CN101159365A - Multi-path optical fiber laser coherent beam combination device and coherent beam combination method - Google Patents
Multi-path optical fiber laser coherent beam combination device and coherent beam combination method Download PDFInfo
- Publication number
- CN101159365A CN101159365A CNA2007100187484A CN200710018748A CN101159365A CN 101159365 A CN101159365 A CN 101159365A CN A2007100187484 A CNA2007100187484 A CN A2007100187484A CN 200710018748 A CN200710018748 A CN 200710018748A CN 101159365 A CN101159365 A CN 101159365A
- Authority
- CN
- China
- Prior art keywords
- fiber
- grating
- laser
- optical
- beam combination
- 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
Landscapes
- Lasers (AREA)
Abstract
The invention discloses a multi-channel optical-fiber laser coherence beam combination device and a coherence beam combination method based on overlapped body grating. The device comprises an optical-fiber coupler, a doping double-clad optical-fiber, a lens, a dichroiscope, a reflector, a polarization controller, a reflector, an overlapped body grating and an output coupling mirror connected in sequence at one side of the optical-fiber grating. The method is able to realize the multi-channel optical-fiber laser coherence beam combination without complex phase detection and control to each beam. The phases of each beam realize interlocking by sharing a resonator composed of the output coupling mirror and the optical-fiber grating. Each beam realizes the coherent superposition in the near-field and far-field to significantly enhance the output power and the brightness of the optical-fiber laser through the overlapped body of grating. The invention features the simple structure and complex structure without increasing as the increase of the beam combination laser, and is able to be widely applied in the field needing the large power optical-fiber laser as the light source, thereby capable of gaining the large power, high beam quality as well as compact high-energy laser system.
Description
Technical field
The present invention relates to a kind of laser technology, be specifically related to a kind of multi-channel optical fibre laser coherence beam combination device and coherent beam combination method based on overlapping body grating.
Background technology
Developing high-power, high light beam quality, efficient, compact high-energy laser system, to satisfy the particularly military demand of various application, is the target of the long-term exploratory development in countries in the world.Fiber laser has efficiently, compactness, good beam quality, heat dissipation characteristics is good and characteristics such as output power stability height, and the pliability of optical fiber makes it can be by crooked and adapt to different installation environments neatly and do not influence the output of light beam.Therefore, the competitiveness of fiber laser has huge market considerably beyond other laser, has broad application prospects in industry, medical treatment and military affairs.At industry and medical field, fiber laser can be used for welding and cutting, weld cleaning, laser engraving, punching, product mark, laser detection and various aspects such as measurement, laser imaging, laser radar system and laser medicine, the little processing of medicine equipment.Militarily, the laser of high power (more than the 100kW) can be used for making up ground, space base, satellite-based and carrier-borne High Energy Laser Weapon System, realization has important strategic and tactical value to effective strike of targets such as enemy's guided missile, aircraft, satellite for fields such as air defense, anti-sky and electrooptical countermeasuress.In recent years, along with the appearance of large model area doubly clad optical fiber and the development of high-power semiconductor laser pumping technology, the power output of fiber laser significantly improves, and the power output of single fiber laser has surpassed kilowatt.Yet owing to be subjected to the restriction of the Physical Mechanism such as nonlinear effect, optical damage and fire damage of doped fiber, the power output of above-mentioned single fiber laser is difficult to satisfy the high-power requirement of high-energy laser system.The power output that wants significantly to improve single laser is suitable difficulty not only, and expense is very expensive.Simultaneously, along with the raising of power output, there are defectives such as beam quality variation in single fiber laser.
Summary of the invention
The purpose of this invention is to provide a kind of simple in structurely, easy to use, cost is low, can increase substantially the power output of laser and the multi-channel optical fibre laser coherence beam combination device based on overlapping body grating of brightness.
Another object of the present invention provides the laser coherence beam combination method.
In order to overcome the deficiencies in the prior art, technical scheme to be solved by this invention is achieved in that the multi-channel optical fibre laser coherence beam combination device based on overlapping body grating, its this invention has outstanding substantive distinguishing features and obvious improvement to be that a fiber grating is connected a fiber coupler, the opposite side of its fiber coupler connects two doping double-cladding optical fibers respectively at least, one side of every doping double-cladding optical fiber all is equipped with lens, one side of each lens has dichroic mirror, be equipped with Polarization Controller between dichroic mirror and the speculum, speculum one side has overlapping body grating, overlapping body grating one side has output coupling mirror, output coupling mirror output beam combination light.Said overlapping body grating is meant in the same area of optical medium and writes down the certain thickness a plurality of grating that has that obtains by holographic method.
The coherent beam combination method of the described multi-channel optical fibre laser coherence beam combination device based on overlapping body grating of a kind of claim 1 is characterized in that comprising:
A, when a fiber grating constitutes one side of a plurality of fiber laser resonant cavitys, when the operation wavelength of each Wavelength of Laser and fiber grating was complementary, each fiber laser worked in same wavelength;
B, fiber grating and output coupling mirror constitute optical resonator;
C, fiber grating and output coupling mirror constitute the common resonant chamber of multi-channel optical fibre laser, output coupling mirror feeds back to the part energy of beam combination power in each fiber laser, the optics vibration of each fiber laser checks and balance, thereby makes the phase place interlocking of each optical-fiber laser;
D, an overlapping body grating are beam combination devices, still be a beam splitter simultaneously, along same direction diffraction, simultaneously, also the beam diffraction that output coupling mirror can be reflected becomes the multichannel beamlet to the incident optical laser that it both can satisfy multichannel the Bragg condition by the Bragg angle;
E, an overlapping body grating two-way multiplexing both can have been realized the beam combination to multi-channel optical fibre laser, and also the laser diffraction that output coupling mirror is reflected becomes multi beam to feed back to the phase place interlocking that each fiber laser is realized each fiber laser output beam;
The laser of stimulated emission is coupled into fiber grating by fiber coupler in f, the doping double-cladding optical fiber;
G, an overlapping body grating are to write down the certain thickness a plurality of grating that has that obtains by holographic method in the same area of optical medium, and the number of its grating equates with the number that needs the beam combination optical-fiber laser;
H, one are as light beam k
1And k
iI=1 wherein, 2 ..., N is respectively with body grating K
G1And K
GiThe Bragg angle α that determines
1And α
iIncident, their diffraction light is along same direction outgoing, the grating vector K of body grating
G1And K
GiBetween an included angle is arranged
i, this angle is by Bragg condition cos (φ
i-β)=K
Gi/ 2k decision, wherein β is the angle of diffraction light and z axle positive direction, i.e. Bragg angle, K
Gi=2 π/d
i, d
iBe the grating constant of i grating, k=2 π n/ λ is the transmission of light beam in optical medium, and λ is the incident light wavelength, and n is the mean refractive index of optical medium.
The present invention compared with prior art has following technique effect:
1, can make each road fiber laser be operated in same optical wavelength by a shared fiber grating;
2, by overlapping body grating, can make each road optical-fiber laser realize near field and far field coherent superposition, reach the purpose that significantly promotes optical-fiber laser power output and brightness;
3, the resonant cavity that constitutes by common optical fiber grating and output coupling mirror need not complicated position phase Detection ﹠ Controling, can realize the position phase interlocking of each road optical-fiber laser, realizes long altogether purpose of interfering output;
4, simple in structure, system complexity is with being increased by the increase of beam combination optical-fiber laser number.
Description of drawings
Fig. 1 is apparatus of the present invention structural principle schematic diagram;
Fig. 2 is the overlapping body grating beam combination of a Fig. 1 schematic diagram;
Embodiment
Accompanying drawing is embodiments of the invention.
Below in conjunction with accompanying drawing content of the present invention is described further:
Shown in Figure 1, a kind of multi-channel optical fibre laser coherence beam combination device based on overlapping body grating, an one fiber grating 1 connects a fiber coupler 2, the opposite side of its fiber coupler 2 connects two doping double-cladding optical fibers 3 respectively at least, one side of every doping double-cladding optical fiber 3 all is equipped with lens 4, one side of each lens 4 has dichroic mirror 5, be equipped with Polarization Controller 6 between dichroic mirror 5 and the speculum 7, speculum 7 one sides have overlapping body grating 8, overlapping body grating 8 one sides have output coupling mirror 9, output coupling mirror 9 output beam combination light 10, described output coupling mirror is meant that reflectivity is about transmission/speculum of 4%, in addition, fiber coupler, output coupling mirror, Polarization Controller all has ripe commercially available prod, is the product that the those of ordinary skill of same domain is known.
The coherent beam combination method of the described multi-channel optical fibre laser coherence beam combination device based on overlapping body grating of a kind of claim 1 comprises:
A, when a fiber grating constitutes one side of a plurality of fiber laser resonant cavitys, when the operation wavelength of each Wavelength of Laser and fiber grating was complementary, each fiber laser worked in same wavelength;
B, fiber grating and output coupling mirror constitute optical resonator;
C, fiber grating and output coupling mirror constitute the common resonant chamber of multi-channel optical fibre laser, output coupling mirror feeds back to the part energy of beam combination power in each fiber laser, the optics vibration of each fiber laser checks and balance the phase place interlocking of each optical-fiber laser;
D, an overlapping body grating are beam combination devices, still beam splitter simultaneously, the incident optical laser that it both can satisfy multichannel the Bragg condition by the Bragg angle along same direction diffraction; Simultaneously, the beam diffraction that also output coupling mirror can be reflected becomes the multichannel beamlet;
E, an overlapping body grating two-way multiplexing both can have been realized the beam combination to multi-channel optical fibre laser, and also the laser diffraction that output coupling mirror is reflected becomes multi beam to feed back to the phase place interlocking that each fiber laser is realized each fiber laser output beam;
The laser of stimulated emission is coupled into fiber grating by fiber coupler in f, the doping double-cladding optical fiber;
G, an overlapping body grating are to write down the certain thickness a plurality of grating that has that obtains by holographic method in the same area of optical medium, and the number of its grating equates with the number that needs the beam combination optical-fiber laser;
H, one are as light beam k
1And k
iI=1 wherein, 2 ..., N is respectively with body grating K
G1And K
GiThe Bragg angle α that determines
1And α
iIncident, their diffraction light is along same direction outgoing, the grating vector K of body grating
G1And K
GiBetween an included angle is arranged
i, this angle is by Bragg condition cos (φ
i-β)=K
Gi/ 2k decision, wherein β is the angle of diffraction light and z axle positive direction, i.e. Bragg angle, K
Gi=2 π/d
i, d
iBe the grating constant of i grating, k=2 π n/ λ is the transmission of light beam in optical medium, and λ is the incident light wavelength, and n is the mean refractive index of optical medium.
As shown in Figure 1, all be operated in same wavelength, adopted 1 xN fiber coupler and a fiber grating in the scheme in order to make each fiber laser.The laser of stimulated emission is coupled into fiber grating by fiber coupler in each doping double-cladding optical fiber, because fiber grating has narrower wavelength selectivity, have only when the operation wavelength of optical maser wavelength and fiber grating is complementary, could form effective light beam feedback, thereby force each fiber laser with identical wavelength work.
Make each road laser realize coherent superposition by overlapping body grating:
Overlapping body grating is exactly to write down the certain thickness a plurality of grating that has that obtains by holographic method in the same area of optical medium, and the number of body grating equates with the number that needs the beam combination optical-fiber laser.Because body grating has narrower spectral selectivity, the light beam of specific wavelength has only fully and to satisfy or just have high diffraction efficiency during near Bragg angle (this angle is determined by body grating) incident, and its diffraction efficiency is very low or approach 0 when incident beam does not satisfy the Bragg condition.
In order to introduce bulk of optical feedback, after overlapping body grating, added an output coupling mirror, constitute an optical resonator jointly by this output coupling mirror and fiber grating.Output coupling mirror can enter overlapping body grating with the sub-fraction reflection of beam combination luminous power.Because a good beam combination device also is a good beam splitter simultaneously, therefore by overlapping body grating two-way multiplexing make light beam that the output coupling mirror reflection enters overlapping body grating by each body grating respectively by separately Bragg angle diffraction, form the multi beam diffraction light.These diffraction lights are coupled into respectively in each fiber laser again and form bulk of optical feedback, all some enters into other fiber laser to the energy of different fiber laser like this, thereby the light generation of each fiber laser is checked and balance, reach the purpose of phase place interlocking.
Shown in Figure 2, light beam k
1And k
i(i=1,2 ..., N) respectively with body grating K
G1And K
GiThe Bragg angle α that determines
1And α
iIncident, for the diffraction light that makes them along same direction outgoing (promptly realizing beam combination), body grating is designed so that grating vector K
G1And K
GiBetween a specific included angle is arranged
i, this angle is by Bragg condition cos (φ
i-β)=K
Gi/ 2k decision, wherein β is the angle of diffraction light and z axle positive direction, i.e. Bragg angle, K
Gi=2 π/d
i, d
iBe the grating constant of i grating, k=2 π n/ λ is the transmission of light beam in optical medium, and λ is the incident light wavelength, and n is the mean refractive index of optical medium.Because the polarization direction of each doped fiber output laser may produce variation at random, therefore in light path shown in Figure 1, added Polarization Controller, made each road laser before the overlapping body grating of incident, keep its polarization direction identical to satisfy light beam coherent condition (being that same frequency, same polarization, phasic difference are constant).
Fiber grating and output coupling mirror constitute resonant cavity, realize the position phase interlocking of each road optical-fiber laser:
In sum, the present invention at first forces each fiber laser to be operated in same wavelength by shared same fiber grating, the resonant cavity that constitutes by output coupling mirror and fiber grating then, can make the phase locking of each light beam, at last by overlapping body grating, can make each light beam all realize coherent superposition, reach the purpose that significantly promotes optical-fiber laser power output and brightness near field and far field.This scheme need not each light beam is carried out complicated position phase Detection ﹠ Controling, can realize the coherent beam combination of multi-channel optical fibre laser, needing can be widely used in the field of large-power optical fiber laser as light source, to design obtain high-power, high light beam quality, efficient, compact high-energy laser system is significant.
Embodiment 1
2 road optical-fiber laser coherent beam combination embodiment
The resonance wavelength of fiber grating is 1550nm, and its reflectivity is about 95%; The employing splitting ratio is 50: 50 1 * 2 fiber coupler; Doped fiber is an erbium and ytterbium codoping large model area doubly clad optical fiber, and length is about 1m respectively; The focal length of lens all is about 1.5cm; Pumping source all is operated near the 980nm wavelength, and the peak power output of each pumping source is about 20W; The output laser power under the pump light excitation of two doped fibers is respectively 5.6W and 6.2W; Because the spectral selectivity of fiber grating, two doped fiber output Wavelength of Laser are 1550nm; Dichroic mirror is about 100% to the reflectivity of 980nm light wave, and the transmissivity of 1550nm light wave is about 100%; Adjust the polarization direction identical (perpendicular to paper) that Polarization Controller makes the output laser of 2 road doped fibers respectively; The reflectivity during with 45 incident is about 98% to the 1550nm light wave for two speculums; Two individual overlap of grating are in the same area of bichromate crystal, and the vector of body grating 1 is parallel with plane of crystal, are about 3.6 ° with the angle of the vector of body grating 2; Adjust speculum, the output laser that makes 2 road doped fibers respectively is with angle [alpha]
1=11.9271 ° and α
2=8.3271 ° of corresponding incident body gratings 1 and body grating 2, output angle β=11.9271 of coherent beam combination laser °, beam combination power is about 10.2W, and beam combination efficient is 86%; Output coupling mirror is about 4% to the reflectivity of 1550nm light wave, its part reflection with beam combination power enters overlapping body grating and is diffracted into 2 bundle light, opposite direction enters respectively in 2 road doped fibers and forms bulk of optical feedback this two-beam along former road, thereby the vibration of 2 road doped fibers is checked and balance, realize the phase place interlocking.
Only need change the number of fiber coupler, doped fiber, pump light source, lens and speculum to the beam combination of multi-channel optical fibre laser, the number of body grating also needs consistent with the number that needs beam combination laser simultaneously.
Embodiment 2
As realize 4 road laser beam combinations, only need to adopt 1 * 4 fiber coupler, the doped fiber of 4 same length, near the pumping source of 4 respective wavelength (if erbium-ytterbium co-doped fiber, the pumping source wavelength should be 980nm), 4 lens, 4 dichroic mirrors and 4 speculums, simultaneously should write down 4 body gratings in advance in optical medium, the angle between grating vector is determined by the Bragg condition, can realize the coherent beam combination of 4 road optical-fiber lasers like this.
Claims (2)
1. multi-channel optical fibre laser coherence beam combination device based on overlapping body grating, it is characterized in that a fiber grating (1) connects a fiber coupler (2), the opposite side of its fiber coupler (2) connects two doping double-cladding optical fibers (3) respectively at least, one side of every doping double-cladding optical fiber (3) all is equipped with lens (4), one side of each lens (4) has dichroic mirror (5), be equipped with Polarization Controller (6) between dichroic mirror (5) and the speculum (7), speculum (7) one sides have overlapping body grating (8), and overlapping body grating (8) one sides have output coupling mirror (9).
2. the coherent beam combination method of the described multi-channel optical fibre laser coherence beam combination device based on overlapping body grating of a claim 1 is characterized in that comprising:
A, when a fiber grating constitutes one side of a plurality of fiber laser resonant cavitys, when the operation wavelength of each Wavelength of Laser and fiber grating was complementary, each fiber laser worked in same wavelength;
B, fiber grating and output coupling mirror constitute optical resonator;
C, fiber grating and output coupling mirror constitute the common resonant chamber of multi-channel optical fibre laser, output coupling mirror feeds back to the part energy of beam combination power in each fiber laser, the optics vibration of each fiber laser checks and balance the phase place interlocking of each optical-fiber laser;
D, an overlapping body grating are beam combination devices, still beam splitter simultaneously, the incident optical laser that it both can satisfy multichannel the Bragg condition by the Bragg angle along same direction diffraction; Simultaneously, the beam diffraction that also output coupling mirror can be reflected becomes the multichannel beamlet;
E, an overlapping body grating two-way multiplexing both can have been realized the beam combination to multi-channel optical fibre laser, and also the laser diffraction that output coupling mirror is reflected becomes multi beam to feed back to the phase place interlocking that each fiber laser is realized each fiber laser output beam;
The laser of stimulated emission is coupled into fiber grating by fiber coupler in f, the doping double-cladding optical fiber;
G, an overlapping body grating are to write down the certain thickness a plurality of grating that has that obtains by holographic method in the same area of optical medium, and the number of its grating equates with the number that needs the beam combination optical-fiber laser;
H, one are as light beam k
1And k
iI=1 wherein, 2 ..., N is respectively with body grating K
G1And K
GiThe Bragg angle α that determines
1And α
iIncident, their diffraction light is along same direction outgoing, the grating vector K of body grating
G1And K
GiBetween an included angle is arranged
i, this angle is by Bragg condition cos (φ
i-β)=K
Gi/ 2k decision, wherein β is the angle of diffraction light and z axle positive direction, i.e. Bragg angle, K
Gi=2 π/d
i, d
iBe the grating constant of i grating, k=2 π n/ λ is the transmission of light beam in optical medium, and λ is the incident light wavelength, and n is the mean refractive index of optical medium.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB2007100187484A CN100546131C (en) | 2007-09-27 | 2007-09-27 | Multi-channel optical fibre laser coherence beam combination device and coherent beam combination method based on overlapping body grating |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CNB2007100187484A CN100546131C (en) | 2007-09-27 | 2007-09-27 | Multi-channel optical fibre laser coherence beam combination device and coherent beam combination method based on overlapping body grating |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN101159365A true CN101159365A (en) | 2008-04-09 |
| CN100546131C CN100546131C (en) | 2009-09-30 |
Family
ID=39307339
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CNB2007100187484A Expired - Fee Related CN100546131C (en) | 2007-09-27 | 2007-09-27 | Multi-channel optical fibre laser coherence beam combination device and coherent beam combination method based on overlapping body grating |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN100546131C (en) |
Cited By (18)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101782436A (en) * | 2010-03-19 | 2010-07-21 | 中国科学院上海光学精密机械研究所 | High-power laser multipath optical fiber sampling time waveform measuring device |
| CN103633548A (en) * | 2013-12-13 | 2014-03-12 | 山东海富光子科技股份有限公司 | Spectrum pulse beam-combining fiber laser device based on volume Bragg gratings |
| CN104577692A (en) * | 2014-12-29 | 2015-04-29 | 北京航天控制仪器研究所 | Frequency spectrum beam combining device for frequency selection of fiber grating |
| CN104852270A (en) * | 2015-05-07 | 2015-08-19 | 燕山大学 | Overlapped grating and chirped grating-based dual-wavelength narrow-linewidth fiber laser |
| CN105092531A (en) * | 2015-08-31 | 2015-11-25 | 浙江大学 | Dual-ring resonant cavity-based Mach-Zehnder interferometer optical biosensor |
| CN106025776A (en) * | 2016-07-25 | 2016-10-12 | 华中科技大学 | Laser coherent beam combination coupled resonant cavity of polarization diffraction grating |
| CN106663913A (en) * | 2014-05-28 | 2017-05-10 | 泰勒斯公司 | System for phasing a large number of laser sources |
| CN107732641A (en) * | 2017-11-10 | 2018-02-23 | 山东大学 | High-capacity optical fiber laser |
| CN108780010A (en) * | 2016-01-18 | 2018-11-09 | 通快科研激光两合公司 | Relative phase for optics coherence tomography laser beam measures |
| CN109327261A (en) * | 2018-10-18 | 2019-02-12 | 武汉光迅电子技术有限公司 | A kind of light channel structure of optical repeater |
| WO2020174461A1 (en) | 2019-02-25 | 2020-09-03 | Elbit Systems Electro-Optics Elop Ltd | Systems, devices and methods for optical beam combining |
| CN111988091A (en) * | 2019-05-24 | 2020-11-24 | 华为技术有限公司 | Spatial light coupling device |
| CN112461415A (en) * | 2020-09-27 | 2021-03-09 | 山东大学 | Full-sea-depth self-adaptive high-precision pressure conduction type cone penetration probe based on FBG (fiber Bragg Grating) |
| CN112461434A (en) * | 2020-09-27 | 2021-03-09 | 山东大学 | Full-sea-depth self-adaptive high-precision full-flow penetration spherical probe based on FBG (fiber Bragg Grating) |
| CN112582859A (en) * | 2020-12-14 | 2021-03-30 | 济南量子技术研究院 | Tunable terahertz wave generation device and method |
| CN113794099A (en) * | 2021-11-15 | 2021-12-14 | 中国工程物理研究院激光聚变研究中心 | Composite spectrum synthesizer |
| CN114243452A (en) * | 2022-02-24 | 2022-03-25 | 深圳市星汉激光科技股份有限公司 | Interlocking light path of semiconductor laser |
| EP3931624A4 (en) * | 2019-02-25 | 2023-03-29 | Elbit Systems Electro-Optics Elop Ltd. | Systems, devices and methods for optical beam combining |
-
2007
- 2007-09-27 CN CNB2007100187484A patent/CN100546131C/en not_active Expired - Fee Related
Cited By (29)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101782436B (en) * | 2010-03-19 | 2011-11-09 | 中国科学院上海光学精密机械研究所 | High-power laser multipath optical fiber sampling time waveform measuring device |
| CN101782436A (en) * | 2010-03-19 | 2010-07-21 | 中国科学院上海光学精密机械研究所 | High-power laser multipath optical fiber sampling time waveform measuring device |
| CN103633548A (en) * | 2013-12-13 | 2014-03-12 | 山东海富光子科技股份有限公司 | Spectrum pulse beam-combining fiber laser device based on volume Bragg gratings |
| CN106663913A (en) * | 2014-05-28 | 2017-05-10 | 泰勒斯公司 | System for phasing a large number of laser sources |
| CN106663913B (en) * | 2014-05-28 | 2019-03-15 | 泰勒斯公司 | System for adjusting the phase of a large amount of laser sources |
| CN104577692A (en) * | 2014-12-29 | 2015-04-29 | 北京航天控制仪器研究所 | Frequency spectrum beam combining device for frequency selection of fiber grating |
| CN104577692B (en) * | 2014-12-29 | 2018-10-09 | 北京航天控制仪器研究所 | A kind of frequency spectrum beam merging apparatus of Frequency Selecting by Fiber Bragg Grating |
| CN104852270B (en) * | 2015-05-07 | 2018-12-07 | 燕山大学 | Dual wavelength narrow cable and wide optical fiber laser based on overlapping grating and chirp grating |
| CN104852270A (en) * | 2015-05-07 | 2015-08-19 | 燕山大学 | Overlapped grating and chirped grating-based dual-wavelength narrow-linewidth fiber laser |
| CN105092531A (en) * | 2015-08-31 | 2015-11-25 | 浙江大学 | Dual-ring resonant cavity-based Mach-Zehnder interferometer optical biosensor |
| US11114814B2 (en) | 2016-01-18 | 2021-09-07 | Trumpf Scientific Lasers Gmbh + Co. Kg | Relative phase measurement for coherent combining of laser beams |
| CN108780010A (en) * | 2016-01-18 | 2018-11-09 | 通快科研激光两合公司 | Relative phase for optics coherence tomography laser beam measures |
| CN108780010B (en) * | 2016-01-18 | 2021-03-12 | 通快科研激光两合公司 | Relative phase measurement for coherently combined laser beams |
| CN106025776B (en) * | 2016-07-25 | 2022-02-15 | 华中科技大学 | Laser coherent beam combination coupling resonant cavity of polarization diffraction grating |
| CN106025776A (en) * | 2016-07-25 | 2016-10-12 | 华中科技大学 | Laser coherent beam combination coupled resonant cavity of polarization diffraction grating |
| CN107732641A (en) * | 2017-11-10 | 2018-02-23 | 山东大学 | High-capacity optical fiber laser |
| CN109327261A (en) * | 2018-10-18 | 2019-02-12 | 武汉光迅电子技术有限公司 | A kind of light channel structure of optical repeater |
| CN109327261B (en) * | 2018-10-18 | 2021-05-11 | 武汉光迅电子技术有限公司 | Light path structure of optical repeater |
| WO2020174461A1 (en) | 2019-02-25 | 2020-09-03 | Elbit Systems Electro-Optics Elop Ltd | Systems, devices and methods for optical beam combining |
| EP3931624A4 (en) * | 2019-02-25 | 2023-03-29 | Elbit Systems Electro-Optics Elop Ltd. | Systems, devices and methods for optical beam combining |
| CN111988091A (en) * | 2019-05-24 | 2020-11-24 | 华为技术有限公司 | Spatial light coupling device |
| US11880068B2 (en) | 2019-05-24 | 2024-01-23 | Huawei Technologies Co., Ltd. | Space optical coupling apparatus |
| CN112461415B (en) * | 2020-09-27 | 2021-12-24 | 山东大学 | Full-sea-depth self-adaptive high-precision pressure conduction type cone penetration probe based on FBG (fiber Bragg Grating) |
| CN112461434A (en) * | 2020-09-27 | 2021-03-09 | 山东大学 | Full-sea-depth self-adaptive high-precision full-flow penetration spherical probe based on FBG (fiber Bragg Grating) |
| CN112461415A (en) * | 2020-09-27 | 2021-03-09 | 山东大学 | Full-sea-depth self-adaptive high-precision pressure conduction type cone penetration probe based on FBG (fiber Bragg Grating) |
| CN112582859A (en) * | 2020-12-14 | 2021-03-30 | 济南量子技术研究院 | Tunable terahertz wave generation device and method |
| CN113794099A (en) * | 2021-11-15 | 2021-12-14 | 中国工程物理研究院激光聚变研究中心 | Composite spectrum synthesizer |
| CN113794099B (en) * | 2021-11-15 | 2023-01-13 | 中国工程物理研究院激光聚变研究中心 | Composite spectrum synthesizer |
| CN114243452A (en) * | 2022-02-24 | 2022-03-25 | 深圳市星汉激光科技股份有限公司 | Interlocking light path of semiconductor laser |
Also Published As
| Publication number | Publication date |
|---|---|
| CN100546131C (en) | 2009-09-30 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN100546131C (en) | Multi-channel optical fibre laser coherence beam combination device and coherent beam combination method based on overlapping body grating | |
| CN105814476B (en) | The intensive ripple multiplexed laser of high brightness | |
| US7535631B2 (en) | Method and apparatus for spectral-beam combining of fiber-amplified laser beams using high-efficiency dielectric diffractive gratings | |
| Ciapurin et al. | Incoherent combining of 100-W Yb-fiber laser beams by PTR Bragg grating | |
| US7199924B1 (en) | Apparatus and method for spectral-beam combining of high-power fiber lasers | |
| CN102484348B (en) | Pulse-width converting apparatus and optical amplifying system | |
| CN105591268A (en) | Large power fiber laser with inner cavity frequency doubling | |
| Wang et al. | 1.8-kW simultaneous spectral and coherent combining of three-tone nine-channel all-fiber amplifier array | |
| TWI474060B (en) | Supercontinuum generation system | |
| CN112542761A (en) | Phase bias-based linear cavity mode-locked fiber laser and control method | |
| Linslal et al. | Challenges in coherent beam combining of high power fiber amplifiers: a review | |
| CN102170082A (en) | All-fiber pulsed fiber laser with composite chamber | |
| CN103069668B (en) | Polarization central authorities for the Coherent coupling of strong intracavity beam extract laser cavity | |
| CN111525376B (en) | Based on TM01Vortex laser generation method for mode light conversion and vortex laser | |
| CN100561296C (en) | Laser mutual injection beam combination coupler | |
| WO2018173101A1 (en) | Laser processing device | |
| CN103236639A (en) | Self-injection structure for realizing isotropic medium output linearly polarized single-frequency laser | |
| US20160276798A1 (en) | Fiber coupled modular laser system | |
| Jain et al. | Passive coherent locking of fiber lasers using volume Bragg gratings | |
| Mel'kumov et al. | Pump radiation distribution in multi-element first cladding laser fibres | |
| CN113937601A (en) | Single polarization state and single longitudinal mode optical fiber laser | |
| CN100392449C (en) | Broadband light source | |
| CN101369717A (en) | Multi-light beam coupling high power semiconductor laser unit | |
| CN213602177U (en) | Linear cavity mode-locked fiber laser based on phase offset | |
| US9246304B2 (en) | Pulse shaping device and pulse shaping method |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| C17 | Cessation of patent right | ||
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20090930 Termination date: 20100927 |