CN102263356A - Single-frequency narrow line width polarization maintaining full-optical fiber pulse laser device - Google Patents
Single-frequency narrow line width polarization maintaining full-optical fiber pulse laser device Download PDFInfo
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- CN102263356A CN102263356A CN 201110148475 CN201110148475A CN102263356A CN 102263356 A CN102263356 A CN 102263356A CN 201110148475 CN201110148475 CN 201110148475 CN 201110148475 A CN201110148475 A CN 201110148475A CN 102263356 A CN102263356 A CN 102263356A
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- 239000013307 optical fiber Substances 0.000 title abstract description 12
- 230000010287 polarization Effects 0.000 title abstract description 6
- 239000000835 fiber Substances 0.000 claims abstract description 68
- 238000005253 cladding Methods 0.000 claims abstract description 28
- 238000000926 separation method Methods 0.000 claims description 10
- 238000001208 nuclear magnetic resonance pulse sequence Methods 0.000 claims description 7
- 238000012163 sequencing technique Methods 0.000 claims description 4
- 230000003287 optical effect Effects 0.000 abstract description 5
- 238000002955 isolation Methods 0.000 abstract description 4
- 238000005086 pumping Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 5
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 230000002269 spontaneous effect Effects 0.000 description 4
- 230000003321 amplification Effects 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 238000001914 filtration Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000009022 nonlinear effect Effects 0.000 description 2
- 238000003199 nucleic acid amplification method Methods 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- 229910052769 Ytterbium Inorganic materials 0.000 description 1
- 230000008033 biological extinction Effects 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 230000000306 recurrent effect Effects 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- -1 ytterbium ion Chemical class 0.000 description 1
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Abstract
The invention relates to a single-frequency narrow line width polarization maintaining full-optical fiber pulse laser device which comprises a continuous single-frequency seed source laser device, wherein a first acoustic optical modulator, a first-level single mode fiber amplifier, a first isolation filter, a second-level single mode fiber amplifier, a second acoustic optical modulator, a second isolation filter and a third-level large-mode-field double-cladding fiber amplifier are arranged along the propagation direction of an output beam of the continuous single-frequency seed source laser device. The output end of a pulse sequential control signal source is respectively connected to the first acoustic optical modulator, the second acoustic optical modulator and a sequential control end of the third-level large-mode-field double-cladding fiber amplifier. The single-frequency narrow line width polarization maintaining full-optical fiber pulse laser device has the characteristics that the structure is simple, the laser repetition frequency and the pulse width are adjustable, the efficiency is high, the single-frequency property is excellent and the light beam quality is high.
Description
Technical field
The present invention relates to pulse optical fiber, particularly a kind of single mode narrow linewidth is protected complete partially fiber pulse laser.
Technical background
Single-frequency linear polarization pulse laser has important application prospects in fields such as remote sensing technology, spectral technique, coherent laser radar detection and coherent communications.In these fields, often require laser linewidth below 10MHz, for the pulse repetition different requirements are arranged also simultaneously.In the prior art, seed inject the solid single frequency laser use more [referring to S.W.Henderson, E.H.Yuen, and E.S.Fry, Opt.Lett, Vol.11, No.11, pp.715 (1986)], this laser output laser energy is bigger, but its pulsewidth is generally narrower, repetition is lower, live width about tens of MHz to hundred MHz, control system complexity particularly is unfavorable for steady in a long-term the application.
Summary of the invention
The present invention is intended to overcome above-mentioned the deficiencies in the prior art, provides a kind of single mode narrow linewidth to protect fiber pulse laser partially entirely, and this laser has that all optical fibre structure, repetition rate and pulsewidth are adjustable, spectral signal-noise ratio is high, characteristics such as compact conformation.
Technical solution of the present invention is as follows:
A kind of single mode narrow linewidth is protected complete partially fiber pulse laser, comprise continuous single-frequency seed source laser, its characteristics are: first sound-optic modulator, first order monomode fiber amplifier, first separation filter, second level monomode fiber amplifier, second sound-optic modulator, second separation filter, the big mould area double-cladding of third level fiber amplifier, the output in pulse sequence control signal source respectively with described first sound-optic modulator, second sound-optic modulator links to each other with the sequencing control end of the big mould area double-cladding of third level fiber amplifier, provide the electric impulse signal of special time relation, control described first sound-optic modulator, the operating time of the big mould area double-cladding of the second sound-optic modulator and third level fiber amplifier.
Laser linewidth＜the 10MHz of described continuous single-frequency seed source laser.
Described first order monomode fiber amplifier and second level monomode fiber Amplifier Gain optical fiber are that single mode is protected inclined to one side gain fibre, and the gain fibre of the big mould area double-cladding of described third level fiber amplifier is that big mould area double-cladding is protected inclined to one side gain fibre.
