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保偏铒镱共掺光纤制备及其激光性能研究

Fabrication and Laser Performance of Polarization-Maintaining Erbium-Ytterbium Co-Doped Fiber
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摘要 随着激光雷达技术的快速发展,激光雷达在军事及民用领域中的应用不断增多。保偏铒镱共掺光纤是1.5μm激光雷达重要的增益介质,对其性能有重要的影响。成功制备出10μm/128μm保偏铒镱共掺光纤,其双折射系数为1.29×10^(-4),在1310 nm处的消光比为24 dB@4 m。基于该光纤搭建了全保偏全光纤主振荡功率放大系统,实验结果显示,当信号波长为1551 nm,光纤长度为7.5 m,940 nm泵浦功率为16.5 W时,输出功率为5.8 W,斜率效率达36%,输出激光的消光比为21 dB。该保偏铒镱共掺光纤具有优异的激光性能,为1.5μm激光雷达系统的国产化提供了新的解决方案。 Objective Lidar has been widely used in wind ranging,automatic drive and sensing mapping.The reflected light signal is obtained through first emitting a Gaussian beam from the laser source and then reflecting after reaching the surface of the object.After the computer analysis,the information of the object such as orientation,attitude and distance can be obtained.However,as for a lidar system,its laser source is an important unit influencing the performance of the whole system.A fiber laser has become the best choice of the light source for a lidar system,because of its good beam quality,high pulse energy and high repetition rate.At the same time,an erbiumytterbium co-doped fiber has attracted the attention of many researches due to its advantages such as“eye-safe”and low atmospheric transmission loss.Therefore,as the most important gain medium for the laser lidar,polarizationmaintaining erbium-ytterbium co-doped fiber has important research significance.In this paper,a 10μm/128μm polarization-maintaining erbium-ytterbium co-doped fiber is successfully fabricated by the modified chemical vapor deposition(MCVD)technique combined with the solution doping technology(SDT).The structural parameters and optical properties of this polarization-maintaining erbium-ytterbium co-doped fiber are measured.And its laser performance is also studied.Methods MCVD combined with SDT is used to fabricate the erbium-ytterbium co-doped fiber.The content(mole fraction)of P_(2)O_(5) in the core is increased by more than 10% with reverse phosphorus doping and gas phase compensation.In order to avoid the defect of the core bursting during drilling,the fiber prefabricated rod is first annealed due to the high stress of its core.Through the Sagnac interferometer and the optical spectrum analyzer(OSA),the birefringence value is measured.The measurement structure is shown in Fig.3.And the measurement structure of polarization extinction ratio is also shown in Fig.5.In order to analyze the laser performance,the structure of an erbium-ytterbium co-doped fiber laser is shown in Fig.6.The seed source has a power of 20 mW and a central wavelength of 1551 nm.An isolator(ISO)connected to the seed is used to protect the seed source.The isolator is followed by a(2+1)×1 forward pump combiner(PC),and one of its pump fiber is used to monitor the backward power and observe the backward spectrum.The 940 nm light generated by the laser diode(LD)is coupled to the active fiber through the pump fiber of the(2+1)×1 backward PC,and the pump power is 16.5 W.The coiling diameter of the active fiber is 10 cm.The cladding pump stripper(CPS)is implemented by coating a high refractive index adhesive to filter cladding light from the fiber.Finally,an isolator is fused at the end to prevent reflection.Results and Discussions The dimension of the fiber is shown in the inset of Fig.2(b).The diameters of core and cladding are measured to be 10.19μm and 128.69μm,respectively.The diameter of the boron rod is measured to be 32.59μm.Figure 2(b)shows the refractive index profile of the prefabricated rod.A numerical aperture of 0.24 is finally achieved.The absorption coefficient measured by the truncation method is 2.42 dB/m at 940 nm.The interference image at 1500--1600 nm is observed in the OSA(Fig.4).The beat length at 1550 nm is calculated to be 9 mm with a birefringence coefficient of 1.29×10^(-4).At the same time,apolarization extinction ratio of 24 dB at 1310 nm is measured through the erbium-ytterbium co-doped fiber with a length of 4 m.As for the laser performance,due to the inherent loss,the final seed power coupling into the active fiber is 17.5 mW.Figure 7(a)shows the slope efficiency under different fiber lengths and pump powers.It can be seen from this figure that the optimal length is 7.5 m.When the pump power is 16.5 W,the output power and the slope efficiency reach the maximum,which are 5.8 Wand 36%,respectively.The polarization extinction ratio is measured to be 21 dB.In addition,as shown in Fig.7(b),the optical-to-optical efficiency tends to be saturated with the increase of pump power at different lengths.After reaching the saturation state,the optical-to-optical efficiency is more than 33%without a downward trend,which indicates that the laser power can be further increased at this time.The spectrum at 7.5 mis shown in Fig.8.It can be observed from this output spectrum that the amplified spontaneous emission(ASE)power increases gradually with the increase of pump power,but the signal-to-noise ratio remains above 50 dB.From the backward spectrum,one can observe that the remaining pump light intensity is stable,which may be caused by the fact that some spiral pump light in the polarization-maintaining fiber is not absorbed by the fiber and the CPS is not added.Meanwhile,there is no parasitic oscillation at 1μm.It shows that the polarization-maintaining erbium-ytterbium co-doped fiber prepared in this paper has good laser performances.Conclusions In this paper,apolarization-maintaining erbium-ytterbium co-doped fiber for lidar is successfully fabricated by MCVD combined with SDT.The performance of this polarization-maintaining fiber is measured.A birefringence coefficient of 1.29×10^(-4) and a polarization extinction ratio of 24 dB@4 m at 1310 nm are achieved.In addition,apolarization-maintaining all-fiber erbium-ytterbium co-doped fiber laser system is built,and the slope efficiency reaches 36%.Above all,the highest efficiency of the polarization-maintaining erbium-ytterbium co-doped fiber is achieved,which provides the possibility for exact localization of a military lidar.
作者 李文臻 陈阳 廖雷 褚应波 戴能利 李进延 Li Wenzhen;Chen Yang;Liao Lei;Chu Yingbo;Dai Nengli;Li Jinyan(Wuhan National Laboratory for Optoelectronics,Huazhong University of Science and Technology,Wuhan 430074,Hubei,China;Wuhan Changjin Laser Technology Co.,Ltd.,Wuhan 430223,Hubei,China)
出处 《中国激光》 EI CAS CSCD 北大核心 2022年第12期275-280,共6页 Chinese Journal of Lasers
基金 国家自然科学基金(61735007,61975061)。
关键词 光纤光学 光纤激光器 铒镱共掺 激光雷达 保偏光纤 fiber optics fiber lasers erbium-ytterbium co-doping lidar polarization-maintaining fiber
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