Generation of Q-switched mode locking controlled rectangular noise-like soliton bunching in a Tm-doped fiber laser

被引:14
作者
Qiao, Tian [1 ,2 ,3 ]
Chen, Weicheng [1 ,2 ,3 ,4 ]
Lin, Wei [1 ,2 ,3 ]
Yang, Zhongmin [1 ,2 ,3 ]
机构
[1] South China Univ Technol, State Key Lab Luminescent Mat & Devices, Guangzhou 510640, Guangdong, Peoples R China
[2] South China Univ Technol, Guangdong Engn Technol Res & Dev Ctr Special Opt, Guangzhou 510640, Guangdong, Peoples R China
[3] South China Univ Technol, Guangdong Prov Key Lab Fiber Laser Mat & Appl Tec, Guangzhou 510640, Guangdong, Peoples R China
[4] Foshan Univ, Sch Phys & Optoelect Engn, Foshan 528000, Peoples R China
来源
OPTICS EXPRESS | 2016年 / 24卷 / 16期
基金
中国国家自然科学基金;
关键词
SATURABLE ABSORBER; PULSE; OSCILLATOR; OPERATION; 2-MU-M;
D O I
10.1364/OE.24.018755
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We report on an interesting phenomenon of the combination of Q-switched mode locked pulses (QSMLP) and rectangular noise-like pulses (RNLP) as a unit in a Tm-doped ring fiber laser which contains a Fabry-Perot (F-P) subcavity based on the nonlinear polarization evolution (NPE) technique. The RNLP and QSMLP are independently generated in the ring cavity and F-P subcavity, respectively. A notable characteristic is that the physical parameters of RNLP, e.g. repetition rate and pulse duration, are controlled by QSMLP. Thus, they form as a composite bunching, which is termed as "Q-switched mode locking controlled rectangular noise-like soliton bunching (QRNSB)". Further investigation shows that the existence of QRNSB only occurs in high pumping conditions, while both fundamental mode-locking pulses and the coexistence of QSMLP and solitons are achieved in low pumping ones. Our work can enrich the understanding of the nonlinear dynamics in fiber lasers. (C) 2016 Optical Society of America
引用
收藏
页码:18755 / 18763
页数:9
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