CN204230625U - The adjustable laser device of a kind of bandwidth sum centre wavelength - Google Patents
The adjustable laser device of a kind of bandwidth sum centre wavelength Download PDFInfo
- Publication number
- CN204230625U CN204230625U CN201420700436.7U CN201420700436U CN204230625U CN 204230625 U CN204230625 U CN 204230625U CN 201420700436 U CN201420700436 U CN 201420700436U CN 204230625 U CN204230625 U CN 204230625U
- Authority
- CN
- China
- Prior art keywords
- wave plate
- collimater
- mirror
- centre wavelength
- light
- 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.)
- Active
Links
Landscapes
- Lasers (AREA)
Abstract
The utility model discloses the adjustable laser device of a kind of bandwidth sum centre wavelength, include pumping source, pumping protection device, pump combiner, gain fibre, first collimator, the first quarter-wave plate, the 1/1st wave plate, the first polarization spectro cube, faraday rotation mirror, the 1/2nd wave plate, the second polarization spectro cube, the mutually perpendicular angle mirror of transmission grating, reflecting surface to, speculum and the second collimater.What this case adopted is non-Linear Rotation polarization locked mode and the combining structure with filter effect in chamber, easy realization simple for structure, angle mirror is to can its incident light direction translation relatively, second collimater can the vertical direction translation of its incident light relatively, when not inserting so in the optical path and replace other unnecessary component any, just can realize the continuous tuning of locked mode bandwidth sum centre wavelength respectively, it is applied widely.
Description
[technical field]
The utility model relates to the adjustable laser device of a kind of bandwidth sum centre wavelength.
[background technology]
Along with the utility model of the end of the eighties in last century and beginning of the nineties Ke Er locked mode, the Ge great research institution of the world that is applied in about femto-second laser sprawls rapidly and comes.The generation of femtosecond laser, the locked mode of main dependence seed source, the seed source of the business fs-laser system of now routine is still made up of solid-state element and laser crystal mostly, the seed source relying on this solid-state laser technology to research and develop requires high to humiture, harsh to environmental requirement, and cost intensive, and be not suitable for the universal of industrial ultrafast laser of future generation.
The development of optical fiber mode-locking technique has in recent years promoted the development of ultrafast fibre laser oscillator greatly, laser based on doped with rare-earth elements optical fiber occurred the eighties in 20th century, the appearance of stable ultrashort pulse laser can follow the method that the people such as Menyuk C R in 1989 propose in Pulsepropagation in an elliptically birefringent Kerr medium, fiber gain media is due to elongated, be easy to heat radiation, under same volume, its surface-to-volume compares large 2 ~ 3 orders of magnitude of solid-state laser, the transverse mode of fiber laser is determined by fiber core and numerical aperture in addition, can not change because of thermal deformation, so be easy to keep single mode running, above-mentioned advantage is that solid-state laser can not be compared.The development experience of fiber laser orphan's locked mode, chirped type is pulse mode-locked, self similarity locked mode is to several stages such as Totally positive dispersion locked modes, the Er-doped fiber of early stage femto second optical fiber laser many employings communication wavelength, so orphan's locked mode (soliton mode locking) and chirped pulse mode-locked (stretched pluse) locked mode become prevailing mechanism, after entering the new century, along with the development of highly doped Yb dosed optical fiber, the locked mode theory of self similarity and Totally positive dispersion is suggested, the single pulse energy spirogram of femtosecond fiber oscillator stage is made to breach 10nJ (Chong A, Renninger W H, Wise F.All-normal-dispersionfemtosecond fiber laser with pulse energy above 20nJ), this development makes people have more expectation to femtosecond fiber oscillator.
