Nothing Special   »   [go: up one dir, main page]

CN104266756A - Broadband infrared scanning beam split device and calibrating method - Google Patents

Broadband infrared scanning beam split device and calibrating method Download PDF

Info

Publication number
CN104266756A
CN104266756A CN201410532246.3A CN201410532246A CN104266756A CN 104266756 A CN104266756 A CN 104266756A CN 201410532246 A CN201410532246 A CN 201410532246A CN 104266756 A CN104266756 A CN 104266756A
Authority
CN
China
Prior art keywords
wavelength
angle
lambda
delta
radiation
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.)
Granted
Application number
CN201410532246.3A
Other languages
Chinese (zh)
Other versions
CN104266756B (en
Inventor
胡德信
韩顺利
侯喜报
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.)
China Electronics Technology Instruments Co Ltd CETI
Original Assignee
CETC 41 Institute
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 CETC 41 Institute filed Critical CETC 41 Institute
Priority to CN201410532246.3A priority Critical patent/CN104266756B/en
Publication of CN104266756A publication Critical patent/CN104266756A/en
Application granted granted Critical
Publication of CN104266756B publication Critical patent/CN104266756B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Spectrometry And Color Measurement (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

The invention provides a broadband infrared scanning beam split device and a calibrating method. The device comprises an LVF, a clamp, a drive motor, a photoelectric switch, a zero position opening, an external pressing ring and an internal pressing ring. The drive motor drives the clamp with a gradual optical filter to conduct rotating scanning test, the internal pressing ring and the external pressing ring of the clamp press the non-working region of the LVF to conduct fixing, assembly is simple and firm, and the high-speed rotating scanning test can be achieved. Compared with a CVF, by the adoption of the scheme, the coating technology difficulty and coating cost are lowered greatly, and through a corresponding wavelength calibrating algorithm, continuous test of broadband infrared radiation can be achieved.

