WO2020155696A1 - 一种多波长单频调q光纤激光器 - Google Patents

一种多波长单频调q光纤激光器 Download PDF

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WO2020155696A1
WO2020155696A1 PCT/CN2019/113798 CN2019113798W WO2020155696A1 WO 2020155696 A1 WO2020155696 A1 WO 2020155696A1 CN 2019113798 W CN2019113798 W CN 2019113798W WO 2020155696 A1 WO2020155696 A1 WO 2020155696A1
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wavelength
laser
fiber
polarization
frequency
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French (fr)
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徐善辉
李坤仪
杨昌盛
赵齐来
冯洲明
杨中民
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华南理工大学
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Priority to US17/427,106 priority Critical patent/US20220131329A1/en
Publication of WO2020155696A1 publication Critical patent/WO2020155696A1/zh

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    • H01S3/11—Mode locking; Q-switching; Other giant-pulse techniques, e.g. cavity dumping
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    • H01S3/11—Mode locking; Q-switching; Other giant-pulse techniques, e.g. cavity dumping
    • H01S3/1123—Q-switching
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    • H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/094003—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light the pumped medium being a fibre
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    • H01S3/09—Processes or apparatus for excitation, e.g. pumping
    • H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
    • H01S3/094—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light
    • H01S3/0941—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode
    • H01S3/09415—Processes or apparatus for excitation, e.g. pumping using optical pumping by coherent light of a laser diode the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
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    • H01S3/13—Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/131—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
    • H01S3/1317—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation by controlling the temperature
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    • H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/14—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range characterised by the material used as the active medium
    • H01S3/16—Solid materials
    • H01S3/1601—Solid materials characterised by an active (lasing) ion
    • H01S3/1603—Solid materials characterised by an active (lasing) ion rare earth
    • H01S3/1616—Solid materials characterised by an active (lasing) ion rare earth thulium

Definitions

  • the present invention belongs to the technical field of fiber lasers, and relates to a multi-wavelength single-frequency Q-switched fiber laser.
  • the Q-switched pulsed fiber laser has the advantages of tunability, simple structure, and easy integration, and therefore has important application prospects in lidar, laser sensing, gas detection, and the like.
  • multi-wavelength single-frequency Q-switched fiber lasers based on general Q-switched pulsed fiber lasers, simultaneously generate comb pulse lasers of different wavelengths in the laser resonator, and ensure that each laser wavelength operates at a single frequency, which is effective
  • the detection accuracy of the pulsed laser as the detection light source is improved, and the detection range of the lidar is greatly expanded. Its application in the differential absorption gas analysis lidar can increase the type of single detection gas and improve the detection efficiency.
  • multi-wavelength laser oscillation can be caused by inserting a fiber ring or a multi-wavelength fiber grating in the resonator.
  • pulsed laser can be realized by inserting a saturable absorber to cause passive Q-switching in the cavity.
  • the absorption coefficient of the saturable absorber will change with the light intensity, thereby changing the absorption loss in the resonant cavity and acting as a Q switch.
  • the saturable absorber has high reflectivity, compact structure, and easy integration. It can form the front and back mirrors of the resonant cavity with the multi-wavelength fiber grating, which is beneficial to shorten the length of the resonant cavity.
  • Shortening the cavity length can make the distance between adjacent laser longitudinal modes in the resonant cavity wider.
  • the reflection bandwidth of each reflection interval of the polarization-maintaining multi-wavelength narrowband fiber grating is narrowed to a certain extent, it can ensure that only one longitudinal mode of the laser at each wavelength reaches Gain threshold, so that the laser maintains single longitudinal mode operation.
  • Gain threshold the laser maintains single longitudinal mode operation.
  • rare earth ions will cause the gain to be uniformly broadened, which will cause mode competition among various wavelengths, which makes it difficult for multi-wavelength pulsed lasers to achieve stable output. Therefore, it is necessary to control the temperature of the resonant cavity.
  • the gain of signal light of different wavelengths can be adjusted, so that the gain of signal light of each wavelength is greater than its loss, thereby realizing the control of the laser wavelength.
  • an optical path with a polarization maintaining structure can make lasers of different wavelengths work in different polarization states, thereby reducing gain competition.
  • the multi-wavelength single-frequency Q-switched fiber laser based on the polarization-maintaining short straight cavity structure has narrow linewidth, compact structure and stable output, and has a wide range of application prospects.
  • the dual-channel pulsed laser was coupled to the output optical path by using a spatial optical path and a frequency multiplier mirror to achieve Dual-channel multi-wavelength pulsed laser output.
  • the Q-switched pulsed lasers required by the above patents (2) and (3) do not realize single longitudinal mode (single frequency) operation at each output wavelength.
  • the purpose of the present invention is to provide a multi-wavelength single frequency Q-switched fiber laser.
  • the invention utilizes the Q-switching characteristics of the saturable absorber, and combines the selection of the signal light wavelength by the polarization-maintaining multi-wavelength narrow-band fiber grating, and the saturable absorber and the polarization-maintaining multi-wavelength narrow-band fiber grating are respectively connected to the ends of the centimeter-level high-gain fiber.
  • the temperature control module is used to accurately control the temperature of the resonant cavity, and under the pumping action of the pump source, a high-performance multi-wavelength single-frequency Q-switched fiber laser can be directly output from the resonant cavity.
  • a multi-wavelength single frequency Q-switched fiber laser including: a Bragg laser resonator, and a cavity temperature control module
  • the Bragg laser resonator includes a high-gain fiber , Saturable absorber and polarization-maintaining multi-wavelength narrow-band fiber grating; both ends of high-gain fiber Connected with saturable absorber and polarization-maintaining multi-wavelength narrow-band fiber grating respectively.
  • Bragg laser resonator is placed in the cavity temperature control module for precise temperature control; the pump end of the polarization-maintaining wavelength division multiplexer is connected to the pump source, The common end of the polarization-maintaining wavelength division multiplexer is connected to the polarization-maintaining multi-wavelength narrow-band fiber grating, and the signal end of the polarization-maintaining wavelength division multiplexer is connected to the input end of the polarization-maintaining optical isolator.
  • the pump light generated by the pump source is input through the pump end of the polarization-maintaining wavelength division multiplexer, and then coupled to the high-gain fiber via the polarization-maintaining multi-wavelength narrow-band fiber grating for pumping, generating multiple wavelengths in the Bragg laser cavity Single-frequency pulse laser, the signal end of the polarization-maintaining wavelength division multiplexer is connected to the input end of the polarization-maintaining optical isolator, and finally the multi-wavelength single-frequency Q-switched fiber laser generated by the Bragg laser resonator is output through the output port of the polarization-maintaining optical isolator .
  • the relaxation time of the saturable absorber is less than 20 ps
  • the reflectivity of the laser signal light of each wavelength is greater than 80%
  • the reflectivity of the pump light is less than 20%.
  • the high gain fiber is a rare earth doped single-mode glass fiber
  • the core component of the high gain fiber includes phosphate glass, germanate glass, silicate glass, and fluoride glass.
  • the core of the high-gain optical fiber is doped with high-concentration luminescent ions, the luminescent ions are a combination of one or more of lanthanide ions and transition metal ions, and the luminescent ion doping concentration is greater than 1x10 19 ions/cm 3 , and it is uniformly doped in its core.
  • the polarization-maintaining multi-wavelength narrow-band fiber grating is to write two or more Bragg gratings with different center wavelengths on the polarization-maintaining fiber, so that it has selective comb reflection on the wavelength of the laser signal.
  • the 3dB reflection bandwidth of each reflection interval of the polarization-maintaining multi-wavelength narrow-band fiber grating is not greater than 0.08 nm; its reflectivity to the wavelength of the laser signal light is greater than 50%.
  • the polarization-maintaining multi-wavelength narrow-band fiber grating and the high-gain fiber are directly butt-coupled by grinding and polishing the respective fiber end faces, or fusion-coupled by a fiber fusion splicer.
  • the resonant cavity temperature control module includes a semiconductor refrigerator (Thermoelectric Cooler, TEC), and the control accuracy of the resonant cavity temperature control module is ⁇ 0.01°C.
  • TEC Thermoelectric Cooler
  • the technical effect of the present invention is that the Q-switching characteristics of the saturable absorber can be used at the same time, combined with the selection of the laser wavelength by the polarization-maintaining multi-wavelength narrowband fiber grating, and the saturable absorber and the protective Partially multi-wavelength narrow-band fiber gratings are connected to the ends of the centimeter-level high-gain fiber to form a distributed Bragg junction Under the continuous excitation of the laser pump source, the working temperature of the resonant cavity can be precisely controlled by the cavity temperature control module, which can realize the simultaneous laser Q-switching and multi-wavelength in the short-line laser cavity. Laser lasing.
  • each wavelength laser operates at a single frequency, and a stable multi-wavelength single-frequency Q-switched pulse can be obtained.
  • the multi-wavelength single-frequency Q-switched fiber laser obtained by the invention can realize full-fiber, with compact structure, stable working performance, easy maintenance and low cost. It is an ideal light source for lidar, laser remote sensing, gas detection and other systems.
  • FIG. 1 is a schematic structural diagram of a multi-wavelength single-frequency Q-switched fiber laser in an embodiment.
  • a multi-wavelength single-frequency Q-switched fiber laser provided by this embodiment includes a saturable absorber 1, a high-gain fiber 3, a polarization-maintaining multi-wavelength narrowband fiber grating 4, and a cavity temperature control module , Pump source 6, polarization maintaining wavelength division multiplexer 5, and polarization maintaining optical isolator 7.
  • one end of the high gain fiber 3 is connected to the saturable absorber i
  • the other end of the high gain fiber 3 is connected to one end of the polarization maintaining multi-wavelength narrowband fiber grating 4, and the three are connected to form a distributed Bragg
  • the single-frequency laser resonant short cavity is the Bragg laser resonant cavity
  • the Bragg laser resonant cavity is placed in the resonant cavity temperature control module 2 for precise temperature control.
  • the pump end of the polarization-maintaining wavelength division multiplexer 5 is connected to the pigtail of the pump source 6, and the common end of the polarization-maintaining wavelength division multiplexer 5 is connected to the other end of the polarization-maintaining multi-wavelength narrowband fiber grating 4.
  • the signal terminal of the division multiplexer 5 is connected to the input terminal of the polarization maintaining optical isolator 7.
  • the multi-wavelength single-frequency Q-switched fiber laser generated by the Bragg laser resonator is output through the output port of the polarization maintaining optical isolator 7.
  • the laser working medium high gain fiber 3 used in this example is a thulium-doped phosphate glass fiber, and the doping concentration of money ions in the core of the phosphate fiber is 4.5 ⁇ 10 2() ions/cm 3 , which is used The length is 2cm.
  • Saturable The absorber 1 is a semiconductor saturable absorption mirror based on mV group semiconductors, with a reflection bandwidth of 1880-2040 nm, a reflectivity near 1950 nm, and a relaxation time of 10 ps.
  • the polarization-maintaining multi-wavelength narrow-band fiber grating 4 in this example writes two Bragg gratings on the same position of the polarization-maintaining fiber, so that the reflection spectrum of the narrow-band fiber grating has four reflection peaks with a wavelength interval of 0.4 nm, where the slow axis
  • the center wavelengths are 1950.4 and 1951.2 nm, and the fast axis center wavelengths are 1950 and 1950.8 nm, respectively.
  • the 3dB reflection bandwidth of each wavelength reflection peak is 0.08 nm, and its reflectivity to the laser signal wavelength is 65%.
  • the saturable absorber 1 and the thulium-doped phosphate glass fiber adopt end-to-face coupling, and the thulium-doped phosphate glass fiber and the polarization-maintaining multi-wavelength narrow-band fiber grating 4 are coupled to each other by grinding their ends, and the three are combined to form a Bragg laser cavity.
  • the Bragg laser resonator is placed in a metal copper tank.
  • the metal copper tank has good wrapping properties for the resonant cavity, can fix and protect the resonant cavity, and use the resonant cavity temperature control module 2 composed of a TEC cooler to perform the entire Bragg laser resonant cavity Accurate temperature control, control accuracy ⁇ 0.01°C.
  • a pump source 6 with a working wavelength of 1610 nm is selected, and its pump output power is 200 mW.
  • the pump source 6 completes the pumping operation of the Bragg laser cavity through a 1610/1950nm polarization-maintaining wavelength division multiplexer 5, and finally the multi-wavelength single frequency Q-switched pulse laser output from the Bragg laser cavity passes through a work center Polarization maintaining optical isolator 7 with a wavelength of 1950 nm is output.
  • a Q-switched pulsed fiber laser output with multiple wavelengths (the working center wavelengths are 1950, 1950.4, 1950.8 and 1951.2 nm respectively) and a single longitudinal mode operation in each wavelength can be finally realized.

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  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

一种多波长单频调Q光纤激光器。激光器包括：可饱和吸收体(1)、高增益光纤(3)、保偏多波长窄带光纤光栅(4)、谐振腔温度控制模块(2)、保偏波分复用器(5)、泵浦源(6)和保偏光隔离器(7)。光纤激光器以高掺杂磷酸盐光纤作为激光增益介质，两端分别与可饱和吸收体、保偏多波长窄带光纤光栅连接，构成短线形激光腔，其短腔长能实现谐振腔内激光单纵模运转，同时腔内结合保偏多波长窄带光纤光栅引起的多波长谐振和可饱和吸收体的被动调Q性能，使谐振腔中实现稳定的多波长单频的脉冲激光输出。多波长单频调Q光纤激光器实现重复频率可调的多个波长脉冲激光同时输出，并且每个波长的激光均保持单频运转，可广泛用于激光雷达、激光传感和气体探测方面。

Description

一种多波长单频调 Q光纤激光器 技术领域
[0001] 本发明属于光纤激光器技术领域， 涉及一种多波长单频调 Q光纤激光器。
背景技术
[0002] 调 Q脉冲光纤激光器由于其具有可调谐、 结构简单、 便于集成等优势， 因此在 激光雷达、 激光传感、 气体探测等方面有着重要的应用前景。 尤其是多波长单 频调 Q光纤激光器， 其在一般调 Q脉冲光纤激光器基础上， 在激光谐振腔内同时 产生不同波长的梳状脉冲激光， 并且保证每个激光波长都以单频运转， 有效提 高了脉冲激光器作为探测光源的探测精度， 大大拓宽了激光雷达的探测种类范 围， 其应用在差分吸收气体分析激光雷达上， 可以增加单次探测气体种类， 提 高探测效率。
[0003] 对于光纤激光器， 可以通过在谐振腔中插入光纤环或多波长光纤光栅来引起多 波长激光振荡。 另一方面， 可以通过插入可饱和吸收体引起谐振腔内被动调 Q来 实现脉冲激光。 可饱和吸收体的吸收系数会随光强变化， 从而改变谐振腔内的 吸收损耗， 起到 Q开关的作用。 且与其他脉冲调制元件相比， 可饱和吸收体反射 率高、 结构紧凑、 易于集成， 与多波长光纤光栅可以组成谐振腔的前后腔镜， 有利于缩短谐振腔腔长。 缩短腔长可以使得谐振腔内相邻激光纵模间隔更宽， 当保偏多波长窄带光纤光栅的每个反射区间反射带宽窄至一定程度， 就能确保 每个波长下只有一个激光纵模达到增益阈值， 从而使得激光器保持单纵模运转 。 此外， 在室温条件下， 由于稀土离子会导致增益均匀展宽， 从而引起的各个 波长之间模式竞争， 导致多波长脉冲激光很难实现稳定输出。 因此需要对谐振 腔进行温度控制， 通过调节谐振腔温度， 可以调节不同波长信号光的增益， 使 得每个波长信号光增益都大于其损耗， 从而实现了激光波长的控制。 另一方面 ， 采用保偏结构的光路可以使不同波长激光工作在不同偏振态， 进而减少增益 竞争。 基于保偏短直腔结构的多波长单频调 Q光纤激光器线宽窄、 结构紧凑、 输 出稳定， 有广泛的应用前景。 [0004] 相关的专利有： （1） 2014年， 中国科学院上海光学精密机械研究所申请了基 于电光晶体调谐腔长的种子注入单频脉冲激光器的专利 [CN 103779776A] , 利用 电光晶体的电光效应， 通过改变驱动电源电压， 改变电光晶体折射率和系统光 学腔长， 形成 Q开关， 实现单频调 Q脉冲激光输出。 但该专利非全光纤化， 结构 复杂， 且只能实现单一波长的单频运转， 没有实现多波长激光同时输出。 （2） 2014年， 山东理工大学申请了多波长可调谐调 Q光纤激光器的专利 [公开号： CN 104377541A] , 利用在拉锥光纤表面覆盖上石墨烯来引起调 Q， 并且光场在拉锥 光纤内产生相位差形成干涉形成多波长激光， 从而实现了多波长可调谐调 Q激光 输出。 （3） 2016年， 中国人民解放军军事医学科学院申请了双通道多波长脉冲 激光器的专利 [公开号： CN 205693132U] , 利用空间光路和倍频镜， 将双通道脉 冲激光耦合到输出光路， 实现了双通道多波长脉冲激光输出。 但是上述专利 （2 ） 和 （3） 所要求的调 Q脉冲激光在每个输出波长激光并未实现单纵模 （单频） 运转。
发明概述
技术问题
问题的解决方案
技术解决方案
[0005] 本发明的目的是提供一种多波长单频调 Q光纤激光器。 本发明利用可饱和吸收 体的调 Q特性， 结合保偏多波长窄带光纤光栅对信号光波长的选择， 把可饱和吸 收体和保偏多波长窄带光纤光栅分别对接在厘米级高增益光纤两端， 构成分布 式布拉格短线形腔结构的激光谐振腔。 通过温度控制模块对谐振腔进行精确温 度控制， 并且在泵浦源的泵浦作用下， 可以直接从谐振腔中输出高性能的多波 长单频调 Q光纤激光。
[0006] 为达到上述目的， 本发明采用如下技术方案。
[0007] 一种多波长单频调 Q光纤激光器， 包括： 布拉格激光谐振腔、 腔温度控制模块
、 高增益光纤、 保偏波分复用器（Wavelength Division Multiplexer， WDM）、 泵浦 源（Laser Diode， LD）和保偏光隔离器（Isolator， ISO）； 所述布拉格激光谐振腔包 括高增益光纤、 可饱和吸收体和保偏多波长窄带光纤光栅； 高增益光纤的两端 分别与可饱和吸收体、 保偏多波长窄带光纤光栅连接， 布拉格激光谐振腔置于 谐振腔温度控制模块中进行精确温度控制； 保偏波分复用器的泵浦端与泵浦源 连接， 保偏波分复用器的公共端与保偏多波长窄带光纤光栅连接， 保偏波分复 用器的信号端与保偏光隔离器的输入端连接。 由泵浦源产生泵浦光经由保偏波 分复用器的泵浦端输入， 再经由保偏多波长窄带光纤光栅耦合到高增益光纤中 进行泵浦， 在布拉格激光谐振腔中产生多波长单频脉冲激光， 保偏波分复用器 的信号端与保偏光隔离器的输入端连接， 最终布拉格激光谐振腔所产生的多波 长单频调 Q光纤激光经保偏光隔离器的输出端口输出。
[0008] 进一步优化的， 所述的可饱和吸收体的弛豫时间小于 20ps， 其对每个波长的激 光信号光的反射率均大于 80%， 对泵浦光的反射率小于 20%。
[0009] 进一步优化的， 所述的高增益光纤为稀土掺杂单模玻璃光纤， 高增益光纤的纤 芯成分包含有磷酸盐玻璃、 锗酸盐玻璃、 硅酸盐玻璃、 氟化物玻璃中的一种以 上， 所述高增益光纤的纤芯掺杂高浓度的发光离子， 所述发光离子为镧系离子 、 过渡金属离子中一种或多种的组合体， 所述发光离子掺杂浓度大于 1x10 19 ions/cm 3,且在其纤芯中是均勻掺杂。
[0010] 进一步优化的， 所述的保偏多波长窄带光纤光栅是在保偏光纤上写入两个或以 上中心波长不同的布拉格光栅， 使得其对激光信号波长有选择性梳状反射。
[0011] 进一步优化的， 所述的保偏多波长窄带光纤光栅的每个反射区间的 3dB反射带 宽均不大于 0.08nm; 其对激光信号光波长的反射率大于 50%。
[0012] 进一步优化的， 所述的保偏多波长窄带光纤光栅和高增益光纤之间是通过研磨 抛光各自的光纤端面后直接对接耦合， 或者通过光纤熔接机熔接耦合。
[0013] 进一步优化的， 所述的谐振腔温度控制模块包括半导体制冷器 (Thermoelectric Cooler, TEC) 谐振腔温度控制模块的控制精度为 ±0.01°C。
发明的有益效果
有益效果
[0014] 与现有技术相比， 本发明的技术效果是： 可以同时利用可饱和吸收体的调 Q特 性， 结合保偏多波长窄带光纤光栅对激光波长的选择， 把可饱和吸收体和保偏 多波长窄带光纤光栅分别对接在厘米级高增益光纤两端， 构成分布式布拉格结 构的短线形激光谐振腔， 在激光泵浦源的连续激励下， 通过谐振腔温度控制模 块对谐振腔的工作温度进行精确控制， 可以实现在短线形腔中同时实现激光的 调 Q和多波长激射， 此外， 由于谐振腔腔长较短且窄带光纤光栅的每个波长的反 射带宽较窄， 保证了每一个波长激光都是单频运转， 可以得到性能稳定的多波 长单频调 Q脉冲激光输出。 该发明获得的多波长单频调 Q光纤激光器可以实现全 光纤化， 其结构紧凑、 工作性能稳定、 易于维护、 成本低， 是激光雷达、 激光 遥感、 气体探测等系统的理想光源。
对附图的简要说明
附图说明
[0015] 图 1为实施例中一种多波长单频调 Q光纤激光器的结构示意图。
[0016] 图中： 1一可饱和吸收体， 2—谐振腔温度控制模块， 3—高增益光纤， 4一保偏 多波长窄带光纤光栅， 5 -保偏波分复用器， 6 -泵浦源， 7 -保偏光隔离器。 发明实施例
本发明的实施方式
[0017] 以下结合附图， 通过具体实施例子对本发明作进一步描述， 需要说明的是本发 明要求保护的范围并不局限于实施例表述的范围。
[0018] 如图 1， 本实施例提供的一种多波长单频调 Q光纤激光器， 其包括可饱和吸收体 1、 高增益光纤 3、 保偏多波长窄带光纤光栅 4、 谐振腔温度控制模块、 泵浦源 6 、 保偏波分复用器 5和保偏光隔离器 7。 各部件之间的结构关系是： 高增益光纤 3 的一端与可饱和吸收体 i连接， 高增益光纤 3的另一端与保偏多波长窄带光纤光 栅 4的一端连接， 三者连接形成分布式布拉格单频激光谐振短腔即布拉格激光谐 振腔， 并将布拉格激光谐振腔置于谐振腔温度控制模块 2中进行精确温度控制。 保偏波分复用器 5的泵浦端与泵浦源 6的尾纤连接， 保偏波分复用器 5的公共端与 保偏多波长窄带光纤光栅 4的另一端连接， 保偏波分复用器 5的信号端与保偏光 隔离器 7的输入端连接。 最终布拉格激光谐振腔所产生的多波长单频调 Q光纤激 光经由保偏光隔离器 7的输出端口输出。
[0019] 本例中所使用的激光工作介质高增益光纤 3为掺铥磷酸盐玻璃光纤， 该磷酸盐 光纤钱离子在纤芯内掺杂浓度为 4.5x10 2() ions/cm 3， 其使用长度为 2cm。 可饱和 吸收体 1为基于 m-V族半导体的半导体可饱和吸收镜， 反射带宽为 1880-2040nm ， 在 1950nm附近的反射率为 90%， 弛豫时间为 10ps。 本例中的保偏多波长窄带 光纤光栅 4是在保偏光纤的同一位置上写入两个布拉格光栅， 使得窄带光纤光栅 反射谱上具有四个波长间隔为 0.4nm的反射峰， 其中慢轴中心波长分别为 1950.4 和 1951.2nm， 快轴中心波长分别为 1950和 1950.8nm， 每个波长反射峰的 3dB反射 带宽均为 0.08nm， 其对激光信号波长的反射率为 65%。 其中， 可饱和吸收体 1与 掺铥磷酸盐玻璃光纤采用端面对接耦合， 掺铥磷酸盐玻璃光纤和保偏多波长窄 带光纤光栅 4通过研磨各自端面对接耦合， 三者结合组成布拉格激光谐振腔。 将 布拉格激光谐振腔置于金属铜槽中， 金属铜槽对谐振腔有良好的包裹性， 能够 固定且保护谐振腔， 并用 TEC制冷器构成的谐振腔温度控制模块 2对整个布拉格 激光谐振腔进行精确温度控制， 控制精度 ±0.01°C。 同时选择工作波长为 1610nm 的泵浦源 6， 其泵浦输出功率为 200mW。 泵浦源 6通过一个 1610/1950nm的保偏波 分复用器 5完成对布拉格激光谐振腔的泵浦抽运作用， 最终布拉格激光谐振腔输 出的多波长单频调 Q脉冲激光经由一个工作中心波长为 1950nm的保偏光隔离器 7 输出。 基于上述方式， 最终可以实现多波长 （工作中心波长分别为 1950， 1950.4 ， 1950.8和 1951.2nm） 且每个波长内单一纵模运转的调 Q脉冲光纤激光输出。

Claims

权利要求书
[权利要求 1] 一种多波长单频调 Q光纤激光器， 其特征在于， 包括： 布拉格激光谐 振腔、 腔温度控制模块 （2） 、 高增益光纤 （3） 、 保偏波分复用器 （ 5） 、 泵浦源 （6） 和保偏光隔离器 （7） ; 所述布拉格激光谐振腔包 括高增益光纤 （3） 、 可饱和吸收体 （1） 和保偏多波长窄带光纤光栅 （4） ； 高增益光纤 （3） 的两端分别与可饱和吸收体 （1） 、 保偏多 波长窄带光纤光栅 （4） 连接， 布拉格激光谐振腔置于谐振腔温度控 制模块 （2） 中进行温度控制； 保偏波分复用器 （5） 的泵浦端与泵浦 源 （6） 连接， 保偏波分复用器 （5） 的公共端与保偏多波长窄带光纤 光栅 （4） 连接， 保偏波分复用器 （5） 的信号端与保偏光隔离器 （7 ） 的输入端连接。
[权利要求 2] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述可饱和吸收体 （1） 的弛豫时间小于 20ps， 其对每个波长的激光 信号光的反射率均大于 80%， 对泵浦光的反射率小于 20%。
[权利要求 3] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述高增益光纤 （3） 为稀土掺杂单模玻璃光纤， 高增益光纤 （3） 的 纤芯成分包含有磷酸盐玻璃、 锗酸盐玻璃、 硅酸盐玻璃、 氟化物玻璃 中的一种以上； 所述高增益光纤 （3） 的纤芯掺杂高浓度的发光离子 ， 所述发光离子为镧系离子、 过渡金属离子中一种或多种的组合体； 所述发光离子掺杂浓度大于 1x10 19ions/cm 3， 且在高增益光纤 （3） 的纤芯中是均匀掺杂。
[权利要求 4] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述保偏多波长窄带光纤光栅 （4） 是在保偏光纤上写入两个或以上 中心波长不同的布拉格光栅， 使得其对激光信号波长有选择性梳状反 射。
[权利要求 5] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述保偏多波长窄带光纤光栅 （4） 的每个反射区间的 3dB反射带宽 均不大于 0.08nm; 其对激光信号光波长的反射率大于 50%。
[权利要求 6] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述保偏多波长窄带光纤光栅 （4） 和高增益光纤 （3） 通过研磨抛光 各自的光纤端面后直接对接耦合， 或者通过光纤熔接机熔接耦合。
[权利要求 7] 如权利要求 1所述的一种多波长单频调 Q光纤激光器， 其特征在于： 所述谐振腔温度控制模块 （2） 包括半导体制冷器 （TEC） 谐振腔 温度控制模块 （2） 的控制精度为 ±0.01°C。
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CN115967002A (zh) * 2022-11-25 2023-04-14 山东省科学院激光研究所 一种多通道快速选择及可调谐单频光纤激光器和使用方法

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