CN108365509A - A kind of optical fiber laser of length scanning - Google Patents
A kind of optical fiber laser of length scanning Download PDFInfo
- Publication number
- CN108365509A CN108365509A CN201810213778.9A CN201810213778A CN108365509A CN 108365509 A CN108365509 A CN 108365509A CN 201810213778 A CN201810213778 A CN 201810213778A CN 108365509 A CN108365509 A CN 108365509A
- Authority
- CN
- China
- Prior art keywords
- optical fiber
- resonant
- light
- mirror
- grating
- 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
- 239000013307 optical fiber Substances 0.000 title claims abstract description 86
- 239000000835 fiber Substances 0.000 claims abstract description 32
- 230000003287 optical effect Effects 0.000 claims abstract description 23
- 239000004065 semiconductor Substances 0.000 claims abstract description 17
- 230000003321 amplification Effects 0.000 claims abstract description 7
- 238000003199 nucleic acid amplification method Methods 0.000 claims abstract description 7
- 239000000203 mixture Substances 0.000 claims abstract description 6
- 239000006185 dispersion Substances 0.000 claims description 6
- 230000010287 polarization Effects 0.000 claims description 3
- 238000001228 spectrum Methods 0.000 abstract description 4
- 230000003595 spectral effect Effects 0.000 description 6
- 238000003384 imaging method Methods 0.000 description 5
- 230000008520 organization Effects 0.000 description 5
- 238000005259 measurement Methods 0.000 description 4
- 238000012014 optical coherence tomography Methods 0.000 description 4
- 238000004611 spectroscopical analysis Methods 0.000 description 3
- 238000004891 communication Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 230000001360 synchronised effect Effects 0.000 description 2
- 230000002792 vascular Effects 0.000 description 2
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000001914 filtration Methods 0.000 description 1
- 230000003760 hair shine Effects 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
- 230000003019 stabilising effect Effects 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/0675—Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
-
- 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
- G01J3/02—Details
- G01J3/10—Arrangements of light sources specially adapted for spectrometry or colorimetry
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
- H01S3/06754—Fibre amplifiers
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- General Physics & Mathematics (AREA)
- Lasers (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention discloses a kind of optical fiber lasers of length scanning, including resonant cavity, fiber optic collimator mirror, the optical fiber filter and speculum that narrow linewidth quickly scans, resonant cavity is by semiconductor optical amplifier, optical fiber circulator and coupler composition, optical fiber filter is made of plane reflection grating and resonant mirror, the fluorescence of semiconductor optical amplifier transmitting passes through optical fiber circulator, fiber optic collimator mirror and resonant mirror are irradiated on plane reflection grating, the incident light of different wave length is diffracted into different directions after plane reflection grating, one of wavelength is impinged perpendicularly under some incidence angle of resonant mirror on speculum and backtracking, it is coupled into semiconductor optical amplifier, resonance amplification forms laser, it is exported via coupler.The present invention generates the very narrow laser light source of line width in each moment, and wavelength does mechanical periodicity or scanning at any time, and signal-to-noise ratio greatly improves, and the resolution ratio of spectrum greatly improves, and sweep speed can be more up to tens of thousands of times per second.
Description
Technical field
The present invention relates to laser light source technical fields, and in particular to a kind of optical fiber laser of length scanning.
Background technology
When optical-fiber laser passes through beam splitter, it is divided into two-way, all the way as light is referred to, another way passes through lens imaging system
When focusing illumination organic organization, there is scattering in organic organization to incident light, when scatter light with reference to the interference of light when, interference signal it is strong
The phase of scattering strength of the degree depending on organic organization, interference signal depends on scattering depth and optical source wavelength, but interference signal
It is very faint.Therefore, the interference of light and reference light is scattered to Mr. Yu's depth, the phase of interference signal only depends on the wave of light
Long, there are one additional phase shifts for the scattering interference of light of different depth.
When the wavelength of light fixes frequency high-velocity scanning, all interference signals from different depth are all with the wavelength of light
The mechanical periodicity of same frequency is done, therefore up to tens thousand of times of amplification can be carried out to the AC signal, is effectively detected out not
Scattering with tissue to light, to realize to the real-time non-invasively imaged of organic organization.Therefore, the key technology of the imaging is wavelength
The fiber laser light source quickly scanned.Specifically, imaging depth depends on scattering loss of the organic organization to light, and depth bounds take
Certainly in the coherence length of optical-fiber laser, depth resolution depends on the range of length scanning.
