Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber

Author:

Haris Hazlihan1ORCID,Jin Tan Sin23,Batumalay Malathy4ORCID,Muhammad Ahmad Razif5ORCID,Sampe Jahariah5ORCID,Markom Arni Munira6,Zain Huda Adnan7,Harun Sulaiman Wadi7ORCID,Hasnan Megat Muhammad Ikhsan Megat1ORCID,Saad Ismail1

Affiliation:

1. Faculty of Engineering, Universiti Malaysia Sabah (UMS), Kota Kinabalu 88400, Sabah, Malaysia

2. School of Engineering, KDU University College, UOW Malaysia, Shah Alam 40150, Selangor, Malaysia

3. KDU University College, UOW Malaysia, George Town 10400, Pulau Pinang, Malaysia

4. Faculty of Data Science & IT, INTI International University, Nilai 71800, Negeri Sembilan, Malaysia

5. Institute of Microengineering and Nanoelectronics (IMEN), Universiti Kebangsaan Malaysia (UKM), Bangi 43600, Selangor, Malaysia

6. School of Electrical Engineering, College of Engineering, Universiti Teknologi MARA, Shah Alam 40450, Selangor, Malaysia

7. Department of Electrical Engineering, Faculty of Engineering, University of Malaya, Kuala Lumpur 50603, Malaysia

Abstract

In this work, we present the generation of two distinct types of soliton pulses using a Bismuth Selenide (Bi2Se3) saturable absorber (SA) synthesized in our laboratory. The soliton pulses were generated in two different laser cavity configurations, resulting in two types of solitons: a soliton pulse with Kelly sidebands and a bunched soliton pulse with peak-dip sidebands. Both solitons operated at the fundamental repetition rate—23.3 MHz (for the soliton with Kelly sidebands) and 13 MHz (for the bunched soliton with peak-dip sidebands). We observed that the accumulation of nonlinear phase shift from the added single mode fiber (SMF) split the single soliton pulse into 44 pulses in a bunched oscillation envelope. At the same time, peak-dip sidebands were imposed on the bunched soliton spectrum due to constructive and destructive interferences between soliton pulse and dispersive waves. The measured pulse width for both solitons were 0.63 ps (for the soliton with Kelly sidebands) and 1.52 ps (for the bunched soliton with peak-dip sidebands), respectively. Our results demonstrate the potential of Bi2Se3 SAs in generating different types of soliton pulses, which could have potential applications in various areas of optical communication and spectroscopy.

Funder

Ministry of Higher Education Malaysia (MOHE) under the Fundamental Research Grant Scheme

Publisher

MDPI AG

Subject

General Materials Science,General Chemical Engineering

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