Double clad rare-earth doped fiber (DCF) is to use multimode pumping with the maximum difference of common single cladding gain optical fiber.In the last few years, although technique and technology improve constantly, the peak power output of single tube single mode 976PUMP is also only at about 1W, and expensive.Compare, developed multimode 976PUMP rapidly in recent years, single tube easily can export tens W W even up to a hundred, and the multimode PUMP of 10W is compared to the single mode PUMP of 1W, its price is only the latter's 1/10th, and the double clad gain fibre amplifying technique constantly emerged in recent years relies on powerful power output and the low price advantage of multimode LD just.Doubly clad optical fiber has two coverings, and inner cladding is smaller, generally only has 5 ~ 10um or large mould field 10 ~ 40um, and inner cladding is used for the transmission of restricting signal light and gain.And surrounding layer general diameter is between 125um ~ 400um, and the numerical aperture had up to 0.46 is used for restriction pump light in internal transmission.Structural design so cleverly; make the more pump light of fiber containment simultaneously; in turn ensure that single mode transport and the amplification of flashlight; this technology and large mould field technology combine; be widely used in the amplifier of communication and laser; but what use in seed source is very few, reason is the restriction of the mode-locking device tolerance power in seed source and the restriction of locked mode mechanism.The people such as the Yue Zhou of the Massachusetts Institute of Technology in 2012 mention in " Nonlinear-polarization-evolution mode-locking in a hybrid cavity:a routetoward low repetition-rate fiber lasers ", they adopt mode pump by NPR mode-locking technique and add that filter effect obtains the locked mode power output of 119mW in an oscillator, single pulse energy is 10nJ to the maximum, and the generally maximum direct output only had about 1 hundred to two hundred milliwatt of our common mode-locked laser, and single pulse energy is in nJ magnitude.The power output of this magnitude uses without general being difficult to of amplification, and this makes the seed source of this type can not directly apply to the ultrafast laser application being similar to the middle low powers such as film delineation.
Therefore, be necessary to overcome the above problems.
[utility model content]
The utility model overcomes the deficiency of above-mentioned technology, provides the adjustable laser device of a kind of bandwidth sum centre wavelength, its flexible adjustment, applied widely.
For achieving the above object, the utility model have employed following technical proposal:
The adjustable laser device of a kind of bandwidth sum centre wavelength, include pumping source 1, described pumping source 1 output is connected with pumping protection device 2 in turn, pump combiner 3, gain fibre 5, and first collimator 7, the emergent light of described first collimator 7 is by the first quarter-wave plate 8, incide in the first polarization spectro cubes 10 after 1/1st wave plate 9, the light that the transmission beam splitting end of described first polarization spectro cubes 10 exports is through faraday rotation mirror 11, incide in the second polarization spectro cubes 13 after 1/2nd wave plate 12, the light that the reflection beam splitting end of described second polarization spectro cubes 13 exports incides in transmission grating 15, be provided with for the diffraction light reflected in parallel through transmission grating 15 being returned the mutually perpendicular angle mirror of reflecting surface of transmission grating 15 to 14 on rear side of described transmission grating 15, described angle mirror can its incident light direction translation relatively to 14, the speculum 16 for the diffraction light for the second time through transmission grating 15 being turned to output is provided with on front side of described transmission grating 15, described speculum 16 turns to the light of output to incide in the second collimater 18 through the second quarter-wave plate 17, described second collimater 18 output is connected with pump combiner 3 one input, described second collimater 18 can the vertical direction translation of its incident light relatively, wherein, the reflection beam splitting end of described first polarization spectro cubes 10 is as the output of fiber laser.
Described first quarter-wave plate the 8, the 1/1st wave plate 9, second quarter-wave plate 17 is all arranged on the wave plate frame of adjustable wave plate incident angle.
Described first polarization spectro cube the 10, second polarization spectro cubes 13 is all arranged on fixing cube mirror holder.
Described 1/2nd wave plate 12 is bonded on described faraday rotation mirror 11, and described faraday rotation mirror 11 is arranged on one and rotates on mirror holder, and described faraday rotation mirror 11 can rotate relative to its rotating shaft.
Described angle mirror is arranged on an angle mirror on translation stage to 14, described angle mirror to 14 can with described angle mirror to the relative angle mirror of translation stage to 14 incident light direction translations.
Described second collimater 18 is arranged on a collimater translation stage, and described second collimater 18 can with the vertical direction translation of relative second collimater 18 incident light of described collimater translation stage.
Pumping source 1 as above is multimode pumping source, and described pumping protection device 2 is multimode pumping protector, and described pump combiner 3 is multimode pump combiner, and described gain fibre 5 is double clad gain fibre; Or described pumping source 1 is mode pump source, described pumping protection device 2 is mode pump protector, and described pump combiner 3 is single mode wavelength division multiplexer, and described gain fibre 5 is single mode gain fibre.