Invention content
The technical problem to be solved by the present invention is to reduce cost, realize that wavelength is swept using ready-made fiber optic communication component
It retouches.
In order to solve the above-mentioned technical problem, it is sharp to be to provide a kind of optical fiber of length scanning for the technical solution adopted in the present invention
Light device, including optical fiber filter and speculum that resonant cavity, fiber optic collimator mirror, narrow linewidth quickly scan, the resonant cavity by
Semiconductor optical amplifier SOA, optical fiber circulator and coupler composition, the optical fiber filter is by plane reflection grating and resonance
Microscope group at,
The fluorescence of the semiconductor optical amplifier SOA transmittings passes through the optical fiber circulator, the fiber optic collimator mirror and institute
It states resonant mirror to be irradiated on the plane reflection grating, the incident light of different wave length is diffracted into after the plane reflection grating
Different directions, one of wavelength impinge perpendicularly on the speculum and former under some incidence angle of the resonant mirror
Road returns, and is coupled into the semiconductor optical amplifier SOA, and resonance amplification forms laser, exported via the coupler.
Preferably, the instantaneous line width of the optical fiber laser depends on the institute that the plane reflection grating and resonant mirror form
State the line width of optical fiber filter.
Preferably, the plane reflection grating diffration grating equation is：
Λ [sin (θ)+sin (β)]=m λ；
Wherein, θ and β is respectively angle of light and the angle of diffraction, and Λ is screen periods, and m is the order of diffraction, and λ is incident light true
Aerial wavelength；
When light again passes by the plane reflection grating along backtracking, grating dispersion is represented by：
Preferably, according to Gaussian beam, the optical fiber filter that is made of the plane reflection grating and resonant mirror
Line width is expressed as：
Wherein, W is width of light beam, and W/cos θ are that light beam is radiated at the width on the plane reflection grating, and N shines for light beam
The raster diffraction stripe number being mapped to；
When the resonant mirror rotates Δ φ angles, incidence angle variation of the light beam on the plane reflection grating is 2 Δs
φ, the maximum rotation angle Δ φ of the resonant mirror0Corresponding wavelength change is wavelength scanning range Δ λ, according to described
Plane reflection grating diffration grating equation, wavelength scanning range Δ λ are represented by：
Δλ≈2Δφ(t)Λcos(θ0)。
Preferably, the cycle period of light turns over line width δ λ much smaller than the optical fiber filterGratingTime.
Preferably, in order to realize wavelength mode locking, the length for the fibre delay line being inserted into the optical path is：
Wherein, f is the frequency of the optical fiber filter, and n is optical fibre refractivity.
Preferably, the wavelength line width of the optical fiber laser output is δ λ, is less than the line width δ λ of the optical fiber filterGrating,
Depending on the resonant loss of the resonant cavity, the coherence length of the optical fiber laser is expressed as：
Preferably, the optical fiber of the fiber optic collimator mirror and the composition resonant cavity is polarization-maintaining single-mode fiber or non-polarization-maintaining list
Mode fiber, when the optical fiber for constituting the resonant cavity is non-polarization-maintaining single-mode fiber, by increasing optical fiber controller adjustment control light
Polarization orientation.
Preferably, dispersion compensation device is equipped between the plane reflection grating and resonant mirror.
Preferably, output end is coupled out light appropriate as feedback, controls the resonant frequency of the resonant mirror, to remain same
Step resonance.
The present invention proposes a kind of optical fiber laser of length scanning, and the very narrow laser light of line width is generated in each moment
Source, and wavelength does mechanical periodicity or scanning at any time, so that complicated spectral measurement is become simple time resolved spectroscopy and measures,
Signal-to-noise ratio greatly improves, and the resolution ratio of spectrum greatly improves, and sweep speed can be more up to tens of thousands of times per second, can be used for optics phase
Dry tomoscan (OCT) is imaged and is diagnosed for eye ground structure and vascular distribution.
Description of the drawings
Fig. 1 is a kind of optical fiber laser structure schematic diagram of length scanning in the present invention；
Fig. 2 is the optical fiber laser structure schematic diagram of medium wave long scan mode locking of the present invention；
Fig. 3 is the output light spectrogram of the optical fiber laser of medium wave long scan of the present invention.
Specific implementation mode
In order to reduce cost, using ready-made fiber optic communication component, the present invention proposes a kind of optical fiber of length scanning
Laser generates the very narrow laser light source of line width in each moment, and wavelength does mechanical periodicity or scanning at any time, makes complexity
Spectral measurement become simple time resolved spectroscopy and measure, can be used for optical coherence tomography (OCT) imaging and use
It is diagnosed in eye ground structure and vascular distribution.
The present invention is described in detail with specific implementation mode with reference to the accompanying drawings of the specification.
An embodiment of the present invention provides a kind of optical fiber lasers of length scanning, as shown in Figure 1, including resonant cavity, optical fiber
The optical fiber filter and speculum 20 that collimating mirror 10, narrow linewidth quickly scan, resonant cavity by semiconductor optical amplifier SOA30,
Optical fiber circulator 40 and coupler 50 form, and optical fiber filter is made of plane reflection grating 60 and resonant mirror 70,
The fluorescence of semiconductor optical amplifier SOA30 transmittings passes through optical fiber circulator 40, fiber optic collimator mirror 10 and resonant mirror 70
It being irradiated on plane reflection grating 60, the incident light of different wave length is diffracted into different directions after plane reflection grating 60,
One of wavelength is impinged perpendicularly under some incidence angle of resonant mirror 70 on speculum 20 and backtracking, is coupled into
Semiconductor optical amplifier SOA30, resonance amplification form laser, are exported via coupler 50.
Resonant mirror 70 can realize length scanning using the off-resonance speculum of high speed resonant speculum or Linear Driving.
The coupling efficiency of coupler 50 is variable, can optimize the line width and power of laser output.
Fiber optical circulator 40 has the function of isolator so that light can only pass through semiconductor optical amplifier according to a direction
SOA30 and amplification of resonating forms laser, then exported by coupler 50.So that the fiber laser light source of length scanning is in each wink
Between generate the very narrow laser light source of line width, and wavelength does mechanical periodicity or scanning at any time, and complicated spectral measurement is made to become letter
Single time resolved spectroscopy measures.
The instantaneous line width of optical fiber laser depends primarily on the optical fiber filtering that plane reflection grating 60 and resonant mirror 70 form
The line width of device.
The diffraction grating equation of plane reflection grating 60 is：
Λ [sin (θ)+sin (β)]=m λ；
Wherein, θ and β is respectively angle of light and the angle of diffraction, and Λ is screen periods, and m is the order of diffraction, and λ is incident light true
Aerial wavelength；
When light again passes by plane reflection grating 60 along backtracking, grating dispersion is represented by：
In view of Gaussian beam, the line width for the optical fiber filter being made of plane reflection grating 60 and resonant mirror 70 indicates
For：
Wherein, W is width of light beam, and W/cos θ are that light beam is radiated at the width on plane reflection grating 60, and N irradiates for light beam
The raster diffraction stripe number arrived, the wider light beam of use can be irradiated to more raster diffraction stripes, so that optical fiber is filtered
The line width of wave device is narrower, in addition, using the plane reflection grating 60 of high fringe density, can equally make the line of optical fiber filter
Width is narrower.
When resonant mirror 70 rotates Δ φ angles, incidence angle variation of the light beam on plane reflection grating 60 is 2 Δ φ, altogether
The maximum rotation angle Δ φ of galvanometer 700Corresponding wavelength change is wavelength scanning range Δ λ, according to plane reflection grating
60 diffraction grating equation, wavelength scanning range Δ λ are represented by：
Δλ≈2Δφ(t)Λcos(θ0)。
We used small variable approximation sinx ≈ x (x ＜ ＜ 1) herein.The maximum rotation angle Δ φ of resonant mirror 700
Corresponding wavelength change is wavelength scanning range Δ λ or free spectral range (FSR).In order to allow the light of some wavelength to exist
The enough numbers of oscillation in resonant cavity and amplified, then the length of resonant cavity must be short as much as possible, the cycle of light one week when
Between line width δ λ are turned over much smaller than optical fiber filterGratingTime.