Description

A kind of broadband infrared scan light-dividing device and calibration steps
Technical field
The invention belongs to infrared radiation spectrophotometric test technical field, in particular a kind of broadband infrared scan light-dividing device and calibration steps.
Background technology
Infrared gradual filter is mainly used in infrared spectral radiant test, at diverse location through different wave length radiation, be used as light-splitting device, require in application that it can cover 3 ~ 5 μm and 8 ~ 14 μm of two infrared atmospheric window mouths, and can fast wavelength sweep be carried out, based on the feature (maximum wavelength is not more than minimum wavelength twice) of coating technique, at present general adopt 3 ~ 4 CVF (circular gradual filter) to be spliced into mode that an annular carries out rotation sweep realizes.But due to CVF coating technique difficulty large (China yet there are no ripe corresponding coating technique), cost is high, limits its widespread use.
Paper " heavy caliber Infrared radiation calibration and error analysis " (infrared and laser engineering, 40th volume the 9th phase, 1624th ~ 1628 pages, in September, 2011), paper " Developing Application of infrared target simulator calibration system " is (infrared with millimeter wave journal, 22nd volume the 4th phase, 251st ~ 255 pages, in August, 2003) and paper " development of infrared spectroradio meter " (infrared and laser engineering, 28th volume the 2nd phase, 14th ~ 17 pages, in April, 1999) all adopt CVF as light-splitting device, coating technique difficulty is large, and cost is high.As shown in Figure 1, incident luminous point 2 converges on CVF1, transmission wave band light intensity be positioned at the infrared eye in dead astern detect, along with CVF1 is under the rotating shaft 3 of motor drives at the uniform velocity in rotary course, detector completes the sweep test of different wave length light intensity.Prior art adopts the mode of CVF light splitting, and CVF device coating technique difficulty is large, and cost is very high, is difficult to be generally used.
Therefore, prior art existing defects, needs to improve.
Summary of the invention
Technical matters to be solved by this invention is for the deficiencies in the prior art, provides a kind of broadband infrared scan light-dividing device and calibration steps.
Technical scheme of the present invention is as follows:
A kind of broadband infrared scan light-dividing device, wherein, comprises fixture, drive motor, optoelectronic switch, outer press ring and inner pressure ring; Described drive motor drive installation has the fixture of gradual filter to carry out rotation sweep test, and the inner pressure ring in fixture and outer press ring are pushed down LVF non-active area and be fixed; When testing, the luminous point that incident camera lens is assembled is beaten on LVF, described fixture rotates under the driving of drive motor, through radiation infrared eye detect, along with the rotation of LVF is to complete the sweep test of different wave length, use optoelectronic switch to detect zero-bit aperture position as zero angle position, all the other positions are determined by counting motor number of steps simultaneously.
A calibration steps for broadband infrared scan light-dividing device, wherein, if the pass that the data recorded after completing the sweep test of different wave length are radiation intensity p and time t/ angle θ is: P=f 1(t)=f 2(θ), if try to achieve the funtcional relationship of angle θ corresponding to wavelength X: θ=f 3(λ) functional relation of namely trying to achieve radiation intensity p and wavelength X in above formula, is substituted into: P=f 2(f 3(λ)).
The calibration steps of described broadband infrared scan light-dividing device, wherein, described wavelength and the relation θ of angle=f 3(λ) computing method are:
If gradual filter operation wavelength is from left to right λ minλ max, be then λ in middle position operation wavelength mid=(λ min+ λ max)/2, find the angle of its correspondence to be θ by location 0, its corresponding relation is: so, at θ 0wavelength corresponding to+Δ θ position is: λ mid+ Δ λ, tries to achieve Δ θ and Δ λ relation, namely sets up the corresponding relation of wavelength and angle;
First try to achieve angle delta θ and optical filter length Δ l position corresponding relation:
Formula 1: Δ l=R*sin Δ θ
Formula 1 is substituted into wavelength Δ λ and optical filter length Δ l function of position relational expression, asks the funtcional relationship obtaining wavelength Δ λ and angle delta θ as follows:
Formula 2: Δ λ=Δ l* (λ maxmin)/l=(R*sin Δ θ) * (λ maxmin)/l
Wherein, l is optical filter total length, and R is spot scan radius.
The calibration steps of described broadband infrared scan light-dividing device, wherein, according to formula 2, the angle obtain test and radial coordinate system are converted to the coordinate system of wavelength and radiation, reach the object of wavelength calibration.
The concrete steps of testing the angle that obtains and radial coordinate system and be converted to the coordinate system of wavelength and radiation wherein, are describedly: according to formula 2, be expressed as by angle delta θ wavelength Δ λ by the calibration steps of described broadband infrared scan light-dividing device:
Δθ = arcsin Δλ * l R * ( λ max - λ min ) ;
Then, angle wavelength is expressed as:
θ 0 + Δθ = λ mid + arcsin Δλ * l R * ( λ max - λ min ) ;
Then the funtcional relationship of radiation p and wavelength Δ λ is:
P = f 2 ( θ 0 + Δθ ) = f 2 ( λ mid + arcsin Δλ * l R * ( λ max - λ min ) ) ,
The angle then test obtained and radial coordinate system are converted to the coordinate system of wavelength and radiation.
Adopt such scheme, greatly reduce coating technique difficulty and coating cost, for the wavelength unevenness in LVF scanning process, devise corresponding wavelength calibration algorithm, to realize wide infrared band spectral radiance continuous sweep.
Accompanying drawing explanation
Fig. 1 is that in prior art, three combination CVF scan light splitting schematic diagram.
Fig. 2 is that the present invention three combination LVF scans light-dividing device structural representation.
Fig. 3 is the inventive method medium wavelength calibration schematic diagram.
Embodiment
Below in conjunction with the drawings and specific embodiments, the present invention is described in detail.
Embodiment 1
The present invention devises one and multi-disc is combined LVF (bar shaped gradual filter) also can carry out high-velocity scanning device for infrared spectral radiant light splitting.As shown in Figure 2, apparatus of the present invention comprise LVF7, fixture 6, drive motor 1, optoelectronic switch 2, zero-bit opening 3, outer press ring 4 and inner pressure ring 5, drive motor 1 drive installation has the fixture 6 of LVF7 to carry out rotation sweep test, inner pressure ring 5 and outer press ring 4 are just in time pushed down LVF7 non-active area and are fixed, assembling is firmly simple, and can realize high-speed rotating scanning test.
In test process, the luminous point that incident camera lens is assembled is beaten on LVF7, the fixture 6 that LVF7 is housed rotates under the driving of drive motor 1, through radiation infrared eye detect, along with the rotation of LVF7 just completes sweep test, meanwhile, detect zero-bit opening 3 position as zero angle position by optoelectronic switch 2, all the other positions are determined by counting motor number of steps.Owing to being rotation sweep, sweep velocity and scanning stabilization all substantially exceed particles mode.
Embodiment 2
On the basis of above-described embodiment, the present invention also provides a kind of calibration steps of broadband infrared scan light-dividing device,
Compared with carrying out scanning light splitting with employing CVF, the present invention greatly reduces coating technique difficulty and coating cost, for the wavelength unevenness in LVF scanning process, devises corresponding wavelength calibration algorithm, to realize wide infrared band spectral radiance continuous sweep.
Carrying out light splitting owing to adopting LVF can keep test wavelength even unlike CVF, adopt in said apparatus test and also have invalid data, to this, devise and adopt said apparatus respective wavelength calibration steps, set up the corresponding relation of wavelength and intensity, to realize wide infrared band spectral radiance follow-on test, as shown in Figure 3:
Because optical filter is uniform angular velocity scanning, therefore, the data recorded be radiation intensity and time/relation of angle: P=f 1(t)=f 2(θ), if the functional relation of angle corresponding to wavelength can be obtained: θ=f 3(λ) functional relation of radiation intensity and wavelength can, so, just be obtained: P=f 2(f 3(λ)).
According to the relevant Principle of plating of gradual filter, on bar shaped gradual filter, wavelength is uniform.Even gradual filter from left to right operation wavelength be λ minλ max, be so λ in middle position operation wavelength mid=(λ min+ λ max)/2, corresponding angle is θ, and its corresponding relation is: so, at the wavelength that θ+Δ θ position is corresponding be: λ mid+ Δ λ.
According to trigonometric function relation, first try to achieve angle delta θ and optical filter extension position Δ l corresponding relation, wherein, Δ θ represents the variable quantity of angle θ, and Δ λ represents that the variable quantity of wavelength X is formula 1:
Δl=R*sinΔθ
Again according to the uniform feature of wavelength on monolithic LVF, above formula is substituted into wavelength and optical filter extension position functional relation, the funtcional relationship that can obtain wavelength Δ λ and angle delta θ is as follows, formula 2:
Δλ=Δl*(λ maxmin)/l=(R*sinΔθ)*(λ maxmin)/l
Wherein, l is optical filter total length, and R is spot scan radius, and Δ l represents the variable quantity of l.The concrete steps that the angle obtain test and radial coordinate system are converted to the coordinate system of wavelength and radiation are: according to formula 2, be expressed as by angle delta θ wavelength Δ λ:
Then, angle wavelength is expressed as:
θ 0 + Δθ = λ mid + arcsin Δλ * l R * ( λ max - λ min ) ;
Then the funtcional relationship of radiation p and wavelength Δ λ is:
the angle then test obtained and radial coordinate system are converted to the coordinate system of wavelength and radiation.
By above-mentioned computing, can obtain the funtcional relationship between angle and wavelength, the angle that finally test can be obtained according to this relational expression and radial coordinate system are converted on the coordinate system of wavelength and radiation, reach the object of wavelength calibration.
Should be understood that, for those of ordinary skills, can be improved according to the above description or convert, and all these improve and convert the protection domain that all should belong to claims of the present invention.

Claims (5)

1. a broadband infrared scan light-dividing device, is characterized in that, comprises fixture, drive motor, optoelectronic switch, outer press ring and inner pressure ring; Described drive motor drive installation has the fixture of gradual filter to carry out rotation sweep test, and the inner pressure ring in fixture and outer press ring are pushed down LVF non-active area and be fixed; When testing, the luminous point that incident camera lens is assembled is beaten on LVF, described fixture rotates under the driving of drive motor, through radiation infrared eye detect, along with the rotation of LVF is to complete the sweep test of different wave length, use optoelectronic switch to detect zero-bit aperture position as zero angle position, all the other positions are determined by counting motor number of steps simultaneously.
2. a calibration steps for broadband infrared scan light-dividing device, is characterized in that, if the pass that the data recorded after completing the sweep test of different wave length are radiation intensity p and time t/ angle θ is: P=f 1(t)=f 2(θ), if try to achieve the funtcional relationship of angle θ corresponding to wavelength X: θ=f 3(λ) functional relation of namely trying to achieve radiation intensity p and wavelength X in above formula, is substituted into: P=f 2(f 3(λ)).
3. the calibration steps of broadband infrared scan light-dividing device as claimed in claim 2, is characterized in that, described wavelength and the relation θ of angle=f 3(λ) computing method are:
If gradual filter operation wavelength is from left to right be then λ in middle position operation wavelength mid=(λ min+ λ max)/2, find the angle of its correspondence to be θ by location 0, its corresponding relation is: so, at θ 0wavelength corresponding to+Δ θ position is: λ mid+ Δ λ, tries to achieve Δ θ and Δ λ relation, namely sets up the corresponding relation of wavelength and angle;
First try to achieve angle delta θ and optical filter length Δ l position corresponding relation:
Formula 1: Δ l=R*sin Δ θ
Formula 1 is substituted into wavelength Δ λ and optical filter length Δ l function of position relational expression, asks the funtcional relationship obtaining wavelength Δ λ and angle delta θ as follows:
Formula 2: Δ λ=Δ l* (λ maxmin)/l=(R*sin Δ θ) * (λ maxmin)/l
Wherein, l is optical filter total length, and R is spot scan radius.
4. the calibration steps of broadband infrared scan light-dividing device as claimed in claim 3, is characterized in that, according to formula 2, the angle obtain test and radial coordinate system are converted to the coordinate system of wavelength and radiation, reach the object of wavelength calibration.
5. the calibration steps of broadband infrared scan light-dividing device as claimed in claim 4, it is characterized in that, describedly by the concrete steps of testing the angle that obtains and radial coordinate system and be converted to the coordinate system of wavelength and radiation be: according to formula 2, angle delta θ wavelength Δ λ is expressed as:
Δθ = arcsin Δλ * l R * ( λ max - λ min ) ;
Then, angle wavelength is expressed as:
θ 0 + Δθ = λ mld + arcsin Δλ * l R * ( λ max - λ min ) ;
Then the funtcional relationship of radiation p and wavelength Δ λ is:
P = f 2 ( θ 0 + Δθ ) = f 2 ( λ mid + arcsin Δλ * l R * ( λ max - λ min ) ) ,
The angle then test obtained and radial coordinate system are converted to the coordinate system of wavelength and radiation.
CN201410532246.3A 2014-10-10 2014-10-10 A kind of broadband infrared scan light-dividing device and calibration steps Expired - Fee Related CN104266756B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410532246.3A CN104266756B (en) 2014-10-10 2014-10-10 A kind of broadband infrared scan light-dividing device and calibration steps

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410532246.3A CN104266756B (en) 2014-10-10 2014-10-10 A kind of broadband infrared scan light-dividing device and calibration steps

Publications (2)

Publication Number Publication Date
CN104266756A true CN104266756A (en) 2015-01-07
CN104266756B CN104266756B (en) 2016-05-25

Family

ID=52158297

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410532246.3A Expired - Fee Related CN104266756B (en) 2014-10-10 2014-10-10 A kind of broadband infrared scan light-dividing device and calibration steps

Country Status (1)

Country Link
CN (1) CN104266756B (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105136742A (en) * 2015-08-21 2015-12-09 董海萍 Cloud spectrum database-based miniature spectrometer and spectrum detection method
CN107144359A (en) * 2017-05-16 2017-09-08 中国电子科技集团公司第四十研究所 The spectrally resolved Enhancement Method of infrared spectroradio meter, infrared spectroradio meter
CN108534898A (en) * 2018-06-06 2018-09-14 首都师范大学 Hyperspectral imager, EO-1 hyperion camera and EO-1 hyperion camera system
CN109683270A (en) * 2018-12-15 2019-04-26 中国科学院长春光学精密机械与物理研究所 A method of can be used for multi-disc gradual filter and precisely aligns
CN112596115A (en) * 2020-10-16 2021-04-02 武汉高德红外股份有限公司 Infrared thermal imaging system with medium-wave double-color switching

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040032584A1 (en) * 2002-08-15 2004-02-19 Tokuyuki Honda Optical channel monitoring device
CN1811381A (en) * 2006-01-24 2006-08-02 天津大学 Spectrograph based on LVF
CN102713543A (en) * 2010-01-21 2012-10-03 浜松光子学株式会社 Spectral device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20040032584A1 (en) * 2002-08-15 2004-02-19 Tokuyuki Honda Optical channel monitoring device
CN1811381A (en) * 2006-01-24 2006-08-02 天津大学 Spectrograph based on LVF
CN102713543A (en) * 2010-01-21 2012-10-03 浜松光子学株式会社 Spectral device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
R.P.WRIGHT .ET AL: "A Long-wavelength infrared Photoluminescence Spectrometer for the Characterization of Semiconductor Materials", 《MATERIALS RESEARCH SOCIETY SYMPOSIUM PROCEEDINGS》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105136742A (en) * 2015-08-21 2015-12-09 董海萍 Cloud spectrum database-based miniature spectrometer and spectrum detection method
CN107144359A (en) * 2017-05-16 2017-09-08 中国电子科技集团公司第四十研究所 The spectrally resolved Enhancement Method of infrared spectroradio meter, infrared spectroradio meter
CN107144359B (en) * 2017-05-16 2019-03-19 中国电子科技集团公司第四十一研究所 The spectrally resolved Enhancement Method of infrared spectroradio meter, infrared spectroradio meter
CN108534898A (en) * 2018-06-06 2018-09-14 首都师范大学 Hyperspectral imager, EO-1 hyperion camera and EO-1 hyperion camera system
CN109683270A (en) * 2018-12-15 2019-04-26 中国科学院长春光学精密机械与物理研究所 A method of can be used for multi-disc gradual filter and precisely aligns
CN112596115A (en) * 2020-10-16 2021-04-02 武汉高德红外股份有限公司 Infrared thermal imaging system with medium-wave double-color switching

Also Published As

Publication number Publication date
CN104266756B (en) 2016-05-25

Similar Documents

Publication Publication Date Title
CN104266756A (en) Broadband infrared scanning beam split device and calibrating method
US10903901B2 (en) Free space optical node with fiber bundle
CN101832912B (en) Terahertz wave fast imaging scanner
WO2016106956A1 (en) Infrared spectrogram correlation intelligent detection method and apparatus
DE112015001069T5 (en) Apparatus and method for detecting a moving object using images in cooperation with spectrum of entire wavelength ranges
CN111537065A (en) Bandwidth design method for spatial modulation full-polarization imaging system
CN108593108A (en) Spectrometer
CN108036856B (en) Real-time calibration system for airborne imaging spectrometer of multi-rotor unmanned aerial vehicle
CN102969651A (en) Rapid K-space linear frequency sweep laser source
CN102980857A (en) Terahertz time-domain spectroscopy system for realizing terahertz rapid imaging by using frequency optical comb
CN103575660A (en) Terahertz-wave scanning imaging system and method for article detection on assembly line
CN103323117B (en) Mobile broadband Fourier transform infrared imaging spectrometer
CN103809167B (en) A kind of FP interference type spectral filter resonance frequency locking device and method
CN203275287U (en) Portable optical filter color wheel type multispectral imaging system
CN103575386B (en) Based on diffuse reflection type high light temporal and spatial sampling measuring method and the device of rotating vane
CN113777072B (en) Apparatus, system, method, medium, and program product for detecting terahertz signal
CN113237559B (en) Multispectral radiation temperature measuring device and using method
CN111579075B (en) Fast detection method for light wave polarization state based on Fourier analysis
CN105300520A (en) Direct sunlight differential absorption spectrometer system based on diffuse reflection plate
CN102998261A (en) Terahertz wave pseudo heat light source-based imaging device
CN211627343U (en) Common-light-path three-phase substance identification and detection system based on unmanned aerial vehicle carrying
CN105044113A (en) Sulfur dioxide gas imager
RU2504800C1 (en) Method of forming radio portrait of object by frequency division parallel processing
CN103913231B (en) Based on the space-time unite modulation fourier transformation imaging spectrometer of light-duty beam splitter
CN108760244B (en) A kind of high-resolution optical information networks device and method

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
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20190226

Address after: 266000 No. 98 Xiangjiang Road, Huangdao District, Qingdao City, Shandong Province

Patentee after: China Electronics Technology Instrument and Meter Co., Ltd.

Address before: 266555 No. 98 Xiangjiang Road, Qingdao economic and Technological Development Zone, Shandong

Patentee before: The 41st Institute of CETC

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: 20160525

Termination date: 20201010