielectric substrate;
所述馈电结构包括:依次相连的扇形枝节、连接线以及微带馈电线,以形成巴伦结构。The feed structure includes: sequentially connected fan-shaped branches, connection lines and microstrip feed lines to form a balun structure.
上述小型化超宽带天线,在天线的辐射贴片上设置了契合电流路径的曲线槽缝,以改善对应频点附近的阻抗匹配,进而有针对性的降低低频处的S11,拓展带宽,而不牺牲天线增益。The above-mentioned miniaturized ultra-wideband antenna is equipped with curved slots that fit the current path on the radiation patch of the antenna to improve the impedance matching near the corresponding frequency point, and then reduce the S11 at the low frequency in a targeted manner to expand the bandwidth without sacrifice antenna gain.
附图说明Description of drawings
图1为一个实施例中一种小型化超宽带天线中天线单元的正面透视图;Fig. 1 is a front perspective view of an antenna unit in a miniaturized ultra-wideband antenna in one embodiment;
图2为一个实施例中一种小型化超宽带天线中天线单元的反面透视图;Fig. 2 is a reverse perspective view of the antenna unit in a miniaturized ultra-wideband antenna in one embodiment;
图3为一个实施例中一种小型化超宽带天线中天线单元的俯视图;Fig. 3 is a top view of the antenna unit in a miniaturized ultra-wideband antenna in one embodiment;
图4为一个实施例中一种小型化超宽带天线中天线单元的仰视图;Fig. 4 is a bottom view of the antenna unit in a miniaturized ultra-wideband antenna in one embodiment;
图5为一个实施例中一种小型化超宽带天线中两个天线单元的第一种示意图;Fig. 5 is a first schematic diagram of two antenna elements in a miniaturized ultra-wideband antenna in an embodiment;
图6为一个实施例中一种小型化超宽带天线中两个天线单元的第二种示意图;Fig. 6 is a second schematic diagram of two antenna elements in a miniaturized ultra-wideband antenna in an embodiment;
图7为一个实施例中一种小型化超宽带天线中两个天线单元的第三种示意图;Fig. 7 is a third schematic diagram of two antenna elements in a miniaturized ultra-wideband antenna in an embodiment;
图8为一个实施例中一种小型化超宽带天线的表面电流分布图,其中,(a)为4GHz处的表面电流分布,(b)为5.5GHz处的表面电流分布;Figure 8 is a surface current distribution diagram of a miniaturized ultra-wideband antenna in an embodiment, wherein (a) is the surface current distribution at 4GHz, and (b) is the surface current distribution at 5.5GHz;
图9为一个实施例中一种小型化超宽带天线中三次拟合曲线函数提取图,其中,(a)为表面电流曲线图,(b)为根据表面电流曲线提取的散点图,(c)为根据提取的散点图拟合的三次曲线图;Fig. 9 is a cubic fitting curve function extraction figure in a kind of miniaturized ultra-wideband antenna in one embodiment, wherein, (a) is the surface current curve figure, (b) is the scatter diagram extracted according to the surface current curve, (c ) is the cubic curve figure fitted according to the scatter plot extracted;
图10为一个实施例中一种小型化超宽带天线中拟合曲线槽缝和矩形槽缝的S11对比图;Fig. 10 is a S11 comparison diagram of a fitting curve slot and a rectangular slot in a miniaturized ultra-wideband antenna in one embodiment;
图11为一个实施例中一种小型化超宽带天线中超表面子镜的结构图,其中,(a)为俯视图,(b)为侧视图;Fig. 11 is a structural diagram of a metasurface sub-mirror in a miniaturized ultra-wideband antenna in an embodiment, wherein (a) is a top view, and (b) is a side view;
图12为一个实施例中一种小型化超宽带天线中四角钉型与十字型超表面子镜的折射率对比图;Fig. 12 is a comparison diagram of the refractive index of a four-cornered nail type and a cross-shaped metasurface sub-mirror in a miniaturized ultra-wideband antenna in one embodiment;
图13为一个实施例中一种小型化超宽带天线中超表面子镜的性能参数图;Fig. 13 is a performance parameter diagram of a metasurface mirror in a miniaturized ultra-wideband antenna in an embodiment;
图14为一个实施例中一种小型化超宽带天线中超表面子镜的不同排布方式下的增益对比图;Fig. 14 is a gain comparison diagram under different arrangements of metasurface mirrors in a miniaturized ultra-wideband antenna in one embodiment;
图15为一个实施例中一种小型化超宽带天线在超表面子镜和空气的界面处的入射和透射波;Fig. 15 is the incident and transmitted waves of a kind of miniaturized ultra-broadband antenna at the interface of metasurface mirror and air in one embodiment;
图16为一个实施例中一种小型化超宽带天线的S11和S22曲线图;FIG. 16 is a graph of S11 and S22 of a miniaturized ultra-wideband antenna in an embodiment;
图17为一个实施例中一种小型化超宽带天线的S12曲线图;Fig. 17 is an S12 curve diagram of a miniaturized ultra-wideband antenna in an embodiment;
图18为一个实施例中一种小型化超宽带天线的增益曲线图;FIG. 18 is a gain curve diagram of a miniaturized ultra-wideband antenna in an embodiment;
图19为一个实施例中一种小型化超宽带天线中两个天线单元在5 GHz的辐射方向图,其中,(a)为一个天线单元,(b)为另一个天线单元;Figure 19 is a radiation pattern diagram of two antenna elements at 5 GHz in a miniaturized ultra-wideband antenna in one embodiment, wherein (a) is one antenna element, and (b) is another antenna element;
图20为一个实施例中一种小型化超宽带天线中两个天线单元在9 GHz的辐射方向图,其中,(a)为一个天线单元,(b)为另一个天线单元;Fig. 20 is a radiation pattern diagram of two antenna elements in a miniaturized ultra-wideband antenna at 9 GHz in one embodiment, where (a) is one antenna element, and (b) is another antenna element;
图21为一个实施例中一种小型化超宽带天线中两个天线单元在13 GHz的辐射方向图,其中,(a)为一个天线单元,(b)为另一个天线单元。Fig. 21 is a radiation pattern at 13 GHz of two antenna units in a miniaturized ultra-wideband antenna in an embodiment, where (a) is one antenna unit, and (b) is another antenna unit.
附图标记说明:Explanation of reference signs:
介质基板1,辐射贴片2,槽缝3,超表面透镜4;Dielectric substrate 1, radiation patch 2, slot 3, metasurface lens 4;
扇形枝节51,连接线52,微带馈电线53。Fan-shaped branches 51, connection lines 52, and microstrip feed lines 53.
具体实施方式Detailed ways
为了使本申请的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本申请进行进一步详细说明。应当理解,此处描述的具体实施例仅仅用以解释本申请,并不用于限定本申请。基于本申请中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本申请保护的范围。In order to make the purpose, technical solution and advantages of the present application clearer, the present application will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain the present application, and are not intended to limit the present application. Based on the embodiments in this application, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the scope of protection of this application.
需要说明,本申请实施例中所有方向性指示(诸如上、下、左、右、前、后……)仅用于解释在某一特定姿态(如附图所示)下各部件之间的相对位置关系、运动情况等,如果该特定姿态发生改变时,则该方向性指示也相应地随之改变。It should be noted that all directional indications (such as up, down, left, right, front, back...) in the embodiments of the present application are only used to explain the relationship between the components in a certain posture (as shown in the figure). Relative positional relationship, movement conditions, etc., if the specific posture changes, the directional indication will also change accordingly.
另外,在本申请中如涉及“第一”、“第二”等的描述仅用于描述目的,而不能理解为指示或暗示其相对重要性或者隐含指明所指示的技术特征的数量。由此,限定有“第一”“第二”的特征可以明示或者隐含地包括至少一个该特征。在本申请的描述中,“多组”的含义是至少两组,例如两组,三组等,除非另有明确具体的限定。In addition, descriptions such as "first", "second" and so on in this application are used for description purposes only, and should not be understood as indicating or implying their relative importance or implicitly indicating the quantity of indicated technical features. Thus, a feature defined as "first" and "second" may explicitly or implicitly include at least one of the features. In the description of the present application, "multiple groups" means at least two groups, such as two groups, three groups, etc., unless specifically defined otherwise.
在本申请中,除非另有明确的规定和限定,术语“连接”、“固定”等应做广义理解,例如,“固定”可以是固定连接,也可以是可拆卸连接,或成一体;可以是机械连接,也可以是电连接,还可以是物理连接或无线通信连接;可以是直接相连,也可以通过中间媒介间接相连,可以是两个元件内部的连通或两个元件的相互作用关系,除非另有明确的限定。对于本领域的普通技术人员而言,可以根据具体情况理解上述术语在本申请中的具体含义。In this application, unless otherwise clearly specified and limited, the terms "connection" and "fixation" should be understood broadly, for example, "fixation" can be a fixed connection, a detachable connection, or an integral body; It can be a mechanical connection, an electrical connection, a physical connection or a wireless communication connection; it can be a direct connection or an indirect connection through an intermediary, it can be an internal connection between two components or an interaction relationship between two components, unless expressly defined otherwise. Those of ordinary skill in the art can understand the specific meanings of the above terms in this application according to specific situations.
另外,本申请各个实施例之间的技术方案可以相互结合,但是必须是以本领域普通技术人员能够实现为基础,当技术方案的结合出现相互矛盾或无法实现时应当认为这种技术方案的结合不存在,也不在本申请要求的保护范围之内。In addition, the technical solutions of the various embodiments of the present application can be combined with each other, but it must be based on the realization of those skilled in the art. When the combination of technical solutions is contradictory or cannot be realized, it should be considered as a combination of technical solutions. Does not exist, nor is it within the scope of protection required by this application.
本申请提供了一种小型化超宽带天线,如图1至图7所示,在一个实施例中,包括:天线单元。The present application provides a miniaturized ultra-wideband antenna, as shown in FIG. 1 to FIG. 7 , and in one embodiment, it includes: an antenna unit.
天线单元包括:一个介质基板1以及两个辐射贴片2;两个辐射贴片均设在介质基板的正面。The antenna unit includes: a dielectric substrate 1 and two radiation patches 2; the two radiation patches are both arranged on the front side of the dielectric substrate.
介质基板1采用的材料为Rogers5880,介电常数为2.2,损耗角正切为0.0009,介质基板的厚度为0.508mm。The material used for the dielectric substrate 1 is Rogers 5880, the dielectric constant is 2.2, the loss tangent is 0.0009, and the thickness of the dielectric substrate is 0.508 mm.
辐射贴片2上设有多个槽缝3;辐射贴片与槽缝关于介质基板的同一中心线呈轴对称分布。The radiation patch 2 is provided with a plurality of slots 3; the radiation patch and the slots are distributed axially symmetrically with respect to the same central line of the dielectric substrate.
槽缝3的数量、位置和形状按照表面电流最小或表面电流小于0.1A/m的电流路径分布。这种基于表面电流路径的槽缝结构,能够更有效地依附于辐射贴片,使得电流沿着槽缝流动的路径变得更长,延长了电流的有效路径,将能量约束在槽缝附近,很好地改善对应频点附近的阻抗匹配,进而有针对性的降低低频处的S11,拓展带宽,并实现了小型化。The number, position and shape of the slots 3 are distributed according to the current path with the minimum surface current or a surface current less than 0.1A/m. This slot structure based on the surface current path can be more effectively attached to the radiation patch, making the path of the current flowing along the slot longer, extending the effective path of the current, and confining the energy near the slot. The impedance matching near the corresponding frequency point is well improved, and then the S11 at the low frequency is reduced in a targeted manner, the bandwidth is expanded, and miniaturization is realized.
具体地,对天线相应频点处(要降低频点处)的表面电流进行路径分析,选取表面电流最小或表面电流小于0.1A/m的电流路径曲线,通常情况下,曲线关于天线呈轴对称分布。槽缝的数量、位置和形状分别与天线对应频点处表面电流最小路径的数量、位置和形状相同,或者,槽缝的数量、位置和形状分别与天线对应频点处表面电流小于0.1A/m路径的数量、位置和形状相同。需要说明,当不同频点处的一个以上电流路径重合时,电流路径的数量不重复计算,对应位置仅设置一个槽缝即可。Specifically, analyze the path of the surface current at the corresponding frequency point of the antenna (at the point where the frequency is to be reduced), and select the current path curve with the smallest surface current or a surface current less than 0.1A/m. Usually, the curve is axisymmetric with respect to the antenna distributed. The number, position and shape of the slots are the same as the number, position and shape of the minimum path of the surface current at the corresponding frequency point of the antenna, or the number, position and shape of the slots are respectively the same as the surface current at the corresponding frequency point of the antenna is less than 0.1A/ The m paths are the same in number, location and shape. It should be noted that when more than one current path at different frequency points overlaps, the number of current paths is not counted repeatedly, and only one slot is required for the corresponding position.
优选地,电流路径通过曲线拟合。Preferably, the current path is by curve fitting.
进一步优选地,电流路径通过三次多项式曲线拟合,三次多项式曲线通过三次多项式拟合函数得到,以最大限度的改善对应频点附近的阻抗匹配,这种三次多项式曲线拟合的槽缝结构更加契合电流路径,更好拓展带宽。Further preferably, the current path is fitted by a cubic polynomial curve, and the cubic polynomial curve is obtained by a cubic polynomial fitting function, so as to maximize the impedance matching near the corresponding frequency point, and the slot structure of this cubic polynomial curve fitting fits better The current path can better expand the bandwidth.
更进一步优选地,天线单元为Vivaldi天线,以两个辐射贴片作为Vivaldi天线的两个辐射臂,从而进一步拓展带宽,提高增益和定向辐射能力。传统的Vivaldi天线为了获得良好的性能需要较大的尺寸,限制了Vivaldi天线的应用范围,而本申请在Vivaldi天线上设计了契合电流路径的槽缝,因此相当于在超宽带的基础上进一步实现了小型化。Further preferably, the antenna unit is a Vivaldi antenna, and two radiation patches are used as two radiation arms of the Vivaldi antenna, so as to further expand the bandwidth, improve the gain and directional radiation capability. The traditional Vivaldi antenna requires a large size in order to obtain good performance, which limits the application range of the Vivaldi antenna. However, this application designs a slot on the Vivaldi antenna that fits the current path, so it is equivalent to a further realization on the basis of ultra-wideband miniaturization.
上述小型化超宽带天线,在天线的辐射贴片上设置了契合电流路径的曲线槽缝,以最大程度改善对应频点附近的阻抗匹配,进而有针对性的降低低频处的S11,在不牺牲增益的前提下拓展带宽。The above-mentioned miniaturized ultra-wideband antenna is equipped with curved slots that fit the current path on the radiation patch of the antenna, so as to improve the impedance matching near the corresponding frequency point to the greatest extent, and then reduce the S11 at low frequencies in a targeted manner without sacrificing Expand the bandwidth under the premise of gain.
在一个实施例中,天线单元还包括:设在介质基板的正面的超表面透镜4;超表面透镜与两个辐射贴片间隔设置,且超表面透镜关于介质基板的一条中心线呈轴对称分布。In one embodiment, the antenna unit further includes: a metasurface lens 4 arranged on the front side of the dielectric substrate; the metasurface lens is spaced from two radiation patches, and the metasurface lens is distributed axially symmetrically with respect to a center line of the dielectric substrate .
优选地,超表面透镜的折射率大于空气的折射率。Preferably, the refractive index of the metasurface lens is greater than that of air.
进一步优选地,超表面透镜包括:多个间隔阵列分布的超表面子镜;多个超表面子镜的数量沿着从介质基板边缘朝向介质基板中心线的方向呈斐波那契数列递增,以形成相位补偿透镜结构,增强波束的方向性,从而提高天线增益,尤其是在高频处的增益提升明显。Further preferably, the metasurface lens includes: a plurality of metasurface submirrors distributed in an array at intervals; the number of the plurality of metasurface submirrors increases in a Fibonacci sequence along the direction from the edge of the medium substrate toward the centerline of the medium substrate, to A phase compensation lens structure is formed to enhance the directivity of the beam, thereby increasing the antenna gain, especially at high frequencies.
