CN211579185U - All-fiber femtosecond chirped pulse amplification system - Google Patents
All-fiber femtosecond chirped pulse amplification system Download PDFInfo
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- CN211579185U CN211579185U CN201922414593.7U CN201922414593U CN211579185U CN 211579185 U CN211579185 U CN 211579185U CN 201922414593 U CN201922414593 U CN 201922414593U CN 211579185 U CN211579185 U CN 211579185U
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- 239000000835 fiber Substances 0.000 title claims abstract description 151
- 230000003321 amplification Effects 0.000 title claims abstract description 47
- 238000003199 nucleic acid amplification method Methods 0.000 title claims abstract description 47
- 239000013307 optical fiber Substances 0.000 claims abstract description 30
- 238000005086 pumping Methods 0.000 claims abstract description 16
- 239000006185 dispersion Substances 0.000 claims description 13
- 238000001228 spectrum Methods 0.000 claims description 7
- 238000001069 Raman spectroscopy Methods 0.000 claims description 5
- 239000004038 photonic crystal Substances 0.000 claims description 3
- 238000002310 reflectometry Methods 0.000 claims description 3
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- 229910052769 Ytterbium Inorganic materials 0.000 claims description 2
- 230000004927 fusion Effects 0.000 claims description 2
- 229910052761 rare earth metal Inorganic materials 0.000 claims description 2
- 239000004065 semiconductor Substances 0.000 claims description 2
- NAWDYIZEMPQZHO-UHFFFAOYSA-N ytterbium Chemical compound [Yb] NAWDYIZEMPQZHO-UHFFFAOYSA-N 0.000 claims description 2
- 238000007493 shaping process Methods 0.000 abstract description 14
- 238000013507 mapping Methods 0.000 abstract description 11
- 230000010354 integration Effects 0.000 abstract description 4
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- 238000013459 approach Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- 239000000654 additive Substances 0.000 description 1
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Abstract
The utility model provides a full optical fiber femto second chirp pulse amplification system based on frequency domain-time domain mapping pulse plastic includes: a femtosecond pulse seed source, an all-fiber pulse shaper, a fiber amplifier and a pulse compressor. The all-fiber pulse shaper comprises a first pumping source, a wavelength division multiplexer, a first gain fiber, a first circulator, a fiber chirped Bragg grating compressor, a second pumping source, a fiber combiner, a second gain fiber, a second circulator and a fiber chirped Bragg grating stretcher. The utility model discloses an all-fiber pulse shaper has been introduced in the chirped pulse amplification system, and parabola pulse shaping process can be accomplished in the structure of all-fiber, need not additionally to introduce space components and parts. The system stability and the integration are considered while the output of the femtosecond pulse with higher energy and peak power is ensured.
Description
Technical Field
The utility model belongs to laser technology and nonlinear optics field especially relate to a fine femto second chirp pulse amplification system of full gloss based on frequency domain-time domain mapping pulse shaping.
Background
The femtosecond laser pulse has important application in the fields of ultrafast micro-nano processing, ultrafast nonlinear optics, terahertz generation, time-resolved spectroscopy and the like. The femtosecond laser can be generated through a solid laser and a fiber laser, wherein the femtosecond fiber laser can work at megahertz pulse frequency, has the outstanding advantages of good beam quality, high efficiency, good heat dissipation, compact structure and the like, and gradually shows unique advantages in the aspects of laser additive manufacturing, radar remote sensing, biomedical treatment and the like.
As the fiber core of the optical fiber is small in size and relatively concentrated in energy, the transmission distance of the pulse in the optical fiber is long, the nonlinear effect becomes the most main factor for preventing the performance of the fiber femtosecond laser from being improved, and the compressed pulse is split and distorted due to the accumulation of a large amount of nonlinear effect. It is difficult for the conventional technology to directly obtain the femtosecond laser output with high average power and high peak power in the optical fiber. Thanks to the utility model of Chirp Pulse Amplification (CPA), the femtosecond fiber laser technology is rapidly developing. The chirped pulse amplification technology mainly comprises four parts: a laser oscillator (seed source), a pulse stretcher, a laser amplifier, and a pulse compressor. The basic principle is as follows: before the seed laser pulse is amplified, the time domain of the seed laser pulse is broadened to a hundred picoseconds or nanosecond order by a dispersion device, then the power of the broadened pulse in a laser amplifier is improved, and finally the pulse is compressed to a femtosecond order by a pulse compressor to compensate the dispersion introduced by a preceding stage. The purpose of pulse broadening is to reduce the intensity of laser pulses in the amplification process, so that the peak power of the pulses is below the damage threshold of system elements, thereby avoiding the damage to the optical elements of the amplifier caused by overhigh power of ultrashort pulses after amplification, weakening or overcoming various nonlinear effects possibly caused by high-intensity laser in the amplification process, and enabling the pulse energy in the optical fiber to be improved by several orders of magnitude. Particularly in the aspect of a high-average-power femtosecond fiber laser, full-fiber femtosecond pulse output with average power of hundred watt and pulse energy of micro-focus magnitude can be realized by the CPA technology, and the peak power can reach ten megawatt magnitude.
With the continuous expansion of the application field of ultrafast laser, the demand of femtosecond laser with high energy and high peak power is gradually increased. How to realize high peak power laser output in a fiber femtosecond laser system is a hot spot and a difficulty of scientific research. At present, three methods for realizing high-peak power femtosecond pulse output in a fiber laser system mainly comprise: the first is a linear chirp pulse amplification method, which expands the laser output by an oscillator by a large dispersion grating expander of a space optical structure, then couples the expanded laser into a double-clad gain fiber and an active photonic crystal fiber rod with a large mode field area again for amplification, and finally compresses by using a grating pair. In the method, the high-order dispersion of the stretcher and the compressor can be matched with each other, the nonlinear effect introduced in the amplification process is small, the femtosecond pulse output with high energy and high peak power can be realized, but a large number of free space devices are introduced into the system, so that the whole system is relatively complex, the stability is reduced, and the integration is difficult. In addition, the linear amplification process is also influenced by the gain narrowing effect, so that the spectrum before compression is obviously narrowed, and a shorter femtosecond pulse cannot be obtained after compression, thereby limiting the improvement of the peak power of the pulse. The second method is nonlinear amplification, which can use positive dispersion transmission fiber to widen pulse, and the nonlinearity generated in the amplification process can compensate the third-order dispersion introduced by the system, so as to obtain femtosecond pulse with higher quality. The disadvantage of this method is that the grating angle needs to be adjusted accurately to ensure the matching of third-order dispersion and nonlinearity, and the precision requirement for grating adjustment is high. The third method is self-similar amplification, and the principle of the method is that in the process of transmitting pulses in an optical fiber amplifier, when gain, dispersion and nonlinearity reach certain conditions, the shape of the pulses evolves towards a parabola shape, the frequency chirp accumulated in the amplification process of the parabola shape pulses is linear and can be compressed by a grating compressor, so that the problem of compressed pulse distortion caused by nonlinear accumulation in the amplifier is solved. The method utilizes the nonlinear effect in the optical fiber, so that the spectrum is broadened, and laser pulses smaller than hundred femtoseconds can be obtained after compression. But the disadvantage is that the conditions for maintaining self-similar amplification are harsh, and the pulses are compressed to near femtosecond order in advance, so the pulse compressor must be introduced before the amplifier, which increases the complexity of the system. In addition, the self-similar amplification system is limited by the stimulated Raman scattering effect and the fiber gain bandwidth, the output energy is generally maintained at a micro-focus level, and the output of higher energy cannot be realized. In addition, the generation of parabolic pulses can be accomplished in a manner that temporally shapes the pulses, but this approach requires the introduction of a spatial light modulator, which also increases the cost and complexity of the system.
SUMMERY OF THE UTILITY MODEL
The problems that a linear chirped pulse system has many free space components, a complex structure, low stability, difficulty in integration and obvious gain narrowing effect are solved; the nonlinear amplification system needs to accurately adjust dispersion and an amplifier, and has strict requirements on operation; a compressor is additionally required to be introduced into the self-similar amplification system, so that the problem of complex structure is caused, and the problem of self-similar pulse energy limitation is caused by stimulated Raman scattering and gain bandwidth limitation; the use of the spatial light modulator for pulse shaping has the problems of high cost and complex structure. The utility model provides an all-fiber femtosecond chirp pulse amplification system which has an all-fiber structure, can realize high energy and high peak power laser output and is based on frequency domain-time domain mapping pulse shaping. The laser pulse output by the seed source firstly carries out parabolic shaping on a spectrum through a nonlinear amplification process in an optical fiber amplifier, then linear chirp is introduced through an optical fiber grating stretcher, and based on a frequency domain-time domain mapping effect, the time domain of the stretched pulse also approaches to a parabolic shape. The pulse after shaping is amplified, linear frequency chirp can be generated, and compared with the traditional mode, the method can effectively reduce the influence on compressed pulses caused by nonlinear effect accumulation. In addition, the method can realize parabolic pulse amplification of hundred picoseconds, and compared with self-similar amplification, long pulse can improve the threshold value of stimulated Raman scattering of the system, and is easy to realize higher power output. The scheme does not need to adopt an additional free space component, the pulse shaping and pulse amplification process can be completed in an all-fiber structure, and the all-fiber structure is easy to integrate and stable in performance while high-energy and high-peak-power femtosecond pulse output is realized.
In order to achieve the above purpose, the utility model adopts the following technical scheme:
an all-fiber femtosecond chirped pulse amplification system based on frequency domain-time domain mapping pulse shaping comprises a femtosecond pulse seed source, an all-fiber pulse shaper, a fiber amplifier and a pulse compressor. The all-fiber pulse shaper comprises a first pumping source, a wavelength division multiplexer, a first gain fiber, a first circulator, a fiber chirped Bragg grating compressor, a second pumping source, a fiber combiner, a second gain fiber, a second circulator and a fiber chirped Bragg grating stretcher. The output end of the femtosecond pulse source is connected with the signal input end of a first wavelength division multiplexer of the all-fiber pulse shaper, the output fiber of the first pumping source is connected with the pumping input end of the first wavelength division multiplexer, the common output end of the first wavelength division multiplexer is connected with one end of a first gain fiber, the other end of the first gain fiber is connected with the input end of a first circulator, the reflecting end of the first circulator is connected with the input end of a fiber chirped Bragg grating compressor, the output end of the first circulator is connected with the signal input end of a fiber combiner, the output end of a second pumping source is connected with the pumping input end of the fiber combiner, the common end of the fiber combiner is connected with one end of a second gain fiber, the other end of the second gain fiber is connected with the input end of a second circulator, the reflecting end of the second circulator is connected with the input end of a fiber chirped Bragg grating stretcher, the output end of the second circulator is connected with the input end of the optical fiber amplifier, and the output end of the optical fiber amplifier is input to the pulse compressor after being collimated.
Preferably, the center wavelength of the femtosecond pulse seed source is 1020-1080nm, the full width at half maximum of the spectrum is 1-50nm, the pulse width is 0.2-10ps, the repetition frequency is 0.5-100MHz, and the pulse energy is 0.1-50 nJ.
Preferably, the first pump source and the second pump source are semiconductor lasers, solid lasers, gas lasers, fiber lasers or raman lasers, the output fiber is a single-mode fiber or a multimode fiber, and the range of the central wavelength λ of the output pump light is as follows: 700nm ≦ λ ≦ 1030 nm.
Preferably, the first gain fiber and the second gain fiber are fibers doped with ytterbium (Yb) rare earth ions, and the fibers can be single-clad fibers or double-clad step-index fibers or double-clad photonic crystal fibers.
Preferably, the center wavelength of the fiber chirped Bragg grating compressor is 1020-1080nm, the full width at half maximum of the spectrum is 10-50nm, the reflectivity is 10% -99%, and the negative dispersion value β can be provided2At-0.1 to-0.5 ps2In the meantime.
Preferably, the center wavelength of the fiber chirped Bragg grating stretcher is 1020-1080nm, the full width at half maximum of the spectrum is 10-50nm, the reflectivity is 10% -99%, and the value of the provided positive dispersion β can be provided2At 10 to 50ps2In the meantime.
Preferably, the optical fiber amplifier consists of a two-stage or multi-stage ytterbium-doped optical fiber amplifier.
Preferably, the optical fiber amplifiers adopt a fiber fusion coupling mode between each stage.
Preferably, the core diameter of each gain fiber of the optical fiber amplifier is 6-50 μm.
Preferably, the pulse compressor is one or more of a transmission grating pair compressor, a reflection grating pair compressor, a chirped volume bragg grating compressor and a hollow-core optical fiber.
The utility model provides a full optical fiber femto second chirp pulse amplification system based on frequency domain-time domain mapping pulse plastic, core device are full optical fiber ization pulse shaper, carry out the plastic to the pulse through nonlinear effect and the chirped fiber grating in the optic fibre, reduce the influence that the pulse received nonlinear effect. Then, a multistage optical fiber amplifier is adopted for power boosting, and finally, a compressor is used for pulse compression.
The utility model has the advantages that: the chirped pulse amplification system is provided with the all-fiber pulse shaper, and the parabolic pulse shaping process can be completed in an all-fiber structure without additionally introducing space components. The system stability and the integration are considered while the output of the femtosecond pulse with higher energy and peak power is ensured.
Drawings
Fig. 1 is a schematic structural diagram of an all-fiber femtosecond chirped pulse amplification system based on frequency domain-time domain mapping pulse shaping according to an embodiment of the present invention.
Fig. 2 is a schematic structural diagram of an all-fiber pulse shaper according to an embodiment of the present invention.
The optical fiber chirped Bragg grating optical fiber amplifier comprises a femtosecond pulse seed source 1, an all-fiber pulse shaper 2, an optical fiber amplifier 3, a pulse compressor 4, a first pump source 201, a wavelength division multiplexer 202, a first gain fiber 203, a first circulator 204, a first circulator 205, an optical fiber chirped Bragg grating compressor 206, a second pump source 207, an optical fiber combiner 208, a second gain fiber 209, a second circulator 210 and an optical fiber chirped Bragg grating stretcher.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more clearly understood, the present invention will be further explained with reference to the accompanying drawings and embodiments, and the specific embodiments described herein are only used for explaining the present invention, but not limiting the present invention.
As shown in fig. 1, an embodiment of the present invention provides an all-fiber femtosecond chirped pulse amplification system based on frequency domain-time domain mapping pulse shaping, including: the device comprises a femtosecond pulse seed source 1, an all-fiber pulse shaper 2, a fiber amplifier 3 and a pulse compressor 4. As shown in fig. 2, the all-fiber pulse shaper includes: a first pump source 201, a wavelength division multiplexer 202, a first gain fiber 203, a first circulator 204, a fiber chirped bragg grating compressor 205, a second pump source 206, a fiber combiner 207, a second gain fiber 208, a second circulator 209, and a fiber chirped bragg grating stretcher 210. The output end of the femtosecond pulse seed source 1 is connected with the signal input end of the wavelength division multiplexer 202 of the all-fiber pulse shaper 2, the output fiber of the first pump source 201 is connected with the pump input end of the wavelength division multiplexer 202, the common output end of the wavelength division multiplexer 202 is connected with one end of the first gain fiber 203, the other end of the first gain fiber 203 is connected with the input end of the first circulator 204, the reflecting end of the first circulator 204 is connected with the input end of the fiber chirped bragg grating compressor 205, the output end of the first circulator 204 is connected with the signal input end of the fiber combiner 207, the output end of the second pump source 206 is connected with the pump input end of the fiber combiner 207, the common end of the fiber combiner 207 is connected with one end of the second gain fiber 208, the other end of the second gain fiber 208 is connected with the input end of the second circulator 209, the reflecting end of the second circulator 209 is connected with the input end of the fiber chirped bragg grating stretcher 210, the output end of the second circulator 209 is connected to the input end of the optical fiber amplifier 3, and the output end of the optical fiber amplifier 3 is collimated and then input to the pulse compressor 4 for pulse compression.
The pulse generated by the femtosecond pulse seed source 1 enters an all-fiber pulse shaper 2, the power is amplified after the pulse reaches a first gain fiber 203 through a wavelength division multiplexer 202, the pulse width is smaller after the pulse passes through a first circulator 204 and a fiber chirped Bragg grating compressor 205, the peak power is improved, the pulse enters a second gain fiber 208 through a fiber combiner 207, the nonlinear amplification is carried out in the second gain fiber 208, the spectral shape of the pulse is changed, the power of a first pumping source 201 and the power of a second pumping source 206 are optimized, the approximately parabolic spectral shaping effect can be obtained, the spectrally shaped pulse passes through the second circulator 208 and the fiber chirped Bragg grating stretcher 210, the parabolic broadened pulse with the order of hundreds of picoseconds can be obtained according to the frequency domain-time domain mapping effect, and the pulse has the nonlinear inhibition capability, the shaped pulse is input into an optical fiber amplifier 3 for amplification, and finally enters a pulse compressor 4 for pulse compression.
The utility model provides a compact structure, stable performance, can realize the all-fiber femto second chirp pulse amplification system based on frequency domain-time domain mapping pulse shaping of high peak power. Based on the frequency domain-time domain mapping principle of nonlinear amplification and dispersion guidance, the full-fiber pulse shaper is adopted to widen the pulse to be amplified in the time domain and simultaneously carry out parabolic shaping, and the pulse distortion problem caused by nonlinear accumulation can be effectively inhibited in the amplification process of the shaped pulse, so that the method can realize high-energy and high-peak-power laser output. Compared with the traditional mode, the structure has no free space component except the pulse compressor, and is high in stability and strong in environmental adaptability. In addition, the structure can realize laser output with higher energy and higher pulse quality under the same broadening amount, and has wide application prospect.
Claims (10)
1. An all-fiber femtosecond chirped pulse amplification system is characterized by comprising a femtosecond pulse seed source, an all-fiber pulse shaper, a fiber amplifier and a pulse compressor; wherein, all-fiber pulse shaper includes: the device comprises a first pumping source, a wavelength division multiplexer, a first gain fiber, a first circulator, a fiber chirped Bragg grating compressor, a second pumping source, a fiber combiner, a second gain fiber, a second circulator and a fiber chirped Bragg grating stretcher; the output end of the femtosecond pulse source is connected with the signal input end of a first wavelength division multiplexer of the all-fiber pulse shaper, the output fiber of the first pumping source is connected with the pumping input end of the first wavelength division multiplexer, the common output end of the first wavelength division multiplexer is connected with one end of a first gain fiber, the other end of the first gain fiber is connected with the input end of a first circulator, the reflecting end of the first circulator is connected with the input end of a fiber chirped Bragg grating compressor, the output end of the first circulator is connected with the signal input end of a fiber combiner, the output end of a second pumping source is connected with the pumping input end of the fiber combiner, the common end of the fiber combiner is connected with one end of a second gain fiber, the other end of the second gain fiber is connected with the input end of a second circulator, the reflecting end of the second circulator is connected with the input end of a fiber chirped Bragg grating stretcher, the output end of the second circulator is connected with the input end of the optical fiber amplifier, and the output end of the optical fiber amplifier is input to the pulse compressor after being collimated.
2. The all-fiber femtosecond chirped pulse amplification system of claim 1, wherein the center wavelength of the femtosecond pulse seed source is 1020-.
3. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the first pump source and the second pump source are semiconductor lasers, solid lasers, gas lasers, fiber lasers or raman lasers, the output fiber is a single-mode fiber or a multi-mode fiber, and the central wavelength λ of the output pump light is in the range of: 700nm ≦ λ ≦ 1030 nm.
4. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the first gain fiber and the second gain fiber are ytterbium (Yb) rare earth ion doped fibers, and the fibers are single-clad fibers or double-clad step-index fibers or double-clad photonic crystal fibers.
5. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the center wavelength of the fiber chirped bragg grating compressor is 1020-2At-0.1 to-0.5 ps2In the meantime.
6. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the center wavelength of the fiber chirped bragg grating stretcher is 1020-1080nm, the full width at half maximum of the spectrum is 10-50nm, the reflectivity is between 10% -99%, and the available positive dispersion value is β2At 10 to 50ps2In the meantime.
7. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the core diameter of each gain fiber of the fiber amplifier is between 6 and 50 μm.
8. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the pulse compressor is one or more of a combination of a transmissive grating pair compressor, a reflective grating pair compressor, a chirped volume bragg grating compressor, and a hollow-core fiber.
9. The all-fiber femtosecond chirped pulse amplification system according to claim 1, wherein the fiber amplifier is composed of a two-stage or multi-stage ytterbium-doped fiber amplifier.
10. The all-fiber femtosecond chirped pulse amplification system according to claim 9, wherein the stages of the fiber amplifier are coupled by fiber fusion.
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| Publication number | Priority date | Publication date | Assignee | Title |
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| CN111064069A (en) * | 2019-12-29 | 2020-04-24 | 北京工业大学 | All-fiber femtosecond chirped pulse amplification system |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| CN111064069A (en) * | 2019-12-29 | 2020-04-24 | 北京工业大学 | All-fiber femtosecond chirped pulse amplification system |
| CN111064069B (en) * | 2019-12-29 | 2024-05-28 | 北京工业大学 | All-fiber femtosecond chirped pulse amplification system |
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