Compared with prior art, the beneficial effects of the utility model are:
1, have employed non-linear rotatory polarization locked mode and there is the combining structure of filter effect in chamber, easy realization simple for structure, angle mirror is to can its incident light direction translation relatively, second collimater can the vertical direction translation of its incident light relatively, when not inserting so in the optical path and replace other unnecessary component any, just can realize the continuous tuning of locked mode bandwidth sum centre wavelength respectively, it is applied widely.
2, the first quarter-wave plate and the 1/1st wave plate are set in turn between first collimator and the first polarization spectro cube, so, by the first quarter-wave plate, the emergent light ovality of first collimator is changed, by the 1/1st wave plate, the polarisation of light direction after by the first quarter-wave plate is changed, two wave plates with the use of light can be changed by the energy ratio after polarizing cubic, the output couple efficiency namely in control impuls locked mode and chamber.
3, between the first polarization spectro cube and the second polarization spectro cube, set gradually faraday rotation mirror and the 2 2/mono-wave plate, so form the relevant isolator effect of a polarization, can the Unidirectional of control chamber inner laser.
4, by arranging the mutually perpendicular angle mirror pair of reflecting surface on rear side of transmission grating, angle mirror is to can its incident light direction translation relatively, translation angle mirror pair like this, can ensure the component propagation all parallel to each other of the different wave length through twice emergent light after transmission grating.
5, the first quarter-wave plate, the 1/1st wave plate, the 1/2nd wave plate, the second quarter-wave plate are all arranged on the wave plate frame of adjustable wave plate incident angle, are convenient to regulate wave plate incident angle.
6, the 1/2nd wave plate is bonded on described faraday rotation mirror, described faraday rotation mirror is arranged on one and rotates on mirror holder, described faraday rotation mirror can rotate relative to its rotating shaft, so, polarisation of light state is regulated by regulating the anglec of rotation of faraday rotation mirror, make that the transmitted light of the second polarization spectro cube is minimum, reverberation is maximum, reach light and turn to the effect with light reverse isolation.
7, described angle mirror is to being arranged on an angle mirror on translation stage, angle mirror to can with described angle mirror to the relative angle mirror of translation stage to the translation of incident light direction, be convenient to translation angle mirror pair.
8, described second collimater is arranged on a collimater translation stage, and the second collimater with the vertical direction translation of the relative second collimater incident light of described collimater translation stage, can be convenient to translation second collimater.
9, pumping source uses multimode pumping, and pumping protection device uses multimode protector, and pump combiner uses multimode pump combiner, and gain fibre uses double clad gain fibre, is convenient to improve pump power and obtain powerful mode-locked laser export.
[accompanying drawing explanation]
Fig. 1 is the index path of this case.
[embodiment]
The utility model feature and other correlated characteristic are described in further detail by embodiment below in conjunction with accompanying drawing, so that the understanding of technical staff of the same trade:
As shown in Figure 1, the adjustable laser device of a kind of bandwidth sum centre wavelength, include pumping source 1, described pumping source 1 output is connected with pumping protection device 2 in turn, pump combiner 3, gain fibre 5, and first collimator 7, the emergent light of described first collimator 7 is by the first quarter-wave plate 8, incide in the first polarization spectro cubes 10 after 1/1st wave plate 9, the light that the transmission beam splitting end of described first polarization spectro cubes 10 exports is through faraday rotation mirror 11, incide in the second polarization spectro cubes 13 after 1/2nd wave plate 12, the light that the reflection beam splitting end of described second polarization spectro cubes 13 exports incides in transmission grating 15, be provided with for the diffraction light reflected in parallel through transmission grating 15 being returned the mutually perpendicular angle mirror of reflecting surface of transmission grating 15 to 14 on rear side of described transmission grating 15, described angle mirror can its incident light direction translation relatively to 14, the speculum 16 for the diffraction light for the second time through transmission grating 15 being turned to output is provided with on front side of described transmission grating 15, described speculum 16 turns to the light of output to incide in the second collimater 18 through the second quarter-wave plate 17, described second collimater 18 output is connected with pump combiner 3 one input, described second collimater 18 can the vertical direction translation of its incident light relatively, wherein, the reflection beam splitting end of described first polarization spectro cubes 10 is as the output of fiber laser.
Described first quarter-wave plate the 8, the 1/1st wave plate 9, second quarter-wave plate 17 is all arranged on the wave plate frame of adjustable wave plate incident angle, wherein, the anglec of rotation of the first quarter-wave plate 8 and the 1/1st wave plate (9) is regulated the locked mode of laser can be regulated whether.
