CN204088868U - The high-power fiber femto-second laser of a kind of 780nm - Google Patents
The high-power fiber femto-second laser of a kind of 780nm Download PDFInfo
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Abstract
The utility model discloses the high-power fiber femto-second laser of a kind of 780nm, this laser comprises laser seed source, laser broadening amplification module, laser compression module, laser freuqency doubling module, and laser seed source and each module connect successively; Wherein, described laser broadening module is made up of chirped pulse broadening submodule, pulse separation submodule and fiber amplifier submodule, and described laser seed source and each module are all operated in 1560nm wave band.The utility model adopts mixed pulses broadenings mode, in less working space by pulse from 100fs broadening to 1ns, the pulse after amplification is compressed to below 100fs through the non-linear of monomode fiber, finally, by nonlinear crystal frequency multiplication to 780nm.The utility model has that stability is high, structure is simple, compact, the advantage such as with low cost.
Description
Technical field
The utility model relates to superlaser technical field, the high-capacity optical fiber laser of especially a kind of 780nm.
Background technology
The femtosecond laser source of 780nm is super continuum light spectrum generation, optical microphotograph imaging, excites the perfect light sources such as Terahertz generation, the research of pumping-detection ultrafast process, non-linear laser spectrum, the retrofit of femtosecond micro-nano, the detection of material ultra-fast dynamics.
780nm femtosecond pulse light source mainly relies on ti sapphire laser to provide traditionally.But ti sapphire laser is bulky, involve great expense, be mainly used in laboratory environment.And because ti sapphire laser loses locked mode, need professional to carry out adjustment locked mode.In addition, the various precison optical components used in ti sapphire laser need the environment of moisture constant, and the stable of laserresonator it is also proposed certain requirement to temperature, the popularization of the ti sapphire laser that these factors limit further.
A kind of scheme of alternative ti sapphire laser is the femtosecond laser being produced 780nm by 1560nm Er-doped fiber femto-second laser frequency multiplication.The characteristic of the high stable that fiber laser has and low cost will make it replace ti sapphire laser at most fields.Many fields need the 780nm laser of high pulse energy, but the damage threshold of the nonlinear effect in fiber amplifier and fiber optic materials limits the further raising of laser pulse energy.
Chirped pulse amplification is the high power pulse amplifying technique of main flow, and this technology was applied in laser by G Mourou and Donna Strickland as far back as 1985.The general principle of this technology utilizes chromatic dispersion material by pulse stretching, then amplifies, and finally utilizes the Material compression pulse of contrary dispersion to obtain high energy pulse.Although chirped pulse amplification can be applied to fiber laser can obtain high energy laser pulse, still there are some unfavorable factors in this scheme.First, chirped pulse amplification requires higher to the spectral width of seed pulse, and comparatively large by the impact of its initial chirp, and is not suitable for the narrower pulse of spectrum; In addition, operating distance needed for CPA (or the stretcher of space structure and compressor reducer, or normal dispersion and abnormal dispersion fiber) is longer, and is not suitable for the fiber laser of Miniaturized portable.
Discrete pulse amplifying technique is another kind of high power pulse amplifying technique, is proposed in 2007 by F. W Wise group.Discrete pulse amplifying technique can avoid the excessively high-peak power of a pulse in high-energy amplification process, it is at a series of pulse trains being axially copied into the equipartition of energy by inceptive impulse, then the energy of whole pulse train is amplified, the pulse number of dispersion is more, and the nonlinear effect reduced in amplification process is more remarkable.Different from chirped pulse amplification, discrete pulse amplifying technique is not carry out broadening based on effect of dispersion paired pulses, but utilizes pulse polarization characteristic by pulse separation, is copied into the less pulse of several energy by inceptive impulse.Therefore, discrete pulse amplifying technique has unique advantage in the generation of high energy pulse: first, inceptive impulse is carried out energy segmentation by this technology, time domain forms a pulse train, all characteristics of each pulse (except polarization state) in pulse train are identical, and are consistent with inceptive impulse, are applicable to the pulse amplifying of various spectral shape, and do not rely on the initial chirp of pulse, be specially adapted to the narrower picopulse of spectrum and amplify; Secondly, by the mode of palarization multiplexing, pulse-separator unit can be multiplexed with pulse combination device, unite two into one by pulse beam splitting and conjunction bundle, decrease the complexity of system.
But discrete pulse amplifying device is when carrying out ultrashort pulse amplification process, and particularly transform limit is in the pulse of below 100fs, comparatively difficulty.The high-order dispersion Cumulate Sum high-order nonlinear accumulation of ultrashort pulse in optical fiber and optical fibre device, the very serious compression quality reducing pulse.
Utility model content
The purpose of this utility model is for the deficiency of prior art in ultrashort pulse amplification process and the one 780 nm high-power fiber femto-second laser provided, the utility model is in conjunction with the advantage of two kinds of pulse stretching modes, in less working space by pulse from 100fs broadening to 1ns, pulse after amplification is compressed to 100 below fs through the non-linear of monomode fiber, finally, by nonlinear crystal frequency multiplication to 780 nm.The utility model has that stability is high, structure is simple, compact, the advantage such as with low cost, for the fields such as super continuous spectrums generation, Terahertz generation, optical microphotograph imaging provide a solution that can replace Ti∶Sapphire laser femtosecond laser light source.
The concrete technical scheme realizing the utility model object is:
The high-power fiber femto-second laser of a kind of 780nm, feature is: this laser comprises laser seed source, laser broadening amplification module, laser compression module, laser freuqency doubling module, and laser seed source, laser broadening amplification module, laser compression module and laser freuqency doubling module connect successively; Wherein, described laser broadening module is made up of chirped pulse broadening submodule, pulse separation submodule and fiber amplifier submodule, and chirped pulse broadening submodule, pulse separation submodule are connected successively with fiber amplifier submodule; Described laser seed source, chirped pulse broadening submodule, pulse separation submodule, fiber amplifier submodule and pulse compression module are all operated in 1560nm wave band.
Described chirped pulse broadening submodule is made up of dispersion compensating fiber, optical fiber collimator, spatial light isolator, dispersion compensating fiber is positive dispersion fiber or the negative dispersion optical fiber of seed light wave band, the output pulses generation of laser seed source can be made respectively just to warble or bear to warble.
Described positive dispersion fiber or negative dispersion optical fiber are monomode fiber, multimode fiber, doubly clad optical fiber or large mode area pcf.
Described pulse separation submodule is made up of the pulse-separator unit based on birefringece crystal or polarization beam apparatus, can produce the subpulse of multiple dependence polarization separation, and subpulse is warbled for just warbling or bearing.
Described fiber amplifier submodule adopts Faraday speculum to form the dual channel structure of palarization multiplexing, and seed light is amplified through gain fibre for twice.
Described fiber amplifier submodule can be operated in positive chirped pulse amplification (chirped pulse amplification CPA), negative chirped pulse amplification (De-chirped pulse amplification, DPA) pattern, nonlinear pulse amplification or self similarity chirped pulse amplification pattern.Obtain video stretching by Self-phase modulation, overcome conventional amplification process intermediate frequency spectrum and to narrow effect, obtain the frequency spectrum wider than seed injection light pulse; In discrete pulse amplification process, polarization separation subpulse can rely on dispersion and nonlinear effect to realize pulse from compression.
Described pulse separation submodule and fiber amplifier submodule, based on Faraday speculum, twice path commute through gain fibre and pulse separation submodule before and after the polarization separation subpulse making orthogonal polarization orientation, light path is complementary, automatically synthesizes a high energy pulse after polarization separation subpulse amplifies.
Described laser compression module comprises optical fiber collimator, a section single-mould fiber and optical fiber collimator, and wherein, the 2nd order chromatic dispersion of monomode fiber is contrary with the dispersion characteristics of dispersion compensating fiber, can compress the later pulse of amplification.
Described laser freuqency doubling module is made up of condenser lens, collimating lens and frequency-doubling crystal, and condenser lens, frequency-doubling crystal and collimating lens successively light path connect, and produce 780nm femtosecond pulse.
The high-power fiber femto-second laser of 780nm of the present utility model, no matter be use positive chirped pulse amplification, negative chirped pulse amplification, nonlinear pulse to amplify or self similarity chirped pulse amplification pattern, path commute before and after the subpulse Faraday speculum of orthogonal polarization orientation, light path is complementary, and the polarization coupling after polarization separation subpulse amplifies is not by the impact of amplification mode.
The high-power fiber femto-second laser of 780nm of the present utility model, no matter be the optical fiber using positive dispersion or negative dispersion, the polarization coupling after polarization separation subpulse amplifies is not by the impact of optical fiber dispersion.
The high-power fiber femto-second laser of 780nm of the present utility model can be multi-stage cascade structure for amplifying.
Laser freuqency doubling module of the present utility model adopts condenser lens, collimating lens and frequency-doubling crystal to carry out nonlinear frequency conversion.
The optical-fiber laser amplifying technique of the high-power fiber femto-second laser of 780nm of the present utility model, can be extended to its all band, and the nonlinear frequency conversion of corresponding times of frequency module also can be extended to other corresponding wave bands.
The beneficial effects of the utility model are:
The utility model is in conjunction with the advantage of chirped pulse amplification and discrete pulse amplifying technique, obtain the light-pulse generator of a kind of high power, high pulse energy, high optical quality, pass through nonlinear crystal frequency multiplication again to 780 nm wave bands, can replace or alternative Ti∶Sapphire laser femto-second laser.Be embodied in:
, the utility model by conjunction with chirped pulse amplification and discrete pulse amplifying technique, can expeditiously by the pulse stretching within 100 fs to 1ns, reduce the nonlinear effect in amplification process significantly.
(2), the utility model realizes high energy pulse by monomode fiber and exports, and avoids using traditional large mould field optical fiber.Large mould field optical fiber is generally photon crystal structure, and bending radius is comparatively large, be unfavorable for fiber reel around and encapsulation.The utility model adopts monomode fiber or the optical fiber close with monomode fiber physical dimension, effectively reduces fused fiber splice and coupling loss, achieves all optical fibre structure.Meanwhile, monomode fiber ensure that the laser beam quality of high-quality.
(3), the utility model adopt pulse stretching mode structure to be applicable to the fiber amplifier of multiple project organization.
(4), the utility model adopts discrete pulse technology by femtosecond pulse broadening to psec or nanosecond pulse.Compare and only adopt chirped pulse amplification, avoid introducing a large amount of high-order dispersion, high-quality pulse compression can be realized.
(5), in the utility model, overcome the rigors to the spectral width of incident pulse, spectral position and chirping characteristics in high-energy amplification process.
(6), amplifying technique of the present utility model is applicable to multiple wave band, the pulse stretching amplification of various spectral region.
Accompanying drawing explanation
Fig. 1 is the utility model structured flowchart;
Fig. 2 is the optical fiber femtosecond laser structural representation of the utility model conllinear yttrium vanadate of just warbling and polarizing beam splitter cube mixed pulses broadening mode;
Fig. 3 is the optical fiber femtosecond laser structural representation that the utility model bears conllinear yttrium vanadate and the polarizing beam splitter cube mixed pulses broadening mode of warbling;
Fig. 4 is the optical fiber femtosecond laser structural representation of the utility model non-colinear yttrium vanadate of just warbling and polarizing beam splitter cube mixed pulses broadening mode;
Fig. 5 is the optical fiber femtosecond laser structural representation of the utility model conllinear yttrium vanadate of just warbling and non-colinear yttrium vanadate mixed pulses broadening mode.
Embodiment
Consult Fig. 1, the utility model is made up of laser seed source 100, laser broadening amplification module 200, laser compression module 300 and laser freuqency doubling module 400.Laser seed source 100, laser broadening amplification module 200, laser compression module 300 are connected with laser freuqency doubling module 400 successively light path; Laser seed source 100 provides the laser pulse of stable femtosecond magnitude.Laser broadening amplification module 200 comprises chirped pulse broadening submodule 210, discrete pulse broadening submodule 220 and fiber amplifier submodule 230.The 2nd order chromatic dispersion characteristic of the dispersion compensating fiber 211 in the monomode fiber 301 used in laser compression module 300 and chirped pulse broadening module 200 is contrary, can to carrying out pulse compression after amplifying.Laser freuqency doubling module 400 is made up of condenser lens, collimating lens and frequency-doubling crystal, for the generation of 780nm femtosecond pulse.After the stable femtosecond pulse that laser seed source 100 provides enters laser amplifying module 200, first pass through chirped pulse broadening submodule 210 broadening to picosecond magnitude, then pulse separation submodule 220 is passed through by picopulse broadening to nanosecond order, pulse after broadening enters fiber amplifier submodule 230 and amplifies, and the pulse after amplification synthesizes a high energy pulse by pulse separation submodule 220 again.The monomode fiber 301 of high energy pulse after amplification in laser compression module 300 compression residue further chirp value, obtains ultrafast femtosecond pulse.High energy femtosecond pulse carries out frequency multiplication by laser freuqency doubling module 400 and obtains high power 780nm pulse.
Embodiment 1
Consulting Fig. 2, is 780 nm high-power fiber femto-second lasers of a kind of conllinear yttrium vanadate of just warbling of the present utility model and polarizing beam splitter cube mixed pulses broadening mode.
The femtosecond pulse that Erbium doped fiber laser oscillator stage 100 exports; by 2nd order chromatic dispersion 1560nm be positive dispersion compensating fiber 211 by pulse stretching to 1ps; then pulse is exported by optical fiber collimator 212, and the spatial light isolator 213 through a 1560nm is used for protecting seed light.Laser obtains linearly polarized laser by one piece of polarizing beam splitter cube 221.The linearly polarized laser pulse obtained is by the conllinear pulse-separator unit 222 based on yttrium vanadate crystal.The parallel interface of optical axis due to yttrium vanadate quartz crystal, and be 45 ° with the polarization direction angle of incident light, each pulse separation becomes o polarized pulses and e polarized pulses, and obtains time delay due to refractive index difference, becomes the crystal of multiple proportion by pulse stretching to 100ps by using multiple length.Then by the pulse-separator unit 223 based on polarizing beam splitter cube.The polarization direction of incident light and polarizing beam splitter cube angle are 45 °, each pulse separation becomes s polarized pulses and p polarized pulses, and walk due to s light and obtain time delay from more long light path, become the yttrium vanadate crystal of multiple can by pulse stretching to 10 ns by using polylith length.Pulse after broadening, by after optical fiber collimator 231, passes into double clad erbium and ytterbium codoping gain fibre 234, two power output 8W by pump combiner 233, the semiconductor laser 232 of centre wavelength 976 nm connects pump combiner 233 as pumping source.The operation wavelength 1560nm of end connecting fiber tail optical fiber of gain fibre 234, the high power faraday polariscope 235 of half-twist.Through the reflection of Faraday mirror 235, seed light passes twice through gain fibre 234 and obtains high efficiency amplification.Amplify later laser pulse second time through pulse-separator unit 223 and 222, and be merged into a high energy laser pulse at the s polarised light output of polarizing beam splitter cube 221.High energy pulse after amplification is coupled into a section single-mould fiber 302 by optical fiber collimator 301, and monomode fiber provides negative 2nd order chromatic dispersion by pulse compression to below 100fs.Ultrashort pulse after compression is exported by optical fiber collimator 303, and the lithium columbate crystal 402 using 1560nm anti-reflection non-spherical lens 401 to be polarized to a block periodicity by Laser Focusing carries out frequency multiplication, by the ultrashort pulse non-linear conversion of 1560nm to 780nm.The ultrashort pulse that frequency multiplication obtains uses the anti-reflection non-spherical lens 403 of 780nm to carry out collecting and collimate the ultrashort high energy pulse obtaining 780nm.
Embodiment 2
Consult Fig. 3, for a kind of 780 nm high-power fibers bearing conllinear yttrium vanadate and the polarizing beam splitter cube mixed pulses broadening mode of warbling of the present utility model swash femtosecond light device.
The femtosecond pulse that Erbium doped fiber laser oscillator stage 100 exports; by 2nd order chromatic dispersion 1560nm be negative monomode fiber 211 by pulse stretching to 1ps; then pulse is exported by optical fiber collimator 212, and the spatial light isolator 213 through a 1560nm is used for protecting seed light.Laser obtains linearly polarized laser by one piece of polarizing beam splitter cube 221.The linearly polarized laser pulse obtained is by the conllinear pulse separation 222 based on yttrium vanadate crystal.The parallel interface of optical axis due to yttrium vanadate crystal, and be 45 ° with the polarization direction angle of incident light, each pulse separation becomes o polarized pulses and e polarized pulses, and obtains time delay due to refractive index difference, becomes the crystal of multiple proportion by pulse stretching to 100ps by using multiple length.Then by the pulse-separator unit 223 based on polarizing beam splitter cube.The polarization direction of incident light and polarizing beam splitter cube angle are 45 °, each pulse separation becomes s polarized pulses and p polarized pulses, and walk due to s light and obtain time delay from more long light path, become the yttrium vanadate crystal of multiple can by pulse stretching to 10 ns by using polylith length.Pulse after broadening, by after optical fiber collimator 231, passes into double clad erbium and ytterbium codoping gain fibre 234, two power output 8W by pump combiner 233, the semiconductor laser 232 of centre wavelength 976 nm connects pump combiner 233 as pumping source.The operation wavelength 1560nm of end connecting fiber tail optical fiber of gain fibre 234, the high power faraday polariscope 235 of half-twist.Through the reflection of Faraday mirror 235, seed light passes twice through gain fibre 234 and obtains high efficiency amplification.Amplify later laser pulse second time through pulse-separator unit 223 and 222, and be merged into a high energy laser pulse at the s polarised light output of polarizing beam splitter cube 221.It is positive dispersion compensating fiber 302 that high energy pulse after amplification is coupled into one section of 2nd order chromatic dispersion at 1560nm by optical fiber collimator 301, by pulse compression to below 100fs.Ultrashort pulse after compression is exported by optical fiber collimator 303, and the lithium columbate crystal 402 using 1560nm anti-reflection non-spherical lens 401 to be polarized to a block periodicity by Laser Focusing carries out frequency multiplication, by the ultrashort pulse non-linear conversion of 1560nm to 780nm.The ultrashort pulse that frequency multiplication obtains uses the anti-reflection non-spherical lens 403 of 780nm to carry out collecting and collimate the ultrashort high energy pulse obtaining 780nm.
Embodiment 3
Consulting Fig. 4, is 780 nm high-power fiber femto-second lasers of a kind of non-colinear yttrium vanadate of just warbling of the present utility model and polarizing beam splitter cube mixed pulses broadening mode.
The femtosecond pulse that Erbium doped fiber laser oscillator stage 100 exports; by 2nd order chromatic dispersion 1560nm be positive dispersion compensating fiber 211 by pulse stretching to 1ps; then pulse is exported by optical fiber collimator 212, and the spatial light isolator 213 through a 1560nm is used for protecting seed light.Laser obtains linearly polarized laser by one piece of polarizing beam splitter cube 221.The linearly polarized laser pulse obtained is by the conllinear pulse separation 222 based on yttrium vanadate crystal.The parallel interface of optical axis due to yttrium vanadate crystal, and be 45 ° with the angle of interface, each pulse separation becomes o polarized pulses and e polarized pulses, o light direction is constant, e light generation polarization walk from, because light path and refractive index difference obtain time delay, become the crystal of multiple proportion by pulse stretching to 100ps by using multiple length.Then by the pulse-separator unit 223 based on polarizing beam splitter cube: the polarization direction of incident light and polarizing beam splitter cube angle are 45 °, each pulse separation becomes s polarized pulses and p polarized pulses, and walk due to s light and obtain time delay from more long light path, become the yttrium vanadate crystal of multiple can by pulse stretching to 10 ns by using polylith length.Pulse after broadening, by after optical fiber collimator 231, passes into double clad erbium and ytterbium codoping gain fibre 234, two power output 8W by pump combiner 233, the semiconductor laser 232 of centre wavelength 976 nm connects pump combiner 233 as pumping source.The operation wavelength 1560nm of end connecting fiber tail optical fiber of gain fibre 234, the high power faraday polariscope 235 of half-twist.Through the reflection of Faraday mirror 235, seed light passes twice through gain fibre 234 and obtains high efficiency amplification.Amplify later laser pulse second time through pulse-separator unit 223 and 222, and be merged into a high energy laser pulse at the s polarised light output of polarizing beam splitter cube 221.High energy pulse after amplification is coupled into a section single-mould fiber 302 by optical fiber collimator 301, and monomode fiber provides negative 2nd order chromatic dispersion by pulse compression to below 100fs.Ultrashort pulse after compression is exported by optical fiber collimator 303, and the lithium columbate crystal 402 using 1560nm anti-reflection non-spherical lens 401 to be polarized to a block periodicity by Laser Focusing carries out frequency multiplication, by the ultrashort pulse non-linear conversion of 1560nm to 780nm.The ultrashort pulse that frequency multiplication obtains uses the anti-reflection non-spherical lens 403 of 780nm to carry out collecting and collimate the ultrashort high energy pulse obtaining 780nm.
Embodiment 4
Consulting Fig. 5, is 780 nm high-power fiber femto-second lasers of a kind of conllinear yttrium vanadate of just warbling of the present utility model and non-colinear yttrium vanadate mixed pulses broadening mode.
The femtosecond pulse that Erbium doped fiber laser oscillator stage 100 exports; by 2nd order chromatic dispersion 1560nm be positive dispersion compensating fiber 211 by pulse stretching to 1ps; then pulse is exported by optical fiber collimator 212, and the spatial light isolator 213 through a 1560nm is used for protecting seed light.Laser obtains linearly polarized laser by one piece of polarizing beam splitter cube 221.The linearly polarized laser pulse obtained is by the conllinear pulse separation 222 based on yttrium vanadate crystal.The parallel interface of optical axis due to yttrium vanadate crystal, and be 45 ° with the polarization direction angle of incident light, each pulse separation becomes o polarized pulses and e polarized pulses, and obtains time delay due to refractive index difference, becomes the crystal of multiple proportion by pulse stretching to 100ps by using multiple length.The linearly polarized laser pulse obtained is by the non-colinear pulse-separator unit 223 based on yttrium vanadate crystal: the optical axis of crystal is parallel to the plane of incidence, and in the angle of interface be 45 °, each pulse separation becomes o polarized pulses and e polarized pulses, o light direction is constant, e light generation polarization walk from, because light path and refractive index difference obtain time delay, become the crystal of multiple proportion by pulse stretching to 10ns by using multiple length.Pulse after broadening, by after optical fiber collimator 231, passes into double clad erbium and ytterbium codoping gain fibre 234, two power output 8W by pump combiner 233, the semiconductor laser 232 of centre wavelength 976 nm connects pump combiner 233 as pumping source.The operation wavelength 1560nm of end connecting fiber tail optical fiber of gain fibre 234, the high power faraday polariscope 235 of half-twist.Through the reflection of Faraday mirror 235, seed light passes twice through gain fibre 234 and obtains high efficiency amplification.Amplify later laser pulse second time through pulse-separator unit 223 and 222, and be merged into a high energy laser pulse at the s polarised light output of polarizing beam splitter cube 221.High energy pulse after amplification is coupled into a section single-mould fiber 302 by optical fiber collimator 301, and monomode fiber provides negative 2nd order chromatic dispersion by pulse compression to below 100fs.Ultrashort pulse after compression is exported by optical fiber collimator 303, and the lithium columbate crystal 402 using 1560nm anti-reflection non-spherical lens 401 to be polarized to a block periodicity by Laser Focusing carries out frequency multiplication, by the ultrashort pulse non-linear conversion of 1560nm to 780nm.The ultrashort pulse that frequency multiplication obtains uses the anti-reflection non-spherical lens 403 of 780nm to carry out collecting and collimate the ultrashort high energy pulse obtaining 780nm.
Claims (9)
1. the high-power fiber femto-second laser of a 780nm, it is characterized in that: this laser comprises laser seed source (100), laser broadening amplification module (200), laser compression module (300), laser freuqency doubling module (400), laser seed source (100), laser broadening amplification module (200), laser compression module (300) and laser freuqency doubling module (400) connect successively; Wherein, described laser broadening module (200) is made up of chirped pulse broadening submodule (210), pulse separation submodule (220) and fiber amplifier submodule (230), and chirped pulse broadening submodule (210), pulse separation submodule (220) are connected successively with fiber amplifier submodule (230); Described laser seed source (100), chirped pulse broadening submodule (210), pulse separation submodule (220), fiber amplifier submodule (230) and pulse compression module (300) are all operated in 1560nm wave band.
2. optical fiber femtosecond laser according to claim 1, it is characterized in that: described chirped pulse broadening submodule (210) is made up of dispersion compensating fiber (211), optical fiber collimator (212) and spatial light isolator (213), the positive dispersion fiber that dispersion compensating fiber (211) is seed light wave band or negative dispersion optical fiber, can make the output pulses generation of laser seed source (100) just warble or bear to warble.
3. optical fiber femtosecond laser according to claim 2, is characterized in that: described positive dispersion fiber or negative dispersion optical fiber are monomode fiber, multimode fiber, doubly clad optical fiber or large mode area pcf.
4. optical fiber femtosecond laser according to claim 1, it is characterized in that: described pulse separation submodule (220) is made up of the pulse-separator unit based on birefringece crystal or polarization beam apparatus, can produce the subpulse of multiple dependence polarization separation, subpulse is warbled for just warbling or bearing.
5. optical fiber femtosecond laser according to claim 1, is characterized in that: described fiber amplifier submodule (230) adopts Faraday speculum to form the dual channel structure of palarization multiplexing, and seed light is amplified through gain fibre for twice.
6. optical fiber femtosecond laser according to claim 1 or 5, is characterized in that: described fiber amplifier submodule (230) can be operated in positive chirped pulse amplification, negative chirped pulse amplification, nonlinear pulse are amplified or self similarity chirped pulse amplification pattern.
7. optical fiber femtosecond laser according to claim 1, it is characterized in that: described laser compression module (300) comprises optical fiber collimator (301), monomode fiber (302) and optical fiber collimator (303), wherein, the 2nd order chromatic dispersion of monomode fiber (302) is contrary with the dispersion characteristics of dispersion compensating fiber (211), can compress the later pulse of amplification.
8. optical fiber femtosecond laser according to claim 1, it is characterized in that: described pulse separation submodule (220) and fiber amplifier submodule (230), based on Faraday speculum, twice path commute through gain fibre and pulse separation submodule before and after the polarization separation subpulse making orthogonal polarization orientation, light path is complementary, automatically synthesizes a high energy pulse after polarization separation subpulse amplifies.
9. optical fiber femtosecond laser according to claim 1, it is characterized in that: described laser freuqency doubling module (400) is made up of condenser lens (401), collimating lens (403) and frequency-doubling crystal (402), condenser lens (401), frequency-doubling crystal (402) and collimating lens (403) successively light path connect, and produce 780nm femtosecond pulse.
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109298582A (en) * | 2018-09-06 | 2019-02-01 | 中国科学院上海光学精密机械研究所 | Generate the device of high-energy Coherent Wideband continuous spectrum |
| CN112636140A (en) * | 2020-12-17 | 2021-04-09 | 武汉安扬激光技术有限责任公司 | Femtosecond laser with power and pulse width simultaneously locked |
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2014
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109298582A (en) * | 2018-09-06 | 2019-02-01 | 中国科学院上海光学精密机械研究所 | Generate the device of high-energy Coherent Wideband continuous spectrum |
| CN112636140A (en) * | 2020-12-17 | 2021-04-09 | 武汉安扬激光技术有限责任公司 | Femtosecond laser with power and pulse width simultaneously locked |
| CN112636140B (en) * | 2020-12-17 | 2021-11-05 | 武汉安扬激光技术股份有限公司 | Femtosecond laser with power and pulse width simultaneously locked |
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