Generation of Square Pulses at Both Anomalous and Normal Dispersion Regimes in Passively Mode-Locked Erbium-Doped Fiber Laser

被引：0
|
作者：
Xu Z. [1 ]
Jia D. [1 ]
Li Z. [1 ]
Sun X. [1 ]
Ge C. [1 ]
Wang Z. [1 ]
Yang T. [1 ]
Cao X. [2 ]
机构：
[1] Key Laboratory of Fiber Optics and Optical Communication, School of Precision Instrument and Optoelectronics Engineering, Tianjin University, Tianjin
[2] Tianjin Optical Electrical Group Co., Ltd., Tianjin
来源：
Jia, Dongfang (jiadf@tju.edu.cn) | 1600年 / Science Press卷 / 47期
关键词：
Dispersion management; Dissipative soliton resonance; Fiber lasers; Lasers; Nonlinear optical loop mirror; Square pulses;
D O I：
10.3788/CJL202047.1201006
中图分类号：
学科分类号：
摘要：
The passive mode-locked erbium-doped fiber laser based on nonlinear optical loop mirror operating in the dissipative soliton resonance (DSR) region is reported. Square wave pulse output is obtained in the abnormal and normal dispersion regimes respectively. At anomalous dispersion regime, the net cavity dispersion is calculated to be -0.32 ps2. Stable square pluses with maximum temporal pulse duration of 33 ns are obtained when the pump power is adjusted to 481.2 mW. Correspondingly, the single pulse energy is 12.4 nJ. Subsequently, a 7 m long dispersion compensating fiber is employed to compensate the cavity dispersion to make the laser system work at the normal dispersion regime and the net cavity dispersion is 2.85 ps2. Under the same pump power, the maximum temporal duration of the square pulses is 34.3 ns and the single pulse energy is 9.42 nJ. It is shown that DSR square pulses can be generated at both anomalous and normal dispersion regimes under the conditions of balanced cavity parameters. Additionally, the influence of the pump power on the time domain width and single pulse energy of square wave pulse is also studied. The results show that the time domain width and single pulse energy of square wave pulse change linearly with the increase of pump power. © 2020, Chinese Lasers Press. All right reserved.
引用
收藏
相关论文
共 29 条
  • [1] Kramer P, Estraillier P, Rouyer C., Megajoule optical pulse generation system, Proceedings of SPIE, 3047, pp. 587-591, (1997)
  • [2] Skeldon M D, Bui S T, Letzring S A, Et al., Implementation of pulse shaping on the OMEGA laser system, Proceedings of SPIE, 1627, pp. 246-251, (1992)
  • [3] Ngo N Q, Binh L N., New approach for the design of an optical square pulse generator, Applied Optics, 46, 17, pp. 3546-3560, (2007)
  • [4] Wen R H, Hu C Z, Wei K H, Et al., All-PM "figure-of-eight" cavity mode-locked fiber laser and its power amplification, Acta Photonica Sinica, 46, 5, (2017)
  • [5] Mei X S, Yang Z X, Zhao W Q., Laser hole drilling on surface of electronic ceramic substrates, Chinese Journal of Lasers, 47, 5, (2020)
  • [6] Xie G C, Ye Y D, Li J M, Et al., Echo characteristics and range error for pulse laser ranging, Chinese Journal of Lasers, 45, 6, (2018)
  • [7] Peng X, Jordens B, Hooper A, Et al., Generation of programmable temporal pulse shape and applications in micromachining, Proceedings of SPIE, 7193, (2009)
  • [8] Liu C, Mao X L, Mao S S, Et al., Nanosecond and femtosecond laser ablation of brass: particulate and ICPMS measurements, Analytical Chemistry, 76, 2, pp. 379-383, (2004)
  • [9] Chang W, Ankiewicz A, Soto-Crespo J M, Et al., Dissipative soliton resonances in laser models with parameter management, Journal of the Optical Society of America B, 25, 12, pp. 1972-1977, (2008)
  • [10] Chang W, Ankiewicz A, Soto-Crespo J M, Et al., Dissipative soliton resonances, Physical Review A, 78, 2, (2008)
123