CN107064100A - Fiber Raman spectrometer based on dispersion time-varying - Google Patents
Fiber Raman spectrometer based on dispersion time-varying Download PDFInfo
- Publication number
- CN107064100A CN107064100A CN201611042228.2A CN201611042228A CN107064100A CN 107064100 A CN107064100 A CN 107064100A CN 201611042228 A CN201611042228 A CN 201611042228A CN 107064100 A CN107064100 A CN 107064100A
- Authority
- CN
- China
- Prior art keywords
- light
- optical fiber
- fiber
- raman
- raman spectrometer
- 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
- 239000006185 dispersion Substances 0.000 title claims abstract description 31
- 239000013307 optical fiber Substances 0.000 claims abstract description 53
- 238000001069 Raman spectroscopy Methods 0.000 claims abstract description 48
- 239000000835 fiber Substances 0.000 claims abstract description 42
- 238000001514 detection method Methods 0.000 claims abstract description 14
- 230000000644 propagated effect Effects 0.000 claims abstract description 11
- 239000000203 mixture Substances 0.000 claims description 8
- 238000001228 spectrum Methods 0.000 claims description 8
- KPHWPUGNDIVLNH-UHFFFAOYSA-M diclofenac sodium Chemical compound [Na+].[O-]C(=O)CC1=CC=CC=C1NC1=C(Cl)C=CC=C1Cl KPHWPUGNDIVLNH-UHFFFAOYSA-M 0.000 claims description 7
- 238000012360 testing method Methods 0.000 claims description 7
- 238000000034 method Methods 0.000 claims description 6
- 230000005540 biological transmission Effects 0.000 claims description 4
- 239000004038 photonic crystal Substances 0.000 claims description 4
- 238000005316 response function Methods 0.000 claims description 4
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 3
- 229910021389 graphene Inorganic materials 0.000 claims description 3
- 230000010287 polarization Effects 0.000 claims description 3
- 238000010998 test method Methods 0.000 claims description 2
- 230000008878 coupling Effects 0.000 claims 1
- 238000010168 coupling process Methods 0.000 claims 1
- 238000005859 coupling reaction Methods 0.000 claims 1
- 239000000975 dye Substances 0.000 claims 1
- 230000005622 photoelectricity Effects 0.000 claims 1
- 230000003595 spectral effect Effects 0.000 abstract description 8
- 230000003287 optical effect Effects 0.000 abstract description 6
- 238000013461 design Methods 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 description 6
- 238000001237 Raman spectrum Methods 0.000 description 5
- 210000001367 artery Anatomy 0.000 description 4
- 210000003462 vein Anatomy 0.000 description 4
- UHOVQNZJYSORNB-UHFFFAOYSA-N Benzene Chemical compound C1=CC=CC=C1 UHOVQNZJYSORNB-UHFFFAOYSA-N 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 238000004080 punching Methods 0.000 description 3
- 238000000926 separation method Methods 0.000 description 2
- 239000007787 solid Substances 0.000 description 2
- 244000088413 Matthiola incana Species 0.000 description 1
- 235000011378 Matthiola incana Nutrition 0.000 description 1
- 240000007594 Oryza sativa Species 0.000 description 1
- 235000007164 Oryza sativa Nutrition 0.000 description 1
- 238000003841 Raman measurement Methods 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000009659 non-destructive testing Methods 0.000 description 1
- 235000009566 rice Nutrition 0.000 description 1
- 235000021547 stock Nutrition 0.000 description 1
- 238000004416 surface enhanced Raman spectroscopy Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/65—Raman scattering
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/44—Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
- Spectrometry And Color Measurement (AREA)
Abstract
The invention discloses a kind of fiber Raman spectrometer based on dispersion time-varying, including laser detection system and Raman spectroscopic detection system, it is a kind of using the different phenomenon of speed that different frequency is propagated in dispersive optical fiber, so as to tell the spectrometer of the spectral signature of Raman signal in time domain.Spectrometer does not need traditional light-splitting device, while avoiding complex optical path design, can improve mechanical stability, and device size and weight can be reduced again, saves cost again portable.
Description
Technical field
The present invention relates to Raman spectrometer field, and in particular to a kind of fiber Raman spectrometer based on dispersion time-varying.
