CN209526207U - The control of micro- band beams and polarization changer based on graphene - Google Patents

The control of micro- band beams and polarization changer based on graphene Download PDF

Info

Publication number
CN209526207U
CN209526207U CN201920330673.1U CN201920330673U CN209526207U CN 209526207 U CN209526207 U CN 209526207U CN 201920330673 U CN201920330673 U CN 201920330673U CN 209526207 U CN209526207 U CN 209526207U
Authority
CN
China
Prior art keywords
graphene
band
control
micro
polarization changer
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
CN201920330673.1U
Other languages
Chinese (zh)
Inventor
陆卫兵
陈昊
刘震国
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.)
Southeast University
Original Assignee
Southeast University
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 Southeast University filed Critical Southeast University
Priority to CN201920330673.1U priority Critical patent/CN209526207U/en
Application granted granted Critical
Publication of CN209526207U publication Critical patent/CN209526207U/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Carbon And Carbon Compounds (AREA)

Abstract

The utility model discloses a kind of microwave section beam-controller and polarization changer based on graphene, belongs to microwave device technology field, graphene band is arranged on PVC substrate in PVC substrate, FR4 medium and the metal base plate from top to bottom set gradually;Graphene band includes single-layer graphene band and multi-layer graphene band.Micro- band beams based on graphene of the utility model control and polarization changer structure is simple, the sheet resistance of graphene can be applied different voltage by DC voltage source to it and be controlled, static method is utilized in the utility model, i.e., grows the graphene of respective impedance directly to verify to design.The utility model concrete function includes direction controlling and convert the polarized state of reflected beam to reflected beam, application, the application for graphene in microwave section such as can be used for orienting, is stealthy and having sprawled road.

Description

The control of micro- band beams and polarization changer based on graphene
Technical field
The utility model belongs to microwave device technology field, is related to the control of micro- band beams and polarization based on graphene and becomes Parallel operation.
Background technique
Beam direction control and the transformation of wave beam polarization state are either in the basic research of electromagnetism still in electromagnetic device skill It is all critically important project in terms of art, in fields such as reflector antenna, beam formed antenna, satellite communication, mobile communications Suffer from important application.From the perspective of electromagnetism, beam direction control and the transformation of wave beam polarization state are had relied on pair The control of electromagnetic wave phase.
In recent years, with the development on Meta Materials and super surface, people have completely new means to the phase controlling of electromagnetic wave, Device based on phase controlling also flourishes accordingly.As a kind of two-dimensional Meta Materials, super surface has lightweight, easily Physical characteristic, it is often more important that, expected from people can be obtained by the change of the parameters such as shape, size to sub-wavelength unit Reflection or transmission phase value, and then by different array arrangements, form various functional devices.Traditional is pasted based on metal Once fixed, function also determines the Meta Materials shape of piece therewith, lacks tunable characteristic and restructural characteristic.
In order to solve this drawback, Adjustable Diode is widely used among the phase controlling in super surface to electromagnetic wave, and And it is applied to beam direction control (T.J.Cui, M.Q.Qi, X.Wan, J.Zhao, and Q.Cheng, " Coding metamaterials,digital metamaterials and programmable metamaterials,”Light Sci.Appl., vol.3, p.e218,2014.), wave beam polarization state transformation (Fern á ndez, O., G ó mez,Vegas,A., Molina-Cuberos,G.J.,&Barba,I.“Diode switchable chiral metamaterial structure Forpolarization manipulation, " 2017IEEE MTT-S InternationalConference179,2017) Equal fields.However, the device based on Adjustable Diode exists, welding is complicated, and the numerous disadvantage of feeder line is caused to its practical application It is inconvenient.
Graphene starts the brand-new material of development for 2004 as one kind, in mechanics, electricity, optics, biochemistry etc. Aspect shows outstanding performance, such as has most fast electron mobility (15000cm2/v/cm), superelevation not temperature controlled Charge carrier mobility (200000cm2/v/s) and efficient Fermi velocity (106m/s) close to the light velocity.Graphene is also Fabulous mechanical performance, Young's modulus 1.0TPa, in addition, it there are also fabulous electron conductivity and flexibilities.
Exactly because these properties of graphene, vast researcher give high attention rate.By more than ten The development in year, existing Many researchers will carry out phase controlling to electromagnetic wave using graphene, and then reach beam direction tune Control (T.Yatooshi, A.Ishikawa, and K.Tsuruta, " Terahertz wavefront control bytunablemetasurface made of graphene ribbons,”Appl.Phys.Lett.,vol.3,no.5, Pp.788,2015) and polarization state converts (Yu X., Gao X., Qiao W., et al.Broadband Tunable PolarizationConverter Realized by Graphene-Based Metamaterial,IEEEPhotonics Technol.Lett.28,2399,2016), but these work are based on theory, and in the majority with Terahertz frequency range.And lead at present The common microwave section of letter technology, the work for carrying out phase controlling using graphene is seldom, to find out its cause, graphene is in microwave section Characteristic is equivalent to one layer of adjustable resistive film, the imaginary part very little of impedance, it is difficult to generate high-amplitude and phase change is abundant anti- Characteristic is penetrated, therefore, it is necessary to carry out patterned process to graphene, so as to " the equivalent imaginary part " of acquisition;In addition, microwave section application is wanted Ask the size of graphene larger, the growth of large-area graphene just becomes the difficult point for hindering its practical application with patterning.2018 Year, this seminar is in (Chen H., Lu W.B., Liu Z.G., Zhang J., Zhang A.Q., Wu B.Experimental Demonstration of Microwave Absorber Using Largearea Multilayer-Graphene based Frequency Selective Surface, IEEETrans.Microw.Theory Tech., 66,3087,2018) in work It solves the problems, such as that large-area graphene is patterned, provides possibility to carry out phase controlling in microwave section using graphene.
Utility model content
Purpose of utility model: the purpose of this utility model is to provide the controls of micro- band beams and polarization based on graphene Converter relies on large-area graphene patterning techniques, using graphene band, from theory to experimentally demonstrating graphene A possibility that microwave section carries out beam direction control and wave beam polarization conversion, beaten for graphene in the large-scale application of microwave section Solid foundation is descended.
Technical solution: in order to realize above-mentioned purpose of utility model, the utility model adopts the following technical solution:
Based on graphene micro- band beams control and polarization changer, including from top to bottom set gradually PVC substrate, Graphene band is arranged on the PVC substrate in FR4 medium and metal base plate;The graphene band includes single layer stone Black alkene band and multi-layer graphene band.
Further, the PVC substrate with a thickness of 70 μm, relative dielectric constant 3.5.
Further, the relative dielectric constant of the FR4 medium is 4.4, with a thickness of 3mm.
Further, the graphene band is a kind of periodic structure, structural cycle 7mm.
Further, the single-layer graphene band and multi-layer graphene band are arranged at intervals on PVC substrate.
Further, when micro- band beams control and polarization changer are used as the direction of control reflected beam, graphite The width of alkene band (single-layer graphene band and multi-layer graphene band) is 2.1mm;When micro- band beams control and polarization When converter is used as the polarized state for changing reflected beam, graphene band (single-layer graphene band and multi-layer graphene band) Width be set to 3.5mm.When the graphene strips bandwidth is 2.1mm, the beam scanning function of different angle is realized;When When the graphene strips bandwidth is 3.5mm, the function of wave beam polarized state transformation is realized.
The utility model has the advantages that compared with prior art, the control of micro- band beams and polarization based on graphene of the utility model Transformer configuration is simple, and the sheet resistance of graphene can be applied different voltage by DC voltage source to it and be controlled, directly The graphene of respective impedance is grown to verify to design.The utility model concrete function includes to reflected beam progress side To control and the polarized state of reflected beam is converted, the application such as can be used for orienting, is stealthy, is graphene in microwave section Using having sprawled road.
Detailed description of the invention
Fig. 1 is the control of micro- band beams and polarization changer structural schematic diagram based on graphene;
Fig. 2 is the control of micro- band beams and polarization changer unit top view based on graphene;
Fig. 3 be device as beam-controller when, the reflected phase characteristics of structural unit;
Fig. 4 be device as beam-controller when, array structure reflecting lobes distribution emulation and test result;
Fig. 5 be device as polarization changer when, the reflected phase characteristics of structural unit;
Fig. 6 be device as polarization changer when, the emulation and test result of the back wave polarized state of array structure.
Specific embodiment
The structure of the utility model and performance are described further with reference to the accompanying drawing.
As shown in figures 1 to 6, appended drawing reference are as follows: single-layer graphene band 1, multi-layer graphene band 2, PVC substrate 3, FR4 are situated between Matter 4, metal base plate 5 and graphene band 6.
The control of micro- band beams and polarization changer based on graphene, including the PVC substrate from top to bottom set gradually 3, graphene band 6 is arranged in FR4 medium 4 and metal base plate 5 on PVC substrate 3;Graphene band 6 includes single-layer graphene item Band 1 and multi-layer graphene band 2.
PVC substrate 3 with a thickness of 70 μm, relative dielectric constant 3.5.The relative dielectric constant of FR4 medium 4 is 4.4, thick Degree is 3mm.Graphene band 6 is a kind of periodic structure, structural cycle 7mm.Single-layer graphene band 1 and Multi-layer graphite Alkene band 2 is arranged at intervals on PVC substrate 3.
When micro- band beams control and polarization changer are used as the direction of control reflected beam, graphene band 6 Width is 2.1mm;When micro- band beams control and polarization changer are used as the polarized state for changing reflected beam, graphene The width of band 6 is set to 3.5mm.
The preparation method of the control of micro- band beams and polarization changer based on graphene, includes the following steps:
1) using matlab and equivalent circuit theory to graphene band, PVC substrate 3, FR4 medium 4, metal base plate 5 into Row modeling, by parameter scanning, optimization obtains the strip width value and band sheet resistance value of best performance.The result shows that working as graphite When alkene strip width is 2.1mm, institute's utility model device has good wave beam control function, and graphene strips bandwidth is When 3.5mm, institute's utility model device has the function of good polarization conversion;
2) designed model is modeled using business software CST, simulates the characteristic of array;
3) processing preparation is carried out to array designed by above step, and tests its performance;
It, can be by graphene band 6 (single-layer graphene band 1, multilayer according to the difference in incidence wave direction in step 1) Graphene band 2) it is equivalent to connecting for resistance and inductance or connecting for resistance and capacitor, equivalent resistance, inductance, capacitor Formula can be found in (Luukkonen O, Simovski C, Granet G, Simple and accurate analytical model of planar grids and high-impedance surfaces comprising metal strips or Patches.IEEE Trans.Antennas Propag.56,1624,2008.) and (Costa, F., Monorchio, A., & Manara,G.Analysis and design of ultrathin electromagnetic absorbers comprising resistively loaded high impedance surfaces,IEEE Trans.Antennas Propag.58,1551,2010.).Remaining component, including PVC substrate 3, FR4 medium 4, metal base plate 5 can be with respective Standard transmission line model characterizes;
In step 2), what the emulation of array was used is time-domain simulation method, graphene band 6 (single-layer graphene band 1, Multi-layer graphene band 2) it is simulated with the impedance boundary condition of zero thickness, the sheet resistance of graphene is set as 5 Ω/sq and 2000 Ω/sq is open boundary to the boundary condition that model applies.When artificial reflections beam direction and reflected beam polarized state, add Add far field probe;
In step 3), single-layer graphene band 1 is grown using copper foil, and multi-layer graphene band 2 is grown using nickel foil, Growing method is CVD method, and after growth, graphene band 6 is transferred on PVC3;Finally, the PVC that graphene band 6 will be had Substrate 3 fits on 4 plate of FR4 medium of metal base plate 5 (copper bottom).
Fig. 1 is microwave section beam-controller and polarization changer structural schematic diagram based on graphene.Single-layer graphene item It is indicated respectively with different patterns with 1 and multi-layer graphene band 2.In order to facilitate differentiation, in figure, we are by different levels Spacing structure has gone out certain distance, in fact, graphene band 6 (single-layer graphene band 1, multi-layer graphene band 2) and PVC Substrate 3, FR4 medium 4, metal base plate 5 fit closely together.
Fig. 2 is microwave section beam-controller and polarization changer unit top view based on graphene, wherein the week of unit Phase is 7mm, and the width of graphene band 6 is depending on its function.When the device is used as the direction of control reflected beam, graphene The width of band 6 is set to 2.1mm, and when the device is used as the polarized state for changing reflected beam, the width of graphene band 6 is fixed For 3.5mm.
Fig. 3 be institute's utility model device as beam-controller when, the reflected phase characteristics of structural unit, at this point, addition The direction of an electric field that is actuated to polarize along band.It can be seen from the figure that the sheet resistance when graphene is respectively 5 Ω/sq and 2000 When Ω/sq, the reflected phase of the two reaches 180 ° in 13GHz, is based on this, we carry out different arrays using both units Arrangement, it is hereby achieved that different reflected beam directions.
Fig. 4 be institute's utility model device as beam-controller when, Fig. 4 (a) and Fig. 4 (b) are the anti-of array structure respectively The emulation and test result of ejected wave valve distribution.For convenience of description, array as shown in Figure 1 be two multi-layer graphene bands 2, two Single-layer graphene band 1 distributes alternately, and is denoted as (N=2).And so on, in Fig. 4, emulate and test (N=4) and (N=2) Situation, it can be seen that emulation and the main lobe direction of reflected beam tested have changed to 55.5 ° from 24.3 °.Fig. 3 and Fig. 4 Result embody the good reflected beam direction controlling ability of institute's utility model device.
Fig. 5 be institute's utility model device as polarization changer when, the reflected phase characteristics of structural unit, the phase in figure What difference reflected is the difference reflected between wave phase under incident polarization respectively x- polarization and y- polarization.It can from figure Out, when the sheet resistance of graphene is 5 Ω/sq, phase difference can generate from less than 90 ° to being greater than 270 ° of traversal;And work as graphite The sheet resistance of alkene be 2000 Ω/sq when, phase difference almost keep 0 ° it is constant.
Fig. 6 be institute's utility model device as polarization changer when, the emulation of the back wave polarized state of array structure and Test result.It can be seen from the figure that the axis ratio of back wave is generated in 7GHz and 11GHz or so when graphene sheet resistance very little Minimum (<2dB), and generate a maximum (>40dB) in 9GHz or so, illustrates in these frequency points, and back wave is compared to entering Ejected wave, polarized state experienced from linear polarization to left-hand circular polarization, linear polarization to crossed linear polarization, linear polarization to right-handed circular polarization Transformation.When graphene sheet resistance is very big, the axis ratio of back wave remains at 20dB or more, in conjunction with the phase difference value in Fig. 5 It is found that back wave maintains the polarized state of incidence wave.It is good anti-that the result of Fig. 5 and Fig. 6 embodies institute's utility model device Ejected wave polarization state ability to transform.

Claims (6)

1. the control of micro- band beams and polarization changer based on graphene, it is characterised in that: including from top to bottom setting gradually PVC substrate (3), FR4 medium (4) and metal base plate (5), on the PVC substrate (3) be arranged graphene band (6);Institute The graphene band (6) stated includes single-layer graphene band (1) and multi-layer graphene band (2).
2. the control of micro- band beams and polarization changer according to claim 1 based on graphene, it is characterised in that: institute The PVC substrate (3) stated with a thickness of 70 μm, relative dielectric constant 3.5.
3. the control of micro- band beams and polarization changer according to claim 1 based on graphene, it is characterised in that: institute The relative dielectric constant for the FR4 medium (4) stated is 4.4, with a thickness of 3mm.
4. the control of micro- band beams and polarization changer according to claim 3 based on graphene, it is characterised in that: institute The graphene band (6) stated is a kind of periodic structure, structural cycle 7mm.
5. the control of micro- band beams and polarization changer according to claim 1 based on graphene, it is characterised in that: institute The single-layer graphene band (1) and multi-layer graphene band (2) stated are arranged at intervals on PVC substrate (3).
6. the control of micro- band beams and polarization changer according to claim 1 based on graphene, it is characterised in that: when When micro- band beams control and polarization changer are used as the direction of control reflected beam, the width of graphene band (6) is 2.1mm;When micro- band beams control and polarization changer are used as the polarized state for changing reflected beam, graphene band (6) width is set to 3.5mm.
CN201920330673.1U 2019-03-15 2019-03-15 The control of micro- band beams and polarization changer based on graphene Expired - Fee Related CN209526207U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201920330673.1U CN209526207U (en) 2019-03-15 2019-03-15 The control of micro- band beams and polarization changer based on graphene

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201920330673.1U CN209526207U (en) 2019-03-15 2019-03-15 The control of micro- band beams and polarization changer based on graphene

Publications (1)

Publication Number Publication Date
CN209526207U true CN209526207U (en) 2019-10-22

Family

ID=68231805

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201920330673.1U Expired - Fee Related CN209526207U (en) 2019-03-15 2019-03-15 The control of micro- band beams and polarization changer based on graphene

Country Status (1)

Country Link
CN (1) CN209526207U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109786965A (en) * 2019-03-15 2019-05-21 东南大学 The control of micro- band beams and polarization changer based on graphene and preparation method thereof

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109786965A (en) * 2019-03-15 2019-05-21 东南大学 The control of micro- band beams and polarization changer based on graphene and preparation method thereof
CN109786965B (en) * 2019-03-15 2024-05-07 东南大学 Microwave section beam control and polarization converter based on graphene and preparation method thereof

Similar Documents

Publication Publication Date Title
Chen et al. Experimental demonstration of microwave absorber using large-area multilayer graphene-based frequency selective surface
Li et al. Design of a tunable low-frequency and broadband radar absorber based on active frequency selective surface
Zhang et al. Weather-manipulated smart broadband electromagnetic metamaterials
CN109326889B (en) Frequency selection surface electromagnetic wave transmission amplitude modulator based on graphene
CN211123332U (en) Graphene-based broadband adjustable terahertz wave absorber
CN109786965A (en) The control of micro- band beams and polarization changer based on graphene and preparation method thereof
Wang et al. Dendritic wideband metamaterial absorber based on resistance film
CN209526207U (en) The control of micro- band beams and polarization changer based on graphene
CN110658571A (en) Graphene-based broadband adjustable terahertz wave absorber
Yang et al. Design and reflectivity analysis of high temperature wave-absorbing coatings with circular periodic structure
CN111755833A (en) Multi-band active metamaterial wave absorber
Xing et al. Wideband microwave absorber with dynamically tunable absorption based on graphene and random metasurface
CN110797665A (en) Graphene-based microwave band dynamic adjustable wave absorber and preparation method thereof
Chen et al. Full polarization transformation using graphene in microwave frequencies
CN210430118U (en) Microwave band dynamic adjustable wave absorber based on graphene
Dorrah et al. Pencil-beam single-point-fed Dirac leaky-wave antenna on a transmission-line grid
Pang et al. Dynamically controlling electromagnetic reflection using reconfigurable water-based metasurfaces
CN216928948U (en) Broadband adjustable absorber based on I-shaped hollow graphene
Zeng et al. Tunable and broadband radar absorber based on PIN diodes controllable FSS
CN114400455A (en) Based on VO2Phase-change temperature-control reconfigurable polarization converter
Xu et al. Radar absorbing material applied to precise RCS regulation of complex scatterer structure
Wei et al. Graphene-based active tunable metasurfaces for dynamic terahertz absorption and polarization conversion
Xie et al. An optically transparent broadband microwave absorber based on resistive frequency selective surface
He et al. An ultra-wideband metamaterial absorber with active frequency selective surface
CN116111364B (en) Ultra-wideband coherent perfect absorber with terahertz wave band based on graphene super surface

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20191022