Obtain pulse train by first sound-optic modulator modulation continuous laser, obtain the power amplification output of high-gain again by two-stage monomode fiber amplifier, obtain the high impulse energy by big mould area double-cladding fiber amplifier at last and amplify output.Inter-stage adopts separation filter to reduce nonlinear effect and ASE effect, and second sound-optic modulator also can change laser pulse frequency when further reducing the amplified spontaneous emission effect.
Described first sound-optic modulator and second sound-optic modulator are for to carry out sequencing control synchronously by the signal of telecommunication, the signal of telecommunication that the output of pulse sequence control signal source has the special time relation is loaded into respectively on the driving power of described first sound-optic modulator and second sound-optic modulator, and driving power is exported the switch of corresponding ping guide sound optical modulator.Thereby make second sound-optic modulator to carry out selection of time to the pulse train that first sound-optic modulator produces, allow laser pulse pass through, and when no pulse, stop amplified spontaneous emission light, also can select by whether laser pulse simultaneously, thereby change laser pulse frequency.
The big mould area double-cladding of described third level fiber amplifier is when being applied to hang down recurrent frequency pulse laser output, adopt the pulse pump mode, the control signal of output of pulse sequence control signal source and acousto-optic modulator has the switching time of the signal of telecommunication control pumping of special time relation, to improve the pumping utilization ratio and to reduce amplified spontaneous emission.
Described single mode gain fibre is all the high inclined to one side gain fibre of guarantor that absorbs with big mould area double-cladding gain fibre, and the output end face of big mould area double-cladding optical fiber is the inclined-plane.
Technique effect of the present invention:
The present invention utilizes the optical fiber laser amplifier structure of high-gain to obtain the output of high-octane single mode narrow linewidth pulse laser, adopts three grades of structure for amplifying of different gains optical fiber to make the optical fiber laser amplifier can high efficiency output high energy pulse.Adopt separation filter to reduce nonlinear effect and ASE effect greatly between amplifier stage.Adopting two acousto-optic modulators to be used has not only further reduced the amplified spontaneous emission effect but also can control laser pulse width and frequency more flexibly, thereby make output laser pulse repetition and pulsewidth all adjustable, and improved the single-frequency performance of laser, make whole amplifier simple in structure, be easy to control, adapt to the different application occasion.
Description of drawings
Fig. 1 protects complete partially fiber pulse laser structural representation for single mode narrow linewidth of the present invention;
Fig. 2 protects first sound-optic modulator in the complete partially fiber pulse laser for single mode narrow linewidth of the present invention, and the second sound-optic modulator and the third level are amplified the control impuls timing diagram when adopting pulse pump
Fig. 3 is monomode fiber amplifier architecture figure of the present invention
Fig. 4 is the big mould area double-cladding of a present invention fiber amplifier structure chart
Among the figure: the continuous single-frequency seed source laser of 1-, the 2-first sound-optic modulator, 3-first order monomode fiber amplifier, the 4-first filtering isolator, 5-second level monomode fiber amplifier, the 6-second sound-optic modulator, the 7-second filtering isolator, the big mould area double-cladding of 8-fiber amplifier, 9-pulse sequence control signal source, 301-single-mode tail fiber coupling pumping source, 302-wavelength division multiplexer (WDM), the 303-single mode is protected inclined to one side gain fibre, 801-multimode pigtail coupling pumping source, the 802-pump combiner, 803-is big, and the mould area double-cladding is protected inclined to one side gain fibre.
Embodiment
The invention will be further described below in conjunction with embodiment and accompanying drawing, but should not limit protection scope of the present invention with this.
See also Fig. 1, Fig. 1 protects complete partially fiber pulse laser structural representation for single mode narrow linewidth of the present invention.As seen from the figure, single mode narrow linewidth of the present invention is protected complete partially fiber pulse laser, comprise continuous single-frequency seed source laser 1, the direction of propagation along described continuous single-frequency seed source laser 1 output beam is successively: first sound-optic modulator 2, first order monomode fiber amplifier 3, first separation filter 4, second level monomode fiber amplifier 5, second sound-optic modulator 6, second separation filter 7, the big mould area double-cladding of third level fiber amplifier 8, the output in pulse sequence control signal source 9 respectively with described first sound-optic modulator 2, second sound-optic modulator 6 links to each other with the sequencing control end of the big mould area double-cladding of third level fiber amplifier 8, provide the electric impulse signal of special time relation, control described first sound-optic modulator 2, the operating time of the big mould area double-cladding of the second sound-optic modulator 6 and third level fiber amplifier 8.
Described continuous single-frequency seed source laser 1 produces pulse train by first sound-optic modulator 2, after amplifying, first order monomode fiber amplifier 3 carries out isolation filter by 4 pairs of amplifying lasers of first separation filter, and then further amplify through second level monomode fiber amplifier 5, and carry out acoustooptic modulation again by second sound-optic modulator 6, carry out isolation filter through second separation filter 7 afterwards, and finally amplify output by the big mould area double-cladding of third level fiber amplifier 8, pulse sequence control signal source 9 provides the electric impulse signal with special time relation, controls described first sound-optic modulator 2, the operating time of the third level amplifier when second sound-optic modulator 6 and employing pulse pump.Fig. 2 is a first sound-optic modulator, the second sound-optic modulator and the third level are amplified the control impuls timing diagram when adopting pulse pump, Fig. 3 is monomode fiber amplifier architecture figure, 301-single-mode tail fiber coupling pumping source, 302-wavelength division multiplexer (WDM), the 303-single mode is protected inclined to one side gain fibre, and Fig. 4 is big mould area double-cladding fiber amplifier structure chart.801-multimode pigtail coupling pumping source, the 802-pump combiner, 803-is big, and the mould area double-cladding is protected inclined to one side gain fibre.
Lifting a specific embodiment below is described below:
As shown in Figure 1, centre wavelength is 1064nm, the seed source laser 1 of output single-frequency continuous laser, produce repetition 10KHz by first sound-optic modulator 2, the pulse train of pulsewidth 500ns, protect the amplifier 3 that inclined to one side Yb dosed optical fiber constitutes via the two-stage single mode, after 5, select pulse to produce repetition 100Hz by second sound-optic modulator 6, the pulse train of pulsewidth 500ns, the big mould area double-cladding of afterbody fiber amplifier 8 adopts core diameter 25 μ m (NA=0.06), inner cladding diameter 250 μ m (NA=0.46), the big mould area double-cladding optical fiber of doping ytterbium ion in the fibre core, obtain pulse energy and surpass 100 μ J, the amplification output of polarization extinction ratio＞14dB.
In sum, experiment shows that the present invention compares with technology formerly, single mode narrow linewidth of the present invention is protected complete partially fiber pulse laser and is had characteristics simple in structure, that be easy to control, its pulse repetition frequency and pulse duration are adjustable simultaneously, the linear polarization pulse laser of output narrow linewidth, high-peak power has improved lasing efficiency greatly.
Claims (3)
1. a single mode narrow linewidth is protected complete partially fiber pulse laser, comprise continuous single-frequency seed source laser (1), it is characterized in that being successively: first sound-optic modulator (2) along the direction of propagation of described continuous single-frequency seed source laser (1) output beam, first order monomode fiber amplifier (3), first separation filter (4), second level monomode fiber amplifier (5), second sound-optic modulator (6), second separation filter (7), the big mould area double-cladding of third level fiber amplifier (8), the output in pulse sequence control signal source (9) respectively with described first sound-optic modulator (2), second sound-optic modulator (6) links to each other with the sequencing control end of the big mould area double-cladding of third level fiber amplifier (8), provide the electric impulse signal of special time relation, control described first sound-optic modulator (2), the operating time of second sound-optic modulator (6) and the big mould area double-cladding of third level fiber amplifier (8).
2. single mode narrow linewidth according to claim 1 is protected complete partially fiber pulse laser, it is characterized in that the laser linewidth＜10MHz of described continuous single-frequency seed source laser (1).
3. single mode narrow linewidth according to claim 1 is protected complete partially fiber pulse laser, the gain fibre (303) that it is characterized in that described first order monomode fiber amplifier (3) and second level monomode fiber amplifier (5) is protected inclined to one side gain fibre for single mode, and the gain fibre (803) of the big mould area double-cladding of described third level fiber amplifier (8) is protected inclined to one side gain fibre for big mould area double-cladding.
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| CN 201110148475 CN102263356B (en) | 2011-06-03 | 2011-06-03 | Single-frequency narrow line width polarization maintaining full-optical fiber pulse laser device |
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Cited By (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103050874A (en) * | 2013-01-16 | 2013-04-17 | 山东海富光子科技股份有限公司 | High-power pulse type singe-frequency all-fiber laser system |
| CN104752941A (en) * | 2014-08-25 | 2015-07-01 | 深圳市创鑫激光股份有限公司 | Pulse width adjusting fiber laser based on UWB (Ultra Wide Band) light source |
| CN104752946A (en) * | 2014-08-25 | 2015-07-01 | 深圳市创鑫激光股份有限公司 | Pulse width adjusting fiber laser based on broadband seed resource |
| CN105244747A (en) * | 2015-09-23 | 2016-01-13 | 中国工程物理研究院应用电子学研究所 | High-energy long pulse laser obtaining device, method and application |
| CN106356703A (en) * | 2016-09-09 | 2017-01-25 | 中国科学院上海光学精密机械研究所 | High-perturbation-resistance laser seed source system based on single-polarization transmission fibers |
| CN110957626A (en) * | 2019-12-18 | 2020-04-03 | 株洲菲斯罗克光电技术有限公司 | Spectral rotary mirror and hybrid integrated microminiature ASE light source device |
| CN112490840A (en) * | 2020-11-26 | 2021-03-12 | 浙江热刺激光技术有限公司 | System and method for inhibiting continuous components in laser pulse traveling wave amplification process |
| CN112531451A (en) * | 2020-11-02 | 2021-03-19 | 深圳市圭华智能科技有限公司 | Laser time domain synchronous control system |
| CN112636149A (en) * | 2020-11-08 | 2021-04-09 | 罗根激光科技（武汉）有限公司 | mJ power amplifier suitable for 1064nm subnanosecond pulse |
| CN116435859A (en) * | 2023-05-23 | 2023-07-14 | 上海科乃特激光科技有限公司 | Pulse fiber laser system |
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| US20080089366A1 (en) * | 2006-05-15 | 2008-04-17 | Polaronyx, Inc. | High energy short pulse fiber laser achieved by combining pulse shaping, polarization shaping and spectral shaping |
| US20100158054A1 (en) * | 2006-11-27 | 2010-06-24 | Centre National De La Recherche Scientifique-Cnrs | Laser system with picosecond pulse emission |
| CN201044323Y (en) * | 2007-04-27 | 2008-04-02 | 中国科学院上海光学精密机械研究所 | Single-longitudinal modular Q laser with slave drive chamber length control |
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Cited By (14)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103050874A (en) * | 2013-01-16 | 2013-04-17 | 山东海富光子科技股份有限公司 | High-power pulse type singe-frequency all-fiber laser system |
| CN104752941A (en) * | 2014-08-25 | 2015-07-01 | 深圳市创鑫激光股份有限公司 | Pulse width adjusting fiber laser based on UWB (Ultra Wide Band) light source |
| CN104752946A (en) * | 2014-08-25 | 2015-07-01 | 深圳市创鑫激光股份有限公司 | Pulse width adjusting fiber laser based on broadband seed resource |
| CN104752941B (en) * | 2014-08-25 | 2016-10-26 | 深圳市创鑫激光股份有限公司 | Adjustable pulse width pulse optical fiber based on ultra broadband light source |
| CN104752946B (en) * | 2014-08-25 | 2016-11-16 | 深圳市创鑫激光股份有限公司 | Adjustable pulse width pulse optical fiber based on broadband seed source |
| CN105244747A (en) * | 2015-09-23 | 2016-01-13 | 中国工程物理研究院应用电子学研究所 | High-energy long pulse laser obtaining device, method and application |
| CN106356703A (en) * | 2016-09-09 | 2017-01-25 | 中国科学院上海光学精密机械研究所 | High-perturbation-resistance laser seed source system based on single-polarization transmission fibers |
| CN106356703B (en) * | 2016-09-09 | 2018-11-20 | 中国科学院上海光学精密机械研究所 | The laser seed source system based on single polarisation transfer optical fiber of highly resistance perturbation |
| CN110957626A (en) * | 2019-12-18 | 2020-04-03 | 株洲菲斯罗克光电技术有限公司 | Spectral rotary mirror and hybrid integrated microminiature ASE light source device |
| CN112531451A (en) * | 2020-11-02 | 2021-03-19 | 深圳市圭华智能科技有限公司 | Laser time domain synchronous control system |
| CN112636149A (en) * | 2020-11-08 | 2021-04-09 | 罗根激光科技（武汉）有限公司 | mJ power amplifier suitable for 1064nm subnanosecond pulse |
| CN112490840A (en) * | 2020-11-26 | 2021-03-12 | 浙江热刺激光技术有限公司 | System and method for inhibiting continuous components in laser pulse traveling wave amplification process |
| CN116435859A (en) * | 2023-05-23 | 2023-07-14 | 上海科乃特激光科技有限公司 | Pulse fiber laser system |
| CN116435859B (en) * | 2023-05-23 | 2024-03-29 | 上海科乃特激光科技有限公司 | Pulse fiber laser system |
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Date of cancellation: 20230105 Granted publication date: 20131030 Pledgee: Bank of China Limited Nanjing Gulou Branch Pledgor: NANJING MOVELASER TECHNOLOGY Co.,Ltd. Registration number: Y2022980003807 |
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Address after: 210000 Building B2, Hongfeng Science Park, Kechuang Road, Nanjing Economic and Technological Development Zone, Jiangsu Province Patentee after: Nanjing Mulai Laser Technology Co.,Ltd. Address before: Room 0601, Building C, Xingzhi Science Park, Xingzhi Road, Nanjing Economic and Technological Development Zone, Jiangsu 210046 Patentee before: Nanjing Mulai Laser Technology Co.,Ltd. |
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| CP02 | Change in the address of a patent holder |