Background technology
Raman line is to be found first when Study of Liquid benzene is scattered India physicist Raman nineteen twenty-eight, and it is a kind of
Scattering spectrum.When illumination is mapped on object, there is part light to occur in inelastic scattering, scattered light except identical with incident light
Elastic component it is outer (Rayleigh scattering), also have the composition for increasing than incident light frequency and reducing, the composition that wherein frequency reduces claims
For stockes line, the composition of frequency increase is referred to as anti-stockes line, and twenty percent crossover rate, which is symmetrically distributed in, excites light frequency
Both sides.
This result for mainly being interacted by the optical phonon in molecular vibration, lattice and excitation source of Ramam effect.
When a photon and a molecule interact, a unstable virtual energy state is entered after one photon of molecule absorption,
Then a photon can be radiated quickly, if the at this moment vibration of molecule or rotational energy level are higher than initial energy level, then transmitting
The frequency of photon will be lower than primary photon, referred to as stokes light, otherwise the vibration of molecule or rotational energy level are than initial low, light
The energy of son can increase, and frequency can be improved, and be referred to as anti-Stokes light, record what photon frequency occurred by Raman spectrometer
The change of rule is referred to as Raman spectrum.
Each material has specific vibration or rotational energy level, to that should have a specific Raman line, and it is general not with
Incident wavelength changes and changed, so Raman line is also referred to as fingerprint spectral line, is widely used in the demarcation of object components.
Current Raman spectrum analysis instrument develops into main following several forms:Confocal microscope Raman spectrum, resonance raman
Spectrum, SERS and the enhanced Raman scattering of needle surface, these spectrometers are all by space spectroscopic modes
To obtain spectral information, it is necessary to which the lens of grating and anaberration, light path design is complicated, calibration is also comparatively laborious, and machinery is steady
It is qualitative not high；Simultaneously in the case where CCD sizes are certain, it is impossible to while meeting big spectral measurement ranges and high spectral resolution
It is required that.
The content of the invention
The present invention provides the weight that a kind of fiber Raman spectrometer purpose based on dispersion time-varying is to mitigate spectrometer, together
When ensure resolution ratio in the case of again can expand spectral measurement ranges.
The technical scheme is that：A kind of fiber Raman spectrometer based on dispersion time-varying include laser detection system and
Raman spectroscopic detection system.
Described laser detection system includes pulse laser, first collimator and acousto-optic modulator.
Described Raman spectroscopic detection system includes the second collimater, coupler, the first photodetector and the two the second
Detector, oscillograph, ordinary optic fibre and dispersive optical fiber.
The pulse laser is connected with first collimator by optical fiber, and acousto-optic modulator is opposing parallel with first collimator
Place.
Second collimater is connected with coupler by optical fiber, and the coupler passes through common with the first photodetector
Optical fiber is connected；The coupler is connected with the second photodetector by dispersive optical fiber；First photodetector and second
Photodetection is connected by universal serial bus with oscillograph respectively.
It is preferred that, the ordinary optic fibre length specific dispersion fiber lengths are short.
It is preferred that, the coupler is 3dB photo-couplers.
It is preferred that, the laser is optical fiber locked mode soliton laser, and the laser uses nonlinear polarization rotation side
Formula locked mode, graphene locked mode, make dye passive locked mode or active mode locking.
It is preferred that, the dispersive optical fiber is distributed linear chirp grating or photonic crystal fiber.
It is preferred that, the spectrometer also includes prism group and lens combination.
It is preferred that, the prism group includes reflecting prism and two to colour splitting prism, and the reflecting prism and two is to color separation rib
Mirror is placed in longitudinal direction relative level；The lens group includes front end object lens and rear end object lens, and the lens group is placed in sample
And second between collimater.
