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

In this work, we present the generation of two distinct types of soliton pulses using a Bismuth Selenide (Bi(2)Se(3)) 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 p...

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Autores principales: Haris, Hazlihan, Jin, Tan Sin, Batumalay, Malathy, Muhammad, Ahmad Razif, Sampe, Jahariah, Markom, Arni Munira, Zain, Huda Adnan, Harun, Sulaiman Wadi, Hasnan, Megat Muhammad Ikhsan Megat, Saad, Ismail
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10180442/
https://www.ncbi.nlm.nih.gov/pubmed/37177083
http://dx.doi.org/10.3390/nano13091538
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author Haris, Hazlihan
Jin, Tan Sin
Batumalay, Malathy
Muhammad, Ahmad Razif
Sampe, Jahariah
Markom, Arni Munira
Zain, Huda Adnan
Harun, Sulaiman Wadi
Hasnan, Megat Muhammad Ikhsan Megat
Saad, Ismail
author_facet Haris, Hazlihan
Jin, Tan Sin
Batumalay, Malathy
Muhammad, Ahmad Razif
Sampe, Jahariah
Markom, Arni Munira
Zain, Huda Adnan
Harun, Sulaiman Wadi
Hasnan, Megat Muhammad Ikhsan Megat
Saad, Ismail
author_sort Haris, Hazlihan
collection PubMed
description In this work, we present the generation of two distinct types of soliton pulses using a Bismuth Selenide (Bi(2)Se(3)) 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 Bi(2)Se(3) SAs in generating different types of soliton pulses, which could have potential applications in various areas of optical communication and spectroscopy.
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spelling pubmed-101804422023-05-13 Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber Haris, Hazlihan Jin, Tan Sin Batumalay, Malathy Muhammad, Ahmad Razif Sampe, Jahariah Markom, Arni Munira Zain, Huda Adnan Harun, Sulaiman Wadi Hasnan, Megat Muhammad Ikhsan Megat Saad, Ismail Nanomaterials (Basel) Communication In this work, we present the generation of two distinct types of soliton pulses using a Bismuth Selenide (Bi(2)Se(3)) 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 Bi(2)Se(3) SAs in generating different types of soliton pulses, which could have potential applications in various areas of optical communication and spectroscopy. MDPI 2023-05-03 /pmc