CN101294848A - Fourier transform interference spectrometer based on slow ray light velocity controlling technology - Google Patents
Fourier transform interference spectrometer based on slow ray light velocity controlling technology Download PDFInfo
- Publication number
- CN101294848A CN101294848A CNA2008100645398A CN200810064539A CN101294848A CN 101294848 A CN101294848 A CN 101294848A CN A2008100645398 A CNA2008100645398 A CN A2008100645398A CN 200810064539 A CN200810064539 A CN 200810064539A CN 101294848 A CN101294848 A CN 101294848A
- Authority
- CN
- China
- Prior art keywords
- light
- fourier transform
- spectrometer
- controlling technology
- light velocity
- 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
Links
Images
Abstract
The invention aims to provide a Fourier transformation interferometer spectrometer with high spectral resolution, small volume and high stability. The spectrometer can be used for measuring spectrum and is based on the slow light velocity controllable technology. The spectrometer changes the traveling time of light in limited distance by utilizing the slow light technology, that is, utilizing the technology to change the optical path difference between two light paths on the part of interferometer in the spectrometer and enlarging the optical path difference, thereby obviously improving the spectrum sensitivity of the spectrometer, eliminating a control system and a collimating system required for moving a reflecting mirror, simplifying the spectrometer, eliminating vibration and positioning errors and improving stability.
Description
Technical field
The present invention relates to a kind of optical instrument, is exactly a kind of Fourier transform interference spectrometer based on slow ray light velocity controlling technology specifically.
Technical background
In the Fourier transform spectrometer,, most crucial part is an interferometer, is determining highest resolution and other performance index of spectrometer.No matter be the air bearing interferometer, the mechanical bearing interferometer, two index glass mechanical rotation formula interferometers all require a light light path in the two-way light to change, and realize this requirement by mobile index glass usually.But, form to interfere between the two-beam to require index glass and fixed mirror strict vertical.Yet no matter be air bearing method or mechanical bearing method, it is not exclusively vertical that small skew in the index glass moving process or vibration interference all can influence two minute surfaces, even if adopted the dynamic collimation measure, also lag behind, can't eliminate fully, and make equipment more complicated, volume increases, operation inconvenience.In addition, distance that index glass moves and speed all can influence the resolution of interferometer, the long more resolution of displacement is good more in theory, and the interferometer index glass moving range of traditional structure is subjected to the restriction of instrument volume, can not accomplish several meters even tens meters long, this has further limited the resolution of spectrometer.
Summary of the invention
The object of the present invention is to provide a kind ofly can be used for measure spectrum, have the spectral resolution height, volume is little, stability is high Fourier transform interference spectrometer based on slow ray light velocity controlling technology.The object of the present invention is achieved like this: the principle of work of described Fourier transform interference spectrometer based on slow ray light velocity controlling technology is as follows: light is through behind the beam splitter, be divided into two-way light, one the tunnel directly gets to catoptron, another Lu Zexian is through the slower rays medium, get on the catoptron, just two catoptrons are all fixed again; The control of optical path difference is to realize by the light velocity of the light of process in the control slower rays medium, like this, instrument is taken up room to be dwindled, and can make the spectral resolution of instrument higher than original spectrometer, because by the slower rays technology, can make group index become very big, in some cases even up to 10
6So, can make the optical path difference of two light beams very big, just can make spectral resolution very high.
The present invention is based on the Fourier transform interference spectrometer of slow ray light velocity controlling technology, also have following technical characterictic:
(1) described Fourier transform interference spectrometer based on slow ray light velocity controlling technology, the two-way reflection of light mirror that interferometer partly forms interference in the optical system are all fixing.
(2) described Fourier transform interference spectrometer based on slow ray light velocity controlling technology utilizes the slower rays medium to change the optical path difference of two-way light in the interferometer.
(3) described Fourier transform interference spectrometer based on slow ray light velocity controlling technology utilizes the group velocity control system to make the light group velocity realize the slower rays transmission in the slower rays medium.
(4) described Fourier transform interference spectrometer based on slow ray light velocity controlling technology, spectral resolution and group index are proportional.
The present invention uses slow ray light velocity controlling technology and replaces the index glass mobile technology, and all fixing structure of this bimirror has effectively overcome interference such as vibration and external disturbance, improves stability.And light velocity controlling technology can obtain very big group delay, is equivalent to the very big index glass displacement in the conventional interference instrument, has effectively improved spectral resolution, has dwindled the volume of instrument.
Description of drawings
Fig. 1 is conventional interference instrument structure and slower rays interferometer structure contrast synoptic diagram;
Fig. 2 is a structured flowchart of the present invention.
Embodiment
The invention will be further described below in conjunction with accompanying drawing.
Claims (5)
1. Fourier transform interference spectrometer based on slow ray light velocity controlling technology, the course of work is as follows: light is divided into two-way light through behind the beam splitter, one the tunnel directly gets to catoptron, another Lu Zexian gets on the catoptron through the slower rays medium again, and just two catoptrons are all fixed; The control of optical path difference is to realize by the light velocity of the light of process in the control slower rays medium, like this, instrument is taken up room to be dwindled, and can make the spectral resolution of instrument higher than original spectrometer, because by the slower rays technology, can make group index become very big, in some cases even up to 10
6So, can make the optical path difference of two light beams very big, just can make spectral resolution very high.
2. the Fourier transform interference spectrometer based on slow ray light velocity controlling technology according to claim 1 is characterized in that: the two-way reflection of light mirror that interferometer partly forms interference in the optical system is all fixing.
3. the Fourier transform interference spectrometer based on slow ray light velocity controlling technology according to claim 1 is characterized in that: utilize the slower rays medium to change the optical path difference of two-way light in the interferometer.
4. the Fourier transform interference spectrometer based on slow ray light velocity controlling technology according to claim 1 is characterized in that: utilize the group velocity control system to make the light group velocity realize the slower rays transmission in the slower rays medium.
5. the Fourier transform based on slow ray light velocity controlling technology according to claim 1 is interfered kaleidophon, and it is characterized in that: spectral resolution and group index are proportional.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN200810064539A CN100595533C (en) | 2008-05-19 | 2008-05-19 | Fourier transform interference spectrometer based on slow ray light velocity controlling technology |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN200810064539A CN100595533C (en) | 2008-05-19 | 2008-05-19 | Fourier transform interference spectrometer based on slow ray light velocity controlling technology |
Publications (2)
Publication Number | Publication Date |
---|---|
CN101294848A true CN101294848A (en) | 2008-10-29 |
CN100595533C CN100595533C (en) | 2010-03-24 |
Family
ID=40065272
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN200810064539A Expired - Fee Related CN100595533C (en) | 2008-05-19 | 2008-05-19 | Fourier transform interference spectrometer based on slow ray light velocity controlling technology |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN100595533C (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102207459A (en) * | 2010-03-31 | 2011-10-05 | 中国科学院电子学研究所 | Fourier transform chip spectrometer based on integrated light technique |
CN102538715A (en) * | 2011-12-28 | 2012-07-04 | 哈尔滨工业大学 | Dual-frequency laser interferometer straightness measurement device based on slow light materials and measurement method thereof |
CN102564354A (en) * | 2011-12-28 | 2012-07-11 | 哈尔滨工业大学 | Angle measuring device and angle measuring method of double-frequency laser interferometer based on slow-light material |
CN103712691A (en) * | 2013-12-23 | 2014-04-09 | 聚光科技(杭州)股份有限公司 | Fourier transformation spectrograph |
CN103900693A (en) * | 2014-02-18 | 2014-07-02 | 哈尔滨工业大学 | Difference snapshooting type imaging spectrometer and imaging method |
CN104142179A (en) * | 2014-07-28 | 2014-11-12 | 奉化市宇创产品设计有限公司 | Static fixed mirror interferometer |
-
2008
- 2008-05-19 CN CN200810064539A patent/CN100595533C/en not_active Expired - Fee Related
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102207459A (en) * | 2010-03-31 | 2011-10-05 | 中国科学院电子学研究所 | Fourier transform chip spectrometer based on integrated light technique |
CN102538715A (en) * | 2011-12-28 | 2012-07-04 | 哈尔滨工业大学 | Dual-frequency laser interferometer straightness measurement device based on slow light materials and measurement method thereof |
CN102564354A (en) * | 2011-12-28 | 2012-07-11 | 哈尔滨工业大学 | Angle measuring device and angle measuring method of double-frequency laser interferometer based on slow-light material |
CN103712691A (en) * | 2013-12-23 | 2014-04-09 | 聚光科技(杭州)股份有限公司 | Fourier transformation spectrograph |
CN103900693A (en) * | 2014-02-18 | 2014-07-02 | 哈尔滨工业大学 | Difference snapshooting type imaging spectrometer and imaging method |
CN103900693B (en) * | 2014-02-18 | 2015-11-18 | 哈尔滨工业大学 | A kind of fast illuminated imaging spectrometer of difference and formation method |
CN104142179A (en) * | 2014-07-28 | 2014-11-12 | 奉化市宇创产品设计有限公司 | Static fixed mirror interferometer |
Also Published As
Publication number | Publication date |
---|---|
CN100595533C (en) | 2010-03-24 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN100595533C (en) | Fourier transform interference spectrometer based on slow ray light velocity controlling technology | |
JP5725165B2 (en) | Fourier transform spectrometer and Fourier transform spectroscopic method | |
CN102486408B (en) | Light splitting method for multi-light-path interferometer, and multi-light-path interferometer adopting light splitting method | |
CN107764203A (en) | Dual wavelength phase shift interference non-spherical measuring method and device based on part penalty method | |
CN110940830B (en) | Two-axis accelerometer structure based on two-dimensional grating and four-quadrant detector | |
CN104713649B (en) | A kind of Fourier transform spectrometer, interferometer | |
CN107144537B (en) | Method and system for measuring visible light Fourier transform absorption spectrum | |
CN203572578U (en) | Portable Fourier near-infrared spectroscopy | |
WO2014117158A1 (en) | Self calibration for mirror positioning in optical mems interferometers | |
CN111964663B (en) | Optical fiber ring distributed polarization crosstalk bidirectional simultaneous measurement device and method | |
US9557221B1 (en) | Interferometer for Fourier transform infrared spectrometry | |
CN102486572B (en) | Method for implementing multiple light paths | |
JP2013033099A (en) | Optical delay device and optical delay method | |
CN109579995B (en) | Method and device for enhancing static birefringence interference spectrum resolution | |
Zehao et al. | FMCW LiDAR with an FM nonlinear kernel function for dynamic-distance measurement | |
CN101329200A (en) | Two-way output double-corner reflection body interferometer | |
CN106225730B (en) | The big working distance autocollimation of portable combined zeroing high-precision laser and method | |
CN106247992B (en) | A kind of high-precision, wide scope and big working distance autocollimation and method | |
CN201897569U (en) | Interferometer with multiple optical distances | |
CN202329812U (en) | Multiple-optical path interferometer with variable optical path number | |
JP2022138127A (en) | Single beam 3 degree of freedom laser interferometer based on dual line scan camera | |
CN102865821B (en) | Optical-circuit balance type high speed, high resolution laser heterodyne interference measurement method and device | |
CN106052549B (en) | The big working distance autocollimation of combination zeroing high dynamic precision and method | |
CN208012761U (en) | A kind of wide spectrum high-resolution spectra interferometric measuring means | |
CN103162833A (en) | Interference spectroscopical method capable of changing optical distance number and interferometer using the same |
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 | ||
C17 | Cessation of patent right | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20100324 Termination date: 20120519 |