A kind of fiber Raman spectrometer method of testing based on dispersion time-varying, methods described comprises the following steps：
1) pulse laser sends pulse laser, and spatial light is formed after first collimator or speculum；
2) a portion light is selected using acousto-optic modulator so that go out light frequency for tens to hundreds of hertz；
3) pulse laser reaches and is reflected and scattered behind object under test surface, and a portion light passes through the second collimater quilt
Optical fiber is collected；
4) reflection and scattered light collected enter coupler by optical fiber, are divided into two-way light；
5) wherein light is propagated in ordinary optic fibre all the way, it is more advanced enter photodetector in, in oscilloscope display pulse, make
For the moment of start time 0；
6) another road light is propagated in dispersive optical fiber, because each frequency content light propagation constant differs in dispersive optical fiber
Sample, another part reflected light and Raman diffused light are after dispersive optical fiber, and the light of different frequency composition reaches the time of detector
It is different, if the receptance function of the detector is f (t)；
7) in the case where parameter is fixed, the delay letter that light of the demarcation with different wave length is propagated in two-way optical fiber
Number, i.e. λ=g (t)；
8) time response function according to measured by fixed relationship, obtains the spectrum of reflected light and Raman light：Raman(λ)
=f (g-1(λ)), its time graph responded is shown on oscillograph.
The beneficial effects of the invention are as follows：A kind of fiber Raman spectrometer based on dispersion time-varying eliminates original space point
Light composition and ccd array detector, the substitute is dispersive optical fiber and high speed detector, can mitigate the weight of spectrometer,
Again can ensure resolution ratio while more extended measurements spectral region；Spectrometer does not need traditional light-splitting device, avoids simultaneously
Complex optical path design, can improve mechanical stability, and device size and weight are reduced again, save cost again portable.This
Spectrometer is the spectrometer differentiated in time domain, and its precision is the speed of response decision by detector, but its measurement range not by
Limitation, and conventional spectrometers are the light splitting on spatial domain, and its resolution ratio is determined by grating length, meet it is high-precision simultaneously, nothing
Method meets the measurement of a wide range of spectrum.
Brief description of the drawings
With reference to the accompanying drawing enclosed, the present invention more purpose, function and advantages will pass through the as follows of embodiment of the present invention
Description is illustrated, wherein：
Fig. 1 shows a kind of structural representation of the fiber Raman spectrometer based on dispersion time-varying of the present invention；
Fig. 2 shows a kind of structural representation of the fiber Raman spectrometer embodiment 2 based on dispersion time-varying of the present invention.
Embodiment
By reference to one exemplary embodiment, the purpose of the present invention and function and the side for realizing these purposes and function
Method will be illustrated.However, the present invention is not limited to one exemplary embodiment as disclosed below；Can by multi-form come
It is realized.The essence of specification is only to aid in the detail of the various equivalent modifications Integrated Understanding present invention.
Hereinafter, embodiments of the invention will be described with reference to the drawings.In the accompanying drawings, identical reference represents identical
Or similar part, or same or like step.
Embodiment 1
Fig. 1 is a kind of structural representation of the fiber Raman spectrometer based on dispersion time-varying of the present invention.As shown in figure 1, one
Planting the fiber Raman spectrometer based on dispersion time-varying includes laser detection system and Raman spectroscopic detection system.
Laser detection system includes pulse laser 101, first collimator 102 and acousto-optic modulator 103；Pulse laser
101 are connected with first collimator 102 by optical fiber, acousto-optic modulator 103 and the opposing parallel placement of first collimator 102, acousto-optic
The pulsed light that modulator 103 is sent reaches testing sample 104 just.
Pulse laser 101 is optical fiber locked mode soliton laser, and pulse laser 101 can use nonlinear polarization rotation
Mode locked mode can also be graphene or dye passive locked mode can also be active mode locking, and locked mode mode is determined according to actual conditions
It is fixed.
Raman spectroscopic detection system includes the second collimater 110, coupler 105, the first photodetector 108 and the second light
Electric explorer 111, oscillograph 109, ordinary optic fibre 106 and dispersive optical fiber 107.
Second collimater 110 is connected with coupler 105 by optical fiber, and coupler 105 passes through with the first photodetector 108
Ordinary optic fibre 106 is connected；Coupler 105 is connected with the second photodetector 111 by dispersive optical fiber 107；First photodetection
The photodetection 111 of device 108 and second is connected by universal serial bus with oscillograph 109 respectively.
Length specific dispersion 107 length of optical fiber of ordinary optic fibre 106 are short.The dispersion of ordinary optic fibre 106 is small, and pulse is short, forms sharp arteries and veins
Punching；The optical fiber of dispersive optical fiber 107 is long, and abbe number is big so that the light delay of two frequencies of each nanometer intervals wavelength can be arrived
500ps or so；Coupler 105 is 3dB photo-couplers；Dispersive optical fiber 107 can be that distributed linear chirp grating can also be
Photonic crystal fiber.
There is more complicated index distribution on the cross section of photonic crystal fiber, usually contain the gas of multi-form arrangement
Hole, the yardstick of stomata is with optical wavelength substantially in same magnitude and through the whole length of device, and the glistening light of waves can be limited in low
Propagate in the fiber cores area of refractive index.
Distributed linear chirp grating is the grating that a kind of longitudinal direction of screen periods along optical fiber changes.
The pulse laser 101 that the present embodiment is used is optical fiber locked mode soliton laser.
The specific method that a kind of fiber Raman spectrometer based on dispersion time-varying obtains spectrum comprises the following steps：
1) optical fiber locked mode soliton laser 101 sends the pulse laser of about 1 micron wave length, and pulse width arrives several for tens
Hundred femtoseconds, spatial light is become after first collimator 102；
2) because the repetition rate of mode-locked laser is very high, a portion light is selected using acousto-optic modulator 103 so that
Go out light frequency for tens to hundreds of hertz；
3) pulse laser reaches and is reflected and scattered behind the surface of testing sample 104, and a portion light can be accurate by second
Straight device 110 is collected by optical fiber；
4) reflection and scattered light collected enter 3dB photo-couplers 105 by optical fiber, are divided into two-way light；
5) wherein light is propagated in ordinary optic fibre 106 all the way, it is more advanced enter photodetector 108 in, because dispersion is small, arteries and veins
Punching is very short, can be a very sharp pulse in oscillograph 109, be used as the moment of start time 0；
6) another road light is propagated in dispersive optical fiber 107, due in each frequency content light propagation constant of dispersive optical fiber 107
Different, another part reflected light and Raman diffused light are after dispersive optical fiber 107, and the light of different frequency composition reaches detector
Time it is different, if the receptance function of the detector be f (t), for moment t is 0 at the time of being previously noted；
7) in the case where parameter is fixed, can demarcate that the light with different wave length propagates in this two-way optical fiber prolongs
When function, i.e. λ=g (t)；
8) according to fixed relationship above and measured time response function, pulse laser is opened up by dispersive optical fiber 107
It is wide after reach at a high speed the second photodetector 111, its respond time graph show on oscillograph 109, obtain reflected light with
The spectrum of Raman light：Raman (λ)=f (g-1(λ))。
Utilize the relation of delay and dispersion, it is possible to obtain corresponding Raman spectrum.Arteries and veins needed for close-in measurement mode
It is very small to rush energy, therefore laser pulse need not be amplified, nor infringement sample surfaces, is a kind of real
Non-Destructive Testing.
Embodiment 2
Fig. 2 is a kind of structural representation of the fiber Raman spectrometer embodiment 2 based on dispersion time-varying of the present invention.This implementation
The difference of example and embodiment 1 is：Added in the structure chart of embodiment 1 reflecting prism 211, two to dichronic mirror 212 and thoroughly
Mirror system 213, realizes that remote Raman Measurement technology suppresses bias light and avoids the influence of fluorescence.
Reflecting prism 211 and testing sample 204 are placed in two reflection directions to dichronic mirror 212, lens combination 213 along light path
It is placed in two transmission directions to dichronic mirror 212.
Wherein, reflecting prism 211 and two is not limited to isosceles right angle to the shape of dichronic mirror 212, can realize laser beam
Reflection and transmission.
The pulse laser 210 that the present embodiment is used is solid state laser Nd:YAG laser.
A kind of specific method of the fiber Raman spectrometer telemeasurement technology based on dispersion time-varying comprises the following steps：
1) solid state laser Nd:YAG laser 210 sends the pulse laser of about 1.064 micron wave lengths, and pulse width is
150 femtoseconds；
2) because the repetition rate of laser is very high, it is necessary to select a portion light using acousto-optic modulator 203 so that
Go out light frequency for tens to hundreds of hertz；
3) pulsed light reaches testing sample 204 after reflecting prism 211 and two reflects to dichronic mirror 212, and two to color separation
Mirror 212 is that shortwave direction is reflected, and long wave direction is transmitted；
4) the reflected impulse light of testing sample 204, is transmitted through two to dichronic mirror 212, and reflected light and scattered light pass through optical lens
Mirror system 213, becomes directional light into collimater 202, the front lens bore of optical lens system is 2 inches to 4 inches, is surveyed
Distance is tried from 1 to 20m；
5) reflected light and scattered light enter 3dB photo-coupler 205, are divided into two-way light；
6) wherein light is propagated in ordinary optic fibre 206 all the way, it is more advanced enter photodetector 208 in, because dispersion is small, arteries and veins
Punching is very short, can be a very sharp pulse in oscillograph 209, be used as the moment of start time 0；
7) light is propagated in dispersive optical fiber 207 all the way in addition, and because optical fiber is long, abbe number is big so that Mei Yina
The light delay of two frequencies of rice interval wavelength can arrive 500ps or so, be higher than the minimum response time of photodetector, so right
In 200nm spectral region, pulse stretcher to 100ns；
Due to dispersive optical fiber 207, each frequency content light propagation constant is different, another part reflected light and Raman scattering
Light is after dispersive optical fiber 207, and the time of the light arrival detector of different frequency composition is different, if the response letter of the detector
Number is f (t), for moment t is 0 at the time of being previously noted；
8) in the case where parameter is fixed, can demarcate that the light with different wave length propagates in this two-way optical fiber prolongs
When function, i.e. λ=g (t)；
9) according to fixed relationship above, and measured time response function, pulse laser is opened up by dispersive optical fiber 207
It is wide after reach at a high speed the second photodetector 214, its respond time graph show on oscillograph 209, obtain reflected light with
The spectrum of Raman light：Raman (λ)=f (g-1(λ))。
With reference to the explanation of the invention disclosed here and practice, other embodiment of the invention is for those skilled in the art
It all will be readily apparent and understand.Illustrate and embodiment is to be considered only as exemplary, of the invention true scope and purport is equal
It is defined in the claims.
Claims (8)
1. a kind of fiber Raman spectrometer based on dispersion time-varying, the fiber Raman spectrometer includes laser detection system and drawing
Graceful spectrum investigating system；
Described laser detection system includes pulse laser, first collimator and acousto-optic modulator；
Described Raman spectroscopic detection system includes the second collimater, coupler, the first photodetector, the second detector, shown
Ripple device, ordinary optic fibre and dispersive optical fiber；
The pulse laser is connected with first collimator by optical fiber, acousto-optic modulator with first collimator is opposing parallel puts
Put；
Second collimater is connected with coupler by optical fiber, and the coupler and the first photodetector pass through ordinary optic fibre
Connection；The coupler is connected with the second photodetector by dispersive optical fiber；First photodetector and the second photoelectricity
Detection is connected by universal serial bus with oscillograph respectively.
2. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 1, it is characterised in that described common
Fiber lengths specific dispersion fiber lengths are short.
3. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 1, it is characterised in that the coupling
Device is 3dB photo-couplers.
4. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 1, it is characterised in that the laser
Device is optical fiber locked mode soliton laser, and the laser uses nonlinear polarization rotation mode locked mode, graphene locked mode, dyestuff quilt
Dynamic locked mode or active mode locking.
5. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 1, it is characterised in that the dispersion
Optical fiber is distributed linear chirp grating or photonic crystal fiber.
6. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 1, it is characterised in that spectrometer is also
Including prism group and lens combination.
7. a kind of fiber Raman spectrometer based on dispersion time-varying according to claim 6, it is characterised in that the prism
Group includes reflecting prism and two to colour splitting prism, and the reflecting prism is placed in two reflection directions to colour splitting prism；The lens
System includes front end object lens and rear end object lens, and lens group is placed in two transmission directions to colour splitting prism.
8. a kind of method of testing of the fiber Raman spectrometer based on dispersion time-varying described in utilization claim 1, methods described
Comprise the following steps：
1) pulse laser sends pulse laser, and spatial light is formed after first collimator or speculum group；
2) acousto-optic modulator selects a portion light so that go out light frequency for tens hertz to hundreds of hertz；
3) pulse laser reaches and is reflected and scattered behind object under test surface, and a portion light is directly over the second collimater quilt
Optical fiber is collected or two become directional light and collected by the second collimater by optical fiber to dichronic mirror transmission and lens combination collection；
4) reflection and scattered light collected enter coupler by optical fiber, are divided into two-way light；
5) wherein light is propagated in ordinary optic fibre all the way, it is more advanced enter photodetector in, in oscilloscope display pulse, as when
Between the moment of starting point 0；
6) another road light is propagated in dispersive optical fiber, because each frequency content light propagation constant is different in dispersive optical fiber,
Another part reflected light and Raman diffused light are after dispersive optical fiber, and the time of the light arrival detector of different frequency composition differs
Sample, if the receptance function of the detector is f (t)；
7) in the case where parameter is fixed, the delay function that light of the demarcation with different wave length is propagated in two-way optical fiber, i.e. λ
=g (t)；
8) time response function according to measured by fixed relationship, obtains the spectrum of reflected light and Raman light：Raman (λ)=f (g-1(λ)), its respond time graph oscillograph on show.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201610972256 | 2016-11-03 | ||
| CN2016109722568 | 2016-11-03 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN107064100A true CN107064100A (en) | 2017-08-18 |
| CN107064100B CN107064100B (en) | 2019-12-27 |
Family
ID=59618294
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201611042228.2A Active CN107064100B (en) | 2016-11-03 | 2016-11-21 | Optical fiber Raman spectrometer based on dispersion time variation |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN107064100B (en) |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108398244A (en) * | 2018-05-02 | 2018-08-14 | 中国人民解放军国防科技大学 | Optical fiber laser parameter real-time measuring device based on inclined fiber bragg grating |
| CN109884025A (en) * | 2019-01-21 | 2019-06-14 | 东莞理工学院 | A kind of long-range SERS spectra detection system and method |
| CN110454142A (en) * | 2019-05-23 | 2019-11-15 | 王恒 | A kind of cable transmission underground LR laser raman testing tool |
| CN110864806A (en) * | 2019-11-15 | 2020-03-06 | 天津大学 | Real-time spectral measurement system based on grating-centered time domain spread dispersion Fourier transform |
| CN111766228A (en) * | 2020-07-14 | 2020-10-13 | 中国科学院西安光学精密机械研究所 | Non-invasive Raman fiber probe |
| CN113109316A (en) * | 2021-03-25 | 2021-07-13 | 东莞市中科原子精密制造科技有限公司 | Miniaturized spectrum detection module and spectrometer |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101464189A (en) * | 2009-01-06 | 2009-06-24 | 中国海洋大学 | Impulse optical spectrometer based on optical fiber dispersion and measuring method thereof |
| EP2522969A2 (en) * | 2011-05-13 | 2012-11-14 | Sony Corporation | Nonlinear raman spectroscopic apparatus comprising single mode fiber for generating Stokes beam |
| CN104777146A (en) * | 2015-03-30 | 2015-07-15 | 中国电子科技集团公司第三十八研究所 | All-optical-fiber raman spectrometer |
| CN105628678A (en) * | 2016-03-02 | 2016-06-01 | 精快激光科技（苏州）有限公司 | Time-resolved Raman spectrometer |
| CN105866100A (en) * | 2016-05-16 | 2016-08-17 | 浙江医药高等专科学校 | Raman spectrum detection optical path device and detection method thereof |
-
2016
- 2016-11-21 CN CN201611042228.2A patent/CN107064100B/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101464189A (en) * | 2009-01-06 | 2009-06-24 | 中国海洋大学 | Impulse optical spectrometer based on optical fiber dispersion and measuring method thereof |
| EP2522969A2 (en) * | 2011-05-13 | 2012-11-14 | Sony Corporation | Nonlinear raman spectroscopic apparatus comprising single mode fiber for generating Stokes beam |
