CN102110890B - High-gain horn antenna based on non-uniform medium - Google Patents

High-gain horn antenna based on non-uniform medium Download PDF

Info

Publication number
CN102110890B
CN102110890B CN 201110036235 CN201110036235A CN102110890B CN 102110890 B CN102110890 B CN 102110890B CN 201110036235 CN201110036235 CN 201110036235 CN 201110036235 A CN201110036235 A CN 201110036235A CN 102110890 B CN102110890 B CN 102110890B
Authority
CN
China
Prior art keywords
refractive index
medium
horn antenna
antenna
unit
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN 201110036235
Other languages
Chinese (zh)
Other versions
CN102110890A (en
Inventor
杜春雷
袁桂山
董小春
邓启凌
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Institute of Optics and Electronics of CAS
Original Assignee
Institute of Optics and Electronics of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Institute of Optics and Electronics of CAS filed Critical Institute of Optics and Electronics of CAS
Priority to CN 201110036235 priority Critical patent/CN102110890B/en
Publication of CN102110890A publication Critical patent/CN102110890A/en
Application granted granted Critical
Publication of CN102110890B publication Critical patent/CN102110890B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Waveguide Aerials (AREA)
  • Aerials With Secondary Devices (AREA)

Abstract

一种基于非均匀介质的高增益喇叭天线,制作如下:(1)确定天线工作的中心频率f;(2)根据喇叭天线的一般设计方法设计出工作在该中心频率的普通喇叭天线,天线的H面口径为a,E面口径为b,喇叭长度为h;(3)确定置于喇叭口面的非均匀介质的折射率分布n(x,y);(4)利用“工”字型亚波长人工结构材料构建折射率按n(x,y)分布的非均匀介质,采用有限元软件仿真的方式求出每一折射率对应的工字型亚波长人工结构材料单元的结构尺寸。

Figure 201110036235

A kind of high-gain horn antenna based on inhomogeneous medium is made as follows: (1) determine the center frequency f of antenna work; (2) design the common horn antenna that works at this center frequency according to the general design method of horn antenna, the antenna's The diameter of the H surface is a, the diameter of the E surface is b, and the length of the horn is h; (3) determine the refractive index distribution n(x, y) of the heterogeneous medium placed on the horn mouth surface; (4) use the "I" font The sub-wavelength artificial structure material constructs a heterogeneous medium whose refractive index is distributed according to n(x, y), and the structure size of the I-shaped sub-wavelength artificial structure material unit corresponding to each refractive index is calculated by means of finite element software simulation.

Figure 201110036235

Description

A kind of high-gain horn antenna based on non-uniform dielectric
Technical field
The present invention is designed into a kind of horn antenna, particularly a kind of high-gain horn antenna based on non-uniform dielectric.
Background technology
Horn antenna is a kind of directional antenna, and it can regard the waveguide of opening as.The function of loudspeaker is to produce uniform phase front at the bore larger than waveguide, thereby obtains higher directionality.Because its design, easy to manufacture and cost is all lower, horn antenna has widely purposes in real life.
What limit the horn antenna directivity mainly is the inconsistency of phase place on the loudspeaker actinal surface.When electromagnetic wave entered loudspeaker throat and arrives the loudspeaker actinal surface from waveguide, electromagnetic corrugated became sphere by the plane, no longer equated in the power on phase place of magnetic wave of loudspeaker actinal surface.In order to reduce the inconsistency of phase place on the actinal surface, the means that often adopt are to change the subtended angle of loudspeaker or the length of loudspeaker, but adopt above-mentioned means can only reduce phase difference, can not fundamentally eliminate the inconsistent harmful effect of phase place.
Summary of the invention
The technical problem to be solved in the present invention is: overcome the upper mutually inconsistent shortcoming of existing common horn antenna loudspeaker actinal surface, a kind of high-gain horn antenna based on non-uniform dielectric is provided, adopt non-uniform dielectric to eliminate phasic difference, the gain that has improved horn antenna.
Technical solution of the present invention: based on the high-gain horn antenna of non-uniform dielectric, making step is as follows:
(1) determines the centre frequency f of antenna work, centre frequency according to antenna work is designed a horn antenna that is operated in this frequency range according to the method for designing of common horn antenna, the H face bore of described horn antenna is a, and E face bore is b, and horn length is h;
(2) increase one deck non-uniform dielectric at the loudspeaker actinal surface of horn antenna, according to the thickness d of non-uniform dielectric and the non-uniform dielectric refractive index n at origin of coordinates place 0, obtain the refraction index profile n (x, y) of the non-uniform dielectric that places the loudspeaker actinal surface,
Figure BDA0000046613930000011
X wherein, y represent the non-uniform dielectric each point take the Antenna aperture center as the origin of coordinates, the coordinate in the coordinate system of setting up take the horn antenna radiation direction as x axle forward;
(3) change into a plurality of cubic units that the length of side is l with non-uniform dielectric is discrete, obtain the refractive index n (m, n) of each cubic units by the formula in the step (2), wherein (m, n) is the numbering of unit;
(4) FEM (finite element) model of foundation " worker " font sub-wavelength artificial structure material, the equivalent refractive index of employing Finite Element Calculating material, the structural parameters a of change material 0, a 0Be the length of side of " worker " shape metal structure in " worker " font structure, simulation calculation goes out different length of side a 0The equivalent refractive index n of structural correspondence;
(5) by a that obtains in the step (4) 0Obtain the physical dimension of each junior unit in the step (3) with the relation of n, with each unit of this dimensioned, again all unit combination can be obtained the non-uniform dielectric that needs.
N in the described step (2) 0Value should determine that according to minimum and the largest refractive index of the described artificial structure's material in back minimum and the largest refractive index of establishing " worker " font artificial structure material are n Min, n Max, n then 0Satisfy: n min + h 2 + b 2 4 - h d < n 0 < n max .
The length of side l of the cubic units in the described step (3) is less than or equal to 1/10th of antenna operation wavelength.
All regard each cubic units after the non-uniform dielectric discretization as uniform dielectric in the described step (3), because the size of each unit is less than 1/10th wavelength, index step changes and can ignore between unit and the unit, brings the center point coordinate of each unit into formula
Figure BDA0000046613930000022
In can calculate the refractive index of this unit.
" worker " font sub-wavelength artificial structure material in the described step (4) is that the cubic units of l forms by the length of side, and each unit is comprised of three parts: thickness is h 0FR-4 substrate, the thickness that etches in substrate be " worker " font copper metal film of 0.017mm and the medium that wraps up them, wherein the vertical edge width in the middle of " worker " font is w 1, the horizontal edge width on both sides is w up and down 2, the dielectric constant of medium is ε 0
Described medium be air or silicon, the dielectric constant of the medium of selecting is larger, the equivalent refractive index that obtains is also larger.
Utilize the equivalent refractive index implementation of Finite Element Calculating material as follows in the described step (4): to adopt the commercial finite element software of CST or HFSS, set up the model of element of " worker " font artificial structure material, threedimensional model is comprised of three parts: thickness is h 0FR-4 substrate, the thickness that etches in substrate be " worker " font copper metal film of 0.017mm and the medium that wraps up them, wherein to be the vertical edge width in the middle of the l I shape be w to unit length and width height 1, the horizontal edge width on both sides is w up and down 2, the dielectric constant of medium is ε 0The front of model is " worker " font copper film, and the model side is set to periodic boundary condition, and front and back arranges respectively two ripple ports.The frequency range of emulation should comprise the operating frequency of antenna, obtains the scattering parameter of model by simulation calculation, calculates the equivalent refractive index of material according to the scattering parameter method of inversion again.
Each unit of processing adopts the processing method of pcb board in the described step (5), the substrate that is positioned at all unit of same layer can share a large FR-4 sheet material, just etch the I shape metal structure of corresponding size at the diverse location place of sheet material, fill the medium of selecting between every one deck FR-4 sheet material.
The present invention's advantage compared with prior art is:
(1) the present invention adds the last layer non-uniform dielectric at the loudspeaker actinal surface, has fundamentally eliminated the position phase inconsistency on the actinal surface, and the gain that has improved horn antenna can be used for designing the horn antenna of high-gain.
(2) high-gain horn antenna of the present invention is compared with the common horn antenna with identical gain, and length and the bore of loudspeaker are less, are convenient to the miniaturization of device.
(3) " worker " font artificial structure material of the present invention's employing can obtain various refractive indexes easily by the adjustment structure parameter, and the non-constant width of the frequency band of this kind structural material, loss is also little, can go out " worker " font metal structure by direct etching on FR-4 sheet material, and is easy to process.
Description of drawings
Fig. 1 is antenna structure view of the present invention.Left figure is H face view, and right figure is E face view.Curve in the loudspeaker represents the corrugated, can find out after spherical wave is by non-uniform dielectric to have become plane wave from left figure;
Fig. 2 is the non-uniform dielectric discretization schematic diagram among the present invention.Right figure shown discrete after to the mode of each element number, non-uniform dielectric has been separated into 45X35 junior unit, each unit all is one and longly is the cube of l, is comprised of " worker " font sub-wavelength artificial structure material;
Fig. 3 is " worker " font sub-wavelength artificial structure material cell model schematic diagram among the present invention.Yl moiety is copper film among the figure, and purple partly is medium substrate, and translucent blue portion is the medium of lapping;
Fig. 4 is the structural representation of the every layer of material among the present invention.Left figure is the overall distribution situation of every one deck unit, and right figure is the schematic diagram of unit.
Embodiment
As shown in Figure 1, the high-gain horn antenna specific implementation process based on non-uniform dielectric of the present invention is as follows:
(1) the work centre frequency of choosing antenna is 15GHz, determines the H face bore a=90mm of horn antenna according to the method for designing of conventional horn antenna, and E face bore is b=69mm, horn length h=115mm.
(2) get the thickness d=8mm of medium, the refractive index of medium at origin of coordinates place is 2.2, and this moment, the refractive index at origin of coordinates place satisfied Then the refraction index profile of non-uniform dielectric is Calculate as can be known only skewness in the H face of medium by formula, and maximum in the refractive index of initial point, be 2.2, minimum in the refractive index at edge, be 1.14.
(3) because the operation wavelength of antenna is 20mm, non-uniform dielectric can be dispersed and change into the cubic units that the length of side is l=2mm, as shown in Figure 2.Each unit is all regarded uniform medium as, and its refractive index is refractive index corresponding to unit center point.Because the distribution of refractive index is only relevant with the y coordinate figure of unit center point, so be the same in the four-layer structure of x direction, only need to consider one deck structure.45 * 35 unit are all arranged on every one deck, be numbered according to as shown in Figure 2 method, then the refractive index of each unit is:
n ( m , n ) = 2,2 - 13225 + ( 2 m - 46 ) 2 - 115 8
In the formula, (m, n) is the numbering of unit.
(4) FEM (finite element) model of foundation " worker " font sub-wavelength artificial structure material as shown in Figure 3 in order to reduce cost, selects circuit board medium FR-4 commonly used as the substrate of material, searches the specification of this medium and determines that substrate is h in the model 0The FR-4 of=0.2026mm, its dielectric constant are 3.85+i0.02.Given " worker " font copper film vertical edge width is w 1=0.3mm, horizontal edge width are w 2=0.2mm is to guarantee a 0The variations in refractive index of artificial structure's material comprises the zone of 1.14-2.2 during variation.In the CST simulation software, utilize periodic boundary condition to obtain the scattering parameter of material, obtained again the equivalent refractive index of sub-wavelength artificial structure material by the scattering parameter method of inversion, be i.e. every given parameter a 0, all can obtain one to one equivalent refractive index by the method for FEM (finite element) calculation emulation.Change the structural parameters a of material 0(a 0The length of side for " worker " shape metal structure in the I-shaped structure), simulation calculation goes out different length of side a 0The equivalent refractive index n of structural correspondence, such as a 0During=1mm, refractive index is about 1.34, a 0During=1.5mm, refractive index is 1.73, can obtain by that analogy equivalent refractive index about structural parameters a 0Variation relation.
(5) refractive index in the basis (4) is about a 0Curved line relation obtain the structural parameters a of the unit that is numbered (m, n) in the heterogeneous material 0(m, n), so that the refractive index of this unit is n (m, n), all structural parameters of antenna all can obtain.When making material, the substrate of all unit of same layer can be connected together forms a large FR-4 plate.Make-up room only need to etch in position corresponding to each unit accordingly " worker " font structure (as shown in Figure 4), four layers of same sheet material with " worker " font structure is combined to be placed on horn mouth square getting final product in front at last.Spacing during combination between the adjacent panel is l, and the distance of first block of plate and loudspeaker actinal surface is 1/2.
The non-elaborated part of the present invention belongs to techniques well known.

Claims (5)

1.一种基于非均匀介质的高增益喇叭天线制作方法,其特征在于制作步骤如下:1. A method for making a high-gain horn antenna based on a heterogeneous medium, characterized in that the steps of making are as follows: (1)确定天线工作的中心频率f,根据天线工作的中心频率按照普通喇叭天线的设计方法设计出一个工作在该频段的喇叭天线,所述喇叭天线的H面口径为a,E面口径为b,喇叭长度为h;(1) Determine the center frequency f of the antenna work, and design a horn antenna working in this frequency band according to the center frequency of the antenna work according to the design method of the ordinary horn antenna. The H-surface aperture of the horn antenna is a, and the E-surface aperture is b, the horn length is h; (2)在喇叭天线的喇叭口面上增加一层非均匀介质,根据非均匀介质的厚度d和非均匀介质在坐标原点处的折射率n0,求出置于喇叭口面的非均匀介质的折射率分布n(x,y),其中x,y代表非均匀介质各点在以天线口面中心为坐标原点,以喇叭天线辐射方向为x轴正向建立的坐标系中的坐标;(2) Add a layer of inhomogeneous medium on the horn surface of the horn antenna, and calculate the inhomogeneous medium placed on the horn surface according to the thickness d of the inhomogeneous medium and the refractive index n 0 of the inhomogeneous medium at the coordinate origin The refractive index distribution n(x,y) of Among them, x and y represent the coordinates of each point in the heterogeneous medium in the coordinate system established with the center of the antenna aperture as the coordinate origin and the radiation direction of the horn antenna as the positive direction of the x-axis; (3)将非均匀介质离散化成边长为l的多个立方体单元,由步骤(2)中的公式求出每一立方体单元的折射率n(m,n),其中(m,n)为单元的编号;(3) Discretize the inhomogeneous medium into multiple cubic units with side length l, and calculate the refractive index n(m,n) of each cubic unit by the formula in step (2), where (m,n) is the number of the unit; (4)建立“工”字型亚波长人工结构材料的有限元模型,采用有限元法计算材料的等效折射率,改变材料的结构参数a0,a0为工字型结构中“工”形金属结构的边长,仿真计算出不同边长a0的结构对应的等效折射率n;(4) Establish the finite element model of the "I"-shaped sub-wavelength artificial structure material, calculate the equivalent refractive index of the material by using the finite element method, and change the structural parameter a 0 of the material, where a 0 is the "I" in the I-shaped structure The side length of the shaped metal structure is simulated to calculate the equivalent refractive index n corresponding to the structure with different side length a 0 ; (5)由步骤(4)中得到的a0和n的关系得到步骤(3)中每一个小单元的结构尺寸,以该尺寸加工每一个单元,再将所有单元组合即可得到需要的非均匀介质;(5) Obtain the structural size of each small unit in step (3) from the relationship between a 0 and n obtained in step (4), process each unit with this size, and then combine all units to obtain the required non- homogeneous medium; 所述步骤(2)中的n0的取值根据后面所述的人工结构材料的最小和最大折射率来确定,设“工”字型人工结构材料的最小折射率为nmin,最大折射率为nmax,则n0满足: n min + h 2 + b 2 4 - h d < n 0 < n max ; The value of n 0 in the step (2) is determined according to the minimum and maximum refractive index of the artificial structure material described later, assuming that the minimum refractive index of the "I"-shaped artificial structure material is n min , and the maximum refractive index is n max , then n 0 satisfies: no min + h 2 + b 2 4 - h d < no 0 < no max ; 所述步骤(3)中的立方体单元的边长l小于等于天线工作波长的十分之一。The side length l of the cube unit in the step (3) is less than or equal to one tenth of the working wavelength of the antenna. 2.根据权利要求1所述的一种基于非均匀介质的高增益喇叭天线制作方法,其特征在于:所述步骤(4)中的“工”字型亚波长人工结构材料由边长为l的立方体单元组成,每一单元由三部分组成:厚度为h0的FR-4基底、在基底上刻蚀出的厚度为0.017mm的“工”字型金属铜膜以及包裹它们的介质,其中“工”字型中间的竖边宽度为w1、上下两边的横边宽度为w2,介质的介电常数为ε02. A method for manufacturing a high-gain horn antenna based on a heterogeneous medium according to claim 1, characterized in that: the "I"-shaped sub-wavelength artificial structure material in the step (4) has a side length of 1 Each unit consists of three parts: an FR-4 substrate with a thickness of h 0 , an "I"-shaped metal copper film with a thickness of 0.017mm etched on the substrate, and a medium that wraps them. The width of the vertical side in the middle of the "I" font is w 1 , the width of the horizontal side at the upper and lower sides is w 2 , and the dielectric constant of the medium is ε 0 . 3.根据权利要求1所述的一种基于非均匀介质的高增益喇叭天线制作方法,其特征在于:所述的介质的为空气或硅,选用的介质的介电常数越大,得到的等效折射率也越大。3. A kind of method for making a high-gain horn antenna based on a heterogeneous medium according to claim 1, characterized in that: said medium is air or silicon, and the dielectric constant of the selected medium is larger, and the obtained equal The effective refractive index is also larger. 4.根据权利要求1所述的一种基于非均匀介质的高增益喇叭天线制作方法,其特征在于:所述步骤(4)中利用有限元法计算材料的等效折射率具体实施如下:采用CST或者HFSS商用电磁仿真软件,建立“工”字型人工结构材料的单元模型,模型的正面为“工”字型铜膜,模型侧面设置为周期性边界条件,正面和背面分别设置两个波端口,仿真的频段应该包含天线的工作频率,通过仿真计算得到模型的散射参数,再根据散射参数反演法计算出材料的等效折射率。4. A method for manufacturing a high-gain horn antenna based on a heterogeneous medium according to claim 1, characterized in that: the calculation of the equivalent refractive index of the material using the finite element method in the step (4) is specifically implemented as follows: using CST or HFSS commercial electromagnetic simulation software, establish the unit model of "I"-shaped artificial structural materials, the front of the model is "I"-shaped copper film, the side of the model is set as periodic boundary conditions, and two waves are set on the front and back respectively. Port, the frequency band of the simulation should include the working frequency of the antenna, the scattering parameters of the model are obtained through simulation calculation, and then the equivalent refractive index of the material is calculated according to the scattering parameter inversion method. 5.根据权利要求1所述的一种基于非均匀介质的高增益喇叭天线,其特征在于:所述步骤(5)中加工每一个单元采用PCB板的加工方法,位于同一层的所有单元的基底共用一块大的FR-4板材,只是在板材的不同位置处刻蚀出相应尺寸的工字型金属结构,每一层FR-4板材之间填充选用的介质。5. A high-gain horn antenna based on a heterogeneous medium according to claim 1, characterized in that: in the step (5), each unit is processed by a PCB board processing method, and all units located on the same layer The base shares a large FR-4 plate, but the I-shaped metal structure of the corresponding size is etched at different positions of the plate, and the selected medium is filled between each layer of FR-4 plate.
CN 201110036235 2011-02-11 2011-02-11 High-gain horn antenna based on non-uniform medium Expired - Fee Related CN102110890B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 201110036235 CN102110890B (en) 2011-02-11 2011-02-11 High-gain horn antenna based on non-uniform medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 201110036235 CN102110890B (en) 2011-02-11 2011-02-11 High-gain horn antenna based on non-uniform medium

Publications (2)

Publication Number Publication Date
CN102110890A CN102110890A (en) 2011-06-29
CN102110890B true CN102110890B (en) 2013-10-30

Family

ID=44174959

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 201110036235 Expired - Fee Related CN102110890B (en) 2011-02-11 2011-02-11 High-gain horn antenna based on non-uniform medium

Country Status (1)

Country Link
CN (1) CN102110890B (en)

Families Citing this family (25)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102904067B (en) * 2011-07-29 2015-03-11 深圳光启高等理工研究院 Antenna
WO2013013466A1 (en) * 2011-07-26 2013-01-31 深圳光启高等理工研究院 Cassegrain radar antenna
WO2013013468A1 (en) * 2011-07-26 2013-01-31 深圳光启高等理工研究院 Offset feed radar antenna
WO2013013459A1 (en) * 2011-07-26 2013-01-31 深圳光启高等理工研究院 Cassegrain microwave antenna
CN102904037B (en) * 2011-07-26 2015-05-27 深圳光启高等理工研究院 Feed-forward microwave antenna
CN102904032B (en) * 2011-07-26 2015-04-22 深圳光启高等理工研究院 Feedback satellite television antenna and satellite television receiving system thereof
CN102945997B (en) * 2011-08-16 2015-04-22 深圳光启高等理工研究院 Resonant cavity
CN103036026B (en) * 2011-09-29 2016-01-13 深圳光启高等理工研究院 A kind of horn antenna
CN103036025B (en) * 2011-09-29 2015-11-18 深圳光启高等理工研究院 Horn antenna
CN103036030B (en) * 2011-09-29 2016-01-13 深圳光启高等理工研究院 Horn antenna
CN102544743B (en) * 2011-10-28 2014-04-16 深圳光启高等理工研究院 Microwave antenna
CN102593610B (en) * 2012-02-29 2014-04-30 深圳光启创新技术有限公司 Microwave antenna
CN103367929B (en) * 2012-03-31 2016-12-14 深圳光启创新技术有限公司 A kind of antenna for satellite communication in motion
CN103367927B (en) * 2012-03-31 2016-12-14 深圳光启高等理工研究院 Logical satellite antenna during one is quiet
CN103367930B (en) * 2012-03-31 2017-03-22 深圳光启创新技术有限公司 Mobile communications antenna
CN102723603B (en) * 2012-05-30 2015-06-03 深圳光启创新技术有限公司 Horn-shaped antenna
CN102723604B (en) * 2012-05-30 2015-04-15 深圳光启创新技术有限公司 Horn antenna
CN102769189B (en) * 2012-06-29 2015-12-16 深圳光启创新技术有限公司 A kind of horn-lens antenna
CN102760961B (en) * 2012-07-03 2015-03-11 深圳光启创新技术有限公司 Broadband low-dispersion metamaterial
EP2870659A1 (en) * 2012-07-03 2015-05-13 Lisa Dräxlmaier GmbH Antenna system for broadband satellite communication in the ghz frequency range, comprising dielectrically filled horn antennas
CN103682675B (en) * 2012-08-31 2018-04-17 深圳光启创新技术有限公司 A kind of electromagnetic horn
CN103414026B (en) * 2013-07-31 2015-07-22 南京理工大学 A millimeter-wave cone-beam antenna based on circular waveguide TM0n mode
CN103457034B (en) * 2013-09-05 2016-01-20 中国科学院光电技术研究所 Dual-frequency dual-circularly polarized antenna based on arc-shaped chiral artificial structure material
CN110336137B (en) * 2019-07-25 2021-07-27 东南大学 A kind of impedance matching high gain lens antenna and design method thereof
CN110661103A (en) * 2019-10-15 2020-01-07 中国人民解放军63686部队 An X-band low grating lobe circularly polarized antenna

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040008145A1 (en) * 2002-07-11 2004-01-15 Harris Corporation Spatial filtering surface operative with antenna aperture for modifying aperture electric field
CN101272004A (en) * 2008-04-17 2008-09-24 中国科学院光电技术研究所 A Design Method of Horn Antenna with Metal Grid Structure

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040008145A1 (en) * 2002-07-11 2004-01-15 Harris Corporation Spatial filtering surface operative with antenna aperture for modifying aperture electric field
CN101272004A (en) * 2008-04-17 2008-09-24 中国科学院光电技术研究所 A Design Method of Horn Antenna with Metal Grid Structure

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
A broadband metamaterial cylindrical lens antenna;Ma HuiFeng et al.;《Chinese Science Bulletin》;20100731;第55卷(第19期);第2067页左栏第12-14行,图1、7 *
Ma HuiFeng et al..A broadband metamaterial cylindrical lens antenna.《Chinese Science Bulletin》.2010,第55卷(第19期),第2067页左栏第12-14行,图1、7.
Planar Reflector Antenna Design Based on Gradient-index Metamaterials;Wei Xiang Jiang et al.;《Microwave and Millimeter Wave Technology (ICMMT), 2010 International Conference on》;20101231;第431页右栏第1-2行,第432页左栏第41行,右栏第4-8行,公式4,图1(a) *
Wei Xiang Jiang et al..Planar Reflector Antenna Design Based on Gradient-index Metamaterials.《Microwave and Millimeter Wave Technology (ICMMT), 2010 International Conference on》.2010,第431页右栏第1-2行,第432页左栏第41行,右栏第4-8行,公式4,图1(a).

Also Published As

Publication number Publication date
CN102110890A (en) 2011-06-29

Similar Documents

Publication Publication Date Title
CN102110890B (en) High-gain horn antenna based on non-uniform medium
CN108738290B (en) A metamaterial wave absorber and design method
EP3021416A1 (en) Antenna
CN107871934B (en) Two-dimensional luneberg lens based on electromagnetic resonator
CN102081690B (en) MDA (Matrix Decomposition Algorithm)-combined novel SVD (Singular Value Decomposition) method for complex circuit
CN102723541A (en) Method for optimizing cross-shaped annular slot frequency selection surface unit structural body and conformal antenna housing with low radar cross-section (RCS)
CN102354812A (en) Micro-strip antenna housing with high gain
CN102708229A (en) Matrix decomposition and novel singular value decomposition combined method for complex layered medium structures
CN108539393B (en) Horizontal polarization holographic antenna of high-aperture efficiency pencil-shaped wave beam
CN103022033A (en) Array substrate, manufacture method and display device
CN106294894B (en) Finite Element Boundary Integral Method for Rapid Analysis of Electromagnetic Scattering Characteristics of Inhomogeneous Targets
CN104198032A (en) Rectangular opening sound transmission rate and sound transmission loss computing method
CN204948613U (en) Side-surrounding heat pipe and heat dissipation structure thereof
CN104767009A (en) A waveguide integrated artificial surface plasmon device and a filter integrated waveguide substrate
CN115392079A (en) A Calculation Method of Uniform Waveguide Mode Based on Complete Vector Finite Element
CN204243210U (en) patch antenna
CN105486948A (en) A method for rapidly extracting antenna-radome system electric performance parameters
CN104218296B (en) A kind of waveguide based on multi-sheet printed technology and preparation method thereof
WO2012155475A1 (en) Electromagnetic wave beam splitter
CN107220212A (en) A kind of boundary Element method of two-dimentional non-compact border sound scattering
CN106058445B (en) A kind of broadband transmission array antenna based on three-layer metal plate
CN106683402A (en) Road monitoring capture device
CN114465018A (en) A Broadband Omnidirectional Matching Absorber Plate Based on Inhomogeneous Meta-Elements
CN202855893U (en) Left-handed material based X-waveband dual-band dielectric resonator antenna
CN216600205U (en) Circuit board with optical locating point

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20131030

Termination date: 20150211

EXPY Termination of patent right or utility model