As shown in Fig. 2, realize resonance amplification to allow the light of each wavelength to can be transferred through optical fiber filter, it can be in the optical path
Be inserted into one section of fibre delay line, allow just by the wavelength of optical fiber filter at the time of next cycle is identical again by light
Fiber filter, such optical fiber filter is synchronous in resonator cavity resonance with light, i.e., wavelength be locked out or wavelength mode locking optical fiber
Laser.
In order to realize wavelength mode locking, the length for the fibre delay line being inserted into the optical path is：
Wherein, f is the frequency of optical fiber filter, and n is optical fibre refractivity.As f=8kHz, n=1.47, fibre delay line
L=1.275 kilometers of length.When fibre delay line is inserted in the light path of fiber optic collimator mirror 10, it is the length of be inserted in it is humorous
The half of the length for intracavitary of shaking.
The wavelength line width of optical fiber laser output is δ λ, is less than the line width δ λ of optical fiber filterGrating, depend on resonant cavity
The coherence length of resonant loss, optical fiber laser is expressed as：
Fiber optic collimator mirror 10 and the optical fiber for constituting resonant cavity are polarization-maintaining single-mode fiber or non-polarization-maintaining single-mode fiber, work as composition
When the optical fiber of resonant cavity is non-polarization-maintaining single-mode fiber, the polarization orientation for increasing optical fiber controller adjustment control light is needed.
In order to which the wavelength in a broadband can synchronously multipass be made of resonant mirror 70 and plane reflecting grating 60
Optical fiber filter, between plane reflection grating 60 and resonant mirror 70 be equipped with corresponding dispersion compensation device.
Output end is coupled out light appropriate (light that the present embodiment is 10%) as feedback, controls the resonance frequency of resonant mirror 70
Rate, to maintain synchro-resonance, to obtain stable luminous power output.After the resonant frequency of resonant mirror 70 is stablized, pass through tune
The driving current of whole semiconductor optical amplifier SOA30 further maintains light power stabilising.By setting semiconductor optical amplifier
The driving current limit of SOA30 works normally model to ensure that the adjustment of driving current does not exceed semiconductor optical amplifier SOA30
It encloses.
As shown in figure 3, the output light spectrogram of the optical fiber laser quickly scanned for wavelength, in each moment, wavelength is swept
The optical fiber laser output retouched is the very narrow laser light source of a line width.Since wavelength is scanning, time averagely upper this swashs
Radiant is equivalent to wideband light source, and according to the characteristic of laser resonant, power and spectral bandwidth are far wider than similar wideband light source.
Such as 1310 nano waveband semiconductor laser super-fluorescence light source spectral width about 70nm, the scanning of the wave band
Light source is obtained with 150 nanometers.For typical 5 milliwatt wideband light source, power is distributed in 70 nano wave length bandwidth.So
And scanning light source is but readily available 40-50 milliwatts, optical power distribution is in 0.1 nanometer or narrower of wave-length coverage.Unit light
The luminous power of wavelength is 1000-10000 times of common wide light source.Therefore, the fiber laser light source of length scanning removes and is applied to
Optical tomography (OCT) imaging is outer, applies also for light sensing, signal-to-noise ratio greatly improves.
When the measurement of luminous power is synchronous with length scanning, change curve, that is, spectrum of power and time, light source is equal to
One spectrometer.The resolution ratio of spectrum can be much better than bulky expensive spectrometer, and sweep speed can be more up to
Tens of thousands of times per second or higher.This is that conventional spectrograph is unable to reach.
The present invention is not limited to above-mentioned preferred forms, anyone structure change made under the inspiration of the present invention,
The technical schemes that are same or similar to the present invention are each fallen within protection scope of the present invention.
Claims (10)
1. a kind of optical fiber laser of length scanning, which is characterized in that quickly swept including resonant cavity, fiber optic collimator mirror, narrow linewidth
The optical fiber filter and speculum retouched, the resonant cavity is by semiconductor optical amplifier SOA, optical fiber circulator and coupler group
At, the optical fiber filter is made of plane reflection grating and resonant mirror,
The fluorescence of semiconductor optical amplifier SOA transmitting passes through the optical fiber circulator, the fiber optic collimator mirror and described total
Galvanometer is irradiated on the plane reflection grating, and the incident light of different wave length is diffracted into difference after the plane reflection grating
Direction, one of wavelength impinges perpendicularly on the roads the speculum Shang Bingyuan under some incidence angle of the resonant mirror and returns
It returns, is coupled into the semiconductor optical amplifier SOA, resonance amplification forms laser, exported via the coupler.
2. the optical fiber laser of length scanning as described in claim 1, which is characterized in that the instantaneous line of the optical fiber laser
Width depends on the line width for the optical fiber filter that the plane reflection grating and resonant mirror form.
3. the optical fiber laser of length scanning as claimed in claim 2, which is characterized in that the plane reflection grating diffration
Grating equation is：
Λ [sin (θ)+sin (β)]=m λ；
Wherein, θ and β is respectively angle of light and the angle of diffraction, and Λ is screen periods, and m is the order of diffraction, λ be incident light in a vacuum
Wavelength；
When light again passes by the plane reflection grating along backtracking, grating dispersion is represented by：
4. the optical fiber laser of length scanning as claimed in claim 3, which is characterized in that according to Gaussian beam, by described flat
The line width of the optical fiber filter of face reflecting grating and resonant mirror composition is expressed as：
Wherein, W is width of light beam, and W/cos θ are that light beam is radiated at the width on the plane reflection grating, and N is irradiated to for light beam
Raster diffraction stripe number；
When the resonant mirror rotates Δ φ angles, incidence angle variation of the light beam on the plane reflection grating is 2 Δ φ, institute
State the maximum rotation angle Δ φ of resonant mirror0Corresponding wavelength change is wavelength scanning range Δ λ, anti-according to the plane
Grating diffration grating equation is penetrated, wavelength scanning range Δ λ is represented by：
Δλ≈2Δφ(t)Λcos(θ0)。
5. the optical fiber laser of length scanning as claimed in claim 4, which is characterized in that the cycle period of light is much smaller than described
Optical fiber filter turns over line width δ λGratingTime.
6. the optical fiber laser of length scanning as claimed in claim 5, which is characterized in that in order to realize wavelength mode locking, in light
The length for the fibre delay line being inserted into road is：
Wherein, f is the frequency of the optical fiber filter, and n is optical fibre refractivity.
7. the optical fiber laser of length scanning as claimed in claim 6, which is characterized in that the wave of the optical fiber laser output
Long line width is δ λ, is less than the line width δ λ of the optical fiber filterGrating, the resonant loss of the resonant cavity is depended on, the optical fiber swashs
The coherence length of light device is expressed as：
8. the optical fiber laser of length scanning as described in claim 1, which is characterized in that the fiber optic collimator mirror and composition
The optical fiber of the resonant cavity is polarization-maintaining single-mode fiber or non-polarization-maintaining single-mode fiber, when the optical fiber for constituting the resonant cavity is non-polarization-maintaining
When single mode optical fiber, by the polarization orientation for increasing optical fiber controller adjustment control light.
9. the optical fiber laser of length scanning as described in claim 1, which is characterized in that the plane reflection grating and resonance
Dispersion compensation device is equipped between mirror.
10. the optical fiber laser of length scanning as described in claim 1, which is characterized in that output end is coupled out light appropriate
As feedback, the resonant frequency of the resonant mirror is controlled, to maintain synchro-resonance.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201810213778.9A CN108365509B (en) | 2018-03-15 | 2018-03-15 | Optical fiber laser with wavelength scanning function |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201810213778.9A CN108365509B (en) | 2018-03-15 | 2018-03-15 | Optical fiber laser with wavelength scanning function |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN108365509A true CN108365509A (en) | 2018-08-03 |
| CN108365509B CN108365509B (en) | 2024-09-06 |
Family
ID=63000269
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201810213778.9A Active CN108365509B (en) | 2018-03-15 | 2018-03-15 | Optical fiber laser with wavelength scanning function |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN108365509B (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109856823A (en) * | 2019-04-03 | 2019-06-07 | 南开大学 | A kind of wavelength-swept source system and its wavelength tuning method |
Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005347668A (en) * | 2004-06-07 | 2005-12-15 | Sun Tec Kk | Wavelength scanning type fiber laser optical source |
| JP2008107141A (en) * | 2006-10-24 | 2008-05-08 | Institute Of National Colleges Of Technology Japan | Optical wavelength detection type physical quantity measuring sensor using ring resonator and bragg grating |
| JP2008191369A (en) * | 2007-02-05 | 2008-08-21 | Nippon Telegr & Teleph Corp <Ntt> | Filter system the high-speed wavelength-swept light source |
| CN102969651A (en) * | 2012-11-27 | 2013-03-13 | 上海理工大学 | Rapid K-space linear frequency sweep laser source |
| CN103247935A (en) * | 2013-04-19 | 2013-08-14 | 王枫秋 | Optical anisotropy saturable absorption device, manufacturing method and pulse laser based on device |
| CN104697634A (en) * | 2015-03-11 | 2015-06-10 | 华中科技大学 | Very high resolution spectral measurement device and method |
| CN208045930U (en) * | 2018-03-15 | 2018-11-02 | 执鼎医疗科技（杭州）有限公司 | A kind of optical fiber laser of length scanning |
-
2018
- 2018-03-15 CN CN201810213778.9A patent/CN108365509B/en active Active
Patent Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005347668A (en) * | 2004-06-07 | 2005-12-15 | Sun Tec Kk | Wavelength scanning type fiber laser optical source |
| JP2008107141A (en) * | 2006-10-24 | 2008-05-08 | Institute Of National Colleges Of Technology Japan | Optical wavelength detection type physical quantity measuring sensor using ring resonator and bragg grating |
| JP2008191369A (en) * | 2007-02-05 | 2008-08-21 | Nippon Telegr & Teleph Corp <Ntt> | Filter system the high-speed wavelength-swept light source |
| CN102969651A (en) * | 2012-11-27 | 2013-03-13 | 上海理工大学 | Rapid K-space linear frequency sweep laser source |
| CN103247935A (en) * | 2013-04-19 | 2013-08-14 | 王枫秋 | Optical anisotropy saturable absorption device, manufacturing method and pulse laser based on device |
| CN104697634A (en) * | 2015-03-11 | 2015-06-10 | 华中科技大学 | Very high resolution spectral measurement device and method |
| CN208045930U (en) * | 2018-03-15 | 2018-11-02 | 执鼎医疗科技（杭州）有限公司 | A kind of optical fiber laser of length scanning |
Non-Patent Citations (1)
| Title |
|---|
| 曹雪;余有龙;刘盛春;李若明;陈雪峰;: "具有有源闭合腔的光纤光栅传感系统地址查询技术", 光学学报, no. 08 * |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109856823A (en) * | 2019-04-03 | 2019-06-07 | 南开大学 | A kind of wavelength-swept source system and its wavelength tuning method |
Also Published As
| Publication number | Publication date |
|---|---|
| CN108365509B (en) | 2024-09-06 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CA2527930C (en) | Process and apparatus for a wavelength tuning source | |
| JP5898077B2 (en) | Filter ASE sweep source for OCT medical imaging | |
| US7705992B2 (en) | Optical coherence tomography system | |
| US9207121B2 (en) | Cavity-enhanced frequency comb spectroscopy system employing a prism cavity | |
| WO2008093448A9 (en) | Wavelength scanning light source and optical coherence tomography device | |
| CN103181754A (en) | Method and apparatus for performing optical imaging using frequency-domain interferometry | |
| JP2006080384A (en) | Wavelength scanning fiber laser source | |
| CN208045930U (en) | A kind of optical fiber laser of length scanning | |
| CN108365509A (en) | A kind of optical fiber laser of length scanning | |
| CN111227797B (en) | Nonlinear effect enhanced sweep frequency light source | |
| JP5223064B2 (en) | Wavelength scanning laser light source | |
| JPH03278014A (en) | Reflection type optical scanning tunneling microscope | |
| JP2019054223A (en) | Wavelength sweeping light source |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| 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 |