更进一步优选地,超表面子镜包括:一个第一部分以及四个第二部分;第一部分为正方环形结构;第二部分为条形结构;四个第二部分的一个对应端分别与正方环形结构的一边中点垂直相连,另一个对应端向远离第一部分的方向延伸。四角钉型的超表面透镜能够提高天线的增益,同时不增加天线的尺寸,从而在提高了增益的同时实现小型化。需要说明,第一部分与第二部分的宽度相等,第一部分的内环边长与第二部分的长度相等,以实现更高的增益。Still further preferably, the metasurface sub-mirror includes: a first part and four second parts; the first part is a square ring structure; the second part is a strip structure; a corresponding end of the four second parts is respectively connected to the square ring structure The midpoints of one side are vertically connected, and the other corresponding end extends away from the first part. The four-cornered spike-shaped metasurface lens can increase the gain of the antenna without increasing the size of the antenna, thereby achieving miniaturization while increasing the gain. It should be noted that the width of the first part is equal to that of the second part, and the inner ring side length of the first part is equal to the length of the second part, so as to achieve higher gain.
在一个实施例中,天线单元的数量为两个;两个天线单元十字交叉相连。In one embodiment, the number of antenna units is two; the two antenna units are connected in a cross.
优选地,以沿着介质基板长度方向的中心线为对称轴,天线单元上还设有:沿着对称轴分布的插槽;两个天线单元上插槽的方向相反,且两个天线单元上插槽的槽底相对抵接。Preferably, taking the center line along the length direction of the dielectric substrate as the axis of symmetry, the antenna unit is further provided with: slots distributed along the axis of symmetry; the directions of the slots on the two antenna units are opposite, and the slots on the two antenna units are The groove bottoms of the slots are relatively abutted.
上述设置使天线成为双极化天线,能够实现双极化,接收所有的极化信息,具有较强的抗干扰能力,因而可以提高系统的灵敏度,更适用于雷达系统等工程应用。The above settings make the antenna a dual-polarization antenna, which can achieve dual polarization, receive all polarization information, and has strong anti-interference ability, so it can improve the sensitivity of the system and is more suitable for engineering applications such as radar systems.
在一个实施例中,天线单元还包括:设在介质基板的正面的圆形空腔结构以及设在介质基板的背面的馈电结构;馈电结构包括:依次相连的扇形枝节51、连接线52以及微带馈电线53,以形成巴伦结构,从而改善天线阻抗匹配。In one embodiment, the antenna unit further includes: a circular cavity structure arranged on the front of the dielectric substrate and a feeding structure arranged on the back of the dielectric substrate; the feeding structure includes: sequentially connected fan-shaped branches 51, connecting wires 52 And the microstrip feeder 53 to form a balun structure, so as to improve the impedance matching of the antenna.
优选地,微带馈电线采用梯形结构,以实现更好的阻抗匹配。Preferably, the microstrip feeder adopts a trapezoidal structure to achieve better impedance matching.
需要说明,天线采用巴伦结构馈电,馈电端口阻抗为50欧姆,与SMA接口匹配。It should be noted that the antenna is fed by a balun structure, and the impedance of the feed port is 50 ohms, which matches the SMA interface.
在一个具体的实施例中,通过对要降低的目标频点的表面电流的分析和多次取点拟合,得到三次多项式拟合曲线函数:,其中,s为比例系数,通过现有技术计算得到s=2.76841。每个辐射贴片上槽缝的数量为4个,槽缝宽度为4mm,槽缝位置契合电流分布,插槽宽度选择为0.65mm。In a specific embodiment, by analyzing the surface current of the target frequency point to be reduced and fitting multiple times, a cubic polynomial fitting curve function is obtained: , where s is a proportionality coefficient, and s=2.76841 is obtained through prior art calculations. The number of slots on each radiation patch is 4, and the slot width is 4 mm. The position of the slots fits the current distribution, and the slot width is selected as 0.65 mm.
使用电磁全波仿真软件CST对上述天线进行仿真分析和优化,对其结构参数、S11参数、S21参数、天线的增益以及辐射方向图进行了研究。Using the electromagnetic full-wave simulation software CST to simulate and optimize the above-mentioned antenna, its structural parameters, S11 parameters, S21 parameters, antenna gain and radiation pattern are studied.
对于单极化天线,其整体尺寸为,空间体积仅0.3299λ2(mm2),其中,λ是带宽范围内最低频率下的波长,带宽范围2.07-13.86GHz,带宽为148%,增益为12.32dBi。For a single-polarized antenna, its overall dimensions are , the space volume is only 0.3299λ 2 (mm 2 ), where λ is the wavelength at the lowest frequency within the bandwidth range, the bandwidth range is 2.07-13.86GHz, the bandwidth is 148%, and the gain is 12.32dBi.
