Single-longitudinal Mode Thulium-doped Fiber Laser Based on Fabry-Pérot Fiber Bragg Grating Filter and Passive Compound Double-rings Cavity

被引:0
|
作者
Han W.-G. [1 ]
Yan F.-P. [1 ]
Feng T. [2 ]
Cheng D. [1 ]
Li T. [1 ]
Bai Z.-Y. [1 ]
Qin Q. [1 ]
Yang D.-D. [1 ]
Zhang L.-N. [3 ]
Guo Y. [1 ]
Wang W. [1 ]
Guan B. [1 ]
Zhang X. [1 ]
机构
[1] Key Laboratory of All Optical Network and Advanced Telecommunication Network, Ministry of Education, Institute of Lightwave Technology, Beijing Jiaotong University, Beijing
[2] Photonics Information Innovation Center, College of Physics Science & Technology, Hebei University, Baoding
[3] Key Laboratory of Solid Laser Technology, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing
来源
基金
中国国家自然科学基金;
关键词
Fiber Bragg grating; Fiber laser; Single longitudinal mode; Thulium-doped fiber;
D O I
10.37188/CJL.20210215
中图分类号
学科分类号
摘要
A single-longitudinal-mode(SLM) thulium-doped fiber laser based on an F-P narrowband filter and compound rings cavity is proposed. The compound rings incorporated in the cavity can help to achieve SLM lasing by adjusting the cavity FSR and it also plays the role of narrowband filtering. A theoretical model which can numerically calculate the transmission spectrum of the complex multi-ring sub-cavity filter is proposed. The output wavelength of the laser source is 1 941.56 nm, and the optical signal-to-noise ratio is 55.8 dB. The wavelength and power fluctuations within 70 min were less than 0.019 nm and 1.464 dB, respectively. Experimental results also show that the laser operates in a stable SLM state. The frequency noise characteristic of the proposed SLM laser was measured by a homemade unbalanced Michelson interferometer, and laser linewidth under different measurement time was estimated from the frequency noise spectra based on the β-separation line method. The calculated laser linewidth in 2 ms measurement time is 14.194 kHz. © 2021, Science Press. All right reserved.
引用
收藏
页码:1419 / 1426
页数:7
相关论文
共 24 条
  • [1] LIU B, JIA C L, ZHANG H, Et al., DBR-fiber-laser-based active temperature sensor and its applications in the measurement of fiber birefringence [J], Microw. Opt. Technol. Lett, 52, 1, pp. 41-44, (2010)
  • [2] XIONG L Y, HOFMANN P, SCHULZGEN A, Et al., Short monolithic dual-wavelength single-longitudinal-mode DBR phosphate fiber laser [J], Appl. Opt, 53, 18, pp. 3848-3853, (2014)
  • [3] MATSUOKA T, YOSHIKUNI Y, MOTOSUGI G., Dependence of single-longitudinal-mode probability on DFB laser facet structure [J], Electron. Lett, 21, 24, pp. 1151-1152, (1985)
  • [4] CHEN X F, YAO J P, ZENG F, Et al., Single-longitudinal-mode fiber ring laser employing an equivalent phase-shifted fiber Bragg grating [J], IEEE Photon. Technol. Lett, 17, 7, pp. 1390-1392, (2005)
  • [5] RODRIGUEZ-COBO L, QUINTELA M A, ROTA-RODRIGO S, Et al., Single-longitudinal mode laser structure based on a very narrow filtering technique [J], Opt. Express, 21, 8, pp. 10289-10294, (2013)
  • [6] PASCHOTTA R, NILSSON J, REEKIE L, Et al., Single-frequency ytterbium-doped fiber laser stabilized by spatial hole burning [J], Opt. Lett, 22, 1, pp. 40-42, (1997)
  • [7] WANG Z K, SHANG J M, MU K L, Et al., Stable single-longitudinal-mode fiber laser with ultra-narrow linewidth based on convex-shaped fiber ring and sagnac loop [J], IEEE Access, 7, pp. 166398-166403, (2019)
  • [8] FENG S J, MAO Q H, TIAN Y Y, Et al., Widely tunable single longitudinal mode fiber laser with cascaded fiber-ring secondary cavity [J], IEEE Photon. Technol. Lett, 25, 4, pp. 323-326, (2013)
  • [9] GENG J H, WANG Q, JIANG S B., 2 μm fiber laser sources and their applications [C], Proceedings of the SPIE 8164, Nanophotonics and Macrophotonics for Space Environments V, (2011)
  • [10] MENG J, ZHANG W, ZHAO K Q, Et al., Investigation on the performance of a homemade thulium-doped fiber laser oscillator [J], Chin. Opt, 12, 5, pp. 1109-1117, (2019)