CN104538721A - Metamaterial harmonic oscillator based on metal-structure LC resonator and application thereof - Google Patents
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Abstract
Description
技术领域technical field
本发明属于材料领域,涉及一种基于金属结构LC谐振器的超材料谐振子及其应用。The invention belongs to the field of materials, and relates to a metamaterial resonator based on a metal structure LC resonator and an application thereof.
背景技术Background technique
微波器件的小型化和集成化是电子信息产业始终不断要追求的目标。诸如滤波器、耦合器和多工器等众多微波器件都具有电磁信号选择性传输并且要抑制带外信号通过等功能,这些微波器件都要用到的一个核心元件就是谐振器。目前使用的大多数谐振器都是由矩形或其他形状的金属空腔以及体积较大的圆柱形介质做成的,它们一般都占有较大的体积,在低频时更是如此。为了要实现很好的频率选择特性,抑制杂波信号的通过,一般要把若干个这样的谐振子组合起来使用。因此,由若干个这样的谐振器构成的各种微波器件必然要占据更大的体积,这就给微波器件的小型化、集成化带来很大的问题。The miniaturization and integration of microwave devices is the goal that the electronic information industry is constantly pursuing. Many microwave devices, such as filters, couplers, and multiplexers, have functions such as selective transmission of electromagnetic signals and suppression of out-of-band signals. One of the core components used in these microwave devices is the resonator. Most of the resonators in use today are made of rectangular or other shaped metal cavities and large cylindrical dielectrics, which generally occupy a large volume, especially at low frequencies. In order to achieve good frequency selection characteristics and suppress the passage of clutter signals, it is generally necessary to combine several such resonators. Therefore, various microwave devices composed of several such resonators must occupy a larger volume, which brings great problems to the miniaturization and integration of microwave devices.
近十年来,超材料的出现使各种微波器件的小型化和集成化显示出无限的美景。超材料是由人工电磁谐振单元结构周期性排列而成的,每个谐振单元对外界电磁场的响应可以表现为电谐振、磁谐振或电磁谐振,分别用以实现宏观的等效负介电常数和负磁导率。具有负介电常数和负磁导率的谐振子的周期性排列就可实现电磁波的左手传输特性,从而实现自然界的材料无法具有的许多奇异功能。由于超材料使用了较大的谐振单元(与原子分子相比)取代了晶体中的原子或分子,从而使工作频率从x射线--紫外--红外频段降到光波--微波频段。In the past ten years, the emergence of metamaterials has shown infinite beauty in the miniaturization and integration of various microwave devices. Metamaterials are formed by periodic arrangement of artificial electromagnetic resonant unit structures. The response of each resonant unit to the external electromagnetic field can be expressed as electrical resonance, magnetic resonance or electromagnetic resonance, which are used to achieve macroscopic equivalent negative permittivity and negative permeability. The periodic arrangement of harmonic oscillators with negative permittivity and negative magnetic permeability can realize the left-handed transmission characteristics of electromagnetic waves, thereby realizing many strange functions that materials in nature cannot have. Since metamaterials use larger resonant units (compared to atomic molecules) to replace atoms or molecules in crystals, the operating frequency is reduced from x-ray-ultraviolet-infrared frequency bands to light waves-microwave frequency bands.
但是,目前关于超材料的研究大多集中在大量的人工电磁谐振子周期性排列的宏观效果上,对几个甚至是一个这样的超材料谐振子的研究与应用还非常少。However, most of the current research on metamaterials focuses on the macroscopic effect of a large number of artificial electromagnetic harmonic oscillators periodically arranged, and there is very little research and application on several or even one such metamaterial harmonic oscillator.
发明内容Contents of the invention
本发明的目的是提供一种基于金属结构LC谐振器的超材料谐振子及其应用。The object of the present invention is to provide a metamaterial resonator based on a metal structure LC resonator and its application.
本发明提供的超材料谐振子,为导电金属材料本体;所述本体具有一缺口。The metamaterial resonator provided by the present invention is a body of conductive metal material; the body has a gap.
所述导电金属材料具体可为铜。The conductive metal material can specifically be copper.
所述超材料谐振子的电感L部分由所述导电金属材料构成,电容C部分由所述缺口构成,且所述电感L部分的两个端面作为所示电容C部分的电极。The inductance L part of the metamaterial resonator is composed of the conductive metal material, the capacitance C part is composed of the gap, and the two end surfaces of the inductance L part serve as electrodes of the capacitance C part.
所述缺口的形状为任意形状。The shape of the notch is arbitrary.
所述电感L部分和电容C部分组成的结构对电磁波的响应等效为LC谐振。The response of the structure composed of the inductance L part and the capacitance C part to electromagnetic waves is equivalent to LC resonance.
另外,含有上述本发明提供的超材料谐振子的微波器件及该超材料谐振子在制作微波器件中的应用,也属于本发明的保护范围。其中,所述超材料谐振子的个数至少为一个,具体可为两个。所述微波器件具体可为滤波器、耦合器或多工器。In addition, the microwave device containing the metamaterial resonator provided by the present invention and the application of the metamaterial resonator in manufacturing microwave devices also belong to the protection scope of the present invention. Wherein, the number of the metamaterial harmonic oscillator is at least one, specifically two. Specifically, the microwave device may be a filter, a coupler or a multiplexer.
金属结构谐振器的工作状态有电谐振、磁谐振和电磁谐振三种状态,不同的谐振状态对应不同的谐振频率。在具体的实施过程中,可以选择超材料谐振子的任何一种谐振状态。金属结构谐振器的电磁谐振(LC谐振)对应的谐振频率最低,一般选取它为超材料谐振子的耦合谐振状态。The working state of the metal structure resonator has three states: electric resonance, magnetic resonance and electromagnetic resonance, and different resonance states correspond to different resonance frequencies. In a specific implementation process, any resonance state of the metamaterial harmonic oscillator can be selected. The electromagnetic resonance (LC resonance) of the metal structure resonator corresponds to the lowest resonance frequency, which is generally selected as the coupled resonance state of the metamaterial resonator.
对于本发明提供的超材料电磁谐振子而言,它们本身就是一个很好的电磁谐振器。而且,与传统材料和传统方法构成的谐振子相比,这些人工设计的超材料谐振子具有品质因数高、亚波长谐振的特点,它们能把入射电磁波局限在一个非常小的范围内长时间高效地周期性振荡,因而在各种微波器件的小型化、集成化和传输效率等问题上可带来突破性的进展。For the metamaterial electromagnetic resonators provided by the present invention, they themselves are good electromagnetic resonators. Moreover, compared with harmonic oscillators composed of traditional materials and traditional methods, these artificially designed metamaterial harmonic oscillators have the characteristics of high quality factor and sub-wavelength resonance, and they can confine the incident electromagnetic wave to a very small range for a long time. Therefore, it can bring breakthrough progress in the miniaturization, integration and transmission efficiency of various microwave devices.
对于单个超材料谐振子而言,当外界电磁波的频率与该谐振子的谐振频率相等时,电磁波的能量主要集中在超材料谐振子内振荡而无法继续向前传播,由此便形成了一个“陷波点”。之后的电磁能量几乎全部被反射回去而不能透射。但是,如果在此传播方向上有若干个超材料谐振子,情况就大不一样。例如,当两个超材料谐振子依次放在波的传播方向时,两谐振子会根据它们之间距离的不同而分为过耦合、临界耦合和欠耦合三种情况。在临界耦合的情况下,电磁波完全能够被耦合到出射端,传输效率也非常高,在不计损耗的情况下可视为全透射。在欠耦合的情况下,谐振频率处依然有较高的传输效率,但与临界耦合相比时传输效率下降不少。在过耦合的情况下,可以产生分别低于和高于原谐振频率的两个谐振频率点。本发明的多个超材料谐振子之间的耦合可采用任意一种情况。For a single metamaterial resonator, when the frequency of the external electromagnetic wave is equal to the resonant frequency of the resonator, the energy of the electromagnetic wave is mainly concentrated in the metamaterial resonator and cannot continue to propagate forward, thus forming a " notch point". The subsequent electromagnetic energy is almost all reflected back and cannot be transmitted. However, if there are several metamaterial resonators in this propagation direction, the situation is quite different. For example, when two metamaterial harmonic oscillators are placed in the direction of wave propagation in sequence, the two harmonic oscillators will be divided into three situations: over-coupling, critical coupling and under-coupling according to the distance between them. In the case of critical coupling, electromagnetic waves can be fully coupled to the exit end, and the transmission efficiency is also very high, which can be regarded as total transmission without loss. In the case of under-coupling, there is still a high transmission efficiency at the resonant frequency, but compared with the critical coupling, the transmission efficiency drops a lot. In the case of over-coupling, two resonant frequency points respectively lower and higher than the original resonant frequency can be generated. The coupling between the multiple metamaterial harmonic oscillators of the present invention can adopt any situation.
与现有技术相比,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:
本发明解决了用传统材料、传统方法制造的谐振器在各种微波器件中使用时尺寸大、集成度低等问题,采用金属结构LC谐振器实现超材料谐振子。这些超材料谐振子具有品质因数高、亚波长谐振的特点,它们能把入射电磁波局限在一个非常小的范围内长时间高效地周期性振荡,因而在各种微波器件的小型化、集成化和传输效率等问题上具有巨大的优势。The invention solves the problems of large size and low integration when the resonators manufactured by traditional materials and methods are used in various microwave devices, and adopts the metal structure LC resonator to realize the metamaterial resonator. These metamaterial harmonic oscillators have the characteristics of high quality factor and sub-wavelength resonance. They can confine the incident electromagnetic wave to a very small range and periodically oscillate efficiently for a long time. Therefore, they are widely used in the miniaturization, integration and It has huge advantages in transmission efficiency and other issues.
附图说明Description of drawings
图1为基于金属结构LC谐振器的两超材料谐振子之间的临界电磁谐振耦合形成的微波耦合器的示意图。FIG. 1 is a schematic diagram of a microwave coupler formed based on the critical electromagnetic resonance coupling between two metamaterial resonators of a metallic structure LC resonator.
图2为实施例1中微波耦合器的仿真结果图。FIG. 2 is a diagram of the simulation results of the microwave coupler in Embodiment 1.
图3为基于金属结构LC谐振器的两超材料谐振子之间的电磁谐振耦合形成的双频点微波带阻滤波器的示意图Figure 3 is a schematic diagram of a dual-frequency point microwave band-stop filter formed based on the electromagnetic resonance coupling between two metamaterial resonators of a metal structure LC resonator
图4为实施例2中双频点微波带阻滤波器的仿真结果图。FIG. 4 is a diagram of the simulation results of the dual-frequency point microwave band rejection filter in Embodiment 2.
具体实施方式Detailed ways
下面结合具体实施例对本发明作进一步阐述,但本发明并不限于以下实施例。所述方法如无特别说明均为常规方法。所述原材料如无特别说明均能从公开商业途径获得。The present invention will be further described below in conjunction with specific examples, but the present invention is not limited to the following examples. The methods are conventional methods unless otherwise specified. The raw materials can be obtained from open commercial channels unless otherwise specified.
实施例1Example 1
图1为基于金属结构LC谐振器的两超材料谐振子之间的临界电磁谐振耦合形成的微波耦合器的示意图。图中所示的基于金属结构LC谐振器的超材料谐振子是采用印刷电路板技术印制而成的金属铜的开口谐振环结构。该超材料谐振子由铜本体构成,且铜本体具有一缺口。该超材料谐振子的形状为具有一缺口的铜环。铜环的边长为4mm,宽为0.5mm,缺口为0.3mm。缺口部分相当于电容C,其他的金属部分相当于电感L,这样就形成了一个标准的LC谐振器。图1中金属板的厚度为1mm,在它的中心有一半径为2.5mm的圆孔,以使电磁波能够耦合到金属板的另一侧。如果只有圆孔参与耦合,它能够耦合到对面的电磁波非常地微弱。但是,如果在金属板圆孔的两侧各放一个基于开口金属环结构的超材料谐振子,此时的耦合强度如图2所示,在9.5-10GHz的范围内,几乎所有的电磁波都能够耦合到圆孔的对面去。另外,与实现的耦合器的工作波长相比,这里所用的超材料谐振子的尺寸远远小于它的工作波长,即满足亚波长尺度的要求,所以成功地实现了基于金属环结构的超材料谐振子间的耦合而成的小型化微波耦合器。FIG. 1 is a schematic diagram of a microwave coupler formed based on the critical electromagnetic resonance coupling between two metamaterial resonators of a metallic structure LC resonator. The metamaterial resonator based on the metal structure LC resonator shown in the figure is a metal copper split resonator ring structure printed by printed circuit board technology. The metamaterial resonator is composed of a copper body, and the copper body has a gap. The shape of the metamaterial resonator is a copper ring with a gap. The side length of the copper ring is 4mm, the width is 0.5mm, and the gap is 0.3mm. The gap part is equivalent to the capacitance C, and the other metal parts are equivalent to the inductance L, thus forming a standard LC resonator. The thickness of the metal plate in Figure 1 is 1mm, and there is a circular hole with a radius of 2.5mm in its center, so that electromagnetic waves can be coupled to the other side of the metal plate. If only the round hole participates in the coupling, it can couple to the opposite electromagnetic wave very weakly. However, if a metamaterial resonator based on a split metal ring structure is placed on both sides of the circular hole in the metal plate, the coupling strength at this time is shown in Figure 2. In the range of 9.5-10GHz, almost all electromagnetic waves can Coupled to the opposite side of the round hole. In addition, compared with the working wavelength of the implemented coupler, the size of the metamaterial resonator used here is much smaller than its working wavelength, that is, it meets the requirements of the sub-wavelength scale, so the metamaterial based on the metal ring structure is successfully realized A miniaturized microwave coupler formed by coupling between resonators.
实施例2Example 2
图3为基于金属结构LC谐振器的两超材料谐振子之间的电磁谐振耦合形成的双频点微波带阻滤波器的示意图。图中所示的超材料谐振子是采用印刷电路板技术印制而成的金属铜的开口谐振环结构。该超材料谐振子由铜本体构成,且铜本体具有一缺口。该超材料谐振子的形状为具有一缺口的铜环。铜环的边长为5mm,宽为0.75mm,缺口为1mm。缺口部分相当于电容C,其他的金属部分相当于电感L,这样就形成了一个标准的LC谐振器。当两谐振器之间的距离为2mm时,形成的双频点带阻滤波器的透射系数如图4所示。图中在6.1GHz和7.1GHz处有两个明显的陷波点,从而就实现了高性能的带阻滤波器。另外,与实现的滤波器的工作波长相比,这里所用的超材料谐振子的尺寸远远小于它的工作波长,即满足亚波长尺度的要求,所以成功地实现了基于金属环结构的超材料谐振子间的耦合而成的小型化微波带阻滤波器。FIG. 3 is a schematic diagram of a dual-frequency point microwave band-stop filter formed based on electromagnetic resonance coupling between two metamaterial resonators of a metal structure LC resonator. The metamaterial resonator shown in the figure is a metal copper split resonator ring structure printed by printed circuit board technology. The metamaterial resonator is composed of a copper body, and the copper body has a gap. The shape of the metamaterial resonator is a copper ring with a gap. The side length of the copper ring is 5mm, the width is 0.75mm, and the gap is 1mm. The gap part is equivalent to the capacitance C, and the other metal parts are equivalent to the inductance L, thus forming a standard LC resonator. When the distance between the two resonators is 2 mm, the transmission coefficient of the formed dual-frequency point band-stop filter is shown in Figure 4. In the figure, there are two obvious notch points at 6.1GHz and 7.1GHz, thus realizing a high-performance band-stop filter. In addition, compared with the operating wavelength of the realized filter, the size of the metamaterial harmonic oscillator used here is much smaller than its operating wavelength, that is, it meets the requirements of the sub-wavelength scale, so the metamaterial based on the metal ring structure is successfully realized. A miniaturized microwave band-stop filter formed by coupling between harmonic oscillators.
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CN105305091A (en) * | 2015-10-13 | 2016-02-03 | 复旦大学 | Tunable gradient meta-surface-based reflection electromagnetic wave modulator and design method thereof |
CN107404004A (en) * | 2016-05-19 | 2017-11-28 | 深圳超级数据链技术有限公司 | Meta Materials, antenna reflective face, the control method of Meta Materials and device |
CN109728442A (en) * | 2018-11-19 | 2019-05-07 | 浙江大学 | A solid electromagnetic vacuum material based on electric resonance unit |
CN109728442B (en) * | 2018-11-19 | 2020-10-16 | 浙江大学 | A solid electromagnetic vacuum material based on electric resonance unit |
CN112002967A (en) * | 2020-07-20 | 2020-11-27 | 重庆邮电大学 | A "back-symmetric open square slot" type terahertz low-pass angle filter |
CN114512556A (en) * | 2020-11-16 | 2022-05-17 | 北京索通新动能科技有限公司 | Photoelectric detector based on asymmetric metamaterial structure |
CN114512556B (en) * | 2020-11-16 | 2023-11-03 | 北京索通新动能科技有限公司 | A photodetector based on asymmetric metamaterial structure |
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