WO2012129941A1 - Metamaterial - Google Patents

Metamaterial Download PDF

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Publication number
WO2012129941A1
WO2012129941A1 PCT/CN2011/084435 CN2011084435W WO2012129941A1 WO 2012129941 A1 WO2012129941 A1 WO 2012129941A1 CN 2011084435 W CN2011084435 W CN 2011084435W WO 2012129941 A1 WO2012129941 A1 WO 2012129941A1
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WO
WIPO (PCT)
Prior art keywords
substrate
metamaterial
dielectric
structures
dielectric substrate
Prior art date
Application number
PCT/CN2011/084435
Other languages
French (fr)
Chinese (zh)
Inventor
刘若鹏
赵治亚
孙豪文
缪锡根
Original Assignee
深圳光启高等理工研究院
深圳光启创新技术有限公司
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Publication date
Priority claimed from CN201110074026.7A external-priority patent/CN102637959B/en
Priority claimed from CN 201110109047 external-priority patent/CN102480011B/en
Priority claimed from CN 201110109034 external-priority patent/CN102480010B/en
Application filed by 深圳光启高等理工研究院, 深圳光启创新技术有限公司 filed Critical 深圳光启高等理工研究院
Publication of WO2012129941A1 publication Critical patent/WO2012129941A1/en

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Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B33/00Layered products characterised by particular properties or particular surface features, e.g. particular surface coatings; Layered products designed for particular purposes not covered by another single class
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y20/00Nanooptics, e.g. quantum optics or photonic crystals
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q15/00Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
    • H01Q15/02Refracting or diffracting devices, e.g. lens, prism
    • H01Q15/10Refracting or diffracting devices, e.g. lens, prism comprising three-dimensional array of impedance discontinuities, e.g. holes in conductive surfaces or conductive discs forming artificial dielectric
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B2457/00Electrical equipment

Definitions

  • the present invention relates to a metamaterial, and in particular to a supermaterial having a non-uniform dielectric constant. ⁇ Background technique ⁇
  • the metamaterial is generally formed by laminating a plurality of metamaterial functional panels or by other regular arrays.
  • the metamaterial functional panel comprises a dielectric substrate and a plurality of artificial microstructures arrayed on the dielectric substrate, and the existing metamaterial dielectric substrate is a uniform material.
  • Organic or inorganic substrates such as FR4, TP 1 and the like.
  • the plurality of artificial microstructures of the array on the dielectric substrate have specific electromagnetic characteristics and can generate electromagnetic response to an electric field or a magnetic field.
  • the metamaterials can be presented in various kinds. Electromagnetic properties not found in general materials, such as convergence, divergence, and deflection of electromagnetic waves.
  • the existing dielectric substrate is used as a fixed substrate of an artificial microstructure, and since it has a uniform dielectric constant and magnetic permeability as a whole, it does not have a unique response to an electric field or a magnetic field, that is, for the entire metamaterial, the dielectric substrate is not With electromagnetic modulation.
  • the technical problem to be solved by the present invention is to overcome the shortcomings of the lack of functional function of the dielectric substrate of the prior supermaterial, and to provide a metamaterial having a non-uniform dielectric constant distribution of the dielectric substrate, which is modified by changing the dielectric constant of the dielectric substrate.
  • the material has been expanded in function.
  • the technical solution for achieving the object of the present invention is a metamaterial comprising a plurality of arrays of metamaterial functional board metamaterial functional boards comprising a dielectric substrate and a plurality of artificial microstructures arrayed on the dielectric substrate, the dielectric substrate having non-uniformity The dielectric constant distribution.
  • metamaterials are composed of a plurality of super-material functional plate arrays.
  • the artificial microstructure and the dielectric substrate on which it is located can be regarded as the basic components of the super-material function board.
  • Structural unit, the nature of the metamaterial function board depends mainly on multiple basic knots.
  • the electromagnetic properties and array laws of the structural unit are mainly determined by the equivalent dielectric constant and equivalent magnetic permeability of the basic structural unit, and the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure and The dielectric substrate on which it is located is determined jointly.
  • metamaterial functional panels change the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit by changing the structure or size of the artificial microstructure. Finally, a plurality of basic structural units are subjected to a certain law. Arrangement allows the metamaterial function panel to form certain electromagnetic properties, such as electromagnetic modulation for electromagnetic wave convergence, divergence, deflection, and translation.
  • the present invention expands the functional design of the metamaterial functional panel by designing the dielectric substrate to be composed of a plurality of substrate units of different materials, or / and designing the thickness of each substrate unit to be non-uniformly distributed.
  • the dielectric constants in the respective substrate units are different due to different materials.
  • the ratio of the dielectric substrate to the metamaterial basic structural unit in each substrate unit will be Differently, this change in ratio changes the equivalent dielectric constant of the basic structural unit of the metamaterial. Therefore, by using the metamaterial dielectric substrate of the present invention, the local dielectric constant of the entire metamaterial can be changed to expand the application of the metamaterial.
  • the shape of the substrate unit may be arbitrarily designed as needed, depending on the shape of the target region whose dielectric constant is to be changed.
  • the dielectric substrate is a convex ellipsoid or a concave ellipsoid.
  • the side surface of the dielectric substrate is disposed in a plurality of return structures or annular structures, and the thickness of the plurality of return structures or annular structures is different; preferably, the thickness of the plurality of return structures or annular structures is stepped distributed.
  • the substrate unit may be designed as a plurality of return structures or annular structures. After the plurality of return structures or annular structures constitute the dielectric substrate, different substrate units are different materials or/and have different The thickness is such that the dielectric constant of the entire dielectric substrate is non-uniformly distributed.
  • the dielectric constants of the plurality of return structures or the basic units of the annular structure may be increased or decreased by a gradient, or may be alternately distributed in size.
  • the material of the substrate unit it is necessary to select different substrates as the material of the substrate unit according to the dielectric constant distribution of the entire dielectric substrate, and flexibly can be flexibly selected from various ceramic substrates, plastic resin substrates or according to the difference in dielectric constant.
  • the choice of composite substrate is therefore extensive material selectivity.
  • the beneficial effects of the present invention are that by designing the dielectric substrate to be composed of different materials and/or substrate units of different thicknesses, the metamaterial has a non-uniform dielectric constant distribution, providing a richer functional application for the metamaterial.
  • Figure 1 Schematic diagram of the structure of the metamaterial.
  • Figure 3 is a structural view of a dielectric substrate of Embodiment 1.
  • Figure 4 is a diagram showing the overall structure of the supermaterial of the embodiment 2.
  • Figure 5 is a structural view of a dielectric substrate of Embodiment 2.
  • Example 3 is a cross-sectional view of a dielectric substrate.
  • Embodiment 4 Cross-sectional view of a dielectric substrate.
  • Example 4 Side view of a dielectric substrate.
  • Figure 10 is a cross-sectional view of a dielectric substrate of Embodiment 5.
  • Example 5 Side view of a dielectric substrate.
  • Figure 12 is a cross-sectional view of the dielectric substrate of Example 6.
  • Example 6 Side view of a dielectric substrate.
  • Figure 14 Plan view of the dielectric substrate of Embodiment 7.
  • Figure 14 is a cross-sectional view taken along line A-A.
  • Figure 16 Plan view of the dielectric substrate of Embodiment 8.
  • Figure 17 is a cross-sectional view taken along line B-B.
  • Figure 18 is a plan view of the dielectric substrate of Embodiment 9.
  • Figure 19 is a cross-sectional view taken along line A-A.
  • Figure 20 is a plan view of the dielectric substrate of Embodiment 10.
  • Figure 21 a cross-sectional view taken along line B-B of Figure 20.
  • the metamaterial functional panel 100 includes a dielectric substrate 101 and a plurality of artificial microstructures 102 arrayed on the dielectric substrate.
  • the artificial microstructures 102 are located therewith.
  • the dielectric substrate can be viewed as a metamaterial basic structural unit, similar to a crystal lattice in a crystal.
  • 1 is a partial enlarged schematic view of a microstructure of a metamaterial.
  • the actual metamaterial is formed by an array of basic structural units of the order of the number of molecules of the material according to an artificial design.
  • the structure of the artificial microstructure 102 in Fig. 1 is a "work" type structure, and as a specific embodiment, a type-derived type can also be used.
  • the overall structure of the metamaterial includes a multilayer dielectric substrate 101 laminated together and a plurality of artificial microstructures 102 disposed on the dielectric substrate.
  • the structural diagram of the dielectric substrate 101 is shown in FIG. One side is a convex ellipsoid, the other side is a flat plate, and the artificial microstructure 102 is arrayed on the flat side of the dielectric substrate 101.
  • the artificial microstructure we can regard the artificial microstructure, the dielectric substrate occupied by the artificial microstructure, and the space around them as a tiny unit that generates electromagnetic response to electromagnetic waves.
  • the entire metamaterial consists of many tiny units.
  • the present invention utilizes the modified dielectric substrate 101.
  • the thickness of the dielectric substrate 101 in each microcell is changed, and the equivalent dielectric constant and the equivalent magnetic permeability of the entire microcell can be changed.
  • the dielectric substrate 101 is designed as a convex lens.
  • the convex ellipsoid can make the electromagnetic wave passing through the dielectric substrate have a convergence effect, so that the super material can obtain the electromagnetic wave convergence function on the basis of the original functional characteristics, so as to increase the function expansion of the super material.
  • the overall structure of the metamaterial includes a multilayer dielectric substrate 101 laminated together and a plurality of artificial microstructures 102 disposed on the dielectric substrate.
  • the dielectric substrate 101 has a concave ellipsoid on one side and a flat plate on the other side, and the artificial microstructures 102 are arrayed on the flat side of the dielectric substrate 101.
  • the present embodiment can design the dielectric substrate 101 to be a concave ellipsoid like a concave lens, so that the electromagnetic wave passing through the dielectric substrate can have a diverging effect, so that the super-material can obtain electromagnetic wave divergence based on the original functional characteristics. Function to increase the functional expansion of metamaterials.
  • FIG. 6 is a cross-sectional view of the dielectric substrate 101
  • FIG. 7 is a side view of the dielectric substrate 101.
  • One side of the dielectric substrate 101 has a convex shape, and the other side has a flat shape.
  • the array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101.
  • the dielectric substrate 101 has a back shape as seen from the side of the boss-shaped structure.
  • the equivalent dielectric constant and the equivalent magnetic permeability of the various retro-shaped structures of the metamaterial are stepped, and on the other hand, the structural shape of the artificial microstructure 102 is designed and According to the arrangement rule, the metamaterial can obtain certain electromagnetic characteristics.
  • the metamaterial can obtain the corresponding functional characteristics superposition, with more Designed for flexible features and a richer set of features.
  • FIG. 8 is a cross-sectional view of the dielectric substrate 101
  • FIG. 9 is a side view of the dielectric substrate 101.
  • One side of the dielectric substrate 101 has a concave shape, and the other side has a flat shape.
  • the array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101.
  • the dielectric substrate 101 has a ring shape when viewed from the side of the concave-shaped structure.
  • the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the structural shape and arrangement of the artificial microstructure 102 are designed.
  • the law of cloth the metamaterial can obtain certain electromagnetic properties.
  • the metamaterial can obtain the phase.
  • the functional features are superimposed, with more flexible functional design and richer functional applications.
  • FIG. 10 is a cross-sectional view of the dielectric substrate 101
  • FIG. 11 is a side view of the dielectric substrate 101.
  • One side of the dielectric substrate 101 has a square wave structure in which the irregularities are alternately arranged, and the other side has a flat plate shape, and the artificial microstructure 102 is arrayed on the flat side surface of the dielectric substrate 101.
  • the dielectric substrate 101 has a back shape as seen from the side of the square wave structure. .
  • the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the artificial microstructure is designed.
  • the metamaterial can obtain certain electromagnetic properties.
  • the metamaterial can obtain the corresponding function.
  • Feature overlay with more flexible functional design and richer functional applications.
  • FIG. 12 is a cross-sectional view of the dielectric substrate 101
  • FIG. 13 is a side view of the dielectric substrate 101.
  • One side of the dielectric substrate 101 has a square corrugated structure in which irregularities are alternated, and the other side has a flat plate shape.
  • the array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101.
  • the dielectric substrate 101 has a ring shape when viewed from the side of the square wave structure.
  • the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the structural shape of the artificial microstructure 102 is designed. And the arrangement rule, the metamaterial can obtain certain electromagnetic characteristics. On the other hand, through the alternating distribution of the equivalent dielectric constant and the equivalent magnetic permeability of each circular ring structure, the metamaterial can obtain the corresponding functional property superposition. More flexible functional design and richer functional applications.
  • the dielectric substrate 101 is designed to include a plurality of different materials of the return substrate unit 103.
  • the plan view of the dielectric substrate is shown in FIG. 14, and FIG. 15 is a cross-sectional view taken along line AA of FIG.
  • the substrate unit 103 is made of a different material, and the dielectric constant of each material is increased from the periphery to the center. Different packing densities are used to indicate different materials in FIG. 15, wherein a large packing density indicates that the material has a large dielectric constant. A small packing density means that the dielectric constant of the material is small.
  • the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure. 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective return substrate units 103 are made of different materials, the dielectric constants in the different return substrate units 103 on the dielectric substrate 101 are changed. The equivalent dielectric constant of the basic structural unit in the substrate unit 103 will also be changed depending on the associated back substrate unit 103, and finally the metamaterial functional panel 100 has different dielectric constant distributions in different regions. This provides a more flexible design for the functional design of metamaterials.
  • the dielectric constant of the return substrate unit 103 is increased from the periphery to the center, and the material can be flexibly selected from the ceramic substrate, the plastic resin substrate or the composite substrate to make different shapes.
  • the substrate unit 103 is arranged in a different material according to the magnitude of the dielectric constant, so that the metamaterial has a non-uniform dielectric constant distribution as a whole.
  • the size and number of the paper-shaped substrate unit 103 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial.
  • the dielectric constant of each of the returning substrate units 103 is increased from the periphery to the center only as a specific example for convenience of explanation of the present invention.
  • the dielectric constant of each of the returning substrate units 103 is The arrangement rule also needs to be determined according to the predetermined electromagnetic properties of the metamaterial.
  • the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials of the respective back substrate units 103, and through the design approach The design of the artificial microstructure of the super-material function board is combined to achieve the purpose of expanding the functional design path of the super material.
  • the dielectric substrate 101 is designed as an annular substrate unit 104 including a plurality of different materials.
  • a plan view of the dielectric substrate is shown in FIG. 16, and FIG. 17 is a cross-sectional view taken along line BB of FIG.
  • Each annular substrate unit 104 is made of two different materials, and the dielectric constants of the two materials are alternately distributed in size, and different packing densities are represented in FIG.
  • the material in which the packing density is large indicates that the material has a large dielectric constant, and the small packing density indicates that the dielectric constant of the material is small.
  • the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure. 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective annular substrate units 104 are made of different materials, the dielectric constants in the different substrate units on the dielectric substrate 101 are changed, and the respective annular substrate units 104 are The equivalent dielectric constant of the basic structural unit will also be changed depending on the ring substrate unit 104 to which it belongs, and finally the metamaterial functional board 100 has different dielectric constant distributions in different regions, thereby functioning as a metamaterial.
  • the design provides a more flexible design approach.
  • two different materials may be selected, and the different annular substrate units 104 are alternately arranged with different materials, so that the metamaterials are provided as a whole.
  • the size and number of the annular substrate unit 104 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial.
  • the dielectric constants of the respective annular substrate units 104 in the present embodiment are alternately arranged only for the sake of convenience in explaining the present invention.
  • the arrangement law of the dielectric constants of the respective annular substrate units 104 is also required.
  • the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials of the respective annular substrate units 104, and to create artificial materials on the metamaterial functional board by the design approach.
  • the design of the microstructure arrangement rules is combined to achieve the purpose of expanding the functional design approach of the metamaterial.
  • the dielectric substrate 101 is designed to include a plurality of return substrate units 103.
  • the plan view of the dielectric substrate is shown in FIG. 18.
  • FIG. 19 is a cross-sectional view taken along line AA of FIG. 18, wherein each of the return substrate units 103 is made of different materials.
  • the dielectric constant of the material increases from the periphery to the center.
  • Different packing densities are used to indicate different materials in Fig. 3. Among them, the high packing density indicates that the material has a large dielectric constant, and the small packing density indicates the dielectric constant of the material. Small, while the thickness of each of the return substrate units 103 is also increased from the periphery toward the center.
  • the equivalent dielectric constant and equivalent permeability of a plurality of metamaterial basic structural units Since the electromagnetic properties of metamaterials are determined by the equivalent dielectric constant and equivalent permeability of a plurality of metamaterial basic structural units, the equivalent dielectric of a single basic structural unit The constant and the equivalent magnetic permeability are determined by the artificial microstructure 102 and the dielectric substrate 101 in which it is disposed. Therefore, when each of the returning substrate units 103 is made of a different material, it is equivalent to changing the different times on the dielectric substrate 101.
  • the dielectric constant in the substrate unit 103, the equivalent dielectric constant of the basic structural unit in each of the return substrate units 103 will also be changed depending on the associated back substrate unit 103, and finally the metamaterial function board 100 will be changed. There are different dielectric constant distributions in different regions.
  • each of the paper-shaped substrate units 103 is designed to be increased from the periphery toward the center, and the thickness of the paper-shaped substrate unit 103 is different with respect to the meta-material basic structural unit in each of the paper-shaped substrate units 103, and the basic structure of the metamaterial is The proportion of the dielectric substrate 101 in the cell will be different, and therefore the equivalent dielectric constant exhibited by the metamaterial basic structural unit in each of the returned substrate units 103 will be different.
  • the dielectric constant of the metamaterial can be non-uniformly distributed, thereby providing a more flexible design method for the functional design of the metamaterial.
  • the dielectric constant of the return substrate unit 103 is increased from the periphery to the center, and the material can be flexibly selected from the ceramic substrate, the plastic resin substrate or the composite substrate to make different shapes.
  • the substrate unit 103 is arranged in a different material according to the magnitude of the dielectric constant, so that the metamaterial has a non-uniform dielectric constant distribution as a whole.
  • the size, number, and thickness of the paper-shaped substrate unit 103 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial.
  • the dielectric constant of each of the returning substrate units 103 is increased from the periphery to the center only as a specific example for convenience of explanation of the present invention.
  • the dielectric constant of each of the returning substrate units 103 is The arrangement rule also needs to be determined according to the predetermined electromagnetic properties of the metamaterial.
  • the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials and different thicknesses of the respective back substrate units 103, and The design approach is combined with the design of the artificial microstructure arrangement on the metamaterial function board to achieve the purpose of expanding the functional design approach of the metamaterial.
  • Example 10
  • the present embodiment designs the dielectric substrate 101 as an annular substrate unit 104 including a plurality of different materials.
  • a plan view of the dielectric substrate is shown in FIG. 20, and FIG. 21 is 20 is a cross-sectional view taken along line BB, wherein each of the annular substrate units 104 is made of two different materials, and the dielectric constants of the two materials are alternately distributed, and the two different materials are represented by two different packing densities in FIG.
  • the material having a large packing density has a large dielectric constant
  • the small packing density indicates that the dielectric constant of the material is small
  • the thickness of each of the returning substrate units 103 is also alternately thick and thin.
  • the equivalent dielectric constant and equivalent permeability of a single basic structural unit are The structure 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective annular substrate units 104 are made of different materials, the dielectric constants in the different substrate units on the dielectric substrate 101 are changed, and the respective annular substrate units 104 are replaced. The equivalent dielectric constant of the basic structural unit within it will also be changed depending on the ring substrate unit 104 to which it belongs, eventually causing the metamaterial functional panel 100 to have different dielectric constant distributions in different regions.
  • each of the paper-shaped substrate units 103 is designed to be alternately thick and thin, and the thickness of the paper-shaped substrate unit 103 is different with respect to the meta-material basic structural unit in each of the paper-shaped substrate units 103, and the meta-material basic structural unit is
  • the occupation ratio of the dielectric substrate 101 will be different, and therefore the equivalent dielectric constant exhibited by the metamaterial basic structural unit in each of the return substrate units 103 will also be different.
  • the dielectric constants of the annular substrate unit 104 are alternately distributed.
  • two different materials can be selected, and the annular substrate units 104 of two different materials are alternately arranged, thereby making the whole
  • the metamaterial has a non-uniform dielectric constant distribution, and at the same time, in order to better alternate the dielectric constant of the annular substrate unit 104, the thickness of each of the return substrate units 103 is designed to be alternately thick and thin, so that the thickness is alternated. The effect of the distribution of the material and the alternating distribution of the material on the dielectric constant will be more flexible.
  • the size, number, and thickness of the annular substrate unit 104 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial.
  • the dielectric constants of the respective annular substrate units 104 in the present embodiment are alternately arranged only for the sake of convenience in explaining the present invention. In the specific implementation, the arrangement law of the dielectric constants of the respective annular substrate units 104 is also required.
  • the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials and different thicknesses of the respective annular substrate units 104, and through the design approach and the metamaterial.
  • the design of the artificial microstructure arrangement rules on the function board is combined to achieve the purpose of expanding the functional design path of the super material. It can be seen from the above description that the use of metamaterials according to the present invention for non-uniform thicknesses and/or dielectric substrates composed of different materials can make the metamaterials have more abundant functional applications, such as achieving convergence, divergence and deflection of electromagnetic waves. In addition, the dielectric substrate and the artificial microstructure of the metamaterial have various electromagnetic characteristics at the same time, which provides a solution for forming a plurality of unique functions of the metamaterial.
  • paper-shaped substrate unit or the annular substrate unit in the present invention is only one of the specific embodiments, and the shape of the area of the substrate unit can be arbitrarily designed as needed.

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Abstract

A metamaterial comprising multiple metamaterial functional boards (100) arranged in an array. Each metamaterial functional board (100) comprises a dielectric substrate (101) and multiple artificial microstructures (102) arrayed on the dielectric substrate (101). The dielectric substrate (101) is provided with a non-uniform dielectric constant distribution. The non-uniform dielectric constant distribution of the metamaterial provides the metamaterial with increased number of functional applications.

Description

超材料  Super material
【技术领域】 [Technical Field]
本发明涉及一种超材料, 具体地涉及一种具有非均匀介电常数的超材 料。 【背景技术】  The present invention relates to a metamaterial, and in particular to a supermaterial having a non-uniform dielectric constant. 【Background technique】
超材料一般由多个超材料功能板层叠或按其他规律阵列组合而成,超材 料功能板包括介质基板以及阵列在介质基板上的多个人造微结构,现有超材 料的介质基板为均一材质的有机或无机基板, 如 FR4、 TP 1等等。 阵列在介 质基板上的多个人造微结构具有特定的电磁特性,能对电场或磁场产生电磁 响应, 通过对人造微结构的结构和排列规律进行精确设计和控制, 可以使超 材料呈现出各种一般材料所不具有的电磁特性, 如能汇聚、发散和偏折电磁 波等。现有的介质基板作为人造微结构的固定基板, 由于整体上具有均一的 介电常数和磁导率, 所以对电场或磁场不会产生特有的响应, 即对整个超材 料而言, 介质基板不具有电磁调制功能。  The metamaterial is generally formed by laminating a plurality of metamaterial functional panels or by other regular arrays. The metamaterial functional panel comprises a dielectric substrate and a plurality of artificial microstructures arrayed on the dielectric substrate, and the existing metamaterial dielectric substrate is a uniform material. Organic or inorganic substrates such as FR4, TP 1 and the like. The plurality of artificial microstructures of the array on the dielectric substrate have specific electromagnetic characteristics and can generate electromagnetic response to an electric field or a magnetic field. By accurately designing and controlling the structure and arrangement of the artificial microstructures, the metamaterials can be presented in various kinds. Electromagnetic properties not found in general materials, such as convergence, divergence, and deflection of electromagnetic waves. The existing dielectric substrate is used as a fixed substrate of an artificial microstructure, and since it has a uniform dielectric constant and magnetic permeability as a whole, it does not have a unique response to an electric field or a magnetic field, that is, for the entire metamaterial, the dielectric substrate is not With electromagnetic modulation.
【发明内容】 [Summary of the Invention]
本发明所要解决的技术问题是:克服现有超材料的介质基板缺乏功能作 用的缺点, 提供一种介质基板具有非均匀介电常数分布的超材料, 通过改变 介质基板局部的介电常数使超材料在功能上得到应用拓展。  The technical problem to be solved by the present invention is to overcome the shortcomings of the lack of functional function of the dielectric substrate of the prior supermaterial, and to provide a metamaterial having a non-uniform dielectric constant distribution of the dielectric substrate, which is modified by changing the dielectric constant of the dielectric substrate. The material has been expanded in function.
本发明实现发明目的采用的技术方案是, 一种超材料, 包括多个阵列的 超材料功能板超材料功能板包括介质基板以及阵列在介质基板上的多个人 造微结构, 介质基板具有非均匀的介电常数分布。  The technical solution for achieving the object of the present invention is a metamaterial comprising a plurality of arrays of metamaterial functional board metamaterial functional boards comprising a dielectric substrate and a plurality of artificial microstructures arrayed on the dielectric substrate, the dielectric substrate having non-uniformity The dielectric constant distribution.
超材料作为一种对电磁波具有特殊响应和调制特性的新材料,是由多个 超材料功能板阵列组合而成,人造微结构及其所在的介质基板可看作是组成 超材料功能板的基本结构单元,超材料功能板的性质主要取决于多个基本结 构单元的电磁性质和阵列规律。单个基本结构单元的电磁特性主要由该基本 结构单元的等效介电常数和等效磁导率决定,而单个基本结构单元的等效介 电常数和等效磁导率又由人造微结构及其所在的介质基板所共同决定。现有 对超材料功能板的设计都是通过改变人造微结构的结构或大小来改变单个 基本结构单元的等效介电常数和等效磁导率,最后将多个基本结构单元按照 一定的规律进行排布, 可以使超材料功能板形成某些特定的电磁特性, 如对 电磁波的汇聚、 发散、 偏折和平移等电磁调制功能。 As a new material with special response and modulation characteristics to electromagnetic waves, metamaterials are composed of a plurality of super-material functional plate arrays. The artificial microstructure and the dielectric substrate on which it is located can be regarded as the basic components of the super-material function board. Structural unit, the nature of the metamaterial function board depends mainly on multiple basic knots The electromagnetic properties and array laws of the structural unit. The electromagnetic properties of a single basic structural unit are mainly determined by the equivalent dielectric constant and equivalent magnetic permeability of the basic structural unit, and the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure and The dielectric substrate on which it is located is determined jointly. The existing design of metamaterial functional panels is to change the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit by changing the structure or size of the artificial microstructure. Finally, a plurality of basic structural units are subjected to a certain law. Arrangement allows the metamaterial function panel to form certain electromagnetic properties, such as electromagnetic modulation for electromagnetic wave convergence, divergence, deflection, and translation.
本发明为拓展超材料功能板的功能设计方式,通过将介质基板设计为由 多个不同材料的基板单元组成, 或者 /并且设计成各个基板单元的厚度呈非 均匀分布。 一方面, 由于材料不同, 所以各个基板单元内的介电常数不同, 另一方面, 由于各个基板单元的厚度不同, 对于各个基板单元内的超材料基 本结构单元而言, 其介质基板的比例将不同, 该比例的改变会改变超材料基 本结构单元的等效介电常数。 因此, 通过采用本发明的超材料介质基板, 可 以改变整个超材料的局部介电常数使超材料在功能上得到应用拓展。  The present invention expands the functional design of the metamaterial functional panel by designing the dielectric substrate to be composed of a plurality of substrate units of different materials, or / and designing the thickness of each substrate unit to be non-uniformly distributed. On the one hand, the dielectric constants in the respective substrate units are different due to different materials. On the other hand, due to the different thickness of each substrate unit, the ratio of the dielectric substrate to the metamaterial basic structural unit in each substrate unit will be Differently, this change in ratio changes the equivalent dielectric constant of the basic structural unit of the metamaterial. Therefore, by using the metamaterial dielectric substrate of the present invention, the local dielectric constant of the entire metamaterial can be changed to expand the application of the metamaterial.
具体实施时, 所述基板单元的形状可根据需要进行任意设计, 以拟改变 其介电常数的目标区域形状而定。  In a specific implementation, the shape of the substrate unit may be arbitrarily designed as needed, depending on the shape of the target region whose dielectric constant is to be changed.
作为具体实施方式之一, 介质基板为凸椭球形或凹椭球形。  As one of the specific embodiments, the dielectric substrate is a convex ellipsoid or a concave ellipsoid.
作为具体实施方式之一,介质基板的侧面设置成多个回形结构或环形结 构, 多个回形结构或环形结构的厚度不同; 优选地, 多个回形结构或环形结 构的厚度呈阶梯状分布。  As one of the specific embodiments, the side surface of the dielectric substrate is disposed in a plurality of return structures or annular structures, and the thickness of the plurality of return structures or annular structures is different; preferably, the thickness of the plurality of return structures or annular structures is stepped distributed.
作为具体实施方式之一,可以将基板单元设计为多个回形结构或环形结 构, 多个回形结构或环形结构组成介质基板后, 由于不同的基板单元为不同 的材料或者 /并且具有不同的厚度, 所以整个介质基板的介电常数呈非均匀 的分布。  As one of the specific embodiments, the substrate unit may be designed as a plurality of return structures or annular structures. After the plurality of return structures or annular structures constitute the dielectric substrate, different substrate units are different materials or/and have different The thickness is such that the dielectric constant of the entire dielectric substrate is non-uniformly distributed.
作为具体实施方式,多个回形结构或环形结构基本单元的介电常数大小 可按梯度增加或减小, 也可以呈大小交替分布。  As a specific embodiment, the dielectric constants of the plurality of return structures or the basic units of the annular structure may be increased or decreased by a gradient, or may be alternately distributed in size.
本发明在具体实施时,需要根据整个介质基板的介电常数分布选择不同 的基材作为基板单元的材料,根据介电常数大小的不同可以灵活地从各种陶 瓷基材、塑料树脂基材或复合材料基材中选择,因此具有广泛的材料选择性。 本发明的有益效果是, 通过将介质基板设计为由不同材料和 /或不同厚 度的基板单元组成, 使超材料具有非均匀的介电常数分布, 为超材料提供更 为丰富的功能应用。 In the specific implementation of the present invention, it is necessary to select different substrates as the material of the substrate unit according to the dielectric constant distribution of the entire dielectric substrate, and flexibly can be flexibly selected from various ceramic substrates, plastic resin substrates or according to the difference in dielectric constant. The choice of composite substrate is therefore extensive material selectivity. The beneficial effects of the present invention are that by designing the dielectric substrate to be composed of different materials and/or substrate units of different thicknesses, the metamaterial has a non-uniform dielectric constant distribution, providing a richer functional application for the metamaterial.
【附图说明】 [Description of the Drawings]
图 1, 超材料的结构示意图。  Figure 1. Schematic diagram of the structure of the metamaterial.
图 2, 实施例 1超材料的整体结构图。  Figure 2, Example 1 Overall structural view of the metamaterial.
图 3, 实施例 1介质基板的结构图。  Figure 3 is a structural view of a dielectric substrate of Embodiment 1.
图 4, 实施例 2超材料的整体结构图。  Figure 4 is a diagram showing the overall structure of the supermaterial of the embodiment 2.
图 5, 实施例 2介质基板的结构图。  Figure 5 is a structural view of a dielectric substrate of Embodiment 2.
图 6, 实施例 3介质基板的截面图。  Figure 6. Example 3 is a cross-sectional view of a dielectric substrate.
图 7, 实施例 3介质基板的侧面视图。  Figure 7. Example 3 Side view of a dielectric substrate.
图 8, 实施例 4介质基板的截面图。  Figure 8. Embodiment 4 Cross-sectional view of a dielectric substrate.
图 9, 实施例 4介质基板的侧面视图。  Figure 9. Example 4 Side view of a dielectric substrate.
图 10, 实施例 5介质基板的截面图。  Figure 10 is a cross-sectional view of a dielectric substrate of Embodiment 5.
图 11, 实施例 5介质基板的侧面视图。  Figure 11. Example 5 Side view of a dielectric substrate.
图 12, 实施例 6介质基板的截面图。  Figure 12 is a cross-sectional view of the dielectric substrate of Example 6.
图 13, 实施例 6介质基板的侧面视图。  Figure 13. Example 6 Side view of a dielectric substrate.
图 14, 实施例 7的介质基板的平面视图。  Figure 14. Plan view of the dielectric substrate of Embodiment 7.
图 15, 图 14的 A-A剖视图。  Figure 15, Figure 14 is a cross-sectional view taken along line A-A.
图 16, 实施例 8的介质基板的平面视图。  Figure 16. Plan view of the dielectric substrate of Embodiment 8.
图 17, 图 16的 B-B剖视图。  Figure 17, Figure 16 is a cross-sectional view taken along line B-B.
图 18, 实施例 9的介质基板的平面视图。  Figure 18 is a plan view of the dielectric substrate of Embodiment 9.
图 19, 图 18的 A-A剖视图。  Figure 19, Figure 18 is a cross-sectional view taken along line A-A.
图 20, 实施例 10的介质基板的平面视图。  Figure 20 is a plan view of the dielectric substrate of Embodiment 10.
图 21, 图 20的 B-B剖视图。  Figure 21, a cross-sectional view taken along line B-B of Figure 20.
【具体实施方式】 【detailed description】
下面结合附图和实施例对本发明进行详细说明。 超材料的结构示意图参看附图 1, 包括多个层叠超材料功能板 100, 超 材料功能板 100包括介质基板 101以及阵列在介质基板上的多个人造微结构 102, 人造微结构 102与其所在的介质基板可以看成一个超材料基本结构单 元, 类似于晶体中的晶格。 附图 1是超材料微观结构的局部放大示意图, 实 际的超材料是由物质分子数数量级的基本结构单元按照人为设计的排布规 律阵列而成。 附图 1中的人造微结构 102的结构为 "工"字型结构, 作为具 体实施方式, 还可以采用工字衍生型。 The invention will now be described in detail in conjunction with the drawings and embodiments. Referring to FIG. 1, a plurality of stacked metamaterial functional panels 100 are included. The metamaterial functional panel 100 includes a dielectric substrate 101 and a plurality of artificial microstructures 102 arrayed on the dielectric substrate. The artificial microstructures 102 are located therewith. The dielectric substrate can be viewed as a metamaterial basic structural unit, similar to a crystal lattice in a crystal. 1 is a partial enlarged schematic view of a microstructure of a metamaterial. The actual metamaterial is formed by an array of basic structural units of the order of the number of molecules of the material according to an artificial design. The structure of the artificial microstructure 102 in Fig. 1 is a "work" type structure, and as a specific embodiment, a type-derived type can also be used.
本发明采用以下实施例实施:  The invention is implemented using the following embodiments:
实施例 1 Example 1
超材料的整体结构图参看附图 2, 包括层叠在一起的多层介质基板 101 以及设置在介质基板上的多个人造微结构 102, 介质基板 101的结构图参看 附图 3,介质基板 101的一侧为凸椭球形,另一侧为平板状,人造微结构 102 阵列在介质基板 101的平板状侧面上。  Referring to FIG. 2, the overall structure of the metamaterial includes a multilayer dielectric substrate 101 laminated together and a plurality of artificial microstructures 102 disposed on the dielectric substrate. The structural diagram of the dielectric substrate 101 is shown in FIG. One side is a convex ellipsoid, the other side is a flat plate, and the artificial microstructure 102 is arrayed on the flat side of the dielectric substrate 101.
对超材料而言, 我们可以把人造微结构、人造微结构所占用的介质基板 以及二者周围的空间看做一个对电磁波能产生电磁响应的微小单元,整个超 材料由很多个微小单元组成,通过设计各个微小单元内人造微结构 102的结 构形状并将各个人造微结构 102进行有序排列,可以使超材料获得特定的电 磁特性, 如各向异性、 阻抗匹配等等。  For metamaterials, we can regard the artificial microstructure, the dielectric substrate occupied by the artificial microstructure, and the space around them as a tiny unit that generates electromagnetic response to electromagnetic waves. The entire metamaterial consists of many tiny units. By designing the structural shape of the artificial microstructures 102 in each of the minute cells and ordering the individual artificial microstructures 102, the metamaterial can be subjected to specific electromagnetic characteristics such as anisotropy, impedance matching, and the like.
因为各个微小单元的等效介电常数和等效磁导率受人造微结构 102、 人 造微结构 102所占用的介质基板 101以及二者周围的空间所共同影响,所以 本发明利用改变介质基板 101 的厚度来改变各个微小单元内介质基板 101 的占有比例, 进而可以达到改变整个微小单元的等效介电常数和等效磁导 率, 如本实施例通过将介质基板 101设计为一种类似凸透镜的凸椭球形, 可 以使经过介质基板的电磁波具有汇聚效果,使超材料在原有功能特性的基础 上得到电磁波汇聚功能, 以增加超材料的功能拓展。 实施例 2  Since the equivalent dielectric constant and the equivalent magnetic permeability of each microcell are affected by the artificial microstructure 102, the dielectric substrate 101 occupied by the artificial microstructure 102, and the space around them, the present invention utilizes the modified dielectric substrate 101. The thickness of the dielectric substrate 101 in each microcell is changed, and the equivalent dielectric constant and the equivalent magnetic permeability of the entire microcell can be changed. For example, the dielectric substrate 101 is designed as a convex lens. The convex ellipsoid can make the electromagnetic wave passing through the dielectric substrate have a convergence effect, so that the super material can obtain the electromagnetic wave convergence function on the basis of the original functional characteristics, so as to increase the function expansion of the super material. Example 2
超材料的整体结构图参看附图 4, 包括层叠在一起的多层介质基板 101 以及设置在介质基板上的多个人造微结构 102, 介质基板 101的结构图参看 附图 5,介质基板 101的一侧为凹椭球形,另一侧为平板状,人造微结构 102 阵列在介质基板 101的平板状侧面上。 Referring to FIG. 4, the overall structure of the metamaterial includes a multilayer dielectric substrate 101 laminated together and a plurality of artificial microstructures 102 disposed on the dielectric substrate. 5, the dielectric substrate 101 has a concave ellipsoid on one side and a flat plate on the other side, and the artificial microstructures 102 are arrayed on the flat side of the dielectric substrate 101.
根据上述设计原理和思路,本实施例通过将介质基板 101设计为一种类 似凹透镜的凹椭球形, 可以使经过介质基板的电磁波具有发散效果, 使超材 料在原有功能特性的基础上得到电磁波发散功能, 以增加超材料的功能拓 展。 实施例 3  According to the above design principles and ideas, the present embodiment can design the dielectric substrate 101 to be a concave ellipsoid like a concave lens, so that the electromagnetic wave passing through the dielectric substrate can have a diverging effect, so that the super-material can obtain electromagnetic wave divergence based on the original functional characteristics. Function to increase the functional expansion of metamaterials. Example 3
作为上述实施例的变形, 本发明还可以将介质基板 101 设计为如下结 构, 参看附图 6和附图 7, 附图 6为介质基板 101的截面图, 图 7为介质基 板 101的侧面视图, 介质基板 101的一侧为凸台形, 另一侧为平板状, 人造 微结构 102阵列在介质基板 101的平板状侧面上, 从凸台形结构的侧面看, 介质基板 101呈回字形。  As a modification of the above embodiment, the present invention can also be designed as follows. Referring to FIG. 6 and FIG. 7, FIG. 6 is a cross-sectional view of the dielectric substrate 101, and FIG. 7 is a side view of the dielectric substrate 101. One side of the dielectric substrate 101 has a convex shape, and the other side has a flat shape. The array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101. The dielectric substrate 101 has a back shape as seen from the side of the boss-shaped structure.
根据上述设计原理和思路, 本实施例中对于超材料的各个回字形结构, 其等效介电常数和等效磁导率呈阶梯状分布, 一方面, 通过设计人造微结构 102的结构形状和排布规律, 超材料能获得一定的电磁特性, 另一方面, 通 过各个回字形结构等效介电常数和等效磁导率的阶梯状分布,超材料能获得 相应的功能特性叠加, 具有更为灵活的功能设计和更为丰富的功能应用。 实施例 4  According to the above design principles and ideas, in the present embodiment, the equivalent dielectric constant and the equivalent magnetic permeability of the various retro-shaped structures of the metamaterial are stepped, and on the other hand, the structural shape of the artificial microstructure 102 is designed and According to the arrangement rule, the metamaterial can obtain certain electromagnetic characteristics. On the other hand, through the stepwise distribution of the equivalent dielectric constant and the equivalent magnetic permeability of each of the back-shaped structures, the metamaterial can obtain the corresponding functional characteristics superposition, with more Designed for flexible features and a richer set of features. Example 4
作为上述实施例的变形, 本发明还可以将介质基板 101 设计为如下结 构, 参看附图 8和附图 9, 附图 8为介质基板 101的截面图, 图 9为介质基 板 101的侧面视图, 介质基板 101的一侧为凹台形, 另一侧为平板状, 人造 微结构 102阵列在介质基板 101的平板状侧面上, 从凹台形结构的侧面看, 介质基板 101呈环形。  As a modification of the above embodiment, the present invention can also be designed as follows. Referring to FIG. 8 and FIG. 9, FIG. 8 is a cross-sectional view of the dielectric substrate 101, and FIG. 9 is a side view of the dielectric substrate 101. One side of the dielectric substrate 101 has a concave shape, and the other side has a flat shape. The array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101. The dielectric substrate 101 has a ring shape when viewed from the side of the concave-shaped structure.
根据上述设计原理和思路, 本实施例中对于超材料的各个环形结构, 其 等效介电常数和等效磁导率呈阶梯状分布, 一方面, 通过设计人造微结构 102的结构形状和排布规律, 超材料能获得一定的电磁特性, 另一方面, 通 过各个环形结构等效介电常数和等效磁导率的阶梯状分布,超材料能获得相 应的功能特性叠加, 具有更为灵活的功能设计和更为丰富的功能应用。 实施例 5 According to the above design principles and ideas, in the present embodiment, for each annular structure of the metamaterial, the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the structural shape and arrangement of the artificial microstructure 102 are designed. The law of cloth, the metamaterial can obtain certain electromagnetic properties. On the other hand, through the stepped distribution of the equivalent dielectric constant and the equivalent permeability of each ring structure, the metamaterial can obtain the phase. The functional features are superimposed, with more flexible functional design and richer functional applications. Example 5
作为上述实施例的变形, 本发明还可以将介质基板 101 设计为如下结 构, 参看附图 10和附图 11, 附图 10为介质基板 101的截面图, 图 11为介 质基板 101的侧面视图, 介质基板 101的一侧为凹凸交替的方波形结构, 另 一侧为平板状, 人造微结构 102阵列在介质基板 101的平板状侧面上, 从方 波形结构的侧面看, 介质基板 101呈回字形。  As a modification of the above embodiment, the present invention can also be designed as follows. Referring to FIG. 10 and FIG. 11, FIG. 10 is a cross-sectional view of the dielectric substrate 101, and FIG. 11 is a side view of the dielectric substrate 101. One side of the dielectric substrate 101 has a square wave structure in which the irregularities are alternately arranged, and the other side has a flat plate shape, and the artificial microstructure 102 is arrayed on the flat side surface of the dielectric substrate 101. The dielectric substrate 101 has a back shape as seen from the side of the square wave structure. .
根据上述设计原理和思路, 本实施例中对于超材料的各个回字形结构, 其等效介电常数和等效磁导率呈阶梯状分布, 一方面, 通过设计人造微结构 According to the above design principles and ideas, in the present embodiment, for each of the retro-shaped structures of the metamaterial, the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the artificial microstructure is designed.
102的结构形状和排布规律, 超材料能获得一定的电磁特性, 另一方面, 通 过各个回字形结构等效介电常数和等效磁导率的高低交替分布,超材料能获 得相应的功能特性叠加, 具有更为灵活的功能设计和更为丰富的功能应用。 实施例 6 The structure and arrangement of 102, the metamaterial can obtain certain electromagnetic properties. On the other hand, through the alternating distribution of the equivalent dielectric constant and the equivalent permeability of each of the back-shaped structures, the metamaterial can obtain the corresponding function. Feature overlay, with more flexible functional design and richer functional applications. Example 6
作为上述实施例的变形, 本发明还可以将介质基板 101 设计为如下结 构, 参看附图 12和附图 13, 附图 12为介质基板 101的截面图, 图 13为介 质基板 101的侧面视图, 介质基板 101的一侧为凹凸交替的方波形结构, 另 一侧为平板状, 人造微结构 102阵列在介质基板 101的平板状侧面上, 从方 波形结构的侧面看, 介质基板 101呈环形。  As a modification of the above embodiment, the present invention can also be designed as follows. Referring to FIG. 12 and FIG. 13, FIG. 12 is a cross-sectional view of the dielectric substrate 101, and FIG. 13 is a side view of the dielectric substrate 101. One side of the dielectric substrate 101 has a square corrugated structure in which irregularities are alternated, and the other side has a flat plate shape. The array of the artificial microstructures 102 is on the flat side surface of the dielectric substrate 101. The dielectric substrate 101 has a ring shape when viewed from the side of the square wave structure.
根据上述设计原理和思路, 本实施例中对于超材料的各个圆环形结构, 其等效介电常数和等效磁导率呈阶梯状分布, 一方面, 通过设计人造微结构 102的结构形状和排布规律, 超材料能获得一定的电磁特性, 另一方面, 通 过各个圆环形结构等效介电常数和等效磁导率的高低交替分布,超材料能获 得相应的功能特性叠加, 具有更为灵活的功能设计和更为丰富的功能应用。 实施例 7  According to the above design principles and ideas, in the present embodiment, for each annular structure of the metamaterial, the equivalent dielectric constant and the equivalent magnetic permeability are stepped, and on the other hand, the structural shape of the artificial microstructure 102 is designed. And the arrangement rule, the metamaterial can obtain certain electromagnetic characteristics. On the other hand, through the alternating distribution of the equivalent dielectric constant and the equivalent magnetic permeability of each circular ring structure, the metamaterial can obtain the corresponding functional property superposition. More flexible functional design and richer functional applications. Example 7
将介质基板 101设计为包括有多个不同材料的回形基板单元 103, 介质 基板的平面视图参看附图 14, 图 15为图 14的 A-A剖视图, 其中, 各个回 形基板单元 103采用不同的材料,各种材料的介电常数的大小由外围向中心 递增, 图 15中用不同填充密度表示了不同材料, 其中, 填充密度大的表示 材料的介电常数大, 填充密度小的表示材料的介电常数小。 由于单个基本结 构单元的电磁特性主要由该基本结构单元的等效介电常数和等效磁导率决 定, 而单个基本结构单元的等效介电常数和等效磁导率又由人造微结构 102 及其所在的介质基板 101所共同决定, 所以, 当各个回形基板单元 103采用 不同的材料时, 相当于改变了介质基板 101 上各个不同回形基板单元 103 内的介电常数,各个回形基板单元 103内的基本结构单元的等效介电常数随 着其所属回形基板单元 103 的不同也将被改变, 最终使超材料功能板 100 在不同区域内具有不同的介电常数分布,从而为超材料的功能设计提供了更 灵活的设计方式。 The dielectric substrate 101 is designed to include a plurality of different materials of the return substrate unit 103. The plan view of the dielectric substrate is shown in FIG. 14, and FIG. 15 is a cross-sectional view taken along line AA of FIG. The substrate unit 103 is made of a different material, and the dielectric constant of each material is increased from the periphery to the center. Different packing densities are used to indicate different materials in FIG. 15, wherein a large packing density indicates that the material has a large dielectric constant. A small packing density means that the dielectric constant of the material is small. Since the electromagnetic properties of a single basic structural unit are mainly determined by the equivalent dielectric constant and equivalent magnetic permeability of the basic structural unit, the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure. 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective return substrate units 103 are made of different materials, the dielectric constants in the different return substrate units 103 on the dielectric substrate 101 are changed. The equivalent dielectric constant of the basic structural unit in the substrate unit 103 will also be changed depending on the associated back substrate unit 103, and finally the metamaterial functional panel 100 has different dielectric constant distributions in different regions. This provides a more flexible design for the functional design of metamaterials.
本实施例中,要使回形基板单元 103的介电常数的大小由外围向中心递 增,可以灵活地从陶瓷基材、塑料树脂基材或复合材料基材选择合适的材料, 使不同回形基板单元 103按照介电常数的大小采用不同的材料进行排列,从 而在整体上使超材料具有非均匀的介电常数分布。  In this embodiment, the dielectric constant of the return substrate unit 103 is increased from the periphery to the center, and the material can be flexibly selected from the ceramic substrate, the plastic resin substrate or the composite substrate to make different shapes. The substrate unit 103 is arranged in a different material according to the magnitude of the dielectric constant, so that the metamaterial has a non-uniform dielectric constant distribution as a whole.
应当理解,本实施例中回形基板单元 103的大小和数量可以根据需要任 意设计, 以满足超材料的电磁特性要求。 并且, 本实施例中各个回形基板单 元 103 的介电常数大小由外围向中心递增只是为了便于说明本发明而例举 的特例, 具体实施时, 各个回形基板单元 103的介电常数大小的排布规律也 需要根据预定的超材料电磁特性而定,本发明的要旨也在于通过各个回形基 板单元 103采用不同的材料为超材料的电磁特性提供一种设计途径,并通过 该设计途径与超材料功能板上人造微结构排布规律的设计进行组合,以达到 扩展超材料的功能设计途径的目的。 实施例 8  It should be understood that the size and number of the paper-shaped substrate unit 103 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial. Moreover, in the present embodiment, the dielectric constant of each of the returning substrate units 103 is increased from the periphery to the center only as a specific example for convenience of explanation of the present invention. In specific implementation, the dielectric constant of each of the returning substrate units 103 is The arrangement rule also needs to be determined according to the predetermined electromagnetic properties of the metamaterial. The gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials of the respective back substrate units 103, and through the design approach The design of the artificial microstructure of the super-material function board is combined to achieve the purpose of expanding the functional design path of the super material. Example 8
作为本发明的另一种变形,本实施例将介质基板 101设计为包括有多个 不同材料的环形基板单元 104, 介质基板的平面视图参看附图 16, 图 17为 图 16的 B-B剖视图, 其中, 各个环形基板单元 104采用两种不同的材料, 两种材料的介电常数呈大小交替分布, 图 17中用不同填充密度表示了不同 材料, 其中, 填充密度大的表示材料的介电常数大, 填充密度小的表示材料 的介电常数小。由于单个基本结构单元的电磁特性主要由该基本结构单元的 等效介电常数和等效磁导率决定,而单个基本结构单元的等效介电常数和等 效磁导率又由人造微结构 102及其所在的介质基板 101所共同决定, 所以, 当各个环形基板单元 104 采用不同的材料时, 相当于改变了介质基板 101 上各个不同基板单元内的介电常数,各个环形基板单元 104内的基本结构单 元的等效介电常数随着其所属环形基板单元 104的不同也将被改变,最终使 超材料功能板 100在不同区域内具有不同的介电常数分布,从而为超材料的 功能设计提供了更灵活的设计方式。 As another variation of the present invention, the dielectric substrate 101 is designed as an annular substrate unit 104 including a plurality of different materials. A plan view of the dielectric substrate is shown in FIG. 16, and FIG. 17 is a cross-sectional view taken along line BB of FIG. Each annular substrate unit 104 is made of two different materials, and the dielectric constants of the two materials are alternately distributed in size, and different packing densities are represented in FIG. The material in which the packing density is large indicates that the material has a large dielectric constant, and the small packing density indicates that the dielectric constant of the material is small. Since the electromagnetic properties of a single basic structural unit are mainly determined by the equivalent dielectric constant and equivalent magnetic permeability of the basic structural unit, the equivalent dielectric constant and equivalent magnetic permeability of a single basic structural unit are determined by the artificial microstructure. 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective annular substrate units 104 are made of different materials, the dielectric constants in the different substrate units on the dielectric substrate 101 are changed, and the respective annular substrate units 104 are The equivalent dielectric constant of the basic structural unit will also be changed depending on the ring substrate unit 104 to which it belongs, and finally the metamaterial functional board 100 has different dielectric constant distributions in different regions, thereby functioning as a metamaterial. The design provides a more flexible design approach.
本实施例中, 要使环形基板单元 104的介电常数呈大小交替分布, 可以 选择两种不同的材料, 并使不同环形基板单元 104 采用不同的材料交替排 列, 从而在整体上使超材料具有非均匀的介电常数分布。  In this embodiment, in order to alternately distribute the dielectric constants of the annular substrate unit 104, two different materials may be selected, and the different annular substrate units 104 are alternately arranged with different materials, so that the metamaterials are provided as a whole. Non-uniform dielectric constant distribution.
应当理解,本实施例中环形基板单元 104的大小和数量可以根据需要任 意设计, 以满足超材料的电磁特性要求。 并且, 本实施例中各个环形基板单 元 104的介电常数大小交替排列只是为了便于说明本发明而例举的特例,具 体实施时,各个环形基板单元 104的介电常数大小的排布规律也需要根据预 定的超材料电磁特性而定, 本发明的要旨也在于通过各个环形基板单元 104 采用不同的材料为超材料的电磁特性提供一种设计途径,并通过该设计途径 与超材料功能板上人造微结构排布规律的设计进行组合,以达到扩展超材料 的功能设计途径的目的。 实施例 9  It should be understood that the size and number of the annular substrate unit 104 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial. Moreover, the dielectric constants of the respective annular substrate units 104 in the present embodiment are alternately arranged only for the sake of convenience in explaining the present invention. In the specific implementation, the arrangement law of the dielectric constants of the respective annular substrate units 104 is also required. Depending on the predetermined supermaterial electromagnetic properties, the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials of the respective annular substrate units 104, and to create artificial materials on the metamaterial functional board by the design approach. The design of the microstructure arrangement rules is combined to achieve the purpose of expanding the functional design approach of the metamaterial. Example 9
将介质基板 101设计为包括有多个回形基板单元 103, 介质基板的平面 视图参看附图 18, 图 19为图 18的 A-A剖视图, 其中, 各个回形基板单元 103采用不同的材料, 各种材料的的介电常数的大小由周边向中心递增, 图 3中用不同填充密度表示了不同材料, 其中, 填充密度大的表示材料的介电 常数大, 填充密度小的表示材料的介电常数小, 同时各个回形基板单元 103 的厚度也由周边向中心递增。由于超材料的电磁特性是由多个超材料基本结 构单元的等效介电常数和等效磁导率决定,而单个基本结构单元的等效介电 常数和等效磁导率又由人造微结构 102及其所在的介质基板 101 所共同决 定, 所以, 当各个回形基板单元 103采用不同的材料时, 相当于改变了介质 基板 101 上各个不同回形基板单元 103 内的介电常数, 各个回形基板单元 103内的基本结构单元的等效介电常数随着其所属回形基板单元 103的不同 也将被改变,最终使超材料功能板 100在不同区域内具有不同的介电常数分 布。 同时, 将各个回形基板单元 103的厚度设计为由周边向中心递增, 相对 于各个回形基板单元 103内的超材料基本结构单元而言, 回形基板单元 103 的厚度不同, 超材料基本结构单元内介质基板 101的占有比例将不同, 因此 各个回形基板单元 103 内的超材料基本结构单元表现出来的等效介电常数 也会不同。 The dielectric substrate 101 is designed to include a plurality of return substrate units 103. The plan view of the dielectric substrate is shown in FIG. 18. FIG. 19 is a cross-sectional view taken along line AA of FIG. 18, wherein each of the return substrate units 103 is made of different materials. The dielectric constant of the material increases from the periphery to the center. Different packing densities are used to indicate different materials in Fig. 3. Among them, the high packing density indicates that the material has a large dielectric constant, and the small packing density indicates the dielectric constant of the material. Small, while the thickness of each of the return substrate units 103 is also increased from the periphery toward the center. Since the electromagnetic properties of metamaterials are determined by the equivalent dielectric constant and equivalent permeability of a plurality of metamaterial basic structural units, the equivalent dielectric of a single basic structural unit The constant and the equivalent magnetic permeability are determined by the artificial microstructure 102 and the dielectric substrate 101 in which it is disposed. Therefore, when each of the returning substrate units 103 is made of a different material, it is equivalent to changing the different times on the dielectric substrate 101. The dielectric constant in the substrate unit 103, the equivalent dielectric constant of the basic structural unit in each of the return substrate units 103 will also be changed depending on the associated back substrate unit 103, and finally the metamaterial function board 100 will be changed. There are different dielectric constant distributions in different regions. Meanwhile, the thickness of each of the paper-shaped substrate units 103 is designed to be increased from the periphery toward the center, and the thickness of the paper-shaped substrate unit 103 is different with respect to the meta-material basic structural unit in each of the paper-shaped substrate units 103, and the basic structure of the metamaterial is The proportion of the dielectric substrate 101 in the cell will be different, and therefore the equivalent dielectric constant exhibited by the metamaterial basic structural unit in each of the returned substrate units 103 will be different.
由此可知, 通过改变回形基板单元 103的厚度和选择不同的材料, 可以 使超材料的介电常数呈非均匀分布,从而达到为超材料的功能设计提供了更 灵活的设计方式的目的。  It can be seen that by changing the thickness of the substrate unit 103 and selecting different materials, the dielectric constant of the metamaterial can be non-uniformly distributed, thereby providing a more flexible design method for the functional design of the metamaterial.
本实施例中,要使回形基板单元 103的介电常数的大小由外围向中心递 增,可以灵活地从陶瓷基材、塑料树脂基材或复合材料基材选择合适的材料, 使不同回形基板单元 103按照介电常数的大小采用不同的材料进行排列,从 而在整体上使超材料具有非均匀的介电常数分布。  In this embodiment, the dielectric constant of the return substrate unit 103 is increased from the periphery to the center, and the material can be flexibly selected from the ceramic substrate, the plastic resin substrate or the composite substrate to make different shapes. The substrate unit 103 is arranged in a different material according to the magnitude of the dielectric constant, so that the metamaterial has a non-uniform dielectric constant distribution as a whole.
应当理解, 本实施例中回形基板单元 103的大小、数量以及厚度可以根 据需要任意设计, 以满足超材料的电磁特性要求。 并且, 本实施例中各个回 形基板单元 103 的介电常数大小由外围向中心递增只是为了便于说明本发 明而例举的特例, 具体实施时, 各个回形基板单元 103的介电常数大小的排 布规律也需要根据预定的超材料电磁特性而定,本发明的要旨也在于通过各 个回形基板单元 103 采用不同的材料和不同厚度为超材料的电磁特性提供 一种设计途径,并通过该设计途径与超材料功能板上人造微结构排布规律的 设计进行组合, 以达到扩展超材料的功能设计途径的目的。 实施例 10  It should be understood that the size, number, and thickness of the paper-shaped substrate unit 103 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial. Moreover, in the present embodiment, the dielectric constant of each of the returning substrate units 103 is increased from the periphery to the center only as a specific example for convenience of explanation of the present invention. In specific implementation, the dielectric constant of each of the returning substrate units 103 is The arrangement rule also needs to be determined according to the predetermined electromagnetic properties of the metamaterial. The gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials and different thicknesses of the respective back substrate units 103, and The design approach is combined with the design of the artificial microstructure arrangement on the metamaterial function board to achieve the purpose of expanding the functional design approach of the metamaterial. Example 10
作为本发明的另一种变形,本实施例将介质基板 101设计为包括有多个 不同材料的环形基板单元 104, 介质基板的平面视图参看附图 20, 图 21为 图 20的 B-B剖视图, 其中, 各个环形基板单元 104采用两种不同的材料, 两种材料的介电常数呈大小交替分布, 图 21中用两种不同的填充密度表示 了该两种不同材料, 其中, 填充密度大的表示材料的介电常数大, 填充密度 小的表示材料的介电常数小,同时各个回形基板单元 103的厚度也呈厚薄交 替分布。由于超材料的电磁特性是由多个超材料基本结构单元的等效介电常 数和等效磁导率决定,而单个基本结构单元的等效介电常数和等效磁导率又 由人造微结构 102及其所在的介质基板 101所共同决定, 所以, 当各个环形 基板单元 104采用不同的材料时,相当于改变了介质基板 101上各个不同基 板单元内的介电常数,各个环形基板单元 104内的基本结构单元的等效介电 常数随着其所属环形基板单元 104的不同也将被改变,最终使超材料功能板 100在不同区域内具有不同的介电常数分布。同时,将各个回形基板单元 103 的厚度设计为厚薄交替分布,相对于各个回形基板单元 103内的超材料基本 结构单元而言, 回形基板单元 103的厚度不同, 超材料基本结构单元内介质 基板 101的占有比例将不同,因此各个回形基板单元 103内的超材料基本结 构单元表现出来的等效介电常数也会不同。 As another variation of the present invention, the present embodiment designs the dielectric substrate 101 as an annular substrate unit 104 including a plurality of different materials. A plan view of the dielectric substrate is shown in FIG. 20, and FIG. 21 is 20 is a cross-sectional view taken along line BB, wherein each of the annular substrate units 104 is made of two different materials, and the dielectric constants of the two materials are alternately distributed, and the two different materials are represented by two different packing densities in FIG. Among them, the material having a large packing density has a large dielectric constant, and the small packing density indicates that the dielectric constant of the material is small, and the thickness of each of the returning substrate units 103 is also alternately thick and thin. Since the electromagnetic properties of metamaterials are determined by the equivalent dielectric constant and equivalent permeability of a plurality of metamaterial basic structural units, the equivalent dielectric constant and equivalent permeability of a single basic structural unit are The structure 102 and the dielectric substrate 101 in which it is disposed are determined together. Therefore, when the respective annular substrate units 104 are made of different materials, the dielectric constants in the different substrate units on the dielectric substrate 101 are changed, and the respective annular substrate units 104 are replaced. The equivalent dielectric constant of the basic structural unit within it will also be changed depending on the ring substrate unit 104 to which it belongs, eventually causing the metamaterial functional panel 100 to have different dielectric constant distributions in different regions. At the same time, the thickness of each of the paper-shaped substrate units 103 is designed to be alternately thick and thin, and the thickness of the paper-shaped substrate unit 103 is different with respect to the meta-material basic structural unit in each of the paper-shaped substrate units 103, and the meta-material basic structural unit is The occupation ratio of the dielectric substrate 101 will be different, and therefore the equivalent dielectric constant exhibited by the metamaterial basic structural unit in each of the return substrate units 103 will also be different.
本实施例中, 要使环形基板单元 104的介电常数呈大小交替分布, 一方 面, 可以选择两种不同的材料, 并使两种不同材料的环形基板单元 104交替 排列, 从而在整体上使超材料具有非均匀的介电常数分布, 同时, 为更好地 使环形基板单元 104的介电常数呈大小交替分布, 将各个回形基板单元 103 的厚度设计为厚薄交替分布,使厚度的交替分布与材料的交替分布产生的对 介电常数的效果叠加, 设计将更为灵活。  In this embodiment, the dielectric constants of the annular substrate unit 104 are alternately distributed. On the one hand, two different materials can be selected, and the annular substrate units 104 of two different materials are alternately arranged, thereby making the whole The metamaterial has a non-uniform dielectric constant distribution, and at the same time, in order to better alternate the dielectric constant of the annular substrate unit 104, the thickness of each of the return substrate units 103 is designed to be alternately thick and thin, so that the thickness is alternated. The effect of the distribution of the material and the alternating distribution of the material on the dielectric constant will be more flexible.
应当理解, 本实施例中环形基板单元 104的大小、数量和厚度可以根据 需要任意设计, 以满足超材料的电磁特性要求。 并且, 本实施例中各个环形 基板单元 104 的介电常数大小交替排列只是为了便于说明本发明而例举的 特例, 具体实施时, 各个环形基板单元 104的介电常数大小的排布规律也需 要根据预定的超材料电磁特性而定,本发明的要旨也在于通过各个环形基板 单元 104 采用不同的材料和不同的厚度为超材料的电磁特性提供一种设计 途径,并通过该设计途径与超材料功能板上人造微结构排布规律的设计进行 组合, 以达到扩展超材料的功能设计途径的目的。 由上述说明可知, 使用根据本发明非均匀厚度和 /或由不同材料组成的 介质基板的超材料, 可以使超材料具有更为丰富的功能应用, 如实现对电磁 波的汇聚、发散和偏折作用等, 使超材料的介质基板和人造微结构同时具有 各种电磁特性, 为超材料形成多种特有的功能提供了解决方案。 It should be understood that the size, number, and thickness of the annular substrate unit 104 in this embodiment can be arbitrarily designed as needed to meet the electromagnetic characteristics of the metamaterial. Moreover, the dielectric constants of the respective annular substrate units 104 in the present embodiment are alternately arranged only for the sake of convenience in explaining the present invention. In the specific implementation, the arrangement law of the dielectric constants of the respective annular substrate units 104 is also required. According to the predetermined electromagnetic properties of the metamaterial, the gist of the present invention is also to provide a design path for the electromagnetic properties of the metamaterial by using different materials and different thicknesses of the respective annular substrate units 104, and through the design approach and the metamaterial. The design of the artificial microstructure arrangement rules on the function board is combined to achieve the purpose of expanding the functional design path of the super material. It can be seen from the above description that the use of metamaterials according to the present invention for non-uniform thicknesses and/or dielectric substrates composed of different materials can make the metamaterials have more abundant functional applications, such as achieving convergence, divergence and deflection of electromagnetic waves. In addition, the dielectric substrate and the artificial microstructure of the metamaterial have various electromagnetic characteristics at the same time, which provides a solution for forming a plurality of unique functions of the metamaterial.
最后需要说明的是,本发明中的回形基板单元或环形基板单元均只是具 体实施方式之一, 基板单元的区域形状可以根据需要进行任意设计。  Finally, it should be noted that the paper-shaped substrate unit or the annular substrate unit in the present invention is only one of the specific embodiments, and the shape of the area of the substrate unit can be arbitrarily designed as needed.
在上述实施例中, 仅对本发明进行了示范性描述, 但是本领域技术人员 在阅读本专利申请后可以在不脱离本发明的精神和范围的情况下对本发明 进行各种修改。  In the above-described embodiments, the present invention has been exemplarily described, and various modifications of the present invention may be made without departing from the spirit and scope of the invention.

Claims

权 利 要 求 书 Claim
1、 一种超材料, 包括多个阵列的超材料功能板, 所述超材料功能板包 括介质基板以及阵列在介质基板上的多个人造微结构, 其特征在于: 所述介 质基板具有非均匀的介电常数分布。 What is claimed is: 1. A metamaterial comprising a plurality of arrays of metamaterial functional panels, the metamaterial functional panel comprising a dielectric substrate and a plurality of artificial microstructures arrayed on the dielectric substrate, wherein: the dielectric substrate has a non-uniformity The dielectric constant distribution.
2、 根据权利要求 1所述的超材料, 其特征在于: 所述介质基板的厚度 呈非均匀分布。  2. The metamaterial according to claim 1, wherein: the thickness of the dielectric substrate is non-uniformly distributed.
3、 根据权利要求 1所述的超材料, 其特征在于: 所述介质基板由多个 不同材料的基板单元组成。  3. The metamaterial according to claim 1, wherein: the dielectric substrate is composed of a plurality of substrate units of different materials.
4、 根据权利要求 1所述的超材料, 其特征在于: 所述介质基板由多个 不同材料的基板单元组成, 且所述多个基板单元的厚度呈非均匀分布。  4. The metamaterial according to claim 1, wherein: the dielectric substrate is composed of a plurality of substrate units of different materials, and the thickness of the plurality of substrate units is non-uniformly distributed.
5、 根据权利要求 2所述的超材料, 其特征在于: 所述介质基板为凸椭 球形或凹椭球形。  The metamaterial according to claim 2, wherein the dielectric substrate is a convex ellipsoid or a concave ellipsoid.
6、 根据权利要求 2所述的超材料, 其特征在于: 所述介质基板的侧面 为多个回形结构或多个环形结构,所述多个回形结构或多个环形结构的厚度 不同。  The metamaterial according to claim 2, wherein: the side surface of the dielectric substrate is a plurality of back structures or a plurality of ring structures, and the plurality of back structures or the plurality of ring structures have different thicknesses.
7、 根据权利要求 6所述的超材料, 其特征在于: 所述多个回形结构或 多个环形结构的厚度呈阶梯状分布。  7. The metamaterial according to claim 6, wherein: the thickness of the plurality of back structures or the plurality of ring structures is stepped.
8、 根据权利要求 3所述的超材料, 其特征在于: 所述介质基板包括有 多个回形结构或环形结构的基板单元。  The metamaterial according to claim 3, wherein the dielectric substrate comprises a substrate unit having a plurality of return structures or annular structures.
9、 根据权利要求 8所述的超材料, 其特征在于: 其特征在于: 所述多 个回形结构或环形结构的基板单元的介电常数按梯度增大或减小。  9. The metamaterial according to claim 8, wherein: the dielectric constant of the substrate unit of the plurality of return structures or annular structures is increased or decreased by a gradient.
10、 根据权利要求 8所述的超材料, 其特征在于: 所述多个回形结构或 环形结构的基板单元的介电常数的大小交替分布。  The metamaterial according to claim 8, wherein the dielectric constants of the plurality of the return-shaped structures or the ring-shaped substrate units are alternately distributed.
11、 根据权利要求 4所述的超材料, 其特征在于: 所述介质基板包括有 多个回形结构或环形结构的基板单元。  The metamaterial according to claim 4, wherein the dielectric substrate comprises a substrate unit having a plurality of return structures or annular structures.
12、 根据权利要求 11所述的超材料, 其特征在于: 其特征在于: 所述 多个回形结构或环形结构的基板单元的介电常数按梯度增大或减小。 12. The metamaterial according to claim 11, wherein: the dielectric constant of the substrate unit of the plurality of return structures or annular structures is increased or decreased by a gradient.
13、 根据权利要求 11所述的超材料, 其特征在于: 所述多个回形结构 或环形结构的基板单元的介电常数的大小交替分布。 The metamaterial according to claim 11, wherein the dielectric constants of the plurality of the return-shaped structures or the ring-shaped substrate units are alternately distributed.
14、 根据权利要求 1至 13任一所述的超材料, 其特征在于: 所述基板 单元的材料为陶瓷基材、 塑料树脂基材或复合材料基材。  The metamaterial according to any one of claims 1 to 13, wherein the material of the substrate unit is a ceramic substrate, a plastic resin substrate or a composite substrate.
15、 根据权利要求 1至 13任一所述的超材料, 其特征在于: 所述人造 微结构为金属人造微结构。  The metamaterial according to any one of claims 1 to 13, wherein the artificial microstructure is a metal artificial microstructure.
16、 根据权利要求 15所述的的超材料, 其特征在于: 所述金属人造微 结构为工字型或工字衍生型。  The metamaterial according to claim 15, wherein the metal artificial microstructure is of an I-shaped or I-shaped type.
PCT/CN2011/084435 2011-03-25 2011-12-22 Metamaterial WO2012129941A1 (en)

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CN201110074026.7A CN102637959B (en) 2011-03-25 2011-03-25 Metamaterial with dielectric substrate with nonuniform thickness
CN 201110109047 CN102480011B (en) 2011-04-28 2011-04-28 Metamaterial with non-uniform material distribution
CN 201110109034 CN102480010B (en) 2011-04-28 2011-04-28 Inhomogeneous metamaterial
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CN101162800A (en) * 2006-10-10 2008-04-16 西北工业大学 Mobile phone antenna medium substrates with anti-symmetric structure left hand material
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