如图8所示,设计的天线在4GHz处和5.5GHz附近的S11参数大于-10dB,此时设计的天线没有很好的带宽特性,特别在低频处。给出在4GHz处和5.5GHz处的表面电流分布如图8(a)和图8(b)所示,在天线边缘进行波纹处理,根据三次多项式曲线拟合设计槽缝,改变表面电流的路径,将能量更好的约束到槽缝附近,三次多项式曲线拟合的槽缝契合电流路径,以最大限度的改善4GHz和5.5GHz附近的阻抗匹配特性,降低低频阻抗带宽,从而拓展带宽,实现小型化。As shown in Figure 8, the S11 parameters of the designed antenna at 4GHz and 5.5GHz are greater than -10dB. At this time, the designed antenna does not have good bandwidth characteristics, especially at low frequencies. Given the surface current distribution at 4GHz and 5.5GHz, as shown in Figure 8(a) and Figure 8(b), the ripple treatment is performed on the edge of the antenna, and the slot is designed according to the cubic polynomial curve fitting to change the path of the surface current , to better confine the energy to the vicinity of the slots, and the slots fitted by the cubic polynomial curve fit the current path to maximize the impedance matching characteristics near 4GHz and 5.5GHz, reduce the low-frequency impedance bandwidth, thereby expanding the bandwidth and realizing small size change.
如图9所示,进行三次拟合曲线函数提取,具体地:将4GHz处及5.5GHz处需要延长的电流路径转换成曲线如图9(a)所示,通过提取得到如图9(b)所示散点图,将曲线等效转换为数据点,最终将5条曲线拟合为一条三次多项式拟合函数曲线如图9(c),依据上述函数,设计了一种基于电流路径的拟合曲线槽缝Vivaldi天线,相较于传统矩形槽缝加载,拟合曲线槽缝能够更有效地依附于辐射臂结构,使得电流沿着缝隙流动的路径变得更长,延长了电流的有效路径,改善特定频点附近的阻抗匹配,进而有针对性的降低低频处的S11,拓展带宽。As shown in Figure 9, three fitting curve function extractions are performed, specifically: the current paths that need to be extended at 4GHz and 5.5GHz are converted into curves as shown in Figure 9(a), and obtained through extraction as shown in Figure 9(b) As shown in the scatter diagram, the curves are equivalently converted into data points, and finally the five curves are fitted into a cubic polynomial fitting function curve as shown in Figure 9(c). Fitting curve slot Vivaldi antenna, compared with traditional rectangular slot loading, fitting curve slot can be more effectively attached to the radiation arm structure, making the path of current flowing along the slot longer and extending the effective path of current , improve the impedance matching near a specific frequency point, and then reduce the S11 at the low frequency in a targeted manner, and expand the bandwidth.
如图10所示,给出了基于电流路径的三次多项式拟合曲线槽缝和对应矩形槽缝的S11对比图。仿真结果显示,矩形槽缝的带宽范围为2.27GHz-13GHz,而拟合曲线槽缝的带宽范围为2.07GHz-13.86GHz。由此可见,拟合曲线槽缝对带宽的拓展作用更明显,带宽范围在低频处降低了0.2GHz,在高频处提高了0.86GHz,相比而言整个带宽增加了8%。As shown in FIG. 10 , a comparison diagram of S11 between a cubic polynomial fitting curve slot based on a current path and a corresponding rectangular slot is given. The simulation results show that the bandwidth range of the rectangular slot is 2.27GHz-13GHz, and the bandwidth range of the fitting curve slot is 2.07GHz-13.86GHz. It can be seen that the fitting curve slot has a more obvious effect on expanding the bandwidth. The bandwidth range is reduced by 0.2 GHz at low frequencies and increased by 0.86 GHz at high frequencies, compared to an increase of 8% in the entire bandwidth.
如图11所示,设计了四角钉型的相位补偿的超表面子镜结构,其中,宽度都为0.15mm,正方环形结构的边长为1.2mm,钉型(即条形结构)的长度为0.9mm,间距为0.1mm,将该结构设计集成到天线介质基板上作为相位补偿透镜结构来保持小型化的优势,同时提高高频处的增益。四角钉型超表面子镜与十字型超表面子镜的折射率如图12所示。As shown in Figure 11, a four-cornered nail-shaped phase-compensated metasurface submirror structure is designed, in which the width is 0.15mm, the side length of the square ring structure is 1.2mm, and the length of the nail-shaped (ie, bar-shaped structure) is 0.9mm, with a pitch of 0.1mm, the structure design is integrated on the antenna dielectric substrate as a phase compensation lens structure to maintain the advantages of miniaturization while improving the gain at high frequencies. The refractive indices of the four-cornered nail-shaped metasurface mirror and the cross-shaped metasurface mirror are shown in Fig. 12 .
如图13所示,在CST中对该超表面子镜进行频域仿真得到性能参数,在2-14GHz的带宽范围内,,完全覆盖了设计天线的工作频带,即增加的超表面子镜的工作带宽不会影天线的超宽带特性。S12的值接近0,表明设计的超表面子镜的预期损失几乎可以忽略不计。同时,超表面子镜的折射率大于4.45,这使得设计的超表面透镜有大于空气的折射率,能够增强波束的方向性。As shown in Figure 13, the frequency domain simulation of the metasurface submirror in CST is performed to obtain performance parameters. In the bandwidth range of 2-14GHz, , which completely covers the working frequency band of the designed antenna, that is, the increased working bandwidth of the metasurface mirror will not affect the ultra-wideband characteristics of the antenna. The value of S12 is close to 0, indicating that the expected loss of the designed metasurface submirror is almost negligible. At the same time, the refractive index of the metasurface mirror is greater than 4.45, which makes the designed metasurface lens have a refractive index greater than that of air, which can enhance the directivity of the beam.
如图14所示,天线的超表面子镜呈斐波那契数列排布(实线)和等差数列排布(虚线)的对比图。由图14可以看出,当呈等差数列排布时,超表面子镜个数一共为72个;当呈斐波那契数列排布时,超表面子镜个数为66个。斐波那契数列排布方式在超表面子镜个数少了6个的同时,在高频处的增益更高,最高可以增加0.2dBi。这种排布方式相比之下更为优越。As shown in Figure 14, the comparison diagram of the arrangement of the metasurface mirrors of the antenna in Fibonacci sequence (solid line) and arithmetic sequence arrangement (dotted line). It can be seen from FIG. 14 that when arranged in an arithmetic sequence, the number of metasurface mirrors is 72; when arranged in a Fibonacci sequence, the number of metasurface mirrors is 66. The Fibonacci sequence arrangement reduces the number of metasurface sub-mirrors by 6, and at the same time, the gain at high frequencies is higher, which can increase by up to 0.2dBi. This arrangement is superior in comparison.
如图15所示,为电磁波在超表面透镜与空气界面处的传播示意图。将超表面子镜放置在天线的辐射臂之间的主要目的是设计有效折射率n大于的有效表面。具有折射率/>和/>的两种介质之间的界面处的入射波和透射波在两个界面处的波之间的关系可以由公式/>表示。当/>大于/>时,空气中的折射角/>大于透镜中的入射角/>,使得电场集中在天线孔径的中心,从而提高天线的方向性。As shown in FIG. 15 , it is a schematic diagram of propagation of electromagnetic waves at the interface between the metasurface lens and air. The main purpose of placing the metasurface mirror between the radiating arms of the antenna is to design an effective refractive index n greater than effective surface. Has a refractive index /> and /> The relationship between the incident wave at the interface between two media and the transmitted wave at the two interfaces can be given by the formula /> express. when /> greater than /> , the angle of refraction in air /> greater than the angle of incidence in the lens /> , so that the electric field is concentrated in the center of the antenna aperture, thereby improving the directivity of the antenna.
如图16所示,对双极化天线(更具体说,是双极化超表面透镜拟合曲线槽缝Vivaldi天线)进行仿真,得到仿真图。由图16可以看出,双极化天线的带宽为2.17GHz-13.7GHz,两个双极化天线单元与单极化天线的S11略有差异,这和双极化开槽缝对表面电流的改变有关,电流的改变使天线带宽略有减小。其工作带宽达到了145.3%,属于超宽带天线。As shown in FIG. 16 , the dual-polarization antenna (more specifically, the dual-polarization metasurface lens fitting curve slot Vivaldi antenna) is simulated to obtain a simulation diagram. It can be seen from Figure 16 that the bandwidth of the dual-polarized antenna is 2.17GHz-13.7GHz, and the S11 of the two dual-polarized antenna units is slightly different from that of the single-polarized antenna, which is similar to the effect of the dual-polarized slot on the surface current. A change in the current slightly reduces the antenna bandwidth. Its working bandwidth has reached 145.3%, which belongs to ultra-wideband antenna.
如图17所示,对双极化超表面透镜拟合曲线槽缝Vivaldi天线进行仿真,得到仿真S12图。可以看出,双极化天线的隔离度在整个带宽范围内小于-25dB,在80%以上的工作范围内小于-30dB,有较好的隔离特性。As shown in Fig. 17, the simulation of the dual-polarization metasurface lens fitting curve slot Vivaldi antenna is carried out, and the simulation S12 diagram is obtained. It can be seen that the isolation of the dual-polarized antenna is less than -25dB in the entire bandwidth range, and less than -30dB in more than 80% of the working range, which has good isolation characteristics.
图18给出了双极化天线的增益曲线图,以两个天线单元分别为仿真单元1和仿真单元2,可以看出天线的增益在2GHz到14GHz里,最低增益为5.25dBi左右,最高增益为12.32dBi。相比未加超表面透镜的天线,本申请在高频处增益提升明显,最高可以提升0.81dBi。Figure 18 shows the gain curve of the dual-polarized antenna. The two antenna units are simulation unit 1 and simulation unit 2 respectively. It can be seen that the gain of the antenna is between 2GHz and 14GHz, the lowest gain is about 5.25dBi, and the highest gain is It is 12.32dBi. Compared with the antenna without the metasurface lens, the gain of this application is significantly improved at high frequencies, up to 0.81dBi.
图19至图21给出了本申请在工作频带内不同频点的一个天线单元的辐射方向图和另一个天线单元的辐射方向图,从方向图中可以看出一个天线单元和另一个天线单元的的辐射方向图都呈定向辐射特性,证明天线的辐射性能良好。且一个天线单元的和另一个天线单元的方向图略有差异但整体相差不大,差异是由于组成十字交叉双极化天线时,所开插槽不同,导致天线单元的结构略有差异造成的。但天线整体结构相似,使得天线的辐射方向图主波束差别不大。Figures 19 to 21 show the radiation pattern of one antenna unit and the radiation pattern of another antenna unit at different frequency points in the working frequency band of the present application. It can be seen from the pattern that one antenna unit and another antenna unit The radiation patterns of the antennas all show directional radiation characteristics, which proves that the radiation performance of the antenna is good. And the pattern of one antenna unit is slightly different from that of the other antenna unit, but the overall difference is not large. The difference is due to the difference in the slots opened when the cross-cross dual-polarized antenna is formed, resulting in a slight difference in the structure of the antenna unit. . However, the overall structure of the antenna is similar, so that the radiation pattern of the antenna has little difference in the main beam.