Described first polarization spectro cube the 10, second polarization spectro cubes 13 is all arranged on fixing cube mirror holder.
Described 1/2nd wave plate 12 is bonded on described faraday rotation mirror 11, and described faraday rotation mirror 11 is arranged on one and rotates on mirror holder, and described faraday rotation mirror 11 can rotate relative to its rotating shaft, so that the reverse isolation degree of adjustment laser.
Described angle mirror is arranged on an angle mirror on translation stage to 14, described angle mirror to 14 can with described angle mirror to the relative angle mirror of translation stage to 14 incident light direction translations.
Described second collimater 18 is arranged on a collimater translation stage, and described second collimater 18 can with the vertical direction translation of relative second collimater 18 incident light of described collimater translation stage.
As mentioned above, the locked mode mode that this case uses is non-linear rotatory polarization locked mode, output point is the reflection beam splitting end of the first polarization spectro cubes 10, linearly polarized light is through faraday rotation mirror 11, / 2nd wave plate 12 second polarization spectro cubes 13, transmission grating 15, angle mirror is to 14, transmission grating 15, after speculum 16, elliptically polarized light is changed into by the second quarter-wave plate 17, this elliptically polarized light to be coupled in the second collimater 18 and via the nonlinear effect of the monomode fiber in medium and gain fibre, produce non-linear rotatory polarization effect, phasic difference between the elliptical light major and minor axis at the i.e. each position of now pulse is identical, but the light intensity of pulse middle part is higher than the light intensity on edge before and after pulse.When pulse obtains gain amplification through gain fibre, under the nonlinear effect effect of optical fiber, nonlinear phase shift can be produced, because nonlinear phase shift is relevant with light intensity, thus along the nonlinear phase shift difference that pulse different parts produces, thus make the polarization state at each position of pulse there occurs change, minimum Polarization Dependent Loss is experienced with suitable orientation by polarization relative photo isolator by adjusting light pulse polarization direction that the first quarter-wave plate 8 and the 1/1st wave plate 9 make to be exaggerated, the comprehensive function of this nonlinear polarization rotation effect and wave plate and polarization beam splitting cube, make initial light pulse in optical cavity during iterative cycles, the edge, front and back that its intensity is lower is more and more weak, and peak value is more and more stronger, be equivalent to the impact by saturable absorption bulk effect, finally form stable ultrashort pulse to export.Wherein, the cooperation of the first polarization spectro cubes 10, faraday rotation mirror the 11, the 1/2nd wave plate 12, second polarization spectro cubes 13, plays the effect of reverse isolation, forms unidirectional travelling-wave laser.
As mentioned above, the mechanism of this case locked mode, filtering under Totally positive dispersion is very crucial, in prior art, Normal practice is the method adopting the filter plate inserting prior customized parameter, the thickness of filter plate or angle etc. are inserted to the centre wavelength of the spectrum of locked mode or control for bandwidth by changing, but this setting to bandwidth often can not continuously adjustabe, and centre wavelength and bandwidth are difficult to have adjustment concurrently; Prior art also has the method adopting and insert double grating, compensates to just micro-or negative dispersion, carry out locked mode, but the power output after locked mode is on the low side under such net dispersion condition to the dispersion in chamber.This case adds the filtering adjusting device of the new transmission grating 15 based on monolithic under non-linear rotatory polarization effect, and serving under Totally positive dispersion still can the effect at the bandwidth of controlled filtering and the center of filtering.In the present case, light beam is by after transmission grating 15, light can be dispersed along horizontal direction diffraction, this diverging light second time after angle mirror is to 14 reflected in parallel injects transmission grating 15, because back light is parallel with incident light, so secondary separates in different spatial through the different wave length component of the light beam of transmission grating 15, but all keeping parallelisms, this directional light after the second quarter-wave plate 17, intercept by the second collimater 18 partial spectrum.In the present case by regulating angle mirror just can regulate the space width of the spectrum before inciding the second collimater 18 to translation stage, the length of angle mirror to 14 distance transmission gratings 15 is longer in theory, the effect of spectrum widening is more obvious, the density of spectrum when space development is less, the bandwidth that receives by the second collimater 18 fewer, the center regulating the second collimater 18 to accept light by collimater translation stage just can regulate the centre wavelength of spectrum.This method has certain negative dispersion compensation effect concurrently simultaneously in addition, reduces the chirp value exporting light when long optical fibers.
Embodiment 1:
Described pumping source 1 adopts the multimode pumping source of 976nm; maximum power is at 8W; described pumping protection device 2 is multimode pumping protector; maximum tolerance power 20W; described pump combiner 3 is multimode pump combiner; described gain fibre 5 adopts double cladding large mode field to mix ytterbium gain fibre, mode field diameter 10um.
During enforcement, the exit end of pumping protection device 2 is connected by fused fiber splice with pump combiner 3, the pumping incidence end of described pump combiner 3 is 105/125 multimode fiber, numerical aperture is 0.22, the tail optical fiber of pump combiner 3 is that large mould area double-cladding passive gain is fine, core diameter is 10um, and this passive fiber is connected with gain fibre 5 welding; The gain fibre 5 that the present embodiment adopts is absorbed as 4.1dB/m at 976nm place, and this gain fibre 5 is connected with the single-mode tail fiber welding of first collimator 7; The mode field diameter of single-mode tail fiber is that 10um is to match with gain fibre 5.The output of first collimator 7 is first quarter-wave plate 8 of 12.7mm through diameter, diameter is the 1/1st wave plate 9 of 12.7mm, the length of side is first polarization spectro cubes 10 of 10mm, and faraday rotation mirror 11, be driven in transmission grating 15 after second polarization spectro of diameter to be the 1/2nd wave plate 12 of 12.7mm and the length of side be 10mm cubes 13, the length of described transmission grating 15 is greater than 30mm, incident light after transmission grating 15 diffraction and be driven into angle mirror to 14 in, and be again reflected back transmission grating 15 surface, secondary after transmission grating 15 reflect by speculum 16, and be driven into after eventually passing through the second quarter-wave plate 17 in second collimater 18, the described single-mode tail fiber of the second collimater 18 is connected with an input of pump combiner 3.Angle mirror used in this example to 14, speculum 16 is broadband medium film speculum, bandwidth, at more than 100nm, prevents speculum from producing finite length effect to mode-locked spectrum.
In the present embodiment, by regulating angle mirror to make mode-locked spectrum at about 8 ~ 30nm continuously adjustabe to translation stage, by regulating collimater translation stage, the continuous adjustable light from 1020 ~ 1060nm is obtained.
As mentioned above, in this example, the pump power that pumping source 1 imports to pump combiner 3 is about 5W, is the locked mode femtosecond light output obtaining about 820mW near 1060nm in centre wavelength, bandwidth is more than 30nm, and the pulsewidth obtained measured after the compression of chamber external application linear compressor is at about 100fs.In the power output of the reflection beam splitting end of the first polarization spectro cubes 10 more than 800mW, the magnitude substantially exceeding similar femtosecond fiber oscillator only tens mW or hundred milliwatts exports.
Embodiment 2:
Pumping source after described pumping source 1 adopts the single mode of 976nm to close bundle, maximum power is 500mW.Described pumping protection device 2 is mode pump protector, and maximum tolerance power is at 600mW.Described pump combiner 3 adopts single mode wavelength division multiplexer, and described gain fibre 5 adopts the highly doped gain fibre of single covering, and absorption coefficient is 1200dB/m, be 1030nm place mode field diameter is 4 μm at wavelength.
During enforcement, described pump combiner 3 tail optical fiber, first collimator 7 tail optical fiber, the second collimater 18 tail optical fiber are Hi1060 monomode fiber, so that be connected.The output of first collimator 7 is first quarter-wave plate 8 of 12.7mm through diameter, diameter is the 1/1st wave plate 9 of 12.7mm, the length of side is first polarization spectro cubes 10 of 10mm, and faraday rotation mirror 11, be driven in transmission grating 15 after second polarization spectro of diameter to be the 1/2nd wave plate 12 of 12.7mm and the length of side be 10mm cubes 13, the length of described transmission grating 15 is greater than 30mm, incident light after transmission grating 15 diffraction and be driven into angle mirror to 14 in, and be again reflected back transmission grating 15 surface, secondary after transmission grating 15 reflect by speculum 16, and be driven into after eventually passing through the second quarter-wave plate 17 in second collimater 18, the described single-mode tail fiber of the second collimater 18 is connected with an input of pump combiner 3.Angle mirror used in this example to 14, speculum 16 is broadband medium film speculum, bandwidth, at more than 100nm, prevents speculum from producing finite length effect to mode-locked spectrum.
In the present embodiment, by regulating angle mirror to make mode-locked spectrum at about 8 ~ 30nm continuously adjustabe to translation stage; By regulating collimater translation stage, obtain the locked mode light of centre wavelength from 1020 ~ 1050nm diverse location.
As mentioned above, in this example, the pump power that pumping source 1 imports to wavelength division multiplexer 3 is about 450mW, is when carrying out locked mode near 1040nm in centre wavelength, is about 100mW in the power output of the reflection beam splitting end of the first polarization spectro cubes 10.
As mentioned above, what this case was protected is the adjustable laser device of a kind of bandwidth sum centre wavelength, and all technical schemes identical or close with this case structure all should be shown for falling in the protection range of this case.
Claims (8)
1. the adjustable laser device of bandwidth sum centre wavelength, it is characterized in that including pumping source (1), described pumping source (1) output is connected with pumping protection device (2) in turn, pump combiner (3), gain fibre (5), and first collimator (7), the emergent light of described first collimator (7) is by the first quarter-wave plate (8), incide in the first polarization spectro cube (10) after 1/1st wave plate (9), the light of the transmission beam splitting end output of described first polarization spectro cube (10) is through faraday rotation mirror (11), incide in the second polarization spectro cube (13) after 1/2nd wave plate (12), the light that the reflection beam splitting end of described second polarization spectro cube (13) exports incides in transmission grating (15), described transmission grating (15) rear side is provided with for the diffraction light reflected in parallel through transmission grating (15) being returned the mutually perpendicular angle mirror of reflecting surface of transmission grating (15) to (14), described angle mirror can its incident light direction translation relatively to (14), described transmission grating (15) front side is provided with the speculum (16) for the diffraction light for the second time through transmission grating (15) being turned to output, described speculum (16) turns to the light of output to incide in the second collimater (18) through the second quarter-wave plate (17), described second collimater (18) output is connected with pump combiner (3) input, described second collimater (18) can the vertical direction translation of its incident light relatively, wherein, the reflection beam splitting end of described first polarization spectro cube (10) is as the output of fiber laser.
2. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1, is characterized in that described first quarter-wave plate (8), the 1/1st wave plate (9), the second quarter-wave plate (17) are all arranged on the wave plate frame of adjustable wave plate incident angle.
3. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1, is characterized in that described first polarization spectro cube (10), the second polarization spectro cube (13) is all arranged on fixing cube mirror holder.
4. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1, it is characterized in that described 1/2nd wave plate (12) is bonded on described faraday rotation mirror (11), described faraday rotation mirror (11) is arranged on one and rotates on mirror holder, and described faraday rotation mirror (11) can rotate relative to its rotating shaft.
5. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1, it is characterized in that described angle mirror is arranged on an angle mirror on translation stage to (14), described angle mirror to (14) can with described angle mirror to the relative angle mirror of translation stage to (14) incident light direction translation.
6. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1, it is characterized in that described second collimater (18) is arranged on a collimater translation stage, described second collimater (18) can with the vertical direction translation of described collimater translation stage relative second collimater (18) incident light.
7. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1-6 any one; it is characterized in that described pumping source (1) is for multimode pumping source; described pumping protection device (2) is multimode pumping protector; described pump combiner (3) is multimode pump combiner, and described gain fibre (5) is double clad gain fibre.
8. the adjustable laser device of a kind of bandwidth sum centre wavelength according to claim 1-6 any one; it is characterized in that described pumping source (1) is for mode pump source; described pumping protection device (2) is mode pump protector; described pump combiner (3) is single mode wavelength division multiplexer, and described gain fibre (5) is single mode gain fibre.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201420700436.7U CN204230625U (en) | 2014-11-20 | 2014-11-20 | The adjustable laser device of a kind of bandwidth sum centre wavelength |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201420700436.7U CN204230625U (en) | 2014-11-20 | 2014-11-20 | The adjustable laser device of a kind of bandwidth sum centre wavelength |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN204230625U true CN204230625U (en) | 2015-03-25 |
Family
ID=52928677
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201420700436.7U Active CN204230625U (en) | 2014-11-20 | 2014-11-20 | The adjustable laser device of a kind of bandwidth sum centre wavelength |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN204230625U (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104319617A (en) * | 2014-11-20 | 2015-01-28 | 广东量泽激光技术有限公司 | Laser device adjustable in bandwidth and central wavelength |
| CN106058620A (en) * | 2016-05-30 | 2016-10-26 | 四川广正科技有限公司 | Multi-wavelength synchronous output fiber laser based on nonlinear polarization rotation mode locking |
-
2014
- 2014-11-20 CN CN201420700436.7U patent/CN204230625U/en active Active
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104319617A (en) * | 2014-11-20 | 2015-01-28 | 广东量泽激光技术有限公司 | Laser device adjustable in bandwidth and central wavelength |
| CN104319617B (en) * | 2014-11-20 | 2017-10-31 | 广东量泽激光技术有限公司 | A kind of adjustable laser of bandwidth and centre wavelength |
| CN106058620A (en) * | 2016-05-30 | 2016-10-26 | 四川广正科技有限公司 | Multi-wavelength synchronous output fiber laser based on nonlinear polarization rotation mode locking |
| CN106058620B (en) * | 2016-05-30 | 2019-02-22 | 四川广正科技有限公司 | Multi-wavelength synchronism output optical fiber laser based on nonlinear polarization rotation mode locking |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN104319617A (en) | Laser device adjustable in bandwidth and central wavelength | |
| US5440573A (en) | Method and apparatus for controlling laser emmision wavelength using non-linear effects | |
| CN107069410B (en) | A kind of multipurpose bidirectional passive mode-locking full optical fiber laser system | |
| CN106911060B (en) | The high-efficiency high power mid-infrared laser device of Wavelength tunable | |
| CN107154576B (en) | 2 μm of dissipative solitons mode locked fiber lasers based on SMF-SIMF-GIMF-SMF optical fiber structure | |
| CN102368584A (en) | Passive mode-locking ultrashort pulse all-fiber laser with waveband of 2.0 microns | |
| CN103414093A (en) | All-fiber pulsed laser | |
| CN104466636A (en) | Single-frequency Q-switched pulsed fiber laser | |
| CN107465071A (en) | Optical fiber-solid mixed amplification laser system | |
| CN104078826A (en) | Subpicosecond large-mode-field-area photonic crystal fiber SESAM mode-locked laser | |
| CN106469887B (en) | Double-pass amplifier of photonic crystal fiber | |
| JP2006332666A (en) | Short pulse amplification in 1 micron based on all fibers | |
| KR101394720B1 (en) | Method and apparatus to generate high power femtosecond light pulses by combining nonlinear polarization rotation and saturable absortion | |
| CN102664337A (en) | Terahertz wave source based on ytterbium germanium co-doping micro-structural optical fiber narrow-line-width dual-wavelength laser | |
| CN105896249A (en) | High-power broadband tunable soliton-self-similar pulse mode-locked fiber laser | |
| CN204230625U (en) | The adjustable laser device of a kind of bandwidth sum centre wavelength | |
| Wei et al. | High-power femtosecond pulse generation from an all-fiber Er-doped chirped pulse amplification system | |
| CN110323663A (en) | The apparatus and method of the vector ultrashort laser pulse of infrared band in a kind of generation | |
| CN203883307U (en) | Polarizing beam-combining nonlinear rotating mode-locked laser | |
| CN103618208B (en) | A kind of micro integrated ps pulsed laser and ns pulsed laser module of optical fiber coupling | |
| CN113745951A (en) | Laser device | |
| CN104577695A (en) | High-power intracavity frequency-doubled single-frequency laser device | |
| CN211981129U (en) | Multi-wavelength pulse fiber laser | |
| CN212033416U (en) | All-fiber ultrafast laser based on polarization maintaining fiber cross fusion technology | |
| CN204517141U (en) | Gao Zhongying single longitudinal mode laser |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| TR01 | Transfer of patent right | ||
| TR01 | Transfer of patent right |
Effective date of registration: 20220408 Address after: 528400 zone a, third floor, No. 28, Yuquan Road, Torch Development Zone, Zhongshan City, Guangdong Province Patentee after: GUANGDONG HUAKUAI PHOTON TECHNOLOGY CO.,LTD. Patentee after: Guangdong Huayi Laser Technology Co., Ltd Address before: 528400 floor 3, building 2, Shumao building, No. 6, Xiangxing Road, Torch Development Zone, Zhongshan City, Guangdong Province Patentee before: GUANGDONG LIANGZE LASER TECHNOLOGY Co.,Ltd. |