CN109193147B - A Low Profile Filter Antenna Using Slotted Dielectric Patch - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及无线通信技术领域,特别涉及低剖面的介质贴片滤波天线。The present invention relates to the technical field of wireless communication, in particular to a low-profile dielectric patch filter antenna.
背景技术Background technique
在无线通信系统中,天线和滤波器通常被设计成两个独立的部件。在这种情况下,需要它们各自的匹配电路和用于连接它们的附加传输线,这不可避免地增加了系统尺寸,并引入了额外的损耗和负载效应。为了克服这一点,近年来,各种滤波器和天线的协同设计方法(也称滤波天线)得到了广泛的发展。设计方法主要可分为三类。方法一是设计带通/带阻滤波器和天线,然后将它们组合在一起。第二种方法是第一种方法的变形,天线既用作辐射器又用作过滤器的最后一级谐振器。然而,它们都属于级联设计,使得天线结构复杂,体积庞大,尤其是在馈电网络中。为解决级联设计问题,有学者提出了第三种方法:将一些滤波结构嵌入到天线辐射器中以实现增益的带通响应,这意味着天线辐射器本身具有滤波能力。因此,该方法是减小滤波天线尺寸和损耗的有效方法。此外,具有滤波特性的辐射器在双频段阵列中具有吸引力,可以减少在不同频率下工作的元件之间的相互耦合。In wireless communication systems, antennas and filters are usually designed as two separate components. In this case, their respective matching circuits and additional transmission lines for connecting them are required, which inevitably increases the system size and introduces additional losses and loading effects. To overcome this, co-design methods of various filters and antennas (also called filter antennas) have been widely developed in recent years. Design methods can be mainly divided into three categories. One approach is to design bandpass/bandstop filters and antennas and then combine them. The second method is a variation of the first method, where the antenna acts as both a radiator and a final stage resonator of the filter. However, they all belong to cascade design, which makes the antenna structure complex and bulky, especially in the feeding network. To solve the cascade design problem, some scholars have proposed a third method: embedding some filtering structures into the antenna radiator to achieve a gain bandpass response, which means that the antenna radiator itself has filtering capability. Therefore, this method is an effective method to reduce the filter antenna size and loss. Additionally, radiators with filtering properties are attractive in dual-band arrays to reduce mutual coupling between elements operating at different frequencies.
众所周知,介质谐振器天线作为一种典型的天线,具有体积小、重量轻、易于激励等优点。最近几年,介质谐振器滤波天线已成为高频应用的热点。 然而,基于上述第一和第二种方法设计的介质谐振器滤波天线的剖面较高且具有庞大的馈电结构。为了降低介质谐振器天线的剖面,在2013年有学者提出了一种高密度的介质贴片天线,它的主模(最低阶谐振模式)为TE11模式,具有微带贴片的相似电场分布。As we all know, the dielectric resonator antenna, as a typical antenna, has the advantages of small size, light weight, and easy excitation. In recent years, dielectric resonator filter antennas have become a hot spot for high-frequency applications. However, the dielectric resonator filter antenna designed based on the above-mentioned first and second methods has a high profile and a bulky feeding structure. In order to reduce the profile of the dielectric resonator antenna, some scholars proposed a high-density dielectric patch antenna in 2013. Its main mode (the lowest-order resonance mode) is the TE 11 mode and has a similar electric field distribution of the microstrip patch. .
经检索发现,中国发明专利申请CN 105720364 A公开了一种具有高选择性和低交叉极化的双极化滤波天线,无需额外的滤波电路,天线自身集成滤波特性和辐射特性,解决了传统级联型的滤波天线带来的插入损耗与额外尺寸的问题。然而,缺陷在于:其结构复杂,且是在馈电网络上实现滤波特性,而不是天线辐射器本身具有滤波能力。After searching, it is found that the Chinese invention patent application CN 105720364 A discloses a dual-polarization filter antenna with high selectivity and low cross-polarization, no additional filter circuit is required, and the antenna itself integrates filter characteristics and radiation characteristics, which solves the problem of traditional level. The insertion loss and extra size of the filter antenna caused by the connected type. However, the disadvantage is that its structure is complicated, and the filtering characteristic is realized on the feeding network, rather than the filtering ability of the antenna radiator itself.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于:克服上述现有技术的缺陷,提出一种结构简单的采用带槽介质贴片的低剖面滤波天线。天线采用直接馈电的方式对介质贴片进行馈电。借助于介质贴片的非辐射高阶模式和在介质贴片中开设一对内壁印刷金属的槽,可以在不添加任何额外的滤波电路的情况下获得高端和低端两个辐射零点,使得天线辐射器本身具有滤波能力。同时,在对介质贴片开槽的过程中改变了天线的电长度,实现了天线的小型化。The purpose of the present invention is to overcome the above-mentioned defects of the prior art, and to propose a low-profile filter antenna with a simple structure using a slotted dielectric patch. The antenna feeds the dielectric patch by means of direct feeding. With the help of the non-radiating high-order mode of the dielectric patch and a pair of grooves with metal printed on the inner wall in the dielectric patch, two radiation nulls at the high and low ends can be obtained without adding any additional filter circuit, making the antenna The radiator itself has filtering capabilities. At the same time, the electrical length of the antenna is changed in the process of slotting the dielectric patch, thereby realizing the miniaturization of the antenna.
为了达到上述目的,本发明提出的采用带槽介质贴片的低剖面滤波天线,包括自下而上依次层叠设置的金属反射地板、基板和介质贴片,所述基板上表面设有与介质贴片相连的馈线,用于直接馈电,所述介质贴片与馈线相连的一侧对称于该馈线连接处开设有一对内壁印刷金属的槽,所述介质贴片的介电常数大于40。In order to achieve the above purpose, the low-profile filter antenna using a slotted dielectric patch proposed by the present invention includes a metal reflective floor, a substrate and a dielectric patch that are sequentially stacked from bottom to top, and the upper surface of the substrate is provided with a dielectric patch. The feeder connected to the sheet is used for direct power feeding. The side of the dielectric patch connected to the feeder is symmetrically provided with a pair of metal grooves printed on the inner wall at the connection of the feeder. The dielectric constant of the dielectric patch is greater than 40.
本发明介质贴片滤波天线,具有结构简单,制作容易,体积小,剖面低等优点。通过引入的敷银槽,不仅可以实现天线的小型化,还能在较低的频带引入辐射零点,结合由介质贴片的高阶模式产生的高频带辐射零点,天线可以获得良好的滤波性能。通过改变槽的长度和宽度,天线的工作频率及辐射零点所在的位置会同时发生规律性的改变,以便很容易地调谐到所需要的频率进行抑制。The dielectric patch filter antenna of the invention has the advantages of simple structure, easy manufacture, small volume and low profile. Through the introduction of the silver coating groove, not only the miniaturization of the antenna can be realized, but also the radiation null point can be introduced in the lower frequency band. Combined with the high frequency band radiation null point generated by the high-order mode of the dielectric patch, the antenna can obtain good filtering performance. . By changing the length and width of the slot, the operating frequency of the antenna and the position of the radiation null point will change regularly at the same time, so that it is easy to tune to the desired frequency for suppression.
附图说明Description of drawings
下面结合附图对本发明作进一步的说明。The present invention will be further described below in conjunction with the accompanying drawings.
图1是本发明带槽介质贴片滤波天线立体图。FIG. 1 is a perspective view of the slotted dielectric patch filter antenna of the present invention.
图2是本发明带槽介质贴片滤波天线的分解图。FIG. 2 is an exploded view of the slotted dielectric patch filter antenna of the present invention.
图3是本发明带槽介质贴片滤波天线的俯视图。3 is a top view of the slotted dielectric patch filter antenna of the present invention.
图4是无槽介质贴片天线仿真反射系数(S11)和增益曲线图。FIG. 4 is a graph showing the simulated reflection coefficient (S 11 ) and gain of the slotless dielectric patch antenna.
图5是本发明带槽介质贴片滤波天线仿真反射系数(S11)和增益曲线图。FIG. 5 is a graph showing the simulated reflection coefficient (S 11 ) and gain of the slotted dielectric patch filter antenna of the present invention.
图6是本发明带槽介质贴片滤波天线仿真和测试的反射系数(S11)和增益曲线对比图。6 is a comparison diagram of the reflection coefficient (S 11 ) and the gain curve of the simulation and test of the slotted dielectric patch filter antenna of the present invention.
图7是本发明带槽介质贴片滤波天线在4.17GHz频率点下的仿真和测试的天线辐射E面方向图。FIG. 7 is the antenna radiation E-plane pattern of the simulation and test at the frequency point of 4.17 GHz for the slotted dielectric patch filter antenna of the present invention.
图8是本发明带槽介质贴片滤波天线在4.17GHz频率点下的仿真和测试的天线辐射H面方向图。FIG. 8 is the antenna radiation H-plane pattern of the simulation and test at the frequency point of 4.17 GHz for the slotted dielectric patch filter antenna of the present invention.
具体实施方式Detailed ways
下面结合附图和具体实施例对本发明做进一步说明。The present invention will be further described below with reference to the accompanying drawings and specific embodiments.
如图1-图3所示,本实施例采用带槽介质贴片的低剖面滤波天线,包括自下而上依次层叠设置的金属反射地板1、基板2和介质贴片3,基板上表面设有与介质贴片相连的馈线4,用于直接馈电。本例中,基板2为印刷电路板,金属反射地板1印制于印刷电路板2的底面,馈线4印制于印刷电路板2顶面。介质贴片的一个侧面的中部印刷有矩形的金属馈电片5,馈线4与该金属馈电片5连接,介质贴片3与馈线4相连的一侧对称于金属馈电片5开设有一对内壁印刷金属银的矩形槽6,介质贴片3为微波介质陶瓷,其介电常数ε r= 90。本结构的滤波天线中,介质贴片的介电常数需大于40。As shown in Figures 1-3, this embodiment adopts a low-profile filter antenna with a slotted dielectric patch, including a
本实施例天线的参数见下表The parameters of the antenna in this embodiment are shown in the following table
W 1为介质贴的宽度,W 2为基板的宽度,L 1为介质贴片的长度,L 2为基板的长度,h 1为介质贴片的高度,h 2为基板的高度,l为槽长度,w为槽的宽度,d为两槽之间的距离,t为金属馈电片的高度。通过改变槽的长度l和宽度w能够调节天线的工作频率以及辐射零点所在的位置。通过改变金属馈电片的高度t能够调节天线的输入匹配。 W1 is the width of the dielectric patch, W2 is the width of the substrate, L1 is the length of the dielectric patch, L2 is the length of the substrate, h1 is the height of the dielectric patch , h2 is the height of the substrate , l is the slot length, w is the width of the slot, d is the distance between the two slots, and t is the height of the metal feeder. By changing the length l and width w of the slot, the operating frequency of the antenna and the position of the radiation null point can be adjusted. The input matching of the antenna can be adjusted by changing the height t of the metal feeder.
介质贴片由高密度的陶瓷材料制成,用于替代微带金属贴片。介质贴片的主模(最低阶谐振模式)是TM11模式,其电场分布类似于微带贴片的电场分布。图4为直接由微带线馈电的无槽介质贴片天线的仿真反射系数(S11)和增益。由于介质贴片的上表面可近似为磁壁,因此TM11模式的辐射沿y轴方向的两条边,极化方向沿x轴。介质贴片的最低端的高阶模式HEM21的电场分布垂直于馈电微带线,所以不被激励(S11≈0dB)。更重要的是,HEM21模式在x轴极化方向没有辐射元素。因此,在此激励方式下可以得到一个固有的高端辐射零点。同时,高阶模式HEM12其电场分布与馈线平行,可以被激励,并且工作良好。Dielectric patches are made of high-density ceramic materials to replace microstrip metal patches. The dominant mode (lowest-order resonant mode) of the dielectric patch is the TM 11 mode, and its electric field distribution is similar to that of the microstrip patch. Figure 4 shows the simulated reflection coefficient (S 11 ) and gain of a slotless dielectric patch antenna fed directly by a microstrip line. Since the upper surface of the dielectric patch can be approximated as a magnetic wall, the radiation of the TM 11 mode is along the two sides of the y-axis direction, and the polarization direction is along the x-axis. The electric field distribution of the higher-order mode HEM 21 at the lowest end of the dielectric patch is perpendicular to the feeding microstrip line, so it is not excited (S 11 ≈0 dB). More importantly, the HEM 21 mode has no radiating elements in the x-axis polarization direction. Therefore, an inherent high-end radiation zero can be obtained under this excitation mode. At the same time, the higher-order mode HEM 12 , whose electric field distribution is parallel to the feeder, can be excited and works well.
为了在低频段产生另一个辐射零点,以增强选择性,本实施例在介质贴片中蚀刻了一对沿x轴方向的槽,并在三个内表面印刷上银。图5为仿真的S11和增益。从图4和图5可以看出,敷银槽会拉低TM11和HEM21模式的频率。同时,反相电场场与槽垂直,因此附银槽可以在低频段产生另一个辐射零点。随着槽的长度l的增大,天线的工作频率减小,且低端和高端辐射零点是自适应的,具有稳定的高选择性。同时,槽的宽度w主要影响低端辐射零点,而对高端辐射零点影响很小。因此,这两个零可以独立地控制,以便可以很容易地调谐到所需的频率进行抑制。To create another radiation null at low frequencies for enhanced selectivity, this example etched a pair of slots along the x-axis in the dielectric patch and printed silver on three inner surfaces. Figure 5 shows the simulated S11 and gain. As can be seen in Figures 4 and 5, the silvered grooves pull down the frequencies of the TM 11 and HEM 21 modes. At the same time, the inverse electric field is perpendicular to the slot, so the silver slot can generate another radiation null at low frequency. As the length l of the slot increases, the operating frequency of the antenna decreases, and the low-end and high-end radiation nulls are adaptive, with stable high selectivity. At the same time, the width w of the slot mainly affects the low-end radiation zero point, and has little effect on the high-end radiation zero point. Therefore, the two zeros can be independently controlled so that they can be easily tuned to the desired frequency for rejection.
对本实施例介质贴片滤波天线进行测试,测试结果与仿真相吻合,见图6。该天线具有较窄的滤波频带,在中心频率f 0 = 4.17 GHz处S11 < -20 dB,在测量增益响应中可观察到4.02和4.31 GHz处的两个辐射零点,通带边缘陡峭,且具有较高的选择性。在4.17 GHz时测量到的最大增益为4.8 dB。在4.17 GHz频率点的E和H平面辐射图如图7、图8所示。测得的交叉极化比主极化低至少15 dB。从图中可以看出可以观察到模拟和测量结果之间的轻微差异,这可归因于制造和测量的误差。The dielectric patch filter antenna of this embodiment is tested, and the test results are consistent with the simulation, as shown in FIG. 6 . The antenna has a narrow filter band, S11 < -20 dB at center frequency f0 = 4.17 GHz, two radiation nulls at 4.02 and 4.31 GHz are observed in the measured gain response, the passband edge is steep, and Has high selectivity. The maximum gain measured at 4.17 GHz is 4.8 dB. The E and H plane radiation patterns at 4.17 GHz are shown in Figures 7 and 8. The measured cross polarization is at least 15 dB lower than the main polarization. As can be seen from the figure, slight differences between the simulated and measured results can be observed, which can be attributed to manufacturing and measurement errors.
除上述实施例外,本发明还可以有其他实施方式。凡采用等同替换或等效变换形成的技术方案,均落在本发明要求的保护范围。In addition to the above-described embodiments, the present invention may also have other embodiments. All technical solutions formed by equivalent replacement or equivalent transformation fall within the protection scope of the present invention.
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