综上,本申请的天线,设计了契合电流路径的拟合曲线槽缝,利用契合表面电流路径的波纹边缘结构来更加有效的降低对应频点处的S11,最大限度的改善对应频点处的阻抗匹配,拓展带宽,工作频带为2.17GHz-13.7GHz,带宽达到145.3%,整体尺寸为,空间体积仅/>,天线增益在工作频段为5.25dBi-12.32dBi,最高增益达到12.32dBi,隔离度在整个带宽范围内小于-30dB,在80%以上带宽范围内小于-35dB,有较好的隔离特性,S11在天线带宽内小于-15dB,S21基本为0,因而不会对原天线带宽造成影响,该超表面透镜的折射率在4.45-4.55之间,有折射特性。同时,通过增加相位补偿透镜,在未增大尺寸不影响天线小型化的同时增加天线的增益,特别是在高频处的增益。另外,本申请中天线具有较高的增益和隔离度,使得天线适合应用于极化敏感度高的场景,天线的空间尺寸仅为/>,尺寸较小、加工简单、便于携带,实现了天线的小型化,可应用于雷达侦察系统等应用场景。To sum up, the antenna of this application is designed with a fitting curve slot that fits the current path, and utilizes the corrugated edge structure that fits the surface current path to more effectively reduce the S11 at the corresponding frequency point and improve the S11 at the corresponding frequency point to the greatest extent. Impedance matching, extended bandwidth, the working frequency band is 2.17GHz-13.7GHz, the bandwidth reaches 145.3%, and the overall size is , the space volume is only /> , the antenna gain is 5.25dBi-12.32dBi in the working frequency band, the highest gain reaches 12.32dBi, the isolation is less than -30dB in the entire bandwidth range, and less than -35dB in the bandwidth range of more than 80%, which has good isolation characteristics. The antenna bandwidth is less than -15dB, and S21 is basically 0, so it will not affect the original antenna bandwidth. The refractive index of the metasurface lens is between 4.45-4.55, and has refraction characteristics. At the same time, by adding a phase compensation lens, the gain of the antenna, especially the gain at high frequencies, is increased without increasing the size and affecting the miniaturization of the antenna. In addition, the antenna in this application has high gain and isolation, making the antenna suitable for use in scenarios with high polarization sensitivity, and the spatial size of the antenna is only /> , small in size, easy to process, easy to carry, realizes the miniaturization of the antenna, and can be applied to application scenarios such as radar reconnaissance systems.
以上实施例的各技术特征可以进行任意的组合,为使描述简洁,未对上述实施例中的各个技术特征所有可能的组合都进行描述,然而,只要这些技术特征的组合不存在矛盾,都应当认为是本说明书记载的范围。The technical features of the above embodiments can be combined arbitrarily. To make the description concise, all possible combinations of the technical features in the above embodiments are not described. However, as long as there is no contradiction in the combination of these technical features, they should be It is considered to be within the range described in this specification.
以上所述实施例仅表达了本申请的几种实施方式,其描述较为具体和详细,但并不能因此而理解为对本申请专利范围的限制。应当指出的是,对于本领域的普通技术人员来说,在不脱离本申请构思的前提下,还可以做出若干变形和改进,这些都属于本申请的保护范围。因此,本申请专利的保护范围应以所附权利要求为准。The above-mentioned embodiments only express several implementation modes of the present application, and the description thereof is relatively specific and detailed, but should not be construed as limiting the patent scope of the present application. It should be noted that those skilled in the art can make several modifications and improvements without departing from the concept of the present application, and these all belong to the protection scope of the present application. Therefore, the scope of protection of the patent application should be based on the appended claims.
Claims (10)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202310817929.2A CN116565533B (en) | 2023-07-05 | 2023-07-05 | Miniaturized ultra-wideband antenna |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202310817929.2A CN116565533B (en) | 2023-07-05 | 2023-07-05 | Miniaturized ultra-wideband antenna |
Publications (2)
Publication Number | Publication Date |
---|---|
CN116565533A true CN116565533A (en) | 2023-08-08 |
CN116565533B CN116565533B (en) | 2023-09-01 |
Family
ID=87502145
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202310817929.2A Active CN116565533B (en) | 2023-07-05 | 2023-07-05 | Miniaturized ultra-wideband antenna |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN116565533B (en) |
Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH09246849A (en) * | 1996-03-05 | 1997-09-19 | Mitsubishi Electric Corp | Taper slot antenna |
GB0322148D0 (en) * | 2003-09-22 | 2003-10-22 | Thales Plc | An antenna |
KR101697356B1 (en) * | 2016-02-02 | 2017-01-18 | 광운대학교 산학협력단 | Wideband reconfigurable antenna with expanding frequency variable range |
CN107317106A (en) * | 2017-07-05 | 2017-11-03 | 中国人民解放军国防科学技术大学 | Wide band miniaturization Vivaldi antennas can be achieved in one kind |
WO2020244635A1 (en) * | 2019-06-06 | 2020-12-10 | 昆山瀚德通信科技有限公司 | Single-polarized antenna |
CN212366198U (en) * | 2020-07-14 | 2021-01-15 | 湖南大学 | Ultra Wideband Vivaldi Antenna |
US11114766B1 (en) * | 2020-03-05 | 2021-09-07 | Ixi Technology Holdings, Inc. | Tapered slot antenna |
CN113889765A (en) * | 2021-10-19 | 2022-01-04 | 中国人民解放军63660部队 | Method for expanding lower limit of working frequency band of coplanar Vivaldi antenna |
CN114843775A (en) * | 2022-05-30 | 2022-08-02 | 重庆邮电大学 | Novel Palm Leaf Coplanar Vivaldi Array Antenna and Unit Design |
CN115810909A (en) * | 2023-02-09 | 2023-03-17 | 湖南大学 | Array-forming miniaturized antenna for 5G |
-
2023
- 2023-07-05 CN CN202310817929.2A patent/CN116565533B/en active Active
Patent Citations (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH09246849A (en) * | 1996-03-05 | 1997-09-19 | Mitsubishi Electric Corp | Taper slot antenna |
GB0322148D0 (en) * | 2003-09-22 | 2003-10-22 | Thales Plc | An antenna |
KR101697356B1 (en) * | 2016-02-02 | 2017-01-18 | 광운대학교 산학협력단 | Wideband reconfigurable antenna with expanding frequency variable range |
CN107317106A (en) * | 2017-07-05 | 2017-11-03 | 中国人民解放军国防科学技术大学 | Wide band miniaturization Vivaldi antennas can be achieved in one kind |
WO2020244635A1 (en) * | 2019-06-06 | 2020-12-10 | 昆山瀚德通信科技有限公司 | Single-polarized antenna |
US11114766B1 (en) * | 2020-03-05 | 2021-09-07 | Ixi Technology Holdings, Inc. | Tapered slot antenna |
CN212366198U (en) * | 2020-07-14 | 2021-01-15 | 湖南大学 | Ultra Wideband Vivaldi Antenna |
CN113889765A (en) * | 2021-10-19 | 2022-01-04 | 中国人民解放军63660部队 | Method for expanding lower limit of working frequency band of coplanar Vivaldi antenna |
CN114843775A (en) * | 2022-05-30 | 2022-08-02 | 重庆邮电大学 | Novel Palm Leaf Coplanar Vivaldi Array Antenna and Unit Design |
CN115810909A (en) * | 2023-02-09 | 2023-03-17 | 湖南大学 | Array-forming miniaturized antenna for 5G |
Non-Patent Citations (3)
Title |
---|
CHENSONGMIN ET AL.: "A Miniaturized UWB High-Gain Vivaldi Antenna", 2022 INTERNATIONAL APPLIED COMPUTATIONAL ELECTROMAGNETICS SOCIETY SYMPOSIUM (ACES-CHINA) * |
刘红喜;高军;李思佳;张迪;: "Y形缝隙加载小型化超宽带Vivaldi端射天线", 空军工程大学学报(自然科学版), no. 02 * |
李冰: "具有带阻和双频特性的频率可重构天线的研究与设计", 中国优秀硕士学位论文全文数据库 * |
Also Published As
Publication number | Publication date |
---|---|
CN116565533B (en) | 2023-09-01 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US8451189B1 (en) | Ultra-wide band (UWB) artificial magnetic conductor (AMC) metamaterials for electrically thin antennas and arrays | |
Bai et al. | Modified compact antipodal Vivaldi antenna for 4–50-GHz UWB application | |
TWI420738B (en) | Dual polarization antenna structure, radome and design method thereof | |
US7050013B2 (en) | Ultra-wideband planar antenna having frequency notch function | |
CN110380217A (en) | High-gain end-on-fire antenna based on artificial surface plasmon | |
CN105048080B (en) | A kind of omni-directional circular polarization plane antenna based on electro magnetic dipole | |
Nakmouche et al. | Development of a high gain FSS reflector backed monopole antenna using machine learning for 5G applications | |
CN107134648A (en) | A kind of wideband dual polarized electromagnetic dipole antenna of L-band | |
Kim et al. | Compact ultrawideband antenna on folded ground plane | |
CN105071052A (en) | Planar complementation oscillator circularly polarized antenna | |
CN211530188U (en) | Novel end-fire antenna based on split ring resonator | |
TWI245454B (en) | Low sidelobes dual band and broadband flat endfire antenna | |
CN210443662U (en) | Novel K-band high-gain metamaterial microstrip antenna | |
CN109411886B (en) | Broadband high-gain pattern reconfigurable antenna and communication equipment | |
Jizat et al. | Compact size of CPW dual-band meander-line transparent antenna for WLAN applications | |
CN110429379A (en) | With symmetrical and difference beam gap coupling short paster antenna | |
CN108400429A (en) | A kind of ultra wideband dual polarization antenna | |
CN115810909B (en) | A small-size antenna of can arraying for 5G | |
CN116565533B (en) | Miniaturized ultra-wideband antenna | |
CN116598757B (en) | A counter-heel Vivaldi antenna loaded with parasitic structures | |
CN111697326A (en) | Ultra-wideband Vivaldi antenna | |
CN111342240A (en) | Three-dimensional microwave absorber based on coupling gap structure and application thereof | |
KR100449857B1 (en) | Wideband Printed Dipole Antenna | |
Khan et al. | A Compact 28 GHz Millimeter Wave Antenna for Future Wireless Communication. | |
CN211017384U (en) | A multi-beam holographic antenna loaded with matching structure |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |