CN208062255U - A kind of adjustable absorber of graphene - Google Patents
A kind of adjustable absorber of graphene Download PDFInfo
- Publication number
- CN208062255U CN208062255U CN201820431894.3U CN201820431894U CN208062255U CN 208062255 U CN208062255 U CN 208062255U CN 201820431894 U CN201820431894 U CN 201820431894U CN 208062255 U CN208062255 U CN 208062255U
- Authority
- CN
- China
- Prior art keywords
- graphene
- layer
- column
- upper layer
- layer graphene
- 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
Links
Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
The utility model discloses a kind of adjustable absorbers of graphene.It includes lower layer graphene, and dielectric layer, intersects column, upper layer graphene at middle layer graphene;The upper layer of lower layer graphene is dielectric layer, the upper layer of dielectric layer is middle layer graphene, and the upper layer of middle layer graphene is to intersect column, and the upper layer for intersecting column is upper layer graphene, by adding the fermi level of bias voltage adjustment graphene layer, the tuning of THz wave absorption peak is realized.The utility model has compact-sized novel, absorptivity height, control principle simple.
Description
Technical field
The utility model is related to absorber more particularly to a kind of adjustable absorbers of graphene.
Background technology
In recent years, as the THz wave developed on connection electromagnetic spectrum between quite ripe millimeter wave and infrared light
A undoubtedly brand-new research field all hides huge value in all respects.THz wave 0.1~10THz of frequency,
Respective wavelength is 0.03mm~3mm.For a long time, it is generated and detection method due to lacking effective THz wave, and it is traditional
Microwave technology compares with optical technology, and people are very few to the understanding of the wave band properties of electromagnetic radiation, so that the wave band becomes
Terahertz gap in electromagnetic spectrum.With the breakthrough in terahertz emission source and Detection Techniques, the unique superior spy of Terahertz
Property be found and material science, detection of gas, biology and medicine detection, communication etc. show huge application prospect.
It may be said that Terahertz Technology science is not only the important foundation problem in scientific technological advance, but be generation information industry and
The great demand of basic science development.Terahertz system is mainly made of radiation source, sensitive detection parts and various functions device.Its
In, absorber just plays key player.
The current THz wave absorber studied both at home and abroad is mainly to be realized by designing different geometric parameter structures
Adjustable function limits the flexible Application function of absorber in this way, and cost is higher.It can flexible modulation so design is a kind of
The absorber of THz wave absorption peak is very important.For disadvantage mentioned above, the utility model proposes a kind of bias voltage to adjust
The absorber of absorption peak frequency is saved, compact-sized novel, absorptivity height, control principle are simple.
Invention content
The utility model provides a kind of adjustable absorber of graphene, and technical solution is as follows:
Graphene is adjustable, and absorber includes lower layer graphene, and dielectric layer, intersects column, upper layer graphene at middle layer graphene;Under
The upper layer of layer graphene is dielectric layer, and the upper layer of dielectric layer is middle layer graphene, and the upper layer of middle layer graphene is to intersect column, is intersected
The upper layer of column is upper layer graphene.
Based on said program, following preferred embodiment can be further used:
The length of the lower layer graphene be 60 μm~64 μm, width be 60 μm~64 μm, thickness be 0.34nm~
0.35nm.The dielectric layer material is silicon, and length is 60 μm~64 μm, and width is 60 μm~64 μm, is highly 30 μm~32
μm.The middle layer graphene length and width is all 60 μm~64 μm, and thickness is 0.34nm~0.35nm, the middle part subtracted
Divide geometry sizes identical as column is intersected.The intersection column material is silicon, and it is identical by two geometries to intersect column
Rectangle intersect vertically, rectangular length be 56 μm~60 μm, width be 15 μm~17 μm, highly for 35 μm~
37μm.The upper layer graphene 1, which is completely covered on, to intersect on column, and thickness is 0.34nm~0.35nm.By adding bias voltage
The fermi level of graphene layer is adjusted, realizes the tuning of THz wave absorption peak.The present invention has compact-sized novel, absorptivity
High, the advantages that control principle is simple.
Description of the drawings
Fig. 1 is the tomograph of the adjustable absorber of graphene;
Fig. 2 is the middle layer graphene vertical view of the adjustable absorber of graphene;
Fig. 3 is the adjustable absorber of graphene in initial resonant frequency 0.4THz distribution map of the electric field;
Fig. 4 is the performance chart of the adjustable absorber of graphene.
Specific implementation mode
As shown in Figure 1, the adjustable absorber of graphene includes lower layer graphene 5, dielectric layer 4, intersects column at middle layer graphene 3
2, upper layer graphene 1;The upper layer of lower layer graphene 5 is dielectric layer 4, and the upper layer of dielectric layer 4 is middle layer graphene 3, middle level graphite
The upper layer of alkene 3 is to intersect column 2, and the upper layer for intersecting column 2 is upper layer graphene 1.
5 length of lower layer graphene be 60 μm~64 μm, width be 60 μm~64 μm, thickness be 0.34nm~
0.35nm.4 material of dielectric layer be silicon, length be 60 μm~64 μm, width be 60 μm~64 μm, highly for 30 μm~
32μm.3 length and width of middle layer graphene is all 60 μm~64 μm, and thickness is 0.34nm~0.35nm, in subtracting
Between partial geometry shape size it is identical as column 2 is intersected.2 material of intersection column is silicon, and it is complete by two geometries to intersect column 2
Exactly the same rectangle intersects vertically, and rectangular length is 56 μm~60 μm, and width is 15 μm~17 μm, is highly 35
μm~37 μm.The upper layer graphene 1, which is completely covered on, to intersect on column 2, and thickness is 0.34nm~0.35nm.
Embodiment 1
Graphene is adjustable absorber:
In the present embodiment, the structure and each component shape of graphene is adjustable absorber as described above, therefore repeat no more, but
The design parameter of each component is as follows:The length of lower layer graphene is 64 μm, and width is 64 μm, thickness 0.35nm.Dielectric layer material
Material is silicon, and length is 64 μm, and width is 64 μm, is highly 32 μm.Middle layer graphene degree is 64 μm, and width is 64 μm, and thickness is
0.35nm.Intersection column material is silicon, intersects column and is intersected vertically by two identical rectangles of geometry, rectangle
Length be 60 μm, width be 17 μm, be highly 37 μm.Upper layer graphene, which is completely covered on, to intersect on column, thickness 0.35nm.
The property indices of graphene is adjustable absorber are tested using COMSOL Multiphysics softwares, and Fig. 4 is graphene
The performance chart of adjustable absorber, it can be seen that when graphene fermi level is in 0.3eV, the absorption peak of absorber is located at
Frequency is absorptivity 0.998 at 0.4THz;When fermi level reaches 0.6eV, 0.9eV, the absorption peak of absorber distinguishes position
At Frequency point 0.5THz, 0.6THz, corresponding absorptivity is 0.998,0.999, realizes absorption frequency point adjustable function.
Claims (6)
1. a kind of adjustable absorber of graphene, it is characterised in that it includes lower layer graphene (5), dielectric layer (4), middle layer graphene
(3), intersect column (2), upper layer graphene (1);The upper layer of lower layer graphene (5) is dielectric layer (4), and the upper layer of dielectric layer (4) is
Middle layer graphene (3), the upper layer of middle layer graphene (3) are to intersect column (2), and the upper layer for intersecting column (2) is upper layer graphene (1).
2. a kind of adjustable absorber of graphene as described in claim 1, it is characterised in that the length of the lower layer graphene (5)
Degree is 60 μm~64 μm, and width is 60 μm~64 μm, and thickness is 0.34nm~0.35nm.
3. a kind of adjustable absorber of graphene as described in claim 1, it is characterised in that described dielectric layer (4) material is
Silicon, length are 60 μm~64 μm, and width is 60 μm~64 μm, is highly 30 μm~32 μm.
4. a kind of adjustable absorber of graphene as described in claim 1, it is characterised in that the length of the middle layer graphene (3)
Degree and width all be 60 μm~64 μm, thickness be 0.34nm~0.35nm, the middle section geometry sizes subtracted with intersect
Column (2) is identical.
5. a kind of adjustable absorber of graphene as described in claim 1, it is characterised in that described intersection column (2) material is
Silicon intersects column (2) and is intersected vertically by two identical rectangles of geometry, and rectangular length is 56 μm~60
μm, width is 15 μm~17 μm, is highly 35 μm~37 μm.
6. a kind of adjustable absorber of graphene as described in claim 1, it is characterised in that the upper layer graphene (1) is complete
It is covered in and intersects on column (2), thickness is 0.34nm~0.35nm.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201820431894.3U CN208062255U (en) | 2018-03-28 | 2018-03-28 | A kind of adjustable absorber of graphene |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201820431894.3U CN208062255U (en) | 2018-03-28 | 2018-03-28 | A kind of adjustable absorber of graphene |
Publications (1)
Publication Number | Publication Date |
---|---|
CN208062255U true CN208062255U (en) | 2018-11-06 |
Family
ID=63987463
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201820431894.3U Expired - Fee Related CN208062255U (en) | 2018-03-28 | 2018-03-28 | A kind of adjustable absorber of graphene |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN208062255U (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109638471A (en) * | 2018-12-14 | 2019-04-16 | 电子科技大学 | A kind of adjustable two frequency ranges THz absorber based on Fermi's dirac material |
CN116111364A (en) * | 2023-03-28 | 2023-05-12 | 南昌大学 | Ultra-wideband coherent perfect absorber with terahertz wave band based on graphene super surface |
-
2018
- 2018-03-28 CN CN201820431894.3U patent/CN208062255U/en not_active Expired - Fee Related
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109638471A (en) * | 2018-12-14 | 2019-04-16 | 电子科技大学 | A kind of adjustable two frequency ranges THz absorber based on Fermi's dirac material |
CN109638471B (en) * | 2018-12-14 | 2021-01-29 | 电子科技大学 | Adjustable two-frequency-band THz absorber based on Fermi Dirac material |
CN116111364A (en) * | 2023-03-28 | 2023-05-12 | 南昌大学 | Ultra-wideband coherent perfect absorber with terahertz wave band based on graphene super surface |
CN116111364B (en) * | 2023-03-28 | 2024-03-29 | 南昌大学 | Ultra-wideband coherent perfect absorber with terahertz wave band based on graphene super surface |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN207281413U (en) | A kind of terahertz light gate device based on graphene Meta Materials | |
CN108336503A (en) | A kind of graphene electricity tune THz wave absorber | |
CN208062255U (en) | A kind of adjustable absorber of graphene | |
Li et al. | Radiation-pattern-reconfigurable graphene leaky-wave antenna at terahertz band based on dielectric grating structure | |
CN108646325B (en) | A kind of adjustable graphene wide angle Terahertz wave absorbing device of frequency | |
Manuilov et al. | Electron-optical systems for planar gyrotrons | |
CN108963468A (en) | Dual openings ring Terahertz is adjustable absorber | |
CN107942538A (en) | Automatically controlled THz wave amplitude controller | |
Chen et al. | Recent progress in graphene terahertz modulators | |
Mencarelli et al. | Spatial dispersion effects upon local excitation of extrinsic plasmons in a graphene micro-disk | |
CN205691892U (en) | Based on the adjustable terahertz wave attenuator of molybdenum disulfide film structure | |
CN107908020A (en) | Based on infrared phasmon waveguide modulator in graphene | |
CN207587977U (en) | Double frequency Terahertz absorber based on graphene | |
Wu et al. | A dynamically tunable and wide-angle terahertz absorber based on graphene-dielectric grating | |
Li et al. | Study of the electric field enhancement in resonant metasurfaces | |
Ji et al. | Increasing the electrical conductivity of poly (vinylidene fluoride) by KrF excimer laser irradiation | |
CN207611869U (en) | A kind of broadband Terahertz wave absorbing device based on double trapezoid graphene | |
Huang et al. | Terahertz graphene modulator based on hybrid plasmonic waveguide | |
Xia et al. | Dynamically tuning the optical coupling of surface plasmons in coplanar graphene nanoribbons | |
Cai et al. | Optical properties of strontium titanate by ab initio calculation within density functional theory | |
Lin et al. | Optimization of double-layer graphene plasmonic waveguides | |
Xi et al. | An effective CFS-PML implementation for 2-D WLP-FDTD method | |
CN108572491B (en) | Device and method for generating dispersive Cerenkov radiation | |
Xie | Linear and nonlinear optical properties of anisotropic quantum dots in a magnetic field | |
CN105892102A (en) | Terahertz-wave-transmission-type modulator based on graphene |
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: 20181106 Termination date: 20190328 |