CN1415945A - Design of multiple grating spectrograph imaging device - Google Patents
Design of multiple grating spectrograph imaging device Download PDFInfo
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- CN1415945A CN1415945A CN 02137501 CN02137501A CN1415945A CN 1415945 A CN1415945 A CN 1415945A CN 02137501 CN02137501 CN 02137501 CN 02137501 A CN02137501 A CN 02137501A CN 1415945 A CN1415945 A CN 1415945A
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Abstract
This invention relates to multiple grating spectrum imager. spectrum detecting speed. Which applies combinet grating and detector system composed of multisubgrating and multiline array detectors without any mechanical shift of optical parts realizing whole spectrum quick test and analysis.
Description
Technical field
The invention belongs to optical electron device technology field, be specifically related to a kind of multiple grating spectrograph imaging device design.
Background technology
Monochromator is a kind of photon energy and wavelength selector, be a kind of basic spectral analysis and surveying instrument, having a wide range of applications at optics and optoelectronic areas, is the core optical device of numerous spectrometric instruments such as modern Raman and fluorescence spectrum, light absorption, light reflectance spectrum, infrared remote sensing, optical communication spectrum, biochip spectrum and modulated spectrum.Wherein, to the near-infrared region, most widely used is the grating type monochromator near ultraviolet, and this is to have utilized the photon of undulatory property to produce the principle of diffraction on grating.Optical grating construction is generally having and is carved with many equally spaced grooves on the optical substrate of certain size, and as 1200 every millimeter or 1800 every millimeter etc., actual striped number depends on concrete operation wavelength district and designing requirement.Photon drops on these strias, because the effect of diffraction will cause that the amplitude of each light wave and phase place superpose, the photon after the reflection just can be lined up in the space regularly by energy or wavelength, and its relational expression is:
Dsin θ
m=m λ+g
o(1) d is the separation of grating in the formula, θ
mThe wavelength that is the m level be the photon of λ at the spatial distributions angle, g
oBe the constant relevant with design of Optical System, (θ
mBe defined as the angle between reflection diffraction light direction and the grating normal).Therefore, as get m=1, just can on position, different θ angle, obtain the first order diffraction photon of respective wavelength.In the design of traditional raster monochromator, fixedly the incident of photon and exit slit invariant position adopt a mechanical driving device, and rotate at the θ angle of control grating, and wavelength is scanned, and just can obtain needed monochromaticity photon from exit slit.
Adopt the grating monochromator of said structure, need to possess control function in actual use:
1. machinery control grating rotates, and realizes raster scanning.
2. displacement grating.When monochromator during in the work of the wavelength zone of broad, be to improve the wavelength resolution of instrument and obtain best signal to noise ratio (S/N ratio) quality, need change grating according to the spectral wavelength district of being worked.For example, use maximum 200-1100nm wavelength coverages, need 2 blocks of gratings at least at present, even three blocks of gratings, can satisfy the accurate Testing requirement of spectrum line preferably.
3. displacement color filter.By formula (1) as can be known, in certain position, θ angle, the diffraction light of the longer wavelength of m=1 and m=2 (or more high order) shorter wavelength can occur simultaneously.Therefore,, need to use one even several piece optical filter at least,, can satisfy the requirement of detected photon monochromaticity the high order diffraction light elimination of m=2 (or more high order) according to the wavelength applications scope of reality.
In present most of commodity monochromator structures, above-mentioned three control function (raster scanning, displacement grating, displacement color filter) are all undertaken by mechanical transmission structure independently.[list of references 1. grating monochromator product descriptions, OrielCorporation, 250 Long Beach Blvd.Stratford, CT, 06497-0872, USA.List of references 2. grating monochromator product descriptions, Scientific Measurement Systems, Inc.2527 Foresight CircleJunction, CO 81505-1007, USA.] this has increased the design and the structural complexity of instrument on the one hand, has reduced reliability, brings many inconveniences to use on the other hand, when especially replacing grating, needs carry out again precise calibration and adjustment to the wavelength location of system very time-consuming and trouble.
For efficient and the precision that improves length scanning, the planar array type ccd detector has been widely used in can replacing the single-photon detector in the grating type monochromator, in the spectral range of broad wavelength is scanned fast.Owing to the optical grating diffraction subtended angle structure that is subjected to being determined and the restriction of detector size by formula (1), even adopt the planar array type ccd detector, because of its in one dimension direction limited pixel and size, still be difficult to be implemented in and carry out in the spectral range of broad that high-precision all-wave is long to cover scanning with a grating.Therefore, in present most of commodity CCD grating monochromators, still need to adopt polylith grating and optical filter, can realize high-quality and high-precision length scanning [list of references 3.Acton Research Co.USA, SpectroPro300 type monochromator].In above-mentioned commodity CCD grating monochromator design, its tactic pattern is as follows:
Light source → grating G
x→ imaging mirror M
x→ detector D
xGrating G
xBe that one or more grating forms, and by the control of mechanical transmission mechanisms such as step motor, by the diffraction light of grating outgoing through single spheric reflection imaging mirror M
x, focus on the planar array type ccd detector, form spectrum, realize branch wavelength domain scanning and measurement to wavelength.Owing to still need to use mechanical driving device, weakened the advantage that adopts the planar array type ccd detector to a certain extent, limited spectral measurement speed.
In addition, when the control grating rotates,, need to adopt special limit switch, monochromator is caused damage to prevent that mechanical shift is excessive at the two ends of mechanical shift extreme position length wavelength.This has also increased the complicacy of system design and structure.
Summary of the invention
The objective of the invention is to propose a kind of any mechanical transmission mechanism that need not, the multiple grating spectrograph imaging device that system works is reliable, the life-span is long.
The multiple grating spectrograph imaging device that the present invention proposes is on said structure pattern basis, and its shortcoming is improved, and in the present invention, adopts polylith grating G
x, combined type cylindrical mirror optical focusing system M
xWith combined type linear array or planar array detector D
x, need not the mechanical shift and the gear train of any element, grating is fixed, and its normal direction is made assembled arrangement by application requirements, by the diffraction light with different wave length of the different grating outgoing formula cylinder light spectrum image-forming mirror M that is combined
xFocus on, be imaged on and corresponding combined type linear array of different gratings or planar array detector D
xOn.Thereby realize the quick high-resolution imaging of wavelength at full spectral region, can remove the needs that mechanical limit switch is set from, thereby extremely simplify the design and the structure of instrument, increased the reliable long-term working and the life-span of system.The speed of its full spectroscopic data check and analysis only depends on the time of response time of linear array photodetector and subsequent data transmissions, processing, be no more than 0.01 second, the resolution of simultaneously full spectral region can reach 0.08nm, and this is the not available advantage of traditional optical spectrum imagers.
By formula (1) can adopt the polylith grating, and the separation of every block of grating is d, and (also can adopt the separation of different d), for first-order diffraction light, n=1, the diffraction angle distribution of different wave length correspondence is:
Δλ
1＝λ
2-λ
1＝d(sinθ
2-sinθ
1)
Δλ
2＝λ
3-λ
2＝d(sinθ
3-sinθ
2)
Δλ
n＝λ
n+1-λ
n＝d(sinθ
n+1-sinθ
n) (2)
Therefore, n piece grating can be pressed n wavelength zone Δ λ
1, Δ λ
2Δ λ
nArrange along the y direction perpendicular to the plane of incidence, adjust the normal direction of every block of grating, feasible corresponding with each wavelength zone, every block of grating (x direction) in the plane of incidence has identical diffraction subtended angle scope, that is:
Δ θ
1(Δ λ
1)=Δ θ
2(Δ λ
2=...=Δ θ
2(Δ λ
n) in (3) formula:
Δθ＝θ
2-θ
1＝θ
3-θ
2=---=θ
n+1-θ
n
Incident light is through n piece optical grating diffraction, with plane of incidence vertical direction, can form n the end to end wavelength zone of sub-wavelength, constitute and cover λ
1To λ
N+1The full wavelength zone of wavelength.This n the monochromatic collimated beam with identical diffraction subtended angle is f through focal length
1Cylindrical mirror M
1Assemble along the x direction, light spectrum image-forming is being placed focus f
1On form on the focal plane of (or planar array detector) by n linear array detector D.The detected pixel of linear array detector is arranged along the x direction.Because M
1Effect be with spectrum along the Wavelength distribution direction focusing, do not have congregation in the y direction vertical with the plane of incidence, still keep the distribution space of n wavelength zone, and the Pixel Dimensions of linear array detector is limited in the y direction, only account for very little ratio.In order to make full use of of the light distribution of n wavelength zone, adopt n sub-cylindrical mirror M in the y direction
2, focal length is f
2, (f
2＜f
1), they are placed M
1To the light path of detector D.This n cylindrical mirror is arranged in parallel along the y direction, its effect be to each minute wavelength zone light along the y direction focusing, the light of each wavelength zone focused on concentrate on the corresponding with it linear array detector, improve the efficient that is detected of light.Adopt this method, just can exempt any mechanical driving device,, realize the full spectral region that are made of nx Δ λ are carried out high-spectral-resolution measurement and analysis by n limited linear array detector of number of pixels.
According to above-mentioned method for designing, the tactic pattern of multiple grating spectrograph imaging device of the present invention is as follows:
Light source → grating Gx → imaging mirror Mx → detector Dx
Wherein, Gx is made up of the polylith grating, and Mx is a combined type cylinder optical focusing system, and Dx is combined type linear array or planar array detector.Grating is fixed, and its normal direction is made assembled arrangement by application requirements, by the diffraction light with different wave length of the different grating outgoing formula cylinder light spectrum image-forming mirror M that is combined
xFocus on, be imaged on and corresponding combined type linear array of different gratings or planar array detector D
xOn.
Among the present invention, being placed with width between light source and the grating Gx is the adjustable slit S of 0-2mm
1, to inject for light source, the centre also is provided with level crossing M
4With spherical reflector M
3, make light source through S
1, to inject for light source, the centre also is provided with level crossing M
4With spherical reflector M
3, make light source through S
1, M
4To M
3, M
3Emergent light is a directional light.
Gx is made up of n piece grating, and sub-gratings can be plane grating or spheric grating.N can determine according to actual needs.General optional n=1-10, routine n=3-8, n=4-6.The separation of every block of grating is d, and this n piece grating is pressed n wavelength zone Δ λ
1, Δ λ
2Δ λ
nAlong perpendicular to the y of the plane of incidence to arrangement, every block of grating (being the x direction) in the plane of incidence has identical diffraction subtended angle scope, sees formula (3) and formula (4).The position angle of each sub-gratings of Gx is adjustable.
Imaging mirror Mx is that a focal length is f
1Cylindrical mirror M
1, the light that goes out from grating Gx diffraction is assembled along directions X.f
1Design is according to actual needs determined.Detector Dx is made up of n linear array detector or planar array detector D, places M
1Focus on.
In order to make full use of of the light distribution of n wavelength zone, at M in the y direction
1Between detector Dx, correspondence is provided with n sub-cylindrical mirror M
2, M
2Focal length be f
2, f
2＜f
1, this n sub-cylindrical mirror along y to being arranged in parallel, to each minute wavelength zone light along the y direction focusing, the light of each wavelength zone is focused on linear array (face battle array) detector that concentrates on correspondence with it.
In addition, at each sub-gratings G or the sub-cylindrical mirror M of Gx
2Before corresponding color filter is set, with the high order diffraction light elimination of m＞2.
The present invention can realize the high speed and the high resolving power measurement of spectrum owing to the mechanical shift of no any optics in full spectral measurement.Spectral detection speed only is subjected to the linear array of linear array detector response speed and subsequent data transmissions and processing speed.Full spectral measurement speed with 14-16bit Data Dynamic scope can be faster than 0.01 second.When realizing full spectrum fast detecting, spectral resolution is subjected to detector pixel density, the restriction of the focal length and the wavelength number of partitions.In the present embodiment, the highest resolution of spectrum can reach 0.08nm.Adopt the design's method, in conjunction with adopting more long-focal distance optical system, more highdensity linear array and planar array detector, and the more sub-gratings of employing make the wavelength subregion, can obtain higher spectral resolution.
Adopt the optical spectrum imagers of this method design to obtain important application in the optical communication field, realize high-speed, high precision analysis communication spectrum.This method also can be applied to other spectral region, as at visible region, can adopt 1200 lines/mm grating, and adopt silica-based linear array or planar array detector.For the high order order diffraction light of m＞2, can before corresponding sub-gratings or sub-cylindrical mirror, corresponding color filter be set, with the elimination of high order diffraction light.
Description of drawings
Fig. 1. there is not many grating spectrographs synoptic diagram of mechanical displacement component.After lens L focuses on, is 0-2mm adjustable slit S by width by the light of light source S outgoing
1Incident is by level crossing M
4Reflex to spherical mirror M
1, become directional light, incide on the composite grating G that forms by many gratings, regulate the position angle of each sub-gratings, each sub-diffraction spectrum district is dropped in the identical diffraction subtended angle, be reflected onto cylindrical mirror M
1, in the plane of incidence, spectrum line is focused on along the Wavelength distribution direction, be imaged on the focal plane of the multi-thread array detector D of corresponding combined type combined type cylindrical mirror M
2Effect be respectively to the light intensity of each sub-spectral region direction focusing at the vertical incidence face, make the light signal of each sub-spectral region more effectively be received by corresponding linear array detector (or planar array detector).
Embodiment
The invention is further illustrated by the following examples.
In traditional raster monochromator structure, cancel original grating mechanical transmission structure.Adopt optical system and 5 600 lines/mm grating G (also can choose other separation density gratings and more raster count) of 500mm focal length by application requirements, every block of grating is of a size of 20 * 100mm, grating is parallel with minor face, and the effective area of raster that is combined into is 100 * 100mm.5 blocks of gratings are arranged along the y direction vertical with the plane of incidence, adjusted each grating position angle, by formula (3-4) makes that in same diffraction subtended angle the Wavelength distribution difference of each sub-wavelength zone, but wavelength tandem array constitute complete wavelength zone.The dispersion characteristics of this spectrometer are about 3.0nm/mm, and in order to use at the optical communication 1400-1600nm of near-infrared region wavelength zone, the areal coverage that its all-wave is long is about 200nm.In the focal plane position of detector place light spectrum image-forming, cover size along the total detection of Wavelength distribution direction (x direction) and be about 60.0mm.Adopt 5 linear array detectors, each detector covers 12mm spectrographic detection district (being equivalent to the 40nm wavelength zone) approximately.Adopt the InGaAs linear array infrared eye of 512 pixels, the wavelength workspace is 700-1700nm, and each pixel is of a size of 0.024 (H) * 0.080 (V) mm, the test surface that constitutes is about 12.3 (H) * 0.08 (V) mm, wherein, H is expressed as horizontal x direction, and V is vertical y direction.
Therefore, accurately regulate the position angle of every block of grating, make the distribution of its spectrum in identical diffraction subtended angle be respectively 1400-1440nm, 1440-1480nm, 1480-1520nm, 1520-1560nm, 1560-1600nm, promptly the work spectral region of every sub-gratings are 40 nanometers, with every group be (totally 5 groups of the InGaAs linear array detectors of 512 pixels, arrange along the y direction that the plane of incidence is vertical) corresponding, the pairing wavelength resolution of each pixel is 0.08nm.
Incident light enters the adjustable spectrometer of 0-2mm slit, adopts f
1The cylindrical mirror M of=500mm focal length
1Spectrum is assembled along the x direction.M
1Cylindrical mirror is of a size of 100 * 100mm, receives the parallel diffraction light from grating, with focal imaging behind the spectral reflectance on the focal plane of detector D.Adopt 5 f
2The sub-cylindrical mirror M of=250mm focal length
2, size all is 20 * 100mm, focusing surface is a minor face.M
2Mirror places M along the minor face parallel arranged with them
1And in the middle of the position between the D light path, its effect is that light intensity to each sub-spectral region is along the y direction focusing.Regulate each M
2The position angle, the light intensity of 5 sub-spectral region focused on respectively have on 5 linear array detector D that certain intervals arranges.The standard infrared communication optically filtering sheet that adopts the calibrating gas line spectrum source or have a 0.04-0.08nm bandwidth carries out precise calibration to each detector pixel with the distribution of wavelength, fits to calibration curve, does the quantitative test of spectroscopic data and uses.
Claims (6)
1, a kind of multiple grating spectrograph imaging device, has following tactic pattern: light source → grating Gx → imaging mirror Mx → detector Dx, it is characterized in that Gx is made up of the polylith grating, Mx is a combined type cylinder optical focusing system, Dx is combined type linear array or planar array detector, grating is fixed, and its normal direction is made assembled arrangement by application requirements, by the diffraction light with different wave length of the different grating outgoing formula cylinder light spectrum image-forming mirror M that is combined
xFocus on, be imaged on and corresponding combined type linear array of different gratings or planar array detector D
xOn.
2, multiple grating spectrograph imaging device according to claim 1, the sub-gratings number that it is characterized in that establishing Gx is n, this n sub-gratings is pressed n wavelength zone Δ λ
1, Δ λ
2Δ λ
nAlong perpendicular to the y of the plane of incidence to arrangement, every block of grating has identical diffraction subtended angle scope in the plane of incidence:
Δ θ
1(Δ λ
1)=Δ θ
2(Δ λ
2)=...=Δ θ
n(Δ λ
n) in (3) formula:
Δθ＝θ
2-θ
1＝θ
3-θ
2＝……＝θ
n+1-θ
n (4)
The position angle of each sub-gratings of Gx is adjustable.
3, multiple grating spectrograph imaging device according to claim 1 and 2 is characterized in that imaging mirror Mx is the cylindrical mirror M that a focal length is f1
1, detector Dx is made up of n detector D, is positioned at M
1Focus on.
4, multiple grating spectrograph imaging device according to claim 3 is characterized in that the corresponding n of being provided with sub-cylindrical mirror M between M1 and detector Dx
2, M
2Focal length be f
2, f
2＜f
1, n sub-cylindrical mirror along y to being arranged in parallel, to each minute wavelength zone light along the y direction focusing, the light of each wavelength zone is focused on the detector that focuses on correspondence with it.
5, multiple grating spectrograph imaging device according to claim 4 is characterized in that each sub-gratings G or sub-cylindrical mirror M at Gx
2Before be provided with corresponding color filter, elimination high order diffraction light.
6, the described multiple grating spectrograph imaging device of claim 1-5, it is characterized in that being provided with between light source and the grating Gx width is the adjustable slit S of 0-2mm
1, to inject for light source, the centre also is provided with level crossing M
4With spherical mirror M
3, make light source through S
1, M
4To M
3, M
3Emergent light is a directional light.
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|---|---|---|---|
| CN 02137501 CN1204382C (en) | 2002-10-17 | 2002-10-17 | Design of multiple grating spectrograph imaging device |
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|---|---|---|---|
| CN 02137501 CN1204382C (en) | 2002-10-17 | 2002-10-17 | Design of multiple grating spectrograph imaging device |
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| CN101389938B (en) * | 2006-01-20 | 2011-03-09 | 法国宇航院（Onera） | Compact optical interferometer of the trilateral shift type |
| CN1702452B (en) * | 2004-05-24 | 2011-05-04 | 中国科学院光电技术研究所 | Digital micromirror multi-target imaging spectrometer device |
| CN102183304A (en) * | 2011-01-21 | 2011-09-14 | 北京理工大学 | Optical path structure of cylindrical anastigmatic grating dispersion type imaging spectrometer |
| CN102331300A (en) * | 2011-06-14 | 2012-01-25 | 北京卓立汉光仪器有限公司 | Asymmetric monochromator for improving luminous flux and resolution |
| CN105092035A (en) * | 2014-05-09 | 2015-11-25 | 三星电子株式会社 | Spectro-sensor, spectro-sensor module, spectrometer and spectral analysis method |
| CN102183304B (en) * | 2011-01-21 | 2016-12-14 | 北京理工大学 | A kind of optical path structure of cylindrical anastigmatic grating dispersion type imaging spectrometer |
| CN109682469A (en) * | 2014-09-10 | 2019-04-26 | 电子光子集成电路股份有限公司 | Curve grating spectrograph and wavelength multiplexer or demultiplexer with high wavelength resolution |
| CN109917354A (en) * | 2019-04-26 | 2019-06-21 | 上海禾赛光电科技有限公司 | Reception device, laser radar and its echo processing techniques of laser radar |
| CN110411952A (en) * | 2019-07-15 | 2019-11-05 | 复旦大学 | The spectroscopic ellipsometry of more channel of polarization faces array detection obtains system and method |
| CN110780452A (en) * | 2019-11-18 | 2020-02-11 | 北京华捷艾米科技有限公司 | Diffraction optical assembly with adjustable diffraction light spot pattern, projection device and diffraction method |
| CN114113167A (en) * | 2021-11-26 | 2022-03-01 | 中国科学技术大学 | X-ray Talbot-Lau grating phase contrast imaging method |
| CN117269143A (en) * | 2023-11-08 | 2023-12-22 | 山西大学 | High-resolution Raman spectrum detection equipment |
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| CN1702452B (en) * | 2004-05-24 | 2011-05-04 | 中国科学院光电技术研究所 | Digital micromirror multi-target imaging spectrometer device |
| CN101389938B (en) * | 2006-01-20 | 2011-03-09 | 法国宇航院（Onera） | Compact optical interferometer of the trilateral shift type |
| CN102183304A (en) * | 2011-01-21 | 2011-09-14 | 北京理工大学 | Optical path structure of cylindrical anastigmatic grating dispersion type imaging spectrometer |
| CN102183304B (en) * | 2011-01-21 | 2016-12-14 | 北京理工大学 | A kind of optical path structure of cylindrical anastigmatic grating dispersion type imaging spectrometer |
| CN102331300A (en) * | 2011-06-14 | 2012-01-25 | 北京卓立汉光仪器有限公司 | Asymmetric monochromator for improving luminous flux and resolution |
| CN102331300B (en) * | 2011-06-14 | 2013-10-23 | 北京卓立汉光仪器有限公司 | Asymmetric monochromator for improving luminous flux and resolution |
| CN105092035A (en) * | 2014-05-09 | 2015-11-25 | 三星电子株式会社 | Spectro-sensor, spectro-sensor module, spectrometer and spectral analysis method |
| CN105092035B (en) * | 2014-05-09 | 2019-02-01 | 三星电子株式会社 | Spectrum sensor, spectrum sensor module and spectrometer and spectroscopic analysis methods |
| CN109682469A (en) * | 2014-09-10 | 2019-04-26 | 电子光子集成电路股份有限公司 | Curve grating spectrograph and wavelength multiplexer or demultiplexer with high wavelength resolution |
| CN109682469B (en) * | 2014-09-10 | 2021-04-02 | 电子光子集成电路股份有限公司 | Curved grating spectrometer and wavelength multiplexer or demultiplexer with extremely high wavelength resolution |
| CN109917354A (en) * | 2019-04-26 | 2019-06-21 | 上海禾赛光电科技有限公司 | Reception device, laser radar and its echo processing techniques of laser radar |
| CN109917354B (en) * | 2019-04-26 | 2020-06-02 | 上海禾赛光电科技有限公司 | Receiving device of laser radar, laser radar and echo processing method thereof |
| CN110411952A (en) * | 2019-07-15 | 2019-11-05 | 复旦大学 | The spectroscopic ellipsometry of more channel of polarization faces array detection obtains system and method |
| CN110411952B (en) * | 2019-07-15 | 2022-05-20 | 复旦大学 | Elliptical polarization spectrum acquisition system and method for multi-polarization channel surface array detection |
| CN110780452A (en) * | 2019-11-18 | 2020-02-11 | 北京华捷艾米科技有限公司 | Diffraction optical assembly with adjustable diffraction light spot pattern, projection device and diffraction method |
| CN110780452B (en) * | 2019-11-18 | 2021-09-21 | 北京华捷艾米科技有限公司 | Diffraction optical assembly with adjustable diffraction light spot pattern, projection device and diffraction method |
| CN114113167A (en) * | 2021-11-26 | 2022-03-01 | 中国科学技术大学 | X-ray Talbot-Lau grating phase contrast imaging method |
| CN114113167B (en) * | 2021-11-26 | 2024-07-09 | 中国科学技术大学 | X-ray Talbot-Lau grating phase contrast imaging method |
| CN117269143A (en) * | 2023-11-08 | 2023-12-22 | 山西大学 | High-resolution Raman spectrum detection equipment |
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