| CN102778448A (en) * | 2011-05-13 | 2012-11-14 | 索尼公司 | Nonlinear Raman spectroscopic apparatus, microspectroscopic apparatus, and microspectroscopic imaging apparatus |
| CN104777146A (en) * | 2015-03-30 | 2015-07-15 | 中国电子科技集团公司第三十八研究所 | All-optical-fiber raman spectrometer |
| CN105628678A (en) * | 2016-03-02 | 2016-06-01 | 精快激光科技（苏州）有限公司 | Time-resolved Raman spectrometer |
| CN105866100A (en) * | 2016-05-16 | 2016-08-17 | 浙江医药高等专科学校 | Raman spectrum detection optical path device and detection method thereof |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN108398244A (en) * | 2018-05-02 | 2018-08-14 | 中国人民解放军国防科技大学 | Optical fiber laser parameter real-time measuring device based on inclined fiber bragg grating |
| CN109884025A (en) * | 2019-01-21 | 2019-06-14 | 东莞理工学院 | A kind of long-range SERS spectra detection system and method |
| CN110454142A (en) * | 2019-05-23 | 2019-11-15 | 王恒 | A kind of cable transmission underground LR laser raman testing tool |
| CN110864806A (en) * | 2019-11-15 | 2020-03-06 | 天津大学 | Real-time spectral measurement system based on grating-centered time domain spread dispersion Fourier transform |
| CN111766228A (en) * | 2020-07-14 | 2020-10-13 | 中国科学院西安光学精密机械研究所 | Non-invasive Raman fiber probe |
| CN113109316A (en) * | 2021-03-25 | 2021-07-13 | 东莞市中科原子精密制造科技有限公司 | Miniaturized spectrum detection module and spectrometer |
Also Published As
| Publication number | Publication date |
|---|---|
| CN107064100B (en) | 2019-12-27 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN107064100A (en) | Fiber Raman spectrometer based on dispersion time-varying | |
| Monat et al. | Integrated optical auto-correlator based on third-harmonic generation in a silicon photonic crystal waveguide | |
| Yüksel et al. | Analysis and suppression of nonlinear frequency modulation in an optical frequency-domain reflectometer | |
| US8300230B2 (en) | System and method to determine chromatic dispersion in short lengths of waveguides using a 3-wave interference pattern and a single-arm interferometer | |
| Kim et al. | Mapping of intermodal beat length distribution in an elliptical-core two-mode fiber based on Brillouin dynamic grating | |
| EP2096430A2 (en) | Apparatus and method for obtaining images using coherent anti-stokes Raman scattering | |
| CN106093962B (en) | A kind of interference velocity-measuring system and method | |
| Galle et al. | Single-arm three-wave interferometer for measuring dispersion of short lengths of fiber | |
| Volikova et al. | Laser vibrometer-rangefinder based on self-sweeping fiber laser | |
| Pelusi et al. | Terahertz bandwidth RF spectrum analysis of femtosecond pulses using a chalcogenide chip | |
| US10816720B2 (en) | Optical fiber with specialized figure-of-merit and applications therefor | |
| US20220187126A1 (en) | Broadband pulsed light source apparatus | |
| JP4463828B2 (en) | Measuring method, measuring apparatus and measuring program for wavelength dispersion of optical waveguide | |
| Lee et al. | Determination of the differential mode delay of a multimode fiber using Fourier-domain intermodal interference analysis | |
| JP2020190498A (en) | Broad-band pulse light source device, spectroscopic measuring device and spectroscopic measuring method | |
| JPH08334435A (en) | Method and equipment to measure nonlinear refractive index of single-mode optical fiber | |
| Ahn et al. | New optical frequency domain differential mode delay measurement method for a multimode optical fiber | |
| JP2006242634A (en) | Method and apparatus for dispersion measurement of optical transmission medium | |
| CN104344892B (en) | A kind of full optical fiber Frequency Domain Interferometer | |
| Fernández et al. | Method for real-time measurement of the nonlinear refractive index | |
| Rhodes et al. | Accuracy and precision in broadband laser ranging | |
| Rahmouni et al. | Hyperspectral photon-counting optical time domain reflectometry | |
| Inoue et al. | Very long range quasi-Fourier spectroscopy for narrowband lasers | |
| CN109506788A (en) | Optical wavelength measurement system based on Fourier's mode-locked laser | |
| DE102018205722A1 (en) | Distance measurement by reflectometry in optical waveguides |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |