CN113161730B - Orthogonal mode-based planar compact low-coupling quad-polarized MIMO antenna - Google Patents
Orthogonal mode-based planar compact low-coupling quad-polarized MIMO antenna Download PDFInfo
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Abstract
本发明公开了一种基于正交模式的平面紧凑型低耦合四极化MIMO天线,包括基于正交模式的第一辐射体和第二辐射体,所述第一辐射体采用环状结构,所述第二辐射体采用微带贴片结构,在第一辐射体上获得电偶极子(Ex)和磁偶极子(Hz)的辐射模式,在第二辐射体获得两种正交的TM11微带天线模式(Hx、Hy)。本发明充分利用了第一辐射体的内部空间,将第二辐射体置于第一辐射体内,在平面结构内获得四种极化模式,具有结构紧凑、低耦合等特性;通过分形结构降低第二辐射体TM11模式工作频率,与第一辐射体工作于同一频带。本发明有效利用电磁场矢量特性,通过紧凑的结构可以在多径丰富的传播环境中获得大于3×3、接近4×4独立同分布瑞利信道的信道容量。
The invention discloses a plane compact low-coupling quad-polarized MIMO antenna based on an orthogonal mode, comprising a first radiator and a second radiator based on the orthogonal mode, and the first radiator adopts a ring structure, so the The second radiator adopts a microstrip patch structure, and the radiation modes of electric dipole (Ex) and magnetic dipole (Hz) are obtained on the first radiator, and two orthogonal TM11 are obtained on the second radiator Microstrip antenna patterns (Hx, Hy). The invention makes full use of the inner space of the first radiator, places the second radiator in the first radiator, obtains four polarization modes in the plane structure, and has the characteristics of compact structure and low coupling; The working frequency of the TM11 mode of the two radiators is in the same frequency band as the first radiator. The invention effectively utilizes the electromagnetic field vector characteristics, and can obtain a channel capacity greater than 3×3 and close to 4×4 IID Rayleigh channels in a multipath-rich propagation environment through a compact structure.
Description
技术领域technical field
本发明涉及一种天线,特别是一种基于正交模式的平面紧凑型低耦合四极化MIMO天线,可以用于无线通信、大规模MIMO天线阵等领域。The invention relates to an antenna, in particular to a plane compact low-coupling quad-polarized MIMO antenna based on an orthogonal mode, which can be used in the fields of wireless communication, massive MIMO antenna array and the like.
背景技术Background technique
随着无线通信技术的蓬勃发展,频谱资源日趋紧张,尽可能地开发利用现有的频段、提高频谱利用率成为必然趋势。多输入多输出(Multiple-Input Multiple-Output,简称MIMO)技术通过在发射端和接收端分别使用多个发射天线和接收天线,可以建立多个并行的空间子信道,在不增加频谱资源和天线发射功率的情况下,可以成倍提高系统信道质量。近年来,随着5G及下一代移动通信系统中大规模和超大规模MIMO技术的发展,基站及移动终端对天线体积、质量等要求愈来愈高,天线设计向小型化、紧凑型、便携化方向改进,人们迫切需要紧凑型小型化的天线来满足日益增长的市场需求,采用极化分集技术的多极化MIMO天线技术被提出并被证明可以很好地解决这个问题。With the vigorous development of wireless communication technology, spectrum resources are becoming increasingly tight, and it has become an inevitable trend to develop and utilize existing frequency bands as much as possible and improve spectrum utilization. Multiple-Input Multiple-Output (MIMO) technology can establish multiple parallel spatial sub-channels by using multiple transmit and receive antennas at the transmitter and receiver respectively, without increasing spectrum resources and antennas. In the case of transmit power, the system channel quality can be doubled. In recent years, with the development of large-scale and ultra-large-scale MIMO technology in 5G and next-generation mobile communication systems, base stations and mobile terminals have higher and higher requirements for antenna volume and quality, and antenna designs are becoming smaller, more compact, and more portable. With the improvement of the direction, people urgently need compact and miniaturized antennas to meet the growing market demand. The multi-polarization MIMO antenna technology using polarization diversity technology has been proposed and proved to be able to solve this problem well.
多极化天线,也称为矢量天线,可以通过利用空间中所有六个电磁场Ex、Ey、Ez、Hx、Hy、Hz矢量分量在丰富的散射环境中提供最多六个自由度,可以使MIMO天线以空间共点的形式形成多个独立的并行子信道,因此是实现紧凑型MIMO天线阵的一种重要技术。由于实现共点正交、低耦合、结构紧凑的多极化天线比较困难,目前已有的多极化天线多采用双极化和三极化天线的设计,而对四极化以及更多重极化的天线设计则相对较少。Multi-polarized antennas, also known as vector antennas, can make MIMO antennas possible by exploiting all six vector components of the electromagnetic fields Ex, Ey, Ez, Hx, Hy, Hz in space to provide up to six degrees of freedom in a rich scattering environment Forming multiple independent parallel sub-channels in the form of spatial co-location is therefore an important technique for realizing compact MIMO antenna arrays. Due to the difficulty of realizing a multi-polarized antenna with a common point, orthogonality, low coupling and compact structure, the existing multi-polarized antennas mostly adopt the design of dual-polarized and tri-polarized antennas, while for quad-polarized and more heavy-duty antennas Polarized antenna designs are relatively rare.
现有技术的缺点主要包括:(1)电偶极子与环天线相比,结构较为简单,更容易通过不同的极化方向来获得低耦合的多极化天线,但其无法对空间中的磁场分量进行充分地利用。而在由电偶极子和环天线组合而成的多极化天线中,电偶极子和环天线之间的耦合很难去除,特别是在共面的情况下,通常需要添加去耦合网络、EBG等结构来提高端口隔离度,因此由电偶极子和环天线共同组成的多极化低耦合电磁偶极子天线设计难度更高。(2)为了分别获得正交的电场和磁场分量,通常需要将电偶极子天线和环天线单元正交放置,由此组成的立体结构会增加设计和加工难度。目前所提出的几种四极化MIMO天线均为立体结构,天线结构及馈电网络复杂,不利于集成,在一些特定的使用场景中很难得到应用。The disadvantages of the existing technology mainly include: (1) Compared with the loop antenna, the electric dipole has a simpler structure, and it is easier to obtain a low-coupling multi-polarized antenna through different polarization directions, but it cannot be used for the antenna in space. The magnetic field component is fully utilized. In a multi-polarized antenna composed of an electric dipole and a loop antenna, the coupling between the electric dipole and the loop antenna is difficult to remove, especially in the case of coplanarity, it is usually necessary to add a decoupling network , EBG and other structures to improve port isolation, so the design of multi-polarized low-coupling electromagnetic dipole antennas composed of electric dipoles and loop antennas is more difficult. (2) In order to obtain orthogonal electric field and magnetic field components, it is usually necessary to place the electric dipole antenna and the loop antenna unit orthogonally, and the resulting three-dimensional structure will increase the difficulty of design and processing. Several quad-polarized MIMO antennas proposed at present are all three-dimensional structures, and the antenna structures and feeding networks are complex, which is not conducive to integration, and is difficult to be applied in some specific usage scenarios.
发明内容SUMMARY OF THE INVENTION
发明目的:本发明的目的是提供一种低耦合、结构紧凑、利于集成的基于正交模式的平面紧凑型低耦合四极化MIMO天线。Purpose of the invention: The purpose of the present invention is to provide a plane compact low-coupling quad-polarized MIMO antenna based on orthogonal mode, which is low-coupling, compact in structure and convenient for integration.
技术方案:本发明所述的基于正交模式的平面紧凑型低耦合四极化MIMO天线,包括基于正交模式的第一辐射体和第二辐射体,所述第一辐射体采用环状结构,通过不同的激励位置和激励方式,分别控制环上的表面电流方向获得两个正交的辐射模式,即电偶极子(Ex)和磁偶极子(Hz)的辐射模式,具体地,当环上的表面电流均匀同向时,获得磁偶极子(Hz)的辐射模式,此时辐射体上没有电流零点,称之为偶模;当第一辐射体上的表面电流关于x轴对称,方向相反时,得到电偶极子(Ex)的辐射模式,此时辐射体上有一个电流零点,称之为奇模;所述第二辐射体采用微带贴片天线,第二辐射体经过小型化处理,可以在其面积受限的情况下,降低其TM11模式的工作频率,使其与第一辐射体工作在同一带宽内。通过在x轴和y轴两个正交的位置激励,第二辐射体可以获得两个正交的TM11微带天线工作模式(Hy、Hx)。Technical solution: the planar compact low-coupling quad-polarized MIMO antenna based on the orthogonal mode of the present invention includes a first radiator and a second radiator based on the orthogonal mode, and the first radiator adopts a ring structure , through different excitation positions and excitation methods, respectively control the surface current direction on the ring to obtain two orthogonal radiation modes, namely the radiation modes of the electric dipole (Ex) and the magnetic dipole (Hz), specifically, When the surface current on the ring is uniform and in the same direction, the radiation mode of the magnetic dipole (Hz) is obtained. At this time, there is no current zero point on the radiator, which is called an even mode; when the surface current on the first radiator is about the x-axis Symmetric, when the direction is opposite, the radiation mode of the electric dipole (Ex) is obtained. At this time, there is a current zero point on the radiator, which is called an odd mode; the second radiator adopts a microstrip patch antenna, and the second radiation After the body is miniaturized, the operating frequency of its TM11 mode can be reduced to make it work within the same bandwidth as the first radiator when its area is limited. By exciting at two orthogonal positions of the x-axis and the y-axis, the second radiator can obtain two orthogonal operating modes (Hy, Hx) of the TM11 microstrip antenna.
所述第一辐射体由两个同心的、基于零相移传输线的环天线构成。The first radiator consists of two concentric loop antennas based on zero-phase-shift transmission lines.
所述第二辐射体的直径小于第一辐射体圆环的内圈直径,该第二辐射体置于第一辐射体的环状结构内,充分利用环状结构的内部空间。The diameter of the second radiator is smaller than the diameter of the inner circle of the first radiator ring, the second radiator is placed in the annular structure of the first radiator, and the inner space of the annular structure is fully utilized.
所述第二辐射体与第一辐射体工作于同一频带。The second radiator and the first radiator work in the same frequency band.
所述天线还包括天线接地金属板、介质板和微带馈电结构,所述天线接地金属板和第一辐射体置于介质板的上表面,所述第二辐射体和微带馈电结构置于介质板的下表面。The antenna also includes an antenna grounding metal plate, a dielectric plate and a microstrip feeding structure, the antenna grounding metal plate and the first radiator are placed on the upper surface of the dielectric plate, the second radiator and the microstrip feeding structure Place on the lower surface of the media plate.
所述天线还包括馈电端口,该馈电端口包括第一馈电端口、第二馈电端口、第三馈电端口和第四馈电端口,所述第一馈电口通过集总端口给第一辐射体的内环馈电,第二馈电端口通过微带馈电结构给第一辐射体的外环馈电,第三馈电端口和第四馈电端口分别在第二辐射体的x轴和y轴位置激励。The antenna further includes a feed port, the feed port includes a first feed port, a second feed port, a third feed port, and a fourth feed port, and the first feed port is fed through a lumped port. The inner loop of the first radiator is fed, the second feeding port feeds the outer loop of the first radiator through the microstrip feeding structure, and the third feeding port and the fourth feeding port are respectively in the second radiator. x-axis and y-axis position excitation.
所述微带馈电结构采用T型微带线馈电结构。The microstrip feeding structure adopts a T-shaped microstrip line feeding structure.
有益效果:与现有技术相比,本发明具有如下优点:Beneficial effect: Compared with the prior art, the present invention has the following advantages:
(1)本发明充分利用了第一辐射体环状结构的内部空间,将第二辐射体放置于第一辐射体内,在平面结构内通过两个不同的基于模式正交的辐射体的结合获得四种极化模式,具有结构紧凑、低耦合等特性;(1) The present invention makes full use of the inner space of the annular structure of the first radiator, places the second radiator in the first radiator, and obtains the result by combining two different radiators based on mode orthogonality in the plane structure Four polarization modes, featuring compact structure and low coupling;
(2)第二辐射体通过分形结构进行了小型化处理,可以在第二辐射体面积受限的前提下,降低其TM11模式的工作频率,与第一辐射体工作于同一频带;(2) The second radiator is miniaturized by the fractal structure, and the operating frequency of its TM11 mode can be reduced under the premise that the area of the second radiator is limited, and it operates in the same frequency band as the first radiator;
(3)本发明所采用的两个辐射体结构简单,其平面结构易于加工和安装使用;(3) The two radiators used in the present invention have simple structures, and their planar structures are easy to process, install and use;
(4)本发明可以更有效地利用空间中的电磁场矢量特性,在结构紧凑的情况下可以在多径丰富的传播环境中获得大于3×3、接近4×4独立同分布瑞利信道的信道容量。(4) The present invention can more effectively utilize the electromagnetic field vector characteristics in space, and can obtain channels larger than 3×3 and close to 4×4 IID Rayleigh channels in a multipath-rich propagation environment with a compact structure capacity.
附图说明Description of drawings
图1是四极化MIMO天线的结构示意图;FIG. 1 is a schematic structural diagram of a quad-polarized MIMO antenna;
图2是四极化MIMO天线的S参数仿真结果;Figure 2 is the S-parameter simulation result of the quad-polarized MIMO antenna;
图3是四极化MIMO天线的各端口间耦合的仿真结果;Fig. 3 is the simulation result of coupling between each port of quad-polarized MIMO antenna;
图4是四极化MIMO天线第一馈电端口6和第二馈电端口7分别激励时,第一辐射体1上的电流分布图,其中图4a为所述四极化MIMO天线第一馈电端口6激励时,第一辐射体1上的电流分布图,图4b为所述四极化MIMO天线第二馈电端口7激励时,第一辐射体1上的电流分布图;Fig. 4 is the current distribution diagram on the first radiator 1 when the first feed port 6 and the second feed port 7 of the quad-polarized MIMO antenna are excited respectively, wherein Fig. 4a is the first feed of the quad-polarized MIMO antenna When the electrical port 6 is excited, the current distribution diagram on the first radiator 1, FIG. 4b is the current distribution diagram on the first radiator 1 when the second feed port 7 of the quad-polarized MIMO antenna is excited;
图5是四极化MIMO天线第三馈电端口8和第四馈电端口9分别激励时,第二辐射体2上的电场分布图,其中图5a为所述四极化MIMO天线第三馈电端口8激励时,第二辐射体2上的电场分布图,图5b为所述四极化MIMO天线第四馈电端口9激励时,第二辐射体2上的电场分布图;Fig. 5 is the electric field distribution diagram on the second radiator 2 when the third feed port 8 and the
图6是四极化MIMO天线第一馈电端口6激励时的辐射方向图,其中,图6a为xoy面辐射方向图,图6b为yoz面辐射方向图;Fig. 6 is the radiation pattern when the first feed port 6 of the quad-polarized MIMO antenna is excited, wherein, Fig. 6a is the radiation pattern of the xoy surface, and Fig. 6b is the radiation pattern of the yoz surface;
图7是四极化MIMO天线第二馈电端口7激励时的辐射方向图,其中,图7a为xoy面辐射方向图,图7b为yoz面辐射方向图;Fig. 7 is the radiation pattern when the second feed port 7 of the quad-polarized MIMO antenna is excited, wherein Fig. 7a is the radiation pattern of the xoy plane, and Fig. 7b is the radiation pattern of the yoz plane;
图8是四极化MIMO天线第三馈电端口8激励时的辐射方向图,其中,图8a为yoz面辐射方向图,图8b为xoz面辐射方向图;Fig. 8 is the radiation pattern when the third feed port 8 of the quad-polarized MIMO antenna is excited, wherein Fig. 8a is the radiation pattern of the yoz surface, and Fig. 8b is the radiation pattern of the xoz surface;
图9是四极化MIMO天线第四馈电端口9激励时的辐射方向图,其中,图9a为yoz面辐射方向图,图9b为xoz面辐射方向图;Fig. 9 is the radiation pattern when the
图10是第二辐射体2采用Tee-Type分形结构和未采用Tee-Type分形结构时谐振频率的对比图。FIG. 10 is a comparison diagram of the resonance frequency when the second radiator 2 adopts the Tee-Type fractal structure and when the Tee-Type fractal structure is not adopted.
图11是本发明实施例中四极化MIMO天线在办公室环境中实际测得的信道容量的累积分布结果,以及其和3×3、4×4的独立同分布瑞利信道的信道容量对比。11 is the cumulative distribution result of the channel capacity actually measured by the quad-polarized MIMO antenna in the office environment according to the embodiment of the present invention, and the channel capacity comparison with the 3×3 and 4×4 IID Rayleigh channels.
具体实施方式Detailed ways
下面结合附图对本发明的技术方案作进一步说明。The technical solutions of the present invention will be further described below with reference to the accompanying drawings.
如图1所示,本实施例的四极化MIMO天线由第一辐射体1、第二辐射体2、天线接地金属板3、介质板4、T型的馈电结构5和馈电端口构成,所述馈电端口包括第一馈电端口6、第二馈电端口7、第三馈电端口8和第四馈电端口9。其中,第一馈电端口6采用特性阻抗为50Ω的集总端口激励第一辐射体1的内环,第二馈电端口7采用特性阻抗为50Ω的SMA同轴线馈电,通过微带馈电结构5激励第一辐射体1的外环,第三馈电端口8和第四馈电端口9采用特性阻抗为50Ω的SMA同轴线馈电,分别在x轴和y轴激励第二辐射体2。As shown in FIG. 1 , the quad-polarized MIMO antenna of this embodiment is composed of a first radiator 1 , a second radiator 2 , an antenna grounding metal plate 3 , a dielectric plate 4 , a T-
本实施例中,介质板4采用介电常数为4.4的环氧树脂板FR-4,置于xoy面,天线接地金属板3和第一辐射体1放置于介质板4的上表面,第二辐射体2和微带馈电结构5放置于介质板4的下表面。In this embodiment, the dielectric board 4 is an epoxy resin board FR-4 with a dielectric constant of 4.4, which is placed on the xoy surface, the antenna grounding metal plate 3 and the first radiator 1 are placed on the upper surface of the dielectric board 4, the second The radiator 2 and the
第一辐射体1由两个同心的、基于零相移传输线的环天线构成,外环与内环的结构基本相同,与内环相比,外环顺时针地旋转了22.5°。这些具有周期结构的零相移传输线可以在环路中引入串联电容,在相邻部分之间提供很小的相位校正,即使环路的周长与工作波长相当,沿环路流动的电流也保持相位一致。通过两种不同的激励,分别控制环上的表面电流方向。具体地,当馈电端口6激励时,在第一辐射体1上激励出等幅同向的表面电流,可以获得磁偶极子(Hz)的辐射特性;当馈电端口7激励时,在微带馈电线5的作用下,电流在第二馈电端口7处流向两个相反的方向,因为零相移传输线的存在和结构的完全对称,流向两端的电流是等幅反向的,在第一辐射体1上获得等幅反向、均匀对称的表面电流,可以获得水平方向的电偶极子(Ex)的辐射特性。The first radiator 1 is composed of two concentric loop antennas based on zero-phase-shift transmission lines. The structures of the outer loop and the inner loop are basically the same. Compared with the inner loop, the outer loop is rotated clockwise by 22.5°. These zero-phase-shifted transmission lines with periodic structures can introduce series capacitance in the loop, provide little phase correction between adjacent sections, and maintain current flow along the loop even if the loop has a perimeter comparable to the operating wavelength Phase match. With two different excitations, the direction of the surface current on the loop is controlled separately. Specifically, when the feeding port 6 is excited, a surface current of equal magnitude and the same direction is excited on the first radiator 1, and the radiation characteristics of the magnetic dipole (Hz) can be obtained; when the feeding port 7 is excited, the Under the action of the
其中,由于第二辐射体2需要放置于第一辐射体1的环状结构内,其面积受限于第一辐射体1的尺寸,此时,第二辐射体2的工作频率偏高,需要对其进行小型化的处理来降低其TM11模式的工作频率,使之与第一辐射体1工作在同一频段内。具体地,本发明中第二辐射体2采用了一种基于Tee-type分形结构的微带贴片天线。分形结构是一种天线小型化的重要手段,其每个分段在较小的尺度上都具有整个结构的特征,这是自相似的基本性质,经过有限次数的分形几何迭代,分形重复次数增加,天线的最低谐振频率逐渐减小,最终与第一辐射体1工作在同一频段内,并且可以保持两个正交的TM11微带天线工作模式。参阅图10,为采用Tee-Type分形结构的微带贴片天线和相同半径的未采用Tee-Type结构的圆形微带天线的谐振频率对比图。从图中可见,采用Tee-Type结构的微带贴片天线可以有效地将半径相同的微带贴片天线的工作频率从2.8GHz降低至2.45GHz。这使得第二辐射体2在面积有限的情况下,可以与第一辐射体1工作在同一频带内,进而共同组成同一工作频带内的四极化MIMO天线。Among them, since the second radiator 2 needs to be placed in the annular structure of the first radiator 1, its area is limited by the size of the first radiator 1. At this time, the operating frequency of the second radiator 2 is high, and it needs to It is miniaturized to reduce the operating frequency of its TM11 mode, so that it operates in the same frequency band as the first radiator 1 . Specifically, the second radiator 2 in the present invention adopts a microstrip patch antenna based on a Tee-type fractal structure. Fractal structure is an important means of antenna miniaturization. Each segment has the characteristics of the entire structure on a smaller scale. This is the basic property of self-similarity. After a limited number of fractal geometry iterations, the number of fractal repetitions increases. , the lowest resonant frequency of the antenna decreases gradually, and finally works in the same frequency band as the first radiator 1, and can maintain two orthogonal TM11 microstrip antenna operating modes. Referring to FIG. 10 , it is a comparison diagram of the resonance frequencies of the microstrip patch antenna using the Tee-Type fractal structure and the circular microstrip antenna with the same radius without the Tee-Type structure. It can be seen from the figure that the microstrip patch antenna using the Tee-Type structure can effectively reduce the operating frequency of the microstrip patch antenna with the same radius from 2.8GHz to 2.45GHz. This enables the second radiator 2 to work in the same frequency band as the first radiator 1 under the condition of limited area, and then together form a quad-polarized MIMO antenna in the same working frequency band.
其中,通过结合第一辐射体1和第二辐射体2,获得了本发明所述的共点正交、低耦合、结构紧凑的四极化MIMO天线。Wherein, by combining the first radiator 1 and the second radiator 2, the quad-polarized MIMO antenna with a common point orthogonal, low coupling and compact structure according to the present invention is obtained.
进一步的,为了验证所提出四极化天线的MIMO系统性能,我们对本发明所提出的四极化天线进行了加工和实际测试,并对其在实际办公室环境下的信道容量进行了分析。其中,测试收发天线均为本发明实施例提出的四极化MIMO天线,测试时收发天线高度均为1.05米,收发天线距离为1.71米。信道容量C是通过MIMO系统信道容量常用的表达式计算的,具体可以表示为:Further, in order to verify the performance of the MIMO system of the proposed quad-polarized antenna, we process and test the quad-polarized antenna proposed in the present invention, and analyze its channel capacity in an actual office environment. The transmitting and receiving antennas tested are all quad-polarized MIMO antennas proposed in the embodiments of the present invention. During the test, the transmitting and receiving antennas are all 1.05 meters high and the distance between the transmitting and receiving antennas is 1.71 meters. The channel capacity C is calculated by the commonly used expression of the channel capacity of the MIMO system, which can be expressed as:
其中,I表示4×4的单位矩阵,nT=4为发射端口数,det(·)表示求矩阵的行列式,SNR表示信噪比,这里取信噪比SNR=20dB,H采用常用的归一化信道矩阵:其中‖·‖F表示Frobenius范数,K表示分析容量的所有参数。通过这种归一化,可以消除计算中路径损耗对总接收信号功率的影响,并且可以很好地反映环境中多径的丰富程度对MIMO系统信道容量的影响。Among them, I represents a 4×4 unit matrix, n T = 4 is the number of transmit ports, det( ) represents the determinant of the matrix, SNR represents the signal-to-noise ratio, here the signal-to-noise ratio SNR=20dB, and H adopts the commonly used Normalized channel matrix: where ‖· ‖F represents the Frobenius norm, and K represents all parameters of the analytical capacity. Through this normalization, the influence of path loss on the total received signal power in the calculation can be eliminated, and the influence of the abundance of multipath in the environment on the channel capacity of the MIMO system can be well reflected.
参阅图11,为四极化MIMO天线在办公室环境下所获得的信道容量(信噪比SNR为20dB)的累积分布函数结果,作为对比,图11同时给出了3×3、4×4的独立同分布瑞利信道的信道容量结果,如图11所示,本发明所提出的四极化MIMO天线在真实的办公室传播环境中可以获得远大于3×3,接近4×4的独立同分布瑞利信道的信道容量。Referring to Figure 11, it is the cumulative distribution function result of the channel capacity (signal-to-noise ratio SNR is 20dB) obtained by the quad-polarized MIMO antenna in the office environment. The channel capacity results of the IID Rayleigh channel, as shown in Figure 11, the quad-polarized MIMO antenna proposed in the present invention can obtain IID much larger than 3×3 and close to 4×4 in the real office propagation environment The channel capacity of the Rayleigh channel.
如图2所示为四极化MIMO天线的反射系数曲线,可以看出,天线的-10dB阻抗公共带宽为40MHz(2.41-2.45GHz)。Figure 2 shows the reflection coefficient curve of the four-polarized MIMO antenna. It can be seen that the -10dB impedance common bandwidth of the antenna is 40MHz (2.41-2.45GHz).
如图3所示为四极化MIMO天线的耦合曲线,在-10dB阻抗公共带宽内,耦合均低于-15.5dB。Figure 3 shows the coupling curve of the quad-polarized MIMO antenna. In the common bandwidth of -10dB impedance, the coupling is lower than -15.5dB.
图4是四极化MIMO天线第一馈电端口6和第二馈电端口7分别激励时,第一辐射体1上的电流分布图,其中图4a为所述四极化MIMO天线第一馈电端口6激励时,第一辐射体1上的电流分布图,图4b为所述四极化MIMO天线第二馈电端口7激励时,第一辐射体1上的电流分布图,如图4a所示,当第一馈电端口6激励时第一辐射体1上的电流的幅度是相等的,并且由于零相移传输线相位补偿的关系,电流的方向是一致的,从而在金属环上形成了等幅同相的环状电流,其辐射特性可以等效为竖直方向上的磁偶极子天线Hz;如图4b所示,当第二馈电端口7馈电时,在T型微带馈电5的作用下,电流在第二馈电端口7处流向两个相反的方向,由于零相移传输线的存在和结构的完全对称性,流向两端的电流是幅度相等,方向相反,其辐射特性可以等效为水平方向上的电偶极子Ex。Fig. 4 is the current distribution diagram on the first radiator 1 when the first feed port 6 and the second feed port 7 of the quad-polarized MIMO antenna are excited respectively, wherein Fig. 4a is the first feed of the quad-polarized MIMO antenna When the electrical port 6 is excited, the current distribution diagram on the first radiator 1, Figure 4b is the current distribution diagram on the first radiator 1 when the second feed port 7 of the quad-polarized MIMO antenna is excited, as shown in Figure 4a As shown, the amplitudes of the currents on the first radiator 1 are equal when the first feeding port 6 is excited, and due to the relationship of the phase compensation of the zero-phase-shift transmission line, the directions of the currents are the same, thus forming on the metal ring In order to obtain the ring current of equal amplitude and phase, its radiation characteristics can be equivalent to the magnetic dipole antenna Hz in the vertical direction; as shown in Figure 4b, when the second feeding port 7 is fed, the Under the action of the
图5是四极化MIMO天线第三馈电端口8和第四馈电端口9分别激励时,第二辐射体2上的电场分布图,其中图5a为所述四极化MIMO天线第三馈电端口8激励时,第二辐射体2上的电场分布图,图5b为所述四极化MIMO天线第四馈电端口9激励时,第二辐射体2上的电场分布图,如图5a所示,第三馈电端口8馈电时,可以看出电场分布在z轴方向上,其关于x轴对称,关于y轴反对称;同理,如图5b所示,当第四馈电端口9馈电时,同样能看到电场分布在z轴方向上,有区别的是,此时的电场关于y轴对称,关于x轴反对称。基于以上的分析,我们能够得出的结论是:当端口8和端口9分别馈电时,第二辐射体2工作在两个正交的TM11微带天线模式下(Hy,Hx)。Fig. 5 is the electric field distribution diagram on the second radiator 2 when the third feed port 8 and the
图6是四极化MIMO天线第一馈电端口6激励时的辐射方向图,其中,图6a为xoy面辐射方向图,图6b为yoz面辐射方向图,如图6所示,端口6激励时,四极化MIMO天线在xoy面上获得了良好的水平极化全向辐射,在yoz平面获得了“8”字形辐射方向图,符合沿z轴放置的磁偶极子(Hz)的辐射特性。Fig. 6 is the radiation pattern when the first feed port 6 of the quad-polarized MIMO antenna is excited, wherein Fig. 6a is the radiation pattern of the xoy surface, and Fig. 6b is the radiation pattern of the yoz surface. As shown in Fig. 6, port 6 is excited When , the quad-polarized MIMO antenna obtains good horizontally polarized omnidirectional radiation on the xoy plane, and a figure-8 radiation pattern on the yoz plane, which is consistent with the radiation of a magnetic dipole (Hz) placed along the z-axis characteristic.
图7是本发明实施例中四极化MIMO天线第二馈电端口7激励时的辐射方向图,其中,图7a为xoy面辐射方向图,图7b为yoz面辐射方向图,如图7所示,xoy面显示了准“8”字形辐射方向图,在yoz面获得了良好的全向辐射,辐射模式非常接近沿x轴放置的理想电偶极子(Ex)的辐射模式。FIG. 7 is the radiation pattern of the quad-polarized MIMO antenna when the second feed port 7 is excited according to the embodiment of the present invention, wherein FIG. 7a is the radiation pattern of the xoy plane, and FIG. 7b is the radiation pattern of the yoz plane, as shown in FIG. 7 . The xoy plane shows a quasi-"8" radiation pattern, and good omnidirectional radiation is obtained on the yoz plane, the radiation pattern is very close to that of an ideal electric dipole (Ex) placed along the x-axis.
图8是四极化MIMO天线第三馈电端口8激励时的辐射方向图,其中,图8a为yoz面辐射方向图,图8b为xoz面辐射方向图。FIG. 8 is a radiation pattern when the third feed port 8 of the quad-polarized MIMO antenna is excited, wherein FIG. 8a is the radiation pattern of the yoz surface, and FIG. 8b is the radiation pattern of the xoz surface.
图9是四极化MIMO天线第四馈电端口9激励时的辐射方向图,其中,图9a为yoz面辐射方向图,图9b为xoz面辐射方向图,如图9所示,本发明中第三馈电端口8和第四馈电端口9符合两个正交的微带模式(Hy,Hx)的辐射特性;Fig. 9 is the radiation pattern when the
图10为第二辐射体分别为采用Tee-Type分形结构和未采用Tee-Type分形结构时谐振频率的对比图,可以看出,采用Tee-Type分形结构可以有效地降低微带贴片天线的工作频率。Figure 10 is a comparison diagram of the resonant frequency of the second radiator when the Tee-Type fractal structure is used and when the Tee-Type fractal structure is not used. It can be seen that the use of the Tee-Type fractal structure can effectively reduce the frequency of the microstrip patch antenna. working frequency.
图11为本发明所提出的四极化MIMO天线在办公室真实环境中所获得的信道容量的累积分布结果(信噪比SNR=20dB),以及其和3×3、4×4的独立同分布瑞利信道的信道容量对比。如图所示,本发明所提出的四极化MIMO天线在真实环境下可以获得接近4×4的独立同分布瑞利信道的信道容量,远大于3×3的独立同分布瑞利信道的信道容量。Figure 11 is the cumulative distribution result of the channel capacity obtained by the quad-polarized MIMO antenna proposed by the present invention in the real environment of the office (signal-to-noise ratio SNR=20dB), and its independent and identical distribution with 3×3 and 4×4 Channel capacity comparison of Rayleigh channels. As shown in the figure, the quad-polarized MIMO antenna proposed by the present invention can obtain a channel capacity close to the 4×4 IID Rayleigh channel in the real environment, which is much larger than the channel capacity of the 3×3 IID Rayleigh channel. capacity.
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