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CN103700948B - Double cantilever E types reversely nested LHM with adjustable cross metal wire structure - Google Patents

Double cantilever E types reversely nested LHM with adjustable cross metal wire structure Download PDF

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CN103700948B
CN103700948B CN201410011259.6A CN201410011259A CN103700948B CN 103700948 B CN103700948 B CN 103700948B CN 201410011259 A CN201410011259 A CN 201410011259A CN 103700948 B CN103700948 B CN 103700948B
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metal wire
double cantilever
cantilever
dielectric substrate
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CN103700948A (en
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游佰强
金琬晴
戚宇轩
周建华
李海雄
孙越
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Xiamen University
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Abstract

带有可调十字金属线结构的双悬臂E型反向嵌套左手材料,涉及一种左手材料。提供一种带有可调十字金属线结构的双悬臂E型反向嵌套左手材料。设有介电基板、双悬臂E型金属线和十字金属线结构;所述双悬臂E型金属线反向对称刻蚀在介电基板的一侧,交错嵌套的E字结构中间臂断开,所述十字金属线结构设在介电基板背面。实现了左手材料双悬臂E型结构各边长度、两个悬臂E型金属线的耦合度、十字结构正交交叠位置的易于调控,通过调节单元几何参数,实现某个或多个左手频段可控。实现改变入射波方向和电场极化方向而保持磁场极化方向不变时,阵列结构的左手特性不发生改变,拓宽了电磁波的入射角度,可以实现从两个方向上入射同时表现左手特性。

A double cantilever E-type reverse nested left-hand material with an adjustable cross wire structure relates to a left-hand material. A double cantilever E-type reverse nested left hand material with adjustable cross wire construction is available. It is equipped with a dielectric substrate, a double cantilever E-shaped metal wire and a cross metal wire structure; the double cantilever E-shaped metal wire is reversely and symmetrically etched on one side of the dielectric substrate, and the middle arm of the staggered nested E-shaped structure is disconnected , the cross wire structure is arranged on the back side of the dielectric substrate. The length of each side of the double cantilever E-shaped structure of the left-hand material, the coupling degree of the two cantilever E-shaped metal wires, and the cross-structure orthogonal overlapping position are easy to control. By adjusting the geometric parameters of the unit, one or more left-hand frequency bands can be adjusted. control. When changing the incident wave direction and electric field polarization direction while keeping the magnetic field polarization direction unchanged, the left-handed characteristics of the array structure do not change, widen the incident angle of electromagnetic waves, and realize the left-handed characteristics when incident from two directions at the same time.

Description

带有可调十字金属线结构的双悬臂E型反向嵌套左手材料Double cantilever E-type reverse nested left hand material with adjustable cross wire structure

技术领域technical field

本发明涉及一种左手材料,特别是涉及一种可以实现在两个方向上入射、频率特性可控的带有可调十字金属线结构的双悬臂E型反向嵌套左手材料。The invention relates to a left-handed material, in particular to a double-cantilever E-type reverse-nested left-handed material with an adjustable cross wire structure that can realize incidence in two directions and controllable frequency characteristics.

背景技术Background technique

左手材料(left-handedmetamaterials)是一种具有负介电常数和负磁导率的人工复合材料,是由前苏联物理学家Mandelshtam于1940年最初提出的周期分布阵列结构。这种刻蚀在微波电路介质基板上的周期阵列结构能够引起电场和磁场在一定频率范围内的谐振,使得该结构等效介电常数和磁导率同时表现为负值。左手材料的主要特点是,在左手材料中传播的电磁波的相速度和群速度方向相反,电磁波的能量传播方向和相速度方向相反,之间满足左手螺旋关系。20世纪90年代,Pendry等人(V.G.Veselago.TheElectrodynamicsofSubstanceswithSimultanesouslyNegtiveValue[J].SovietPhysics.1968,10:509-514)提出了用周期性金属线组成的理论模型,推导出该结构模型的负介电常数频段。根据Pendry的研究,通过对开口谐振环,即SRRs的周期型排列,可以使材料的磁性特性在一定的频段内呈负值。1996年他首先提出了周期排列的金属细导线在入射频率比等离子体谐振频率低时,会出现介电常数为负的情况,同时给出了计算有效介电常数的解析模型。1999年他的研究小组再一次提出周期放置的开环谐振器阵列,可以表现出负磁导率的特性,并且论文中给出了计算SRR磁导率的模型结构。2000年Smith以平均值法(HsuYJ,HuangYC,LihJS.Electromagneticresonanceindeformedsplitringresonatorsoflefthandedmeta-materials[J].2003,258:161-166)为理论依据,提出了三种直接能够计算左手材料有效介电常数及有效磁导率的方法,分析了左手材料负折射率的解析解构,并得到了左手材料负折射率与材料介电常数和磁导率的关系。2006年,Xu等人的研究向人们展示了SRR阵列有效本构参数张量的提取技术(AntoniadesMA,EleftheriadesGV.Compactlinerleadmetamateralphaseshiftersforbroadbandapplications.[J]IEEEAntennasandWirelessPropagationLetters.2003,2:103-106),指出在本构参数张量提取过程中,可以用等效电路方法来描述物理本质。近年来,左手材料被应用在众多领域,包括电磁学、光学、声学、电磁隐身、通信和医学等领域,成为国内外学者的研究热点。除SRR结构外,很多结构在某个频点或频段已经表现出了左手特性,包括螺旋环型结构、树枝状结构、蘑菇型结构、双S型结构、Z型结构等。但这些结构的左手材料只能在某一个特定入射方向上实现左手特性,因此缺乏应用的灵活性和多样性。Left-handed material (left-handed metamaterials) is an artificial composite material with negative permittivity and negative magnetic permeability. It is a periodic distribution array structure originally proposed by the former Soviet physicist Mandelshtam in 1940. The periodic array structure etched on the dielectric substrate of the microwave circuit can cause the resonance of the electric field and the magnetic field in a certain frequency range, so that the equivalent permittivity and magnetic permeability of the structure exhibit negative values at the same time. The main characteristic of the left-handed material is that the phase velocity of the electromagnetic wave propagating in the left-handed material is opposite to the direction of the group velocity, and the energy propagation direction of the electromagnetic wave is opposite to the direction of the phase velocity. and satisfy the left-handed spiral relationship. In the 1990s, Pendry et al. (VG Veselago. The Electrodynamics of Substances with Simultanesously Negtive Value [J]. Soviet Physics. 1968, 10: 509-514) proposed a theoretical model composed of periodic metal wires, and deduced the negative dielectric constant frequency band of the structural model. According to Pendry's research, through the periodic arrangement of split resonant rings, that is, SRRs, the magnetic properties of the material can be negative in a certain frequency range. In 1996, he first proposed that the dielectric constant of thin metal wires arranged periodically will be negative when the incident frequency is lower than the plasma resonance frequency, and at the same time he gave an analytical model for calculating the effective dielectric constant. In 1999, his research group once again proposed that the periodically placed open-loop resonator array can exhibit the characteristics of negative magnetic permeability, and the model structure for calculating the magnetic permeability of SRR was given in the paper. In 2000, based on the average method (HsuYJ, HuangYC, LihJS.Electromagneticresonanceindeformedsplitringresonatorsoflefthandedmeta-materials[J].2003,258:161-166) as the theoretical basis, Smith proposed three kinds of effective permittivity and effective permeability of left-handed materials that can be directly calculated. The analysis of the negative refractive index of the left-handed material is analyzed by the method of the ratio, and the relationship between the negative refractive index of the left-handed material and the material permittivity and magnetic permeability is obtained. In 2006, the research by Xu et al. showed people the extraction technology of effective constitutive parameter tensor of SRR array (AntoniadesMA, EleftheriadesGV. In the process of quantity extraction, the equivalent circuit method can be used to describe the physical essence. In recent years, left-handed materials have been applied in many fields, including electromagnetics, optics, acoustics, electromagnetic stealth, communication, and medicine, and have become a research hotspot among scholars at home and abroad. In addition to the SRR structure, many structures have shown left-handed characteristics at a certain frequency point or frequency band, including spiral ring structure, dendritic structure, mushroom structure, double S structure, Z structure, etc. However, the left-handed materials of these structures can only achieve left-handed characteristics in a specific incident direction, so they lack the flexibility and diversity of applications.

发明内容Contents of the invention

本发明的目的是提供一种带有可调十字金属线结构的双悬臂E型反向嵌套左手材料。The object of the present invention is to provide a double cantilever E-type reverse nested left-hand material with an adjustable cross wire structure.

本发明设有介电基板、双悬臂E型金属线和十字金属线结构;所述双悬臂E型金属线反向对称刻蚀在介电基板的一侧,交错嵌套的E字结构中间臂断开,所述十字金属线结构设在介电基板背面。The invention is provided with a dielectric substrate, a double cantilever E-shaped metal wire and a cross metal wire structure; the double cantilever E-shaped metal wire is reversely etched symmetrically on one side of the dielectric substrate, and the middle arm of the interlaced nested E-shaped structure disconnected, the cross wire structure is disposed on the back of the dielectric substrate.

所述介电基板可采用微波介电材料基板,介电基板的介电常数可为2~10,优选4.4±5%;介电基板的厚度可为0.25~1.3mm,优选0.40mm±5%。The dielectric substrate can be a microwave dielectric material substrate, the dielectric constant of the dielectric substrate can be 2-10, preferably 4.4±5%; the thickness of the dielectric substrate can be 0.25-1.3mm, preferably 0.40mm±5% .

所述十字金属线可采用带有均匀分布可调十字金属线,所述带有均匀分布可调十字金属线可采用至少2组周期性的双悬臂E型金属线结构阵列,所述十字金属线与双悬臂E型金属线同周期同间距。The cross metal wire can adopt an evenly distributed adjustable cross metal wire, and the evenly distributed adjustable cross metal wire can adopt at least two sets of periodic double cantilever E-type metal wire structure arrays, and the cross metal wire It has the same cycle and the same spacing as the double cantilever E-shaped metal wire.

本发明实现了左手材料双悬臂E型结构各边长度、两个悬臂E型金属线的耦合度、十字结构正交交叠位置的易于调控,通过调节单元几何参数,能够实现某个或多个左手频段可控。由于采用了以上结构,实现了改变入射波方向和电场极化方向而保持磁场极化方向不变时,阵列结构的左手特性不发生改变,拓宽了电磁波的入射角度,这样制备的新型微波左手材料可以实现从两个方向上入射同时表现左手特性,是一种新型的双入射左手材料,具有在实际应用中能够从多方向入射所表现出相同左手性能的优点,实现了左手材料的多维化和多向化。The invention realizes the easy control of the length of each side of the double cantilever E-shaped structure of the left-hand material, the coupling degree of the two cantilever E-shaped metal wires, and the orthogonal overlapping position of the cross structure. By adjusting the geometric parameters of the unit, one or more can be realized. The left-hand band is controllable. Due to the adoption of the above structure, the left-handed characteristics of the array structure do not change when the direction of the incident wave and the polarization direction of the electric field are changed while keeping the polarization direction of the magnetic field unchanged, and the incident angle of the electromagnetic wave is widened. The new microwave left-handed material prepared in this way It is a new type of double-incident left-handed material, which can realize the incident from two directions and show the left-handed characteristics at the same time. It has the advantage of being able to show the same left-handed performance from multi-directional incidents in practical applications, and realizes the multi-dimensionalization and integration of left-handed materials. Multidirectional.

附图说明Description of drawings

图1为本发明实施例中带有均匀分布可调十字金属线结构的双悬臂E型反向嵌套的新型双入射左手材料示意图。FIG. 1 is a schematic diagram of a new double-incidence left-handed material with double-cantilever E-type reverse nesting with a uniformly distributed and adjustable cross wire structure in an embodiment of the present invention.

图2为本发明实施例中左手材料背面的可调十字金属线单元结构。Fig. 2 is the structure of the adjustable cross wire unit on the back of the left-hand material in the embodiment of the present invention.

图3为本发明实施例在一块高性能介电材料微波基板上分别对位刻蚀出周期性的双悬臂E型结构,在沿着波的传播方向上雕刻至少3个单元,并列至少3排的基板在两个方向上构成周期性结构,整体上实现左手特性和双入射左手特性。Figure 3 shows that the embodiment of the present invention etches a periodic double cantilever E-shaped structure on a high-performance dielectric material microwave substrate, and engraves at least 3 units along the propagation direction of the wave, and arranges them in at least 3 rows The substrate forms a periodic structure in two directions, and realizes the left-handed characteristic and the double-incidence left-handed characteristic as a whole.

图4为将相应参数(中心间距为3.00±0.01mm,边长a=2.00±0.01mm,宽度w=0.20±0.01mm,b=2.20±0.01mm,中心边长度,d=0.15±0.01mm,p=0.05±0.01mm,w=0.25±0.01mm,L=3.00±0.01mm)的样品填充于波导内时,波导端口传输系数S12的幅度和端口反射系数S11的幅度。Figure 4 shows the corresponding parameters (center distance is 3.00±0.01mm, side length a=2.00±0.01mm, width w=0.20±0.01mm, b=2.20±0.01mm, center side length, d=0.15±0.01mm, When p=0.05±0.01mm, w=0.25±0.01mm, L=3.00±0.01mm) samples are filled in the waveguide, the amplitude of waveguide port transmission coefficient S12 and port reflection coefficient S11.

图5为将相应参数(中心间距为3.00±0.01mm,边长a=2.00±0.01mm,宽度w=0.20±0.01mm,b=2.20±0.01mm,中心边长度,d=0.15±0.01mm,p=0.05±0.01mm,w=0.25±0.01mm,L=3.00±0.01mm)的样品填充于波导内时,波导端口传输系数S12的相位和端口反射系数S11的相位。Figure 5 shows the corresponding parameters (center distance is 3.00±0.01mm, side length a=2.00±0.01mm, width w=0.20±0.01mm, b=2.20±0.01mm, center side length, d=0.15±0.01mm, When p=0.05±0.01mm, w=0.25±0.01mm, L=3.00±0.01mm) samples are filled in the waveguide, the phase of waveguide port transmission coefficient S12 and port reflection coefficient S11 phase.

图6为图4中的样品的等效介电常数的实部。FIG. 6 is the real part of the equivalent dielectric constant for the samples in FIG. 4 .

图7为图4中的样品的等效磁导率。FIG. 7 shows the equivalent magnetic permeability of the samples in FIG. 4 .

图8为改变电磁波在x轴方向的入射,让电磁波以y轴方向入射,保持磁场极化方向不变。将上述样品填充于波导内时,波导端口传输系数S12的幅度和端口反射系数S11的幅度。Fig. 8 is to change the incidence of the electromagnetic wave in the direction of the x-axis, let the electromagnetic wave enter in the direction of the y-axis, and keep the polarization direction of the magnetic field unchanged. When the above sample is filled in the waveguide, the magnitude of the waveguide port transmission coefficient S12 and the magnitude of the port reflection coefficient S11.

图9为改变电磁波在x轴方向的入射,让电磁波以y轴方向入射,保持磁场极化方向不变。将上述样品填充于波导内时,波导端口传输系数S12的相位和端口反射系数S11的相位。FIG. 9 shows changing the incidence of electromagnetic waves in the direction of the x-axis, making the incidence of electromagnetic waves in the direction of the y-axis, and keeping the polarization direction of the magnetic field unchanged. When the above sample is filled in the waveguide, the phase of the waveguide port transmission coefficient S12 and the phase of the port reflection coefficient S11.

具体实施方式detailed description

以下结合实施例和附图对本发明作进一步说明。The present invention will be further described below in conjunction with embodiment and accompanying drawing.

参见图1~3,本发明实施例设有至少3排高性能介电材料微波基板1;所述高性能介电材料微波基板1的一侧11刻蚀至少3个双悬臂E型金属线单元,所述双悬臂E型金属线单元是由2个反向错位对称嵌套的E型金属线12组成,高性能介电材料微波基板1的另一侧21刻蚀至少3个十字金属线单元22,所述十字金属线单元22和双悬臂E型金属线单元的数目相同,所述十字金属线单元22的横边221与双悬臂E型金属线单元的纵边121垂直,所述十字金属线单元22的纵边222与双悬臂E型金属线单元的纵边121平行,双悬臂E型金属线单元的中心与十字金属线单元的中心在同一水平高度,双悬臂E型金属线单元之间的距离相同,十字金属线单元之间的距离相同。Referring to Figures 1 to 3, the embodiment of the present invention is provided with at least 3 rows of high-performance dielectric material microwave substrates 1; one side 11 of the high-performance dielectric material microwave substrate 1 is etched with at least 3 double cantilever E-type metal wire units , the double cantilever E-type metal wire unit is composed of two E-type metal wires 12 that are reversely dislocated and symmetrically nested, and at least three cross metal wire units are etched on the other side 21 of the microwave substrate 1 made of high-performance dielectric material 22, the number of the cross metal wire unit 22 and the double cantilever E-type metal wire unit are the same, the transverse side 221 of the cross metal wire unit 22 is perpendicular to the longitudinal side 121 of the double cantilever E-type metal wire unit, and the cross metal wire unit The longitudinal side 222 of the line unit 22 is parallel to the longitudinal side 121 of the double cantilever E-type metal wire unit, and the center of the double-cantilever E-type metal wire unit is at the same level as the center of the cross metal wire unit. The distance between them is the same, and the distance between the cross metal wire units is the same.

所述高性能介电材料微波基板1的介电常数为2~10,最好为4.4±5%。厚度可为0.25~1.3mm,最好为0.40mm±5%。The dielectric constant of the high-performance dielectric material microwave substrate 1 is 2-10, preferably 4.4±5%. The thickness can be 0.25~1.3mm, preferably 0.40mm±5%.

所述E型金属线12的外边长a可为2~3mm,金属各边的宽度w=0.05~0.25mm,双悬臂E的内部边的长度b=1~2.5mm,中心边与侧边之间的距离d=0.1~0.5mm,两个悬臂E的对应各边之间的距离p=0.1~0.5mm,厚度为0.01~0.03mm。其典型值为a=2.00±0.01mm,w=0.20±0.01mm,b=2.20±0.01mm,d=0.15±0.01mm,p=0.05±0.01mm,金属线的厚度为0.018mm±5%。The length a of the outer side of the E-shaped metal wire 12 can be 2-3mm, the width w=0.05-0.25mm of each side of the metal, the length b=1-2.5mm of the inner side of the double cantilever E, and the distance between the center side and the side The distance between them is d=0.1-0.5mm, the distance between the corresponding sides of the two cantilevers E is p=0.1-0.5mm, and the thickness is 0.01-0.03mm. Its typical values are a=2.00±0.01mm, w=0.20±0.01mm, b=2.20±0.01mm, d=0.15±0.01mm, p=0.05±0.01mm, and the thickness of the metal wire is 0.018mm±5%.

所述十字金属线22的长度为L=2~6mm,宽度w=0.10~0.30mm,厚度为0.01~0.03mm。其典型值为L=3.00±0.01mm,w=0.25±0.02mm,厚度为0.018mm±5%。The length of the cross wire 22 is L=2-6 mm, the width w=0.10-0.30 mm, and the thickness is 0.01-0.03 mm. Its typical value is L=3.00±0.01mm, w=0.25±0.02mm, and the thickness is 0.018mm±5%.

优化组合后可获取左手材料不同电磁参数,包括等效介电常数和等效磁导率。在3~12GHz范围内可由几何参量调谐控制实现某个频点上等效介电常数和等效磁导率同时为负。After optimizing the combination, different electromagnetic parameters of left-handed materials can be obtained, including equivalent permittivity and equivalent permeability. In the range of 3-12GHz, the equivalent permittivity and equivalent permeability at a certain frequency point can be negative at the same time by geometric parameter tuning control.

本发明采用电路板刻蚀技术,在厚度为0.40mm±5%的聚四氟乙烯基板的某一面刻蚀出至少三个完全相同的金属铜双悬臂E型单元构成周期阵列,周期重复的金属铜双悬臂E型单元必须分布在与双悬臂E型金属铜线的纵边垂直的一条轴线上,中心间距为6.5±3.5mm,金属铜的厚度为0.018mm±5%,对称金属铜双悬臂E型单元的外边长a=2.00±0.01mm,边的宽度w=0.20±0.01mm,双悬臂E型单元中心边的长度b=2.20±0.01mm,中心边与侧边之间的距离d=0.15±0.01mm,两个双悬臂E的对应各边之间的距离p=0.05±0.01mm;聚四氟乙烯基板另一侧对应双悬臂E结构中心位置出刻蚀长度L=3.00±0.01mm,宽度w=0.25±0.02mm的十字金属线周期阵列,重复周期与双悬臂E结构相同。将制成的一个方向上周期阵列结构在高性能介电材料微波基板轴线方向上同样排列至少三排构成如图3所示的周期阵列,相邻基板之间的距离为1.25mm。这样制作而成的周期阵列结构,对单元结构中双悬臂E型结构中各个边的长度宽度和十字金属线长度宽度等几何参量综合优化组合,取不同的值,就可以制成能够工作在特定频段的双悬臂E结构和十字金属线组合而成的左手材料,并且具有不同的等效介电常数、等效磁导率和等效折射率。The invention adopts circuit board etching technology to etch at least three identical metal copper double cantilever E-type units on one side of a polytetrafluoroethylene substrate with a thickness of 0.40mm±5% to form a periodic array, and the periodically repeated metal Copper double cantilever E-type units must be distributed on an axis perpendicular to the longitudinal side of the double cantilever E-type metal copper wire, the center distance is 6.5±3.5mm, the thickness of metal copper is 0.018mm±5%, symmetrical metal copper double cantilever The outer length of the E-type unit is a=2.00±0.01mm, the width of the side is w=0.20±0.01mm, the length of the central side of the double-cantilever E-type unit is b=2.20±0.01mm, and the distance between the central side and the side is d= 0.15±0.01mm, the distance between the corresponding sides of the two double cantilevers E is p=0.05±0.01mm; the other side of the PTFE substrate corresponds to the etching length L=3.00±0.01mm from the center of the structure of the double cantilever E , a periodic array of cross metal wires with a width w=0.25±0.02mm, and the repeat period is the same as that of the double cantilever E structure. The fabricated periodic array structure in one direction is also arranged in at least three rows in the axial direction of the high-performance dielectric material microwave substrate to form a periodic array as shown in Figure 3, and the distance between adjacent substrates is 1.25mm. The periodic array structure made in this way can be made to be able to work in a specific The left-handed material is composed of double cantilever E structure and cross metal wire in the frequency band, and has different equivalent permittivity, equivalent magnetic permeability and equivalent refractive index.

实施例一:Embodiment one:

采用典型PCB制版技术,在厚度为0.40mm±5%覆铜箔厚度e=0.018mm±5%的聚四氟乙烯基板的一侧刻蚀出至少三个完全相同的金属铜双悬臂E型单元结构,由此构成周期阵列,周期重复的金属铜双悬臂E型结构必须排列在与E字结构三个水平边平行的一条轴线上。其中,中心间距为3.00±0.01mm,对称双悬臂E型结构的外边长a=2.00±0.01mm,金属各边的宽度w=0.20±0.01mm,双悬臂E型结构的中心边长度b=2.20±0.01mm,中心边与侧边之间的距离d=0.15±0.01mm,两个双悬臂E型结构的对应各边之间的距离p=0.05±0.01mm。在另一侧刻蚀出中心与双悬臂E型结构中心位置对应且直边垂直于E字结构的三个水平边,具有同样周期的均匀分布可调十字金属线结构阵列,均匀分布的可调十字金属线结构两条相互垂直的线宽度w=0.25±0.01mm,线的长度L=3.00±0.01mm。这样制备而成的在微波入射方向成5个单元结构的周期性左手材料,并列放入波导腔内部使在磁场H的方向上也成3个单元结构的周期性。使得电磁波从x方向入射,测得装入左手材料的波导的端口传输系数和反射系数,波导端口传输系数S12的幅度和端口反射系数S11的幅度如图4所示,波导端口传输系数S12的相位和端口反射系数S11的相位如图5所示,以及由测量系数计算出的等效介电常数如图6所示,等效磁导率如图7所示。结果显示在10GHz附近的频域中,等效介电常数和磁导率均为负值,这表明在10GHz频率附近该结构可以作为一种左手材料来应用。Using typical PCB plate making technology, etch at least three identical metal copper double cantilever E-type units on one side of the PTFE substrate with a thickness of 0.40mm±5% copper clad foil thickness e=0.018mm±5%. The structure constitutes a periodic array, and the periodically repeated metal copper double cantilever E-shaped structure must be arranged on an axis parallel to the three horizontal sides of the E-shaped structure. Among them, the center distance is 3.00±0.01mm, the outer side length of the symmetrical double-cantilever E-shaped structure is a=2.00±0.01mm, the width of each side of the metal is w=0.20±0.01mm, and the length of the central side of the double-cantilever E-shaped structure is b=2.20 ±0.01mm, the distance between the center side and the side side d=0.15±0.01mm, the distance between the corresponding sides of the two double cantilever E-shaped structures p=0.05±0.01mm. On the other side, the center is etched to correspond to the center position of the double cantilever E-shaped structure and the straight sides are perpendicular to the three horizontal sides of the E-shaped structure. There is an array of uniformly distributed and adjustable cross metal wire structures with the same period, and the evenly distributed adjustable The width of the two mutually perpendicular lines of the cross wire structure is w=0.25±0.01mm, and the length of the lines is L=3.00±0.01mm. The thus-prepared periodic left-handed material with five unit structures in the incident direction of the microwave is placed side by side in the waveguide cavity to form a periodicity of three unit structures in the direction of the magnetic field H. The electromagnetic wave is incident from the x direction, and the port transmission coefficient and reflection coefficient of the waveguide loaded with the left-hand material are measured. The amplitude of the waveguide port transmission coefficient S12 and the port reflection coefficient S11 are shown in Figure 4. The phase of the waveguide port transmission coefficient S12 The phase with the port reflection coefficient S11 is shown in Figure 5, and the equivalent dielectric constant calculated from the measured coefficient is shown in Figure 6, and the equivalent magnetic permeability is shown in Figure 7. The results show that in the frequency domain around 10GHz, the equivalent permittivity and permeability are both negative, which indicates that the structure can be used as a left-handed material around 10GHz.

实施例二:Embodiment two:

采用典型PCB制版技术,在厚度为0.40mm±5%覆铜箔厚度e=0.018mm±5%的聚四氟乙烯基板的一侧刻蚀出至少三个完全相同的金属铜双悬臂E型单元结构,由此构成周期阵列,周期重复的金属铜双悬臂E型结构必须排列在与E字结构三个水平边平行的一条轴线上。其中,中心间距为3.00±0.01mm,对称双悬臂E型结构的外边长a=2.00±0.01mm,金属各边的宽度w=0.20±0.01mm,双悬臂E的中心边长度b=2.20±0.01mm,中心边与侧边之间的距离d=0.15±0.01mm,两个双悬臂E型结构的对应各边之间的距离p=0.05±0.01mm。在另一侧刻蚀出中心与双悬臂E型结构中心位置对应且直边垂直于E字结构的三个水平边,具有同样周期的均匀分布可调十字金属线结构阵列,十字金属线结构两条相互垂直的线宽度w=0.25±0.01mm,线的长度L=3.00±0.01mm。这样制备而成的在微波入射方向上成5个单元结构的周期性左手材料,并列放入波导腔内部使在磁场H的方向上成3个单元结构的周期性,但是电磁波从y方向入射,保持磁场极化方向不变,测得装入左手材料的波导的端口传输系数和反射系数,波导端口传输系数S12的幅度和端口反射系数S11的幅度如图8所示,波导端口传输系数S12的相位和端口反射系数S11的相位如图9所示。由图8和9可知,本发明从两个方向入射电磁波时,仿真计算结果没有差异,在10GHz附近的频域内等效介电常数和磁导率都是负值,表明带有均匀分布可调十字金属线结构的双悬臂E型反向嵌套左手材料可以实现在两个相互垂直方向入射的左手特性,是一种双入射左手材料。Using typical PCB plate making technology, etch at least three identical metal copper double cantilever E-type units on one side of the PTFE substrate with a thickness of 0.40mm±5% copper clad foil thickness e=0.018mm±5%. The structure constitutes a periodic array, and the periodically repeated metal-copper double cantilever E-shaped structure must be arranged on an axis parallel to the three horizontal sides of the E-shaped structure. Among them, the center distance is 3.00±0.01mm, the outer side length of the symmetrical double-cantilever E-shaped structure is a=2.00±0.01mm, the width of each side of the metal is w=0.20±0.01mm, and the length of the central side of the double-cantilever E is b=2.20±0.01 mm, the distance between the central side and the side side d=0.15±0.01mm, and the distance between the corresponding sides of the two double cantilever E-shaped structures p=0.05±0.01mm. On the other side, the center is etched corresponding to the center position of the double cantilever E-shaped structure, and the straight sides are perpendicular to the three horizontal sides of the E-shaped structure. An array of uniformly distributed and adjustable cross metal wire structures with the same period is etched. The width of the lines perpendicular to each other is w=0.25±0.01mm, and the length of the lines is L=3.00±0.01mm. The periodic left-handed material with 5 unit structures prepared in this way is placed side by side in the waveguide cavity to form a periodicity of 3 unit structures in the direction of the magnetic field H, but the electromagnetic wave is incident from the y direction, Keeping the polarization direction of the magnetic field unchanged, the port transmission coefficient and reflection coefficient of the waveguide installed in the left-hand material are measured. The magnitude of the waveguide port transmission coefficient S12 and the port reflection coefficient S11 are shown in Figure 8. The waveguide port transmission coefficient S12 The phase and the phase of the port reflection coefficient S11 are shown in FIG. 9 . As can be seen from Figures 8 and 9, when the present invention is incident with electromagnetic waves from two directions, there is no difference in the simulation calculation results, and the equivalent permittivity and magnetic permeability are both negative in the frequency domain around 10 GHz, indicating that there is a uniformly distributed adjustable The double cantilever E-type reverse nested left-handed material with a cross metal wire structure can realize the left-handed characteristics of incidence in two mutually perpendicular directions, and is a double-incidence left-handed material.

Claims (6)

1. with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that be provided with dielectric substrate, double cantilever E type metal wire and cross metal wire structure;Described pair of cantilever E type metal wire reverse symmetry is etched in the side of dielectric substrate, and staggered nested E word structure intermediate arm disconnects, and described cross metal wire structure is located at the opposite side of dielectric substrate;Described double cantilever E types with adjustable cross metal wire structure reversely nested LHM uses at least 2 group the most double cantilever E type metal wire structure array;Described cross metal wire and double cantilever E type metal wires are with cycle same spacing;
The horizontal edge of described cross metal wire unit is vertical with the longitudinal edge of double cantilever E type metal wire unit, the longitudinal edge of described cross metal wire unit is parallel with the longitudinal edge of double cantilever E type metal wire unit, and the center of double cantilever E type metal wire unit and the center of cross metal wire unit are at same level height.
2. as claimed in claim 1 with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that described dielectric substrate uses microwave dielectric material substrate.
3. as claimed in claim 1 with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that the dielectric constant of described dielectric substrate is 2~10.
4. as claimed in claim 3 with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that the dielectric constant of described dielectric substrate is 4.4 ± 5%.
5. as claimed in claim 1 with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that the thickness of described dielectric substrate is 0.25~1.3mm.
6. as claimed in claim 5 with double cantilever E types reversely nested LHM of adjustable cross metal wire structure, it is characterised in that the thickness of described dielectric substrate is 0.40mm ± 5%.
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