Cavity-birefringence-dependent h-shaped pulse generation in a thulium-holmium-doped fiber laser

Significance 

Generation of pulses is an essential aspect of fiber lasers. Pulses are considered to have different profiles and parameters such as fiber gain, nonlinearity, and dispersion. Proper management of such resonant parameters can effectively realize the various pulse profiles and shaping.  Recently, researchers have taken advantage of the advanced technology to explore and uncover different types of pulses. As a result, several particular pulses have been reported up to date. Additionally, some of the laser pulse generation has been performed using 2D-based material devices.

A group of researchers at Jiangsu Normal University, School of Physics and Electronic Engineering in China: Dr Junqing Zhao, Dr Lei Li, Professor Luming Zhao, Professor Dingyuan Tang and Professor Deyuan Shen investigated and unfolded a new laser pulse profile generation technique. The h-shaped pulse was generated in a laser containing thulium-holmium-doped fiber (THF). One most striking point in their contribution is that all desired pulse duty circles (PDCs) could be achieved by managing the cavity birefringence. They also focused on studying the factors that affect its generation such as pump power requirements and its cavity birefringence. This fascinating research work has been published in the journal, Optics Letters.

In their experiments, the research team used an asymmetric nonlinear optical loop mirror (NOLM) for generating the pulses in the THF laser and a wavelength division multiplexer (WDM) to feed the THF with the required pump light. A long piece of high nonlinear fiber (HNLF) was incorporated in the NOLM to enhance the cavity nonlinearity and enhance the peak-power-clamping effect. The light was then reflected and transmitted as a signal. A fiber polarization controller and a fiber optical coupler were employed for the purpose of determining the state of polarization of the light signals transmitted and extracting the output light respectively. Furthermore, the challenge of changing the numbers of cavity birefringence was solved by using polarization maintain fiber (PMF) at varying lengths.

Pump-power tuning indicated that PPC effect could only occur on the flat trailing portion of each achieved h-shaped pulse, whereas the peak power of the leading edge was determined by the launched pump power. Polarization state (PS) switching also resulted in the change of clamped peak power, proving that PPC effect is PS-dependent.

During the study, the authors observed and reported for the first time the highest ever pulse duty cycle (PDC) value for a fiber laser. For instance, the value was approximately 98.2% for a PMF length of 2.3m and pulse duration of only 318.14 ns. Through observation of the formed pulse profiles, the authors confirmed the significance of linear cavity birefringence as a tool for pulse tuning.

As an important finding of this study, the research presented a method of generating h-pulses in a THF laser. For the pulses to be generated more effectively, various parameters were to be taken into consideration. For example, the nonlinearity of the NOLM was improved by using it as an artificial saturable absorber at a much higher aperture. Although the generated h-pulses portrayed some similarities when compared to other pulses uncovered before, it had its unique properties which acted as a distinguishing factor. The difference could be spotted in their various spectral profiles, trailing edge and leading portion. For example, unlike h-pulses, a chair-like pulse possesses a massive trailing edge and more extended leading portion. For the case of the power requirement, it was observed that the longer the PMF length, the more power required for the system.

According to the authors, proper management of the cavity birefringence is the secret of achieving better pulse tuning. It is possible to change birefringence cavity settings by adjusting fiber polarization controller. Varying PMF lengths result in different linear birefringence amount thus further determining the leading portion and trailing edge intensities.

Cavity-birefringence-dependent h-shaped pulse generation in a thulium-holmium-doped fiber laser. Advances in Engineering

About the author

Junqing Zhao received a doctorate in Optical Engineering from Shenzhen University, China, in 2014, for research on pulsed fiber lasers. Since then, he has worked on high power fiber lasers and amplifiers, nonlinear beam generation from fiber systems or based on fiber sources, and particular fiber devices, first at the Shenzhen Key Laboratory of Laser Engineering, Shenzhen University, China, and later at the Optoelectronics Research Centre (ORC), University of Southampton, UK. He is now working at the Jiangsu Key Laboratory of Advanced Laser Materials and Devices, School of Physics and Electronic Engineering, Jiangsu Normal University. He has published some 40 scientific articles.

 

About the author

Luming Zhao received the B.S. and the M.S. degrees in engineering physics from Tsinghua University, Beijing, China, in 1999 and 2002, respectively. He acquired his Ph.D. degree in electrical and electronic engineering from Nanyang Technological University, Singapore, in 2007. Currently, Zhao serves as a Full Professor at the School of Physics and Electronic Engineering, Jiangsu Normal University, China.

His current research interests include soliton dynamics, laser physics and engineering, nonlinear optics and dynamics, ultrafast optics, and optics communications. He has published over 100 journal papers with a citation of more than 5000 times and H-index of 36. Dr. Zhao is an IEEE Senior Member, an OSA member, a SPIE member.

Reference

Junqing Zhao, Lei Li, Luming Zhao, Dingyuan Tang, and Deyuan Shen. Cavity-birefringence-dependent h-shaped pulse generation in a thulium-holmium-doped fiber laser. Optics Letters, Vol. 43, Issue 2, pp. 247-250 (2018)

 

Go To Optics Letters

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