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CN103326222A - Controllable dual-wavelength mode-locking pulse fiber laser - Google Patents

Controllable dual-wavelength mode-locking pulse fiber laser Download PDF

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CN103326222A
CN103326222A CN201310270591XA CN201310270591A CN103326222A CN 103326222 A CN103326222 A CN 103326222A CN 201310270591X A CN201310270591X A CN 201310270591XA CN 201310270591 A CN201310270591 A CN 201310270591A CN 103326222 A CN103326222 A CN 103326222A
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刘雪明
韩冬冬
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XiAn Institute of Optics and Precision Mechanics of CAS
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Abstract

本发明提供一种可控的双波长锁模脉冲激光器,该激光器包括泵浦源和依次形成光回路的波分复用器、掺杂光纤、输出耦合器、锁模器件,波分复用器用于将泵浦光和锁模器件输出的信号光耦合入掺杂光纤;该激光器还包括三端口环形器和偏振控制器,光经过输出耦合器后由三端口环形器a端口进入,然后经由三端口环形器b端口后依次经过不同中心波长的第一光纤光栅和第二光纤光栅反射到三端口环形器c端口输出至锁模器件,偏振控制器用于控制调节第一光纤光栅和第二光纤光栅以实现单波长和双波长激光输出的可控转换。该光纤激光器具有锁模运行稳定、调谐方便、成本低廉、常温运转的优点。

Figure 201310270591

The invention provides a controllable dual-wavelength mode-locked pulsed laser, which includes a pump source, a wavelength division multiplexer, a doped optical fiber, an output coupler, a mode-locked device, and a wavelength division multiplexer that sequentially form an optical circuit. It is used to couple the pump light and the signal light output by the mode-locking device into the doped fiber; the laser also includes a three-port circulator and a polarization controller. After port b of the port circulator, the first fiber grating and the second fiber grating with different central wavelengths are reflected to the three-port circulator c port and output to the mode-locking device. The polarization controller is used to control and adjust the first fiber grating and the second fiber grating In order to realize the controllable conversion of single-wavelength and dual-wavelength laser output. The fiber laser has the advantages of stable mode-locked operation, convenient tuning, low cost and normal temperature operation.

Figure 201310270591

Description

可控的双波长锁模脉冲光纤激光器Controllable dual-wavelength mode-locked pulsed fiber laser

技术领域technical field

本发明涉及一种光纤激光器,具体涉及一种可控的双波长锁模脉冲光纤激光器。The invention relates to a fiber laser, in particular to a controllable dual-wavelength mode-locked pulse fiber laser.

背景技术Background technique

双波长锁模脉冲光纤激光器在现代科学技术的很多领域都有着非常重要的应用,例如密集波分复用系统,光纤传感,光纤色散测量等。在某些应用场合,要求激光器可以在单波长和双波长之间来回切换,实现可控。Dual-wavelength mode-locked pulsed fiber lasers have very important applications in many fields of modern science and technology, such as dense wavelength division multiplexing systems, fiber optic sensing, fiber dispersion measurement, etc. In some applications, it is required that the laser can be switched back and forth between single wavelength and dual wavelength to achieve controllability.

目前,为了实现光纤激光器的双波长锁模脉冲输出有主动锁模技术和被动锁模技术两种选择,主动锁模技术有着重复频率高、线宽窄等优点,但由于腔内锁模调制器的加入,不仅增加了激光器的成本,同时还大大增加了腔内的损耗,降低了激光的脉冲能量;运用被动锁模技术的双波长锁模脉冲光纤激光器也得到了广泛的研究,但在双波长被动锁模光纤器中,其双波长形成机理往往是其腔型自身结构形成的光谱滤波效应,锁模波长的位置受周围环境影响严重,造成锁模波长位置不稳定,对实际应用造成很大的影响。At present, in order to realize the dual-wavelength mode-locked pulse output of fiber lasers, there are two options: active mode-locked technology and passive mode-locked technology. Active mode-locked technology has the advantages of high repetition frequency and narrow line width. Adding it not only increases the cost of the laser, but also greatly increases the loss in the cavity and reduces the pulse energy of the laser; the dual-wavelength mode-locked pulsed fiber laser using passive mode-locking technology has also been extensively studied, but in dual-wavelength In passive mode-locked fiber optics, the formation mechanism of dual wavelengths is often the spectral filtering effect formed by the structure of the cavity itself. The position of the mode-locked wavelength is seriously affected by the surrounding environment, resulting in instability of the position of the mode-locked wavelength, which has a great impact on practical applications. Impact.

发明内容Contents of the invention

为了克服上述背景技术中存在的缺陷,本发明提供一种结构简单,实施方便,常温稳定工作和可以在单波长和双波长之间来回切换实现锁模的可控双波长锁模脉冲光纤激光器。In order to overcome the defects in the above-mentioned background technology, the present invention provides a controllable dual-wavelength mode-locked pulsed fiber laser with simple structure, convenient implementation, stable operation at room temperature, and the ability to switch back and forth between single-wavelength and dual-wavelength to achieve mode-locking.

本发明的技术解决方案如下:Technical solution of the present invention is as follows:

一种可控的双波长锁模脉冲激光器,该激光器包括泵浦源和依次形成光回路的波分复用器、掺杂光纤、输出耦合器、锁模器件,所述波分复用器用于将泵浦光和锁模器件输出的信号光耦合入掺杂光纤;其特殊之处在于:该激光器还包括三端口环形器和偏振控制器,光经过输出耦合器后由三端口环形器a端口进入,然后经由三端口环形器b端口后依次经过不同中心波长的第一光纤光栅和第二光纤光栅反射到三端口环形器c端口输出至锁模器件,所述偏振控制器用于控制调节第一光纤光栅和第二光纤光栅以实现单波长和双波长激光输出的可控转换。A controllable dual-wavelength mode-locked pulsed laser, the laser includes a pump source and a wavelength division multiplexer, a doped optical fiber, an output coupler, and a mode-locked device that sequentially form an optical circuit, and the wavelength division multiplexer is used for The pump light and the signal light output by the mode-locking device are coupled into the doped fiber; the special feature is that the laser also includes a three-port circulator and a polarization controller. After the light passes through the output coupler, the a-port of the three-port circulator Enter, then pass through the b port of the three-port circulator, and then pass through the first fiber grating and the second fiber grating with different center wavelengths to reflect to the c port of the three-port circulator and output to the mode-locking device. The polarization controller is used to control and adjust the first A fiber grating and a second fiber grating are used to realize the controllable conversion of single-wavelength and dual-wavelength laser output.

上述泵浦源、波分复用器、掺杂光纤、输出耦合器、锁模器件、三端口环形器、第一光纤光栅和第二光纤光栅均采用单模光纤熔接,所述偏振控制器夹在第一光纤光栅和第二光纤光栅之间的单模光纤上。The above pump source, wavelength division multiplexer, doped fiber, output coupler, mode-locking device, three-port circulator, first fiber grating and second fiber grating are all spliced by single-mode fiber, and the polarization controller clamp On the single-mode fiber between the first fiber grating and the second fiber grating.

上述锁模器件是碳纳米管锁模器件,其主体是由碳纳米管溶液与聚乙烯醇溶液混合后蒸发制成的薄膜。The above-mentioned mode-locking device is a carbon nanotube mode-locking device, and its main body is a thin film made by mixing a carbon nanotube solution and a polyvinyl alcohol solution and evaporating it.

上述输出耦合器的输出比例为10%。The output ratio of the above output coupler is 10%.

上述掺杂光纤为掺铒光纤,优选型号为Coractive C600的掺铒光纤,泵浦源的工作波长为980nm,波分复用器的频分范围为980/1550nm,第一光纤光栅的中心波长为1549.5nm,第二光纤光栅的中心波长为1559.5nm,第一光纤光栅和第二光纤光栅反射带宽均为1nm.Above-mentioned doped optical fiber is erbium-doped optical fiber, preferred model is the erbium-doped optical fiber of Coractive C600, and the working wavelength of pumping source is 980nm, and the frequency division range of wavelength division multiplexer is 980/1550nm, and the central wavelength of the first fiber grating is 1549.5nm, the center wavelength of the second fiber Bragg grating is 1559.5nm, the reflection bandwidth of the first fiber Bragg grating and the second fiber Bragg grating are both 1nm.

附图说明Description of drawings

图1为本发明的结构示意图;Fig. 1 is a structural representation of the present invention;

图2为本发明双波长锁模时的光谱图;Fig. 2 is the spectrogram when dual-wavelength mode-locking of the present invention;

图3为本发明双波长锁模时的脉冲序列图;Fig. 3 is a pulse sequence diagram during dual-wavelength mode-locking of the present invention;

图4为本发明第一光纤光栅锁模时的光谱图;Fig. 4 is the spectrogram when the first fiber grating of the present invention is mode-locked;

图5为本发明第二光纤光栅锁模时的光谱图;Fig. 5 is the spectrogram when the second fiber grating of the present invention is mode-locked;

其中附图标记为:Wherein reference sign is:

1-泵浦光源;2-波分复用器;3-掺铒光纤;4-输出耦合器;5-环形器;6-偏振控制器;7-碳纳米管锁模器件;8-第一光纤光栅;9-第二光纤光栅。本发明的有益效果如下:1-pump light source; 2-wavelength division multiplexer; 3-erbium-doped fiber; 4-output coupler; 5-circulator; 6-polarization controller; 7-carbon nanotube mode-locking device; 8-first Fiber Bragg grating; 9 - the second fiber Bragg grating. The beneficial effects of the present invention are as follows:

1、该光纤激光器采用了光纤光栅作为波长选择器件,具有波长稳定、常温运转的优点。1. The fiber laser uses a fiber grating as a wavelength selection device, which has the advantages of stable wavelength and normal temperature operation.

2、该光纤激光器采用碳纳米管作为锁模器件,具有锁模运行稳定的优点。2. The fiber laser uses carbon nanotubes as the mode-locking device, which has the advantage of stable mode-locking operation.

3、该光纤激光器采用调节偏振控制器来实现单波长和双波长的转换,具有调谐方便的优点。3. The fiber laser adopts the adjustment polarization controller to realize the conversion of single wavelength and double wavelength, which has the advantage of convenient tuning.

4、该光纤激光器采用了全光纤结构,不用空间光调整器件,故其结构简单易于调整,稳定性好。4. The fiber laser adopts an all-fiber structure without spatial light adjustment devices, so its structure is simple and easy to adjust, and its stability is good.

5、碳纳米管锁模器件的应用,大大的降低了腔内的损耗,提高了激光脉冲能量。5. The application of carbon nanotube mode-locking device greatly reduces the loss in the cavity and improves the laser pulse energy.

6、该光纤激光器所用器件皆为普通光纤激光器所用的普通器件,都已经商用化,故成本非常低廉。6. The components used in the fiber laser are all common components used in common fiber lasers, and all of them have been commercialized, so the cost is very low.

具体实施方式Detailed ways

如图1所示,本发明提供的可控的双波长锁模脉冲光纤激光器包括泵浦光源1、波分复用器2、掺铒光纤3、输出耦合器4、三端口环形器5、第一光纤光栅8、第二光纤光栅9、碳纳米管锁模器件7,上述各个器件均采用单模光纤熔接,偏振控制器6夹在第一光纤光栅和第二光纤光栅之间的单模光纤上。As shown in Figure 1, the controllable dual-wavelength mode-locked pulsed fiber laser provided by the present invention includes a pump light source 1, a wavelength division multiplexer 2, an erbium-doped fiber 3, an output coupler 4, a three-port circulator 5, a A fiber Bragg grating 8, a second fiber Bragg grating 9, and a carbon nanotube mode-locking device 7, each of which is welded with a single-mode fiber, and the polarization controller 6 is a single-mode fiber sandwiched between the first fiber Bragg grating and the second fiber Bragg grating superior.

泵浦光源1选用工作波长为980nm的单模半导体激光器,波分复用器2的频分范围为980nm/1550nm,掺铒光纤3的型号为Coractive C600,在1550nm处色散系数为-9ps/nm/km,长度为5m,输出耦合器4输出比率为10%,第一光纤光栅8和第二光纤光栅9反射带宽均为1nm,所对应中心波长分别为1549.5nm和1559.5nm,偏振控制器6是常用标准器件,偏振控制器6在第一光纤光栅8和第二光纤光栅9之间,三端口环形器5,其中端口a与输出耦合器4连接,端口b与第一光纤光栅8连接,端口c与碳纳米管锁模器件7连接;光由a端口进入,然后经过b端口经过第一光纤光栅8和第二光纤光栅9反射到c端口输出;碳纳米管锁模器件7是自制锁模器件,由碳纳米管溶液与聚乙烯醇溶液混合后蒸发制成的薄膜,然后将薄膜夹在两个跳线头之间,并将跳线头用法兰盘固定;腔内光纤指的是除去输入和输出两段光纤外的其他所有光纤,光纤把各个器件连接起来组成环形激光腔,腔内其他光纤是总长度约为28m的标准单模光纤,在1550nm处其色散参数系数为17ps/nm/km。The pump light source 1 is a single-mode semiconductor laser with an operating wavelength of 980nm, the frequency division range of the wavelength division multiplexer 2 is 980nm/1550nm, the model of the erbium-doped fiber 3 is Coractive C600, and the dispersion coefficient at 1550nm is -9ps/nm /km, the length is 5m, the output ratio of the output coupler 4 is 10%, the reflection bandwidth of the first fiber Bragg grating 8 and the second fiber Bragg grating 9 are both 1nm, and the corresponding center wavelengths are 1549.5nm and 1559.5nm respectively, and the polarization controller 6 It is a commonly used standard device, the polarization controller 6 is between the first fiber Bragg grating 8 and the second fiber Bragg grating 9, and the three-port circulator 5, wherein port a is connected to the output coupler 4, port b is connected to the first fiber Bragg grating 8, Port c is connected to the carbon nanotube mode-locking device 7; light enters from the a port, then passes through the b-port and is reflected to the c-port output through the first fiber grating 8 and the second fiber grating 9; the carbon nanotube mode-locking device 7 is a self-made lock Molded device, a film made by mixing carbon nanotube solution and polyvinyl alcohol solution and evaporating, then sandwiching the film between two jumper heads, and fixing the jumper head with a flange; intracavity optical fiber refers to Except for all other optical fibers except the input and output two sections of optical fiber, the optical fiber connects various devices to form a ring laser cavity. The other optical fibers in the cavity are standard single-mode optical fibers with a total length of about 28m. The dispersion parameter coefficient at 1550nm is 17ps/ nm/km.

本发明采用碳纳米管锁模器件7可饱和吸收体实现自启动锁模。两个不同波长的光纤光栅通过三端口环形器5插入腔内进行光谱滤波,相应于光纤光栅中心波长的光才可以在腔内传输,两个光纤光栅之间由单模光纤连接。偏振控制器6夹在两个光纤光栅之间的单模光纤上,偏振控制器6通过挤压、旋转两个光纤光栅之间的单模光纤,从而改变光纤光栅的反射损耗。当对应于第一光纤光栅8的波长所受的损耗较小,而对应于第二光纤光栅9的波长损耗足够大时,激光腔将放大损耗小的波长而抑制损耗大的波长,从而对应于第一光纤光栅波长8的单波长锁模状态可以实现;反之,对应于第二光纤光栅9波长的单波长锁模状态可以实现。当对应于两个光纤光栅的两个波长的损耗相当,且泵浦光源1功率足够大时,激光腔将同时放大两个波长并实现双波长锁模。因此,调节偏振控制器使不同单波长锁模与双波长锁模可以轻易的转化与完成。The invention adopts the carbon nanotube mode-locking device 7 and saturable absorber to realize self-starting mode-locking. Two fiber gratings with different wavelengths are inserted into the cavity through the three-port circulator 5 for spectral filtering, only the light corresponding to the center wavelength of the fiber grating can be transmitted in the cavity, and the two fiber gratings are connected by a single-mode fiber. The polarization controller 6 is clamped on the single-mode fiber between the two fiber gratings, and the polarization controller 6 changes the reflection loss of the fiber grating by squeezing and rotating the single-mode fiber between the two fiber gratings. When the loss corresponding to the wavelength of the first fiber grating 8 is small, and the wavelength loss corresponding to the second fiber grating 9 is large enough, the laser cavity will amplify the wavelength with small loss and suppress the wavelength with large loss, thus corresponding to The single-wavelength mode-locked state of the first fiber Bragg grating wavelength 8 can be realized; conversely, the single-wavelength mode-locked state corresponding to the wavelength of the second fiber Bragg grating 9 can be realized. When the losses of the two wavelengths corresponding to the two fiber gratings are equal and the power of the pumping light source 1 is large enough, the laser cavity will simultaneously amplify the two wavelengths and realize dual-wavelength mode locking. Therefore, by adjusting the polarization controller, different single-wavelength mode-locking and dual-wavelength mode-locking can be easily converted and completed.

本发明实现双波长自启动锁模的阈值功率约20mw,采用光谱分析仪测量出输出激光的光谱和示波器观察脉冲序列,如图2、图3所示,此时,激光器实现双波长锁模稳定运转;然后通过调节偏振控制器,可以将双波长锁模转换为不同的单波长锁模状态,采用光谱分析仪测量出输出激光的光谱,如图4、图5所示。The present invention realizes that the threshold power of dual-wavelength self-starting mode-locking is about 20mw, and the spectrum of the output laser is measured by a spectrum analyzer and the pulse sequence is observed by an oscilloscope, as shown in Figure 2 and Figure 3. At this time, the laser implements dual-wavelength mode-locking and is stable Then, by adjusting the polarization controller, the dual-wavelength mode-locking can be converted into a different single-wavelength mode-locking state, and the spectrum of the output laser is measured by a spectrum analyzer, as shown in Figure 4 and Figure 5.

Claims (5)

1. controlled dual wavelength Mode-locked laser device, this laser comprises pumping source and forms successively the wavelength division multiplexer of light circuit, doped fiber, output coupler, locked mode device, and described wavelength division multiplexer is used for the flashlight of pump light and the output of locked mode device is coupled into doped fiber; It is characterized in that: this laser also comprises three port circulator and Polarization Controllers, light is entered by three port circulator a ports through behind the output coupler, then reflex to three port circulator c ports via the first fiber grating that passes through successively different centre wavelengths behind the three port circulator b ports and the second fiber grating and export the locked mode device to, described Polarization Controller is used for regulating and controlling the first fiber grating and the controlled conversion of the second fiber grating to realize that single wavelength and dual-wavelength laser are exported.
2. controlled dual wavelength Mode-locked laser device according to claim 1, it is characterized in that: pumping source, wavelength division multiplexer, doped fiber, output coupler, locked mode device, three port circulators, the first fiber grating and the second fiber grating all adopt the monomode fiber welding, and described Polarization Controller is clipped on the monomode fiber between the first fiber grating and the second fiber grating.
3. controlled dual wavelength Mode-locked laser device according to claim 2, it is characterized in that: described locked mode device is carbon nano-tube locked mode device, its main body is the film that evaporation is made after being mixed with poly-vinyl alcohol solution by carbon nano-tube solution.
4. controlled dual wavelength Mode-locked laser device according to claim 3, it is characterized in that: the export ratio of output coupler is 10%.
5. according to claim 1 to 4 arbitrary described controlled dual wavelength Mode-locked laser devices, it is characterized in that: doped fiber is Er-doped fiber, the operation wavelength of pumping source is 980nm, the frequency division scope of wavelength division multiplexer is 980/1550nm, the centre wavelength of the first fiber grating is 1549.5nm, the centre wavelength of the second fiber grating is 1559.5nm, and the first fiber grating and the second fiber grating reflection bandwidth are 1nm.
CN201310270591XA 2013-06-28 2013-06-28 Controllable dual-wavelength mode-locking pulse fiber laser Pending CN103326222A (en)

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CN103633546A (en) * 2013-12-16 2014-03-12 北京工业大学 Dual-wavelength dissipative soliton mode-locked laser
CN103633538A (en) * 2013-11-28 2014-03-12 中国科学院半导体研究所 Picosecond-controllable dual-wavelength fiber laser
CN103855597A (en) * 2014-03-03 2014-06-11 山东大学 Linear polarization ytterbium-doped double-clad fiber laser with dual wavelength switching function and adjusting method thereof
CN104752943A (en) * 2015-04-27 2015-07-01 天津理工大学 Interference structure-based dual-wavelength fiber laser
CN106253040A (en) * 2015-10-14 2016-12-21 北京信息科技大学 A kind of mode locked fiber laser system by Graphene reflecting mirror wavelength switching
CN104158074B (en) * 2014-07-21 2018-01-19 中国科学院西安光学精密机械研究所 Mode-locking all-fiber laser generating method capable of converting dual wavelengths
CN111370984A (en) * 2020-03-20 2020-07-03 北京工业大学 A narrow linewidth nanosecond all-fiber laser amplifier with tunable repetition rate and pulse width
CN113410736A (en) * 2021-05-24 2021-09-17 华南理工大学 Tunable single-frequency pulse fiber laser

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101986483A (en) * 2010-10-08 2011-03-16 北京航空航天大学 Passive mode-locked pulsed laser
CN201946871U (en) * 2010-12-10 2011-08-24 杭州恒川科技有限公司 Switchable multi-wavelength fiber laser and device based on polarization-maintaining fiber grating
CN102368585A (en) * 2011-09-16 2012-03-07 北京工业大学 High-repetition-frequency passive-mode-locking ultrashort-pulse all-fiber laser

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101986483A (en) * 2010-10-08 2011-03-16 北京航空航天大学 Passive mode-locked pulsed laser
CN201946871U (en) * 2010-12-10 2011-08-24 杭州恒川科技有限公司 Switchable multi-wavelength fiber laser and device based on polarization-maintaining fiber grating
CN102368585A (en) * 2011-09-16 2012-03-07 北京工业大学 High-repetition-frequency passive-mode-locking ultrashort-pulse all-fiber laser

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
PETER J. MOORE ET AL.: "Tunable dual-wavelength fiber laser", 《OPTICAL FIBER TECHNOLOGY》 *
ZHENGQIAN LUO ET AL.: "Graphene-based passively Q-switched dual-wavelength erbium-doped fiber laser", 《OPTICS LETTERS》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103633538A (en) * 2013-11-28 2014-03-12 中国科学院半导体研究所 Picosecond-controllable dual-wavelength fiber laser
CN103633538B (en) * 2013-11-28 2016-01-27 中国科学院半导体研究所 Picosecond-controlladual-wavelength dual-wavelength fiber laser
CN103633546A (en) * 2013-12-16 2014-03-12 北京工业大学 Dual-wavelength dissipative soliton mode-locked laser
CN103633546B (en) * 2013-12-16 2016-08-17 北京工业大学 Dual-wavelength dissipative soliton mode-locked laser
CN103855597A (en) * 2014-03-03 2014-06-11 山东大学 Linear polarization ytterbium-doped double-clad fiber laser with dual wavelength switching function and adjusting method thereof
CN104158074B (en) * 2014-07-21 2018-01-19 中国科学院西安光学精密机械研究所 Mode-locking all-fiber laser generating method capable of converting dual wavelengths
CN104752943A (en) * 2015-04-27 2015-07-01 天津理工大学 Interference structure-based dual-wavelength fiber laser
CN106253040A (en) * 2015-10-14 2016-12-21 北京信息科技大学 A kind of mode locked fiber laser system by Graphene reflecting mirror wavelength switching
CN106253040B (en) * 2015-10-14 2018-09-07 北京信息科技大学 A kind of mode locked fiber laser system by graphene speculum wavelength switching
CN111370984A (en) * 2020-03-20 2020-07-03 北京工业大学 A narrow linewidth nanosecond all-fiber laser amplifier with tunable repetition rate and pulse width
CN113410736A (en) * 2021-05-24 2021-09-17 华南理工大学 Tunable single-frequency pulse fiber laser

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