CN103983364B - Metamaterial pixel structure and focal plane array imaging detector using same - Google Patents

Metamaterial pixel structure and focal plane array imaging detector using same Download PDF

Info

Publication number
CN103983364B
CN103983364B CN201410228063.2A CN201410228063A CN103983364B CN 103983364 B CN103983364 B CN 103983364B CN 201410228063 A CN201410228063 A CN 201410228063A CN 103983364 B CN103983364 B CN 103983364B
Authority
CN
China
Prior art keywords
meta materials
pixel structure
top layer
pixel
splitting ring
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
CN201410228063.2A
Other languages
Chinese (zh)
Other versions
CN103983364A (en
Inventor
龚诚
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to CN201410228063.2A priority Critical patent/CN103983364B/en
Publication of CN103983364A publication Critical patent/CN103983364A/en
Application granted granted Critical
Publication of CN103983364B publication Critical patent/CN103983364B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

The invention relates to a metamaterial pixel structure used for terahertz and millimeter wave detection and a focal plane array imaging detector using the metamaterial pixel structure. The metamaterial pixel structure comprises a top layer and a bottom layer. A resonator is formed on the top player and comprises at least one split ring set which is longitudinally arranged, each split ring is provided with a hollowed-out region which is exposed out of the bottom layer and is of a special shape, and therefore the top layer of the metamaterial pixel structure serves both as a micro reflecting mirror and the resonator to form the metamaterial pixel structure. Meanwhile, a double-material cantilever beam actuator is made of a top layer material and a bottom layer material. The focal plane array imaging detector comprises a focal plane array formed by periodically arranging a plurality of metamaterial pixel structures, the metamaterial pixel structures are arranged to form a metamaterial periodical structure, so that high-resolution imaging and high absorptivity of terahertz or millimeter waves are realized, and detection sensitivity is high.

Description

Meta Materials pixel structure and use its focal plane array image-forming detector
Technical field
The invention belongs to Terahertz (THz-Terahertz) and millimeter wave detection and technical field of imaging, it is related to a kind of super Material pixel structure, more particularly to a kind of Meta Materials pixel structure for Terahertz and millimeter wave detection and using this surpass The focal plane array image-forming detector of material pixel structure, is mainly used in non-refrigeration type Terahertz or millimeter wave realtime imaging In system.
Background technology
Terahertz and millimeter wave detection and imaging technique are in national defence, safety check, lossless detection, biologic medical, commercial production, base The fields such as plinth scientific research have a wide range of applications.At present, Meta Materials absorbing structure is applied to terahertz by correlational study both at home and abroad Hereby wave band, solves the problems, such as that terahertz imaging detector absorbance is low.For example:2010, Boston University Hu Tao et al. profit The ray machine sensor array for microwave and terahertz wave band with Meta Materials Design Theory, Meta Materials resonant ring is added double materials Material cantilever beam element;2013, USN graduate Fabio Alves et al. adopted SiOx and Al as bi-material layers cantilever The bi-material of beam, designs and has made the beam type terahertz detector based on Meta Materials;Application No. It is directed to employ in a kind of 201210250324 Chinese patent application " Terahertz focal plane arrays (FPA) based on MEMS technology " Meta Materials absorbing structure is as Terahertz absorbing structure layer.
But the metamaterial structure currently used for terahertz detection and the bi-material layers beam type terahertz imaging spy using it Survey device and be primarily present following shortcoming:1. each metamaterial structure is resonator it is impossible to execute as micro-reflector and cantilever beam Device;2. micro-reflector area is less, is unfavorable for optical read-out;3. the single pixel of detector is by multiple metamaterial modular construction groups Become, need extra addition micro-reflector and cantilever beam executor;4. between pixel and pixel, gap is big, and resolution is low;5. manufacture Complex process, relatively costly.
Content of the invention
In view of the foregoing it is proposed that the present invention is to provide a kind of Meta Materials picture overcoming disadvantages mentioned above at least in part Meta structure and the focal plane array image-forming detector using this Meta Materials pixel structure.
According to the first aspect of the invention, there is provided a kind of Meta Materials pixel structure, described Meta Materials pixel structure comprises Top layer and bottom, described top layer forms resonator, and described resonator includes longitudinally disposed least one set splitting ring, each of which Group splitting ring comprises a splitting ring, and each splitting ring includes exposing bottomShape void region, and onlyShape hollow out One end hollow out extending laterally outward in region goes out top layer.
According to the second aspect of the invention, there is provided a kind of Meta Materials pixel structure, described Meta Materials pixel structure comprises Top layer and bottom, described top layer forms resonator, and described resonator includes longitudinally disposed least one set splitting ring, each of which Group splitting ring comprises two laterally symmetrical back-to-back splitting rings, and each splitting ring includes exposing bottomShape void region, And onlyOne end hollow out extending laterally outward of shape void region goes out top layer, two divisions in each group of splitting ring RingThe vertical section of shape void region is near to form back-to-back symmetrical structure.
The Meta Materials pixel structure that first or second aspect according to the present invention provides, wherein, it is preferred that described resonator It is made up of two groups of longitudinally disposed splitting rings;The size being preferably located at one group of splitting ring of top is more than underlying one The size of group splitting ring.
According to the third aspect of the invention we, there is provided a kind of Meta Materials pixel structure, described Meta Materials pixel structure comprises Top layer and bottom, described top layer forms resonator, and described resonator includes a single splitting ring, and this splitting ring includes E word One end hollow out that the intermediate lateral part of shape void region, only E font void region stretches out goes out top layer, and E font The intermediate lateral part of void region exposes bottom, and other parts are together with bottom hollow out.
The Meta Materials pixel structure being provided according to any one in above-mentioned the first to the third aspect of the present invention, its In, it is preferred that the size of the described resonator being formed is 10 microns~120 microns;
It is preferred that the size of the described resonator being formed is 121 microns~1000 microns;
It is preferred that described top layer constitutes to form metal resonators by metal material, described bottom is by dielectric substance structure Become;
Preferably, described metal material is gold or aluminum, and described dielectric substance is silicon nitride or silicon dioxide.
Wherein, the top layer of metal material, both as micro-reflector, constitutes metamaterial structure, simultaneously by quilting material and bottom again Layer material constitutes bi-material layers cantilever beam executor.
According to the fourth aspect of the invention, there is provided a kind of focal plane array image-forming detector, this imaging detector comprises Press periodic arrangement group by multiple as any one the Meta Materials pixel structure providing in terms of the present invention first, second or third The focal plane arrays (FPA) becoming, wherein, multiple described Meta Materials pixel arrangement form Meta Materials periodic structures, the horizontal cycle is one and surpasses The length of material pixel, longitudinal cycle is the width of a Meta Materials pixel.
Compared with prior art, the Meta Materials pixel structure that the present invention provides is beneficial in that:1. each Meta Materials The top layer of pixel is both used for optical read-out as micro-reflector, and is used for absorbing electromagnetism spoke as resonator composition metamaterial structure Penetrate energy, bi-material layers cantilever beam executor is constituted by quilting material and primer simultaneously;2. micro-reflector area is big, beneficial to light Learn and read imaging.
The focal plane array image-forming detector that the present invention provides is beneficial in that:1. each pixel of such detector It is made up of single Meta Materials pixel, between pixel and pixel, gap is little, high resolution;2. it is capable of to THz wave or milli The high-absorbility of metric wave;3. pixel is sub-wavelength size, breaches the Terahertz or millimetre wavelength limit to object resolution System;4. such detector thickness is nanometer scale, has high detection sensitivity, is capable of high frame frequency Terahertz or millimeter wave Imaging.
Described above is only the general introduction of technical solution of the present invention, in order to better understand the technological means of the present invention, And can be practiced according to the content of description, and in order to allow the above and other objects of the present invention, feature and advantage can Become apparent, below especially exemplified by the specific embodiment of the present invention.
Brief description
Fig. 1 is the schematic diagram of the Meta Materials single band pixel structure of embodiment 1 description.
Fig. 2 is the schematic diagram of the resonator in the Meta Materials single band pixel structure of embodiment 1 description.
Fig. 3 is the schematic diagram of the focal plane arrays (FPA) being made up of multiple Meta Materials single band pixels of embodiment 1 description.
Fig. 4 is the schematic diagram of the Meta Materials two waveband pixel structure of embodiment 2 description.
Fig. 5 is the schematic diagram of the resonator in the Meta Materials two waveband pixel structure of embodiment 2 description.
Fig. 6 is the schematic diagram of the focal plane arrays (FPA) being made up of multiple Meta Materials two waveband pixels of embodiment 2 description.
Fig. 7 is the schematic diagram of the symmetric form Meta Materials single band pixel structure of embodiment 3 description.
Fig. 8 is the schematic diagram of the resonator of symmetric form Meta Materials single band pixel structure of embodiment 3 description.
Fig. 9 is the signal of the focal plane arrays (FPA) being made up of multiple symmetric form Meta Materials single band pixels of embodiment 3 description Figure.
Figure 10 is the schematic diagram of the symmetric form Meta Materials two waveband pixel structure of embodiment 4 description.
Figure 11 is the schematic diagram of the resonator of symmetric form Meta Materials two waveband pixel structure of embodiment 4 description.
Figure 12 is the signal of the focal plane arrays (FPA) being made up of multiple symmetric form Meta Materials two waveband pixels of embodiment 4 description Figure.
Figure 13 is the schematic diagram of the Meta Materials pixel structure of embodiment 5 description.
Figure 14 is the schematic diagram of the resonator in the Meta Materials pixel structure of embodiment 5 description.
Figure 15 is the schematic diagram of the focal plane arrays (FPA) being made up of multiple Meta Materials pixels of embodiment 5 description.
Specific embodiment
In order that technological means, creation characteristic, reached purpose and work(that those of ordinary skill in the art realize to the present invention Effect is easy to understand, and below in conjunction with the accompanying drawings, the present invention is expanded on further.
Embodiment 1:
A kind of Meta Materials single band pixel structure that Fig. 1 provides for the embodiment of the present invention 1, this Meta Materials single band pixel is tied Structure differs larger metal material by two kinds of thermal coefficient of expansions and dielectric substance is constituted, and metal material can be using gold or aluminum, electricity Dielectric material can adopt silicon nitride or silicon dioxide;This Meta Materials single band pixel structure comprises top layer 1 and bottom 2, and top layer 1 is Metal material, bottom 2 is dielectric substance, and metal material top layer 1 forms resonator, and Fig. 2 is that this Meta Materials single band pixel is tied The schematic diagram of the resonator in structure, described resonator includes one group of splitting ring, and this group splitting ring comprises a splitting ring 3, division Ring 3 includes exposing bottomShape void region, and onlyOne end hollow out extending laterally outward of shape void region goes out Top layer;Wherein, top layer 1 is both used for optical read-out as micro-reflector, and is used for as metal resonators composition metamaterial structure Absorption of electromagnetic radiation energy, constitutes bi-material layers cantilever beam executor by top layer 1 metal material and bottom 2 dielectric substance simultaneously. Metal resonators form Meta Materials absorber by periodic arrangement, produce strong resonance to incident electromagnetic wave, realize to specific list The high-absorbility of wave band electromagnetic radiation.Wherein, the size of the described resonator of formation can be 10 microns~120 microns, to be formed Absorb the Meta Materials absorbing structure of terahertz electromagnetic radiation;The size of the described resonator being formed is alternatively 121 microns~1000 Micron, to form the Meta Materials absorbing structure absorbing millimeter wave electromagnetic radiation.
Fig. 3 is the focal plane arrays (FPA) being made up of by periodic arrangement this Meta Materials single band pixel multiple, thus obtaining super material Material focal plane arrays (FPA) single band imaging detector, this imaging detector comprises this focal plane arrays (FPA), wherein, multiple Meta Materials unicasts Section pixel arrangement form Meta Materials periodic structure, the horizontal cycle is the length of a Meta Materials single band pixel, and longitudinal cycle is The width of one Meta Materials single band pixel, the silicon nitride material that connects through between each Meta Materials single band pixel is realized. This Meta Materials focal plane arrays (FPA) single band imaging detector bi-material layers cantilever after absorption of electromagnetic radiation, in Meta Materials pixel Beam temperature raises, and the bi-material thermal coefficient of expansion difference of composition cantilever beam is larger therefore to deflect, the size pair of amount of deflection Should be in the size of electromagnetic radiation energy;For two-dimensional focal plane array, the distribution of each pixel reflecting surface deflection angle just embodies The energy field distribution of target emanation, reads energy field distribution using optical meanss high-speed parallel, thus realizing real-time surface battle array Picture.
Embodiment 2:
A kind of Meta Materials two waveband pixel structure that Fig. 4 provides for the embodiment of the present invention 2, this Meta Materials two waveband pixel is tied Structure differs larger metal material by two kinds of thermal coefficient of expansions and dielectric substance is constituted, and metal material can be using gold or aluminum, electricity Dielectric material can adopt silicon nitride or silicon dioxide;This Meta Materials two waveband pixel structure comprises top layer 4 and bottom 5, and top layer 4 is Metal material, bottom 5 is dielectric substance, and metal material top layer 4 forms resonator, and Fig. 5 is that this Meta Materials two waveband pixel is tied The schematic diagram of the resonator in structure, described resonator includes longitudinally disposed two group splitting ring, and one group of division above The size of ring 6 is more than the size of underlying one group of splitting ring 7, and each group of splitting ring comprises a splitting ring, each division Ring includes exposing bottomShape void region, and onlyOne end hollow out extending laterally outward of shape void region goes out Top layer,;Wherein, top layer 4 is both used for optical read-out as micro-reflector, and is used for as metal resonators composition metamaterial structure Absorption of electromagnetic radiation energy, constitutes bi-material layers cantilever beam executor by top layer 4 metal material and bottom 5 dielectric substance simultaneously. Metal resonators form Meta Materials absorber by periodic arrangement, produce strong resonance to incident electromagnetic wave, realize to specific double The high-absorbility of wave band electromagnetic radiation.Wherein, the size of the described resonator of formation can be 10 microns~120 microns, to be formed Absorb the Meta Materials absorbing structure of terahertz electromagnetic radiation;The size of the described resonator being formed is alternatively 121 microns~1000 Micron, to form the Meta Materials absorbing structure absorbing millimeter wave electromagnetic radiation.
Fig. 6 is the focal plane arrays (FPA) being made up of by periodic arrangement this Meta Materials two waveband pixel multiple, thus obtaining super material Material focal plane arrays (FPA) dual-waveband imaging detector, this imaging detector comprises this focal plane arrays (FPA), wherein, multiple Meta Materials double waves Section pixel arrangement form Meta Materials periodic structure, the horizontal cycle is the length of a Meta Materials two waveband pixel, and longitudinal cycle is The width of one Meta Materials two waveband pixel, the silicon nitride material that connects through between each Meta Materials two waveband pixel is realized. This Meta Materials focal plane arrays (FPA) dual-waveband imaging detector bi-material layers cantilever after absorption of electromagnetic radiation, in Meta Materials pixel Beam temperature raises, and the bi-material thermal coefficient of expansion difference of composition cantilever beam is larger therefore to deflect, the size pair of amount of deflection Should be in the size of electromagnetic radiation energy;For two-dimensional focal plane array, the distribution of each pixel reflecting surface deflection angle just embodies The energy field distribution of target emanation, reads energy field distribution using optical meanss high-speed parallel, thus realizing real-time surface battle array Picture.
Embodiment 3:
A kind of symmetric form Meta Materials single band pixel structure that Fig. 7 provides for the embodiment of the present invention 3, this symmetric form Meta Materials Single band pixel structure differs larger metal material by two kinds of thermal coefficient of expansions and dielectric substance is constituted, and metal material can be adopted With gold or aluminum, dielectric substance can adopt silicon nitride or silicon dioxide;This symmetric form Meta Materials single band pixel structure comprises to push up Layer 8 and bottom 9, top layer 8 is metal material, and bottom 9 is dielectric substance, and metal material top layer 8 forms resonator, and Fig. 8 is should The schematic diagram of the resonator in symmetric form Meta Materials single band pixel structure, described resonator includes one group of splitting ring, this component Driffractive ring comprises laterally symmetrical back-to-back two splitting rings 10,11, and each splitting ring 10,11 includes exposing bottomShape hollow out Region, and onlyOne end hollow out extending laterally outward of shape void region goes out top layer, two points in this group splitting ring Driffractive ring 10,11The vertical section of shape void region is near to form back-to-back symmetrical structure;Wherein, top layer 8 is both as micro- anti- Penetrate mirror for optical read-out, and constitute metamaterial structure as metal resonators and be used for absorption of electromagnetic radiation energy, simultaneously by pushing up Layer 8 metal material and bottom 9 dielectric substance constitute bi-material layers cantilever beam executor.Metal resonators are formed by periodic arrangement Meta Materials absorber, produces strong resonance to incident electromagnetic wave, realizes the high-absorbility to specific single band electromagnetic radiation.Its In, the size of the described resonator of formation can be 10 microns~120 microns, to form the Meta Materials absorbing terahertz electromagnetic radiation Absorbing structure;The size of the described resonator being formed is alternatively 121 microns~1000 microns, absorbs millimeter wave electromagnetism spoke to be formed The Meta Materials absorbing structure penetrated.
Fig. 9 is the focal plane arrays (FPA) being made up of by periodic arrangement this symmetric form Meta Materials single band pixel multiple, thus To symmetric form Meta Materials focal plane arrays (FPA) single band imaging detector, this imaging detector comprises this focal plane arrays (FPA), wherein, many Individual symmetric form Meta Materials single band pixel arrangement form Meta Materials periodic structure, the horizontal cycle is a symmetric form Meta Materials unicast The length of section pixel, longitudinal cycle is the width of a symmetric form Meta Materials single band pixel, each symmetric form Meta Materials unicast The silicon nitride material that connects through between section pixel is realized.This symmetric form Meta Materials focal plane arrays (FPA) single band imaging detector exists After absorption of electromagnetic radiation, the bi-material layers cantilever beam temperature in Meta Materials pixel raises, and the bi-material heat constituting cantilever beam is swollen Swollen coefficient difference is larger therefore to deflect, and the size of amount of deflection corresponds to the size of electromagnetic radiation energy;Burnt flat for two dimension Face array, the distribution of each pixel reflecting surface deflection angle just embodies the energy field distribution of target emanation, using optical meanss High-speed parallel reads energy field distribution, thus realizing the imaging of real-time surface battle array.
Embodiment 4:
A kind of symmetric form Meta Materials two waveband pixel structure that Figure 10 provides for the embodiment of the present invention 4, the super material of this symmetric form Material two waveband pixel structure differs larger metal material by two kinds of thermal coefficient of expansions and dielectric substance is constituted, and metal material can Using gold or aluminum, dielectric substance can adopt silicon nitride or silicon dioxide;This symmetric form Meta Materials two waveband pixel structure comprises Top layer 12 and bottom 13, top layer 12 is metal material, and bottom 13 is dielectric substance, and metal material top layer 12 forms resonator, Figure 11 is the schematic diagram of the resonator in this symmetric form Meta Materials two waveband pixel structure, and described resonator includes longitudinally disposed Two groups of splitting rings, and the size of one group of splitting ring 14 and 15 above is more than underlying one group of splitting ring 16 and 17 Size, each of which group splitting ring comprises two laterally symmetrical back-to-back splitting rings, and each splitting ring includes exposing bottomShape void region, and onlyOne end hollow out extending laterally outward of shape void region goes out top layer, each group of splitting ring In two splitting ringsThe vertical section of shape void region is near to form back-to-back symmetrical structure;Wherein, top layer 12 was both made It is used for optical read-out for micro-reflector, and constitutes metamaterial structure as metal resonators being used for absorption of electromagnetic radiation energy, with When bi-material layers cantilever beam executor is constituted by top layer 12 metal material and bottom 13 dielectric substance.Metal resonators pass through the cycle Arrangement form Meta Materials absorber, produces strong resonance to incident electromagnetic wave, realizes the height suction to specific two waveband electromagnetic radiation Yield.Wherein, the size of the described resonator of formation can be 10 microns~120 microns, to form absorption terahertz electromagnetic radiation Meta Materials absorbing structure;The size of the described resonator being formed is alternatively 121 microns~1000 microns, to form absorption millimeter The Meta Materials absorbing structure of ripple electromagnetic radiation.
Figure 12 is the focal plane arrays (FPA) being made up of by periodic arrangement this symmetric form Meta Materials two waveband pixel multiple, thus To symmetric form Meta Materials focal plane arrays (FPA) dual-waveband imaging detector, this imaging detector comprises this focal plane arrays (FPA), wherein, many Individual symmetric form Meta Materials two waveband pixel arrangement form Meta Materials periodic structure, the horizontal cycle is a symmetric form Meta Materials double wave The length of section pixel, longitudinal cycle is the width of a symmetric form Meta Materials two waveband pixel, each symmetric form Meta Materials double wave The silicon nitride material that connects through between section pixel is realized.This symmetric form Meta Materials focal plane arrays (FPA) dual-waveband imaging detector exists After absorption of electromagnetic radiation, the bi-material layers cantilever beam temperature in Meta Materials pixel raises, and the bi-material heat constituting cantilever beam is swollen Swollen coefficient difference is larger therefore to deflect, and the size of amount of deflection corresponds to the size of electromagnetic radiation energy;Burnt flat for two dimension Face array, the distribution of each pixel reflecting surface deflection angle just embodies the energy field distribution of target emanation, using optical meanss High-speed parallel reads energy field distribution, thus realizing the imaging of real-time surface battle array.
In addition to each Meta Materials single band pixel structure that above-described embodiment provides and each Meta Materials two waveband pixel structure, Resonator in Meta Materials pixel structure also can be made up of multigroup splitting ring, thus obtaining Meta Materials multiband pixel structure, real The now absorption to specific multiband electromagnetic radiation, here is omitted.
Embodiment 5:
A kind of Meta Materials pixel structure that Figure 13 provides for the embodiment of the present invention 5, this Meta Materials pixel structure is by two kinds of heat The larger metal material of coefficient of expansion difference and dielectric substance are constituted, and metal material can be using gold or aluminum, and dielectric substance can Using silicon nitride or silicon dioxide;This Meta Materials pixel structure comprises top layer 18 and bottom 19, and top layer 18 is metal material, bottom 19 is dielectric substance, and metal material top layer 18 forms resonator, and Figure 14 is showing of the resonator in this Meta Materials pixel structure It is intended to, described resonator includes a single splitting ring 20, and this splitting ring 20 includes E font void region, and only E font is engraved One end hollow out that the intermediate lateral part of dummy section stretches out goes out top layer, and the intermediate lateral part of E font void region Expose bottom, other parts are together with bottom hollow out;Wherein, top layer 18 is both used for optical read-out as micro-reflector, makees again Constitute metamaterial structure for metal resonators and be used for absorption of electromagnetic radiation energy, simultaneously by top layer 18 metal material and bottom 19 electricity Dielectric material constitutes bi-material layers cantilever beam executor.Metal resonators form Meta Materials absorber by periodic arrangement, to incidence Electromagnetic wave produce strong resonance, realize high-absorbility to specific band electromagnetic radiation.Wherein, the chi of the described resonator of formation Very little be 10 microns~120 microns, with formed absorb terahertz electromagnetic radiation Meta Materials absorbing structure;The described resonance being formed The size of device is alternatively 121 microns~1000 microns, to form the Meta Materials absorbing structure absorbing millimeter wave electromagnetic radiation.
Figure 15 is the focal plane arrays (FPA) being made up of by periodic arrangement this Meta Materials pixel multiple, thus it is burnt flat to obtain Meta Materials Face array imaging detectors, this imaging detector comprises this focal plane arrays (FPA), wherein, the super material of multiple Meta Materials pixel arrangement form Material periodic structure, the horizontal cycle is the length of a Meta Materials pixel, and longitudinal cycle is the width of a Meta Materials pixel, each The silicon nitride material that connects through between Meta Materials pixel is realized.This Meta Materials focal plane array image-forming detector is absorbing electromagnetism After radiation, the bi-material layers cantilever beam temperature in Meta Materials pixel raises, and constitutes the bi-material thermal coefficient of expansion phase of cantilever beam Difference is larger therefore to deflect, and the size of amount of deflection corresponds to the size of electromagnetic radiation energy;For two-dimensional focal plane array, respectively The distribution of individual pixel reflecting surface deflection angle just embodies the energy field distribution of target emanation, is read using optical meanss high-speed parallel Go out energy field distribution, thus realizing the imaging of real-time surface battle array.
The foregoing describe ultimate principle and principal character and the advantage of the present invention.Those of ordinary skill in the art should Solution, the present invention is not restricted to the described embodiments, merely illustrating the principles of the invention described in above-described embodiment and description, Without departing from the spirit and scope of the present invention, the present invention also has various changes and modifications, and these changes and improvements are all Fall in scope of the claimed invention.Claimed scope is by appending claims and its equivalent circle. Fixed.

Claims (10)

1. a kind of Meta Materials pixel structure, comprises top layer and bottom it is characterised in that described top layer forms resonator, described humorous The device that shakes includes longitudinally disposed least one set splitting ring, and each of which group splitting ring comprises a splitting ring, each splitting ring bag Include and expose bottomShape void region, and onlyOne end hollow out extending laterally outward of shape void region goes out top layer.
2. a kind of Meta Materials pixel structure, comprises top layer and bottom it is characterised in that described top layer forms resonator, described humorous The device that shakes includes longitudinally disposed least one set splitting ring, and each of which group splitting ring comprises two laterally symmetrical back-to-back divisions Ring, each splitting ring includes exposing bottomShape void region, and onlyThe extending laterally outward of shape void region One end hollow out goes out top layer, two splitting rings in each group of splitting ringThe vertical section of shape void region leans against near to be formed Back of the body symmetrical structure.
3. Meta Materials pixel structure as claimed in claim 1 or 2, described resonator is by two groups of longitudinally disposed splitting ring groups Become.
4. Meta Materials pixel structure as claimed in claim 3, wherein, the size of one group of splitting ring above is more than and is located at The size of one group of splitting ring of lower section.
5. a kind of Meta Materials pixel structure, comprises top layer and bottom it is characterised in that described top layer forms resonator, described humorous The device that shakes includes a single splitting ring, and this splitting ring includes E font void region, and only E font void region is middle horizontal Go out top layer to one end hollow out that part stretches out, and the intermediate lateral part of E font void region exposes bottom, this E word The vertical section of the upside lateral part, downside lateral part and left side of shape void region is all together with bottom hollow out.
6. as any one of Meta Materials pixel structure of claim 1 or 2 or 5, wherein, the chi of the described resonator of formation Very little is 10 microns~120 microns.
7. as any one of Meta Materials pixel structure of claim 1 or 2 or 5, wherein, the chi of the described resonator of formation Very little is 121 microns~1000 microns.
8. as any one of Meta Materials pixel structure of claim 1 or 2 or 5, described top layer be made up of metal material with Form metal resonators, described bottom is made up of dielectric substance.
9. Meta Materials pixel structure as claimed in claim 8, described metal material is gold or aluminum, and described dielectric substance is nitrogen SiClx or silicon dioxide.
10. a kind of focal plane array image-forming detector, this imaging detector comprises by multiple as any one in claim 1 or 2 or 5 Individual described Meta Materials pixel structure presses the focal plane arrays (FPA) of periodic arrangement composition it is characterised in that multiple described Meta Materials picture Identical permutation forms Meta Materials periodic structure, and the horizontal cycle is the length of a Meta Materials pixel, and longitudinal cycle is Meta Materials The width of pixel.
CN201410228063.2A 2014-05-27 2014-05-27 Metamaterial pixel structure and focal plane array imaging detector using same Expired - Fee Related CN103983364B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410228063.2A CN103983364B (en) 2014-05-27 2014-05-27 Metamaterial pixel structure and focal plane array imaging detector using same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410228063.2A CN103983364B (en) 2014-05-27 2014-05-27 Metamaterial pixel structure and focal plane array imaging detector using same

Publications (2)

Publication Number Publication Date
CN103983364A CN103983364A (en) 2014-08-13
CN103983364B true CN103983364B (en) 2017-02-15

Family

ID=51275424

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410228063.2A Expired - Fee Related CN103983364B (en) 2014-05-27 2014-05-27 Metamaterial pixel structure and focal plane array imaging detector using same

Country Status (1)

Country Link
CN (1) CN103983364B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2018215765A1 (en) * 2017-05-23 2018-11-29 Sargard Limited Radiation shield

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107478336B (en) * 2017-09-01 2019-07-23 中国科学院电子学研究所 Terahertz imaging array chip and preparation method thereof, imaging system
CN114034395B (en) * 2021-10-13 2024-02-09 北京遥测技术研究所 Terahertz focal plane imaging detector, imaging system and imaging method

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102800986A (en) * 2012-08-02 2012-11-28 中国科学院上海微***与信息技术研究所 Terahertz dual-band metamaterial based on electric resonance

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2008121159A2 (en) * 2006-10-19 2008-10-09 Los Alamos National Security Llc Active terahertz metamaterial devices
US20130314765A1 (en) * 2012-05-25 2013-11-28 The Trustees Of Boston College Metamaterial Devices with Environmentally Responsive Materials

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102800986A (en) * 2012-08-02 2012-11-28 中国科学院上海微***与信息技术研究所 Terahertz dual-band metamaterial based on electric resonance

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
A metamaterial absorber for the terahertz regime:design,fabrication and characterization;Hu Tao et al.;《OPTICS EXPRESS》;20080512;第16卷(第10期);第7181-7188页 *
Bi-material terahertz sensors using metamaterial structures;Fabio Alves et al.;《OPTICS EXPRESS》;20130523;第21卷(第11期);第13256-13271页 *
Microwave and Terahertz wave sensing with metamaterials;Hu Tao et al.;《OPTICS EXPRESS》;20111024;第19卷(第22期);第21621页倒数1-6行,第21622-21623页,图1、2 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2018215765A1 (en) * 2017-05-23 2018-11-29 Sargard Limited Radiation shield

Also Published As

Publication number Publication date
CN103983364A (en) 2014-08-13

Similar Documents

Publication Publication Date Title
Ogawa et al. Wavelength-or polarization-selective thermal infrared detectors for multi-color or polarimetric imaging using plasmonics and metamaterials
CN104458011A (en) Full waveband infrared focal plane array based on MEMS technology
Koechlin et al. Total routing and absorption of photons in dual color plasmonic antennas
US10983047B2 (en) Imaging devices including dielectric metamaterial absorbers and related methods
KR102040149B1 (en) Infrared detector
Ogawa et al. Mushroom plasmonic metamaterial infrared absorbers
CN103983364B (en) Metamaterial pixel structure and focal plane array imaging detector using same
CN111947787B (en) Infrared detector and preparation method thereof
US8958141B1 (en) Ultra-broadband, plasmonic, high-refractive index materials, UBHRI-GRIN-lenses-and other optical components
CN105891609A (en) Thermal mechanical type electromagnetic radiation detector
US10612979B2 (en) Spectral conversion element for electromagnetic radiation
JP6184366B2 (en) Electromagnetic wave sensor device
CN105987757B (en) Terahertz focal plane arrays (FPA) and detection and imaging device
CN102650547B (en) Optical reading method for micro lens array of non-refrigeration infrared imaging system
Suzuki et al. Carbon nanotube-based, serially connected terahertz sensor with enhanced thermal and optical efficiencies
Minin et al. Improvement of a point-contact detector performance using the terajet effect initiated by photonics
Li et al. High-throughput terahertz imaging: progress and challenges
RU160810U1 (en) SUBWAVE WAVE FRONT SENSOR
JP5943764B2 (en) Electromagnetic wave sensor and electromagnetic wave sensor device
JP5706174B2 (en) Infrared sensor and infrared sensor array
RU2414688C1 (en) Terahertz radiation matrix receiver
CN102222813A (en) Terahertz wave axial direction focusing device
Chattopadhyay et al. Planar antenna arrays for CMB polarization detection
CN101498607A (en) Full-hollow structure light modulation thermal imaging focal plane array with silicon support frame work
CN112731579A (en) Pixel polarizing film array, detection device and infrared polarization detector

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: 20170215

Termination date: 20180527

CF01 Termination of patent right due to non-payment of annual fee