CN206619782U - 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices - Google Patents

800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices Download PDF

Info

Publication number
CN206619782U
CN206619782U CN201621353116.4U CN201621353116U CN206619782U CN 206619782 U CN206619782 U CN 206619782U CN 201621353116 U CN201621353116 U CN 201621353116U CN 206619782 U CN206619782 U CN 206619782U
Authority
CN
China
Prior art keywords
optical fiber
fiber laser
gao zhongying
laser
amplifier
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
Application number
CN201621353116.4U
Other languages
Chinese (zh)
Inventor
吕志国
李强龙
杨直
李峰
杨小君
王屹山
赵卫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
XiAn Institute of Optics and Precision Mechanics of CAS
Original Assignee
XiAn Institute of Optics and Precision Mechanics of CAS
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by XiAn Institute of Optics and Precision Mechanics of CAS filed Critical XiAn Institute of Optics and Precision Mechanics of CAS
Priority to CN201621353116.4U priority Critical patent/CN206619782U/en
Application granted granted Critical
Publication of CN206619782U publication Critical patent/CN206619782U/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Lasers (AREA)

Abstract

The utility model discloses one kind 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices, belong to laser technology and non-linear optical field, solve existing apparatus using block titanium gem crystal as the problems such as space optical path caused by gain media is various, complicated, stability is poor.800 ± 100nm wave band Gao Zhongying full optical fiber lasers generation device includes mode locked fiber laser, Polarization Controller, the online polarizer, dispersion delayer, the first optical fiber prime amplifier, frequency controller, the second optical fiber prime amplifier and the main amplifier being sequentially connected by optical fiber.Polarization principle of adjustment and control is carried out based on the pulse exported to mode locked fiber laser, reach shaping spectrum effects, nonlinear effect in optical fiber is combined while by the amplification of subsequent gain optical fiber power, the Gao Zhongying full optical fiber laser device exported with 800 ± 100nm wave bands is realized.Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device can be used as Gao Zhongying titanium precious stone laser amplifier high-performance, highly integrated optical fiber seed source.

Description

800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices
Technical field
The utility model is related to fiber laser device technical field, more particularly to one kind 800 ± 100nm wave band Gao Zhongyings are complete Optical-fiber laser generation device.
Background technology
With the development of laser science, output peak wavelength is widely used in 780nm high energy titanium precious stone laser light source In research fields such as higher hamonic wave generation, chirped pulse generation and astrophysics, with important value.Locked mode titanium precious stone laser kind Component extremely wide emission spectra (700nm-900nm) provides adequate condition for the development of high-peak power ti sapphire laser, makes It still can maintain shorter pulsewidth while high-energy is exported.However, 700nm-900nm Ti∶Sapphire laser mode-locked laser kinds Component needs expensive Nd:YVO4/Nd:YLF frequency multiplication 532nm laser pumpings, cause its expensive, space structure various and It is difficult in maintenance.Secondly, for output wavelength in 700nm-900nm, the μ J of repetition hundred kHz, pulse energy μ J- tens Ti∶Sapphire laser swashs For light device, it is typically the realization of relative difficulty.And hundred kHz, the ti sapphire laser that J grades of pulse energy μ needs to use TEC even liquid nitrogen refrigerating, cause it is complicated and expensive.This is mainly due to the low thermal conductivity of Ti doped saphire With efficiency.These limiting factors promote researcher to try to explore new technological means again to go to realize that cheap, performance is steady Fixed reliable hundred kHz, J grades of μ 700-900nm LASER Light Sources make up the deficiency of existing titanium precious stone laser light source to a certain extent.
Utility model content
In consideration of it, be necessary to provide a kind of high-performance, 800 ± 100nm wave bands highly integrated, non-maintaining and that cost can be reduced Gao Zhongying full optical fiber laser generation device.
One kind 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices, including the locked mode being sequentially connected by optical fiber Optical fiber laser, Polarization Controller, the online polarizer, dispersion delayer, the first optical fiber prime amplifier, frequency controller, second Optical fiber prime amplifier and main amplifier.
In one of the embodiments, the mode locked fiber laser is vibrated using the inclined mode-locked fiber lasers of ytterbium all risk insurance are mixed Device, wherein, mode-locking device is semiconductor saturable absorbing mirror, graphene, CNT or topological insulator.
In one of the embodiments, the power output of the mode locked fiber laser is less than 100mW, centre wavelength 1000-1100nm, 10 ± 5nm of spectral width, repetition are less than 100MHz, and pulse width is less than 20ps.
In one of the embodiments, the Polarization Controller uses Polarization Holding Fibers.
In one of the embodiments, the online polarizer uses polarization-maintaining fiber, and is operated in single polarization state.
In one of the embodiments, the dispersion delayer is less than 2000m polarization-maintaining fibers using length.
In one of the embodiments, the first optical fiber prime amplifier uses length to mix ytterbium single mode gain fibre for 1m Diode fibre core pump laser amplifier, output signal power is less than 250mW.
In one of the embodiments, the frequency controller is used based on acoustooptical effect device or based on optical kerr effect Device.
In one of the embodiments, the second optical fiber prime amplifier is diode pumping ytterbium-doped double-cladded-layer gain fibre Laser amplifier.
In one of the embodiments, the main amplifier is using melting splicing photonic crystal gain fibre laser amplifier Device, photonic crystal gain fibre uses space pumping or bundling device welding pumping, and pump mode is forward pumping or backward pumping.
Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device 100, is realized using all -fiber integrated technology High-performance, highly integrated 700-900nm LASER Light Sources with the output of Gao Zhongying high-energy, overcome existing apparatus and use Ti∶Sapphire laser The shortcomings of space structure is various caused by laser technology, Operation and Maintenance is difficult so that above-mentioned 800 ± 100nm wave bands Gao Zhongying is complete The structure of optical-fiber laser generation device 100 is relatively simple, and cost is relatively low, and has the advantages that highly reliable, non-maintaining.
Brief description of the drawings
Fig. 1 is the structural representation of 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices of an embodiment.
Fig. 2 is the output light spectrogram of mode locked fiber laser 10 of embodiment 1.
Fig. 3 regulates and controls for the output light of mode locked fiber laser 10 of embodiment 1 through Polarization Controller 20 with the online polarizer 30 Output light spectrogram afterwards.
Fig. 4 is defeated in 700-900nm wave bands for 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices of embodiment 1 Go out spectrogram.
Embodiment
In order that the purpose of this utility model, technical scheme and advantage become apparent from, it is right below in conjunction with drawings and Examples The utility model is further elaborated.It should be appreciated that specific embodiment described herein is only to explain this reality With new, it is not used to limit the utility model.
Referring to Fig. 1,800 ± 100nm wave band Gao Zhongying full optical fiber lasers generation device 100 of an embodiment, including The mode locked fiber laser 10 that is sequentially connected by optical fiber, Polarization Controller 20, the online polarizer 30, dispersion delayer 40, One optical fiber prime amplifier 50, frequency controller 60, the second optical fiber prime amplifier 70 and main amplifier 80.
Specifically, Polarization Controller 20 is placed between mode locked fiber laser 10 and the online polarizer 30, modelocked fiber swashs Light device 10 is placed in the front end of Polarization Controller 20, and is connected with Polarization Controller 20 by optical fiber.The laser generator is All -fiber melts splicing construction.The online front end of the polarizer 30 is connected with the other end of Polarization Controller 20 by optical fiber.Dispersion postpones Device 40 is placed in the online rear end of the polarizer 30, and is spliced with the online polarizer 30 by fiber fuse.Mode locked fiber laser 10 is sent out Go out seed pulse sequence to transmit by Polarization Controller 20 and inject therewith after the line polarizer 30 by dispersion delayer 40 successively The adjacent side of the first optical fiber prime amplifier 50.First optical fiber prime amplifier 50 is placed in dispersion delayer 40 and frequency controller 60 Between, the front end of the first optical fiber prime amplifier 50 is connected in the opposite side of dispersion delayer 40 by optical fiber.Frequency controller 60 is placed in The rear end of first optical fiber prime amplifier 50, and melt splicing with the first optical fiber prime amplifier 50.Second optical fiber prime amplifier 70 is placed in Between frequency controller 60 and main amplifier 80.Second optical fiber prime amplifier 70 is placed in the opposite side of frequency controller 60, and with frequency Rate controller 60 is connected by optical fiber.Main amplifier 80 is placed in the opposite side of the second optical fiber prime amplifier 70, and with the second predispersed fiber The melting splicing of amplifier 70, the other end is used as output.
Mode locked fiber laser 10, which is used, mixes the inclined mode-locked fiber lasers oscillator of ytterbium all risk insurance, wherein, mode-locking device can be Semiconductor saturable absorbing mirror, graphene, CNT or topological insulator etc..
The power output of mode locked fiber laser 10<100mW, centre wavelength 1000-1100nm, 10 ± 5nm of spectral width, Repetition<100MHz, pulse width<20ps.
Polarization Controller 20 uses Polarization Holding Fibers.
The online polarizer 30 uses polarization-maintaining fiber, and is operated in single polarization state.
Dispersion delayer 40 use length for<2000m polarization-maintaining fibers.
First optical fiber prime amplifier 50 uses length to be put for 1m ytterbium single mode gain fibre diode fibre core pumping laser of mixing Big device, output signal power<250mW.
Frequency controller 60 is using based on acoustooptical effect device or based on optical kerr effect device.
Second optical fiber prime amplifier 70 is diode pumping ytterbium-doped double-cladded-layer gain fibre laser amplifier.
Main amplifier 80 is using melting splicing photonic crystal gain fibre laser amplifier.Photonic crystal gain fibre can be with Using space pumping or bundling device welding pumping.Pump mode can be forward pumping or backward pumping.
Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device, based on what is exported to mode locked fiber laser Pulse carries out polarization principle of adjustment and control, reaches shaping spectrum effects, and light is combined while by the amplification of subsequent gain optical fiber power Nonlinear effect in fibre, realizes the Gao Zhongying full optical fiber laser device exported with 800 ± 100nm wave bands.Above-mentioned 800 ± 100nm wave band Gao Zhongying full optical fiber lasers generation device can be as Gao Zhongying titanium precious stone laser amplifier high-performance, highly integrated Optical fiber seed source.
Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device 100, is realized using all -fiber integrated technology High-performance, highly integrated 700-900nm LASER Light Sources with the output of Gao Zhongying high-energy, overcome existing apparatus and use Ti∶Sapphire laser The shortcomings of space structure is various caused by laser technology, Operation and Maintenance is difficult so that above-mentioned 800 ± 100nm wave bands Gao Zhongying is complete The structure of optical-fiber laser generation device 100 is relatively simple, and cost is relatively low, and has the advantages that highly reliable, non-maintaining.
Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device 100, using high-gain, high efficiency, bloom Beam quality, outstanding thermal diffusivity optical fiber as gain and transmitting medium, overcome block Ti doped saphire it is inefficient, it is low dissipate The defect such as hot so that it has the advantages that to support Gao Zhongying high-power output.
Above-mentioned 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device 100, using diode laser pumped, gram Titanium precious stone laser technology has been taken using expensive Nd:YVO4/Nd:The defect of YLF frequency double laser pumpings so that it has The advantage of low cost.
Embodiment 1
In 800 ± 100nm wave band Gao Zhongying full optical fiber lasers generation device 100 as shown in Figure 1, mode locked fiber laser 10 select output center wavelength 1030.8nm, spectrum full width at half maximum 10nm, power 22.3mW, pulsewidth 10ps, repetition 45MHz The extreme optical generator of SESAM locked mode all risk insurances.Polarization Controller 20 uses the online optical fiber polarization controller of hand, and fiber type is HI1060.The online polarizer 30 uses PM980 polarization-maintaining fibers.Dispersion delayer 40 is polarization maintaining single mode optical fiber, length For 1100m.First optical fiber prime amplifier 50 selects centre wavelength 976nm, power output 388mW single mode laser diodes, polarization-maintaining Wavelength division multiplexer, length are that 1m polarizes the diode fibre core pumping list that ytterbium single mode gain fibre (PM-YSF-HI) composition is mixed in holding Mould laser amplifier.The full polarization fiber acousto-optic device that frequency controller 60 is produced using Gooch&Housego companies.Second Optical fiber prime amplifier 70 uses centre wavelength 976nm, and power output is 791mW, core diameter 105 μm of multimode laser diodes, polarization-maintainings Pumping laser bundling device, length are that 60cm polarizations keep ytterbium-doped double-cladded-layer gain fibre (PLMA-YDF-10/125-VIII) to constitute Cladding pumping laser amplifier.Main amplifier 80 uses power output 9W, and 105 μm of multimode laser diodes, polarization-maintainings of core diameter are more The length that mould pump combiner and NKT companies produce is 2m, 40 μm of core diameter, 200 μm of polarization-maintaining photonic crystal gain light of cladding diameter The fine melt that fibre is constituted connects gain module.
Above mode locked fiber laser 10, Polarization Controller 20, the online polarizer 30, dispersion delayer 40, the first optical fiber Prime amplifier 50, frequency controller 60, the second optical fiber prime amplifier 70 and main amplifier 80 are spliced using fiber fuse, are not had Any space optical path.The pulse train that mode locked fiber laser 10 is sent is carried out partially through Polarization Controller 20 and the online polarizer 30 Shake regulation and control, and then the wave spectrum output required for obtaining, as shown in Figure 3.
First optical fiber prime amplifier 50 is entered through dispersion delayer 40 by the pulse after spectral modulation, in 388mW 976nm Under single-mode laser pumping, incident spectral modulation pulse mixes ytterbium single mode gain fibre by 1m and is amplified to 210mW.By first Pulse train after optical fiber prime amplifier 50 is downconverted to 275.9kHz by frequency controller 60, by the second optical fiber prime amplifier 70 The output of 10mW, 275.9kHz laser is further obtained after amplification.Main amplifier 80 exports the second optical fiber prime amplifier 70 Amplification pulse laser further amplifies, and in combination with the nonlinear optical effect in amplification process, finally generates 700-900nm Wave band of laser is exported, and output spectrum is as shown in Figure 4.
It the above is only preferred embodiment of the present utility model, it is noted that for the ordinary skill people of the art Member, on the premise of the utility model principle is not departed from, can also make some improvements and modifications, and these improvements and modifications also should It is considered as protection domain of the present utility model.

Claims (10)

1. one kind 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices, it is characterised in that including by optical fiber successively The mode locked fiber laser of connection, Polarization Controller, the online polarizer, dispersion delayer, the first optical fiber prime amplifier, frequency control Device processed, the second optical fiber prime amplifier and main amplifier.
2. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described Mode locked fiber laser, which is used, mixes the inclined mode-locked fiber lasers oscillator of ytterbium all risk insurance, wherein, mode-locking device is that semiconductor saturable is inhaled Receive mirror, graphene, CNT or topological insulator.
3. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described The power output of mode locked fiber laser is less than 100mW, and centre wavelength 1000-1100nm, 10 ± 5nm of spectral width, repetition is small In 100MHz, pulse width is less than 20ps.
4. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described Polarization Controller uses Polarization Holding Fibers.
5. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described The online polarizer uses polarization-maintaining fiber, and is operated in single polarization state.
6. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described Dispersion delayer is less than 2000m polarization-maintaining fibers using length.
7. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described First optical fiber prime amplifier uses length to mix ytterbium single mode gain fibre diode fibre core pump laser amplifier, output letter for 1m Number power is less than 250mW.
8. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described Frequency controller is used based on acoustooptical effect device or based on optical kerr effect device.
9. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that described Second optical fiber prime amplifier is diode pumping ytterbium-doped double-cladded-layer gain fibre laser amplifier.
10. 800 ± 100nm wave bands Gao Zhongying full optical fiber laser generation device as claimed in claim 1, it is characterised in that institute Main amplifier is stated using melting splicing photonic crystal gain fibre laser amplifier, photonic crystal gain fibre uses space pumping Or bundling device welding pumping, pump mode is forward pumping or backward pumping.
CN201621353116.4U 2016-12-09 2016-12-09 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices Active CN206619782U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201621353116.4U CN206619782U (en) 2016-12-09 2016-12-09 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201621353116.4U CN206619782U (en) 2016-12-09 2016-12-09 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices

Publications (1)

Publication Number Publication Date
CN206619782U true CN206619782U (en) 2017-11-07

Family

ID=60229397

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201621353116.4U Active CN206619782U (en) 2016-12-09 2016-12-09 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices

Country Status (1)

Country Link
CN (1) CN206619782U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106451049A (en) * 2016-12-09 2017-02-22 中国科学院西安光学精密机械研究所 800+/-100 nm waveband high-repetition-frequency and all-fiber laser generating device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106451049A (en) * 2016-12-09 2017-02-22 中国科学院西安光学精密机械研究所 800+/-100 nm waveband high-repetition-frequency and all-fiber laser generating device
CN106451049B (en) * 2016-12-09 2023-10-03 中国科学院西安光学精密机械研究所 800 + -100 nm wave band high-repetition frequency all-fiber laser generating device

Similar Documents

Publication Publication Date Title
US9246296B2 (en) Laser or amplifier optical device seeded with nonlinearly generated light
CN101826696A (en) High-energy low-repetition-frequency fiber laser
CN102801095A (en) Generating laser pulses of narrow spectral linewidth based on chirping and stretching of laser pulses and subsequent power amplification
Petrov et al. Picosecond Yb-doped tapered fiber laser system with 1.26 MW peak power and 200 W average output power
CN100470347C (en) Narrow pulse fiber amplifier
CN104466636A (en) Single-frequency Q-switched pulsed fiber laser
Chamorovskiy et al. High-repetition-rate Q-switched holmium fiber laser
Hao et al. Divided-pulse nonlinear amplification and simultaneous compression
CN103972779A (en) Polarization combination nonlinear rotary mode locking method
Su et al. Kilowatt high average power narrow-linewidth nanosecond all-fiber laser
Li et al. Hybrid CPA system comprised by fiber-silicate glass fiber-single crystal fiber with femtosecond laser power more than 90 W at 1 MHz
CN104409952A (en) Double-cladding thulium-doped all-fiber ultrafast laser based on nonlinear polarization rotation mode locking
CN103474868A (en) Thulium-doped all-fiber laser device capable of outputting high-power 2-micron linearly polarized laser
Li et al. Large dispersion-managed broadband high-energy fiber femtosecond laser system with sub 300 fs pulses and high beam quality output
CN206619782U (en) 800 ± 100nm wave band Gao Zhongying full optical fiber laser generation devices
CN106451049A (en) 800+/-100 nm waveband high-repetition-frequency and all-fiber laser generating device
CN103904534A (en) All-fiber active Q-switched laser based on saturable absorption optical fiber
CN203883307U (en) Polarizing beam-combining nonlinear rotating mode-locked laser
Steinmann et al. Compact 7.4 W femtosecond oscillator for white-light generation and nonlinear microscopy
CN203103749U (en) Two-micron wave length all-fiber laser based on nanotube mode locking
Lu et al. Kilowatt peak power pulses from a passively Q-switched Yb-doped fiber laser with a smaller-core Yb-doped fiber as a saturable absorber
Agnesi et al. 150-ps pulse Raman generator pumped by a 1-kHz sub-nanosecond passively Q-switched laser system
Li et al. Hundred micro-joules level high power chirped pulse amplification of femtosecond laser based on single crystal fiber
Rusu et al. All-fiber picosecond laser source based on nonlinear spectral compression
Li et al. Hybrid high energy femtosecond laser system based on Yb: YAG single crystal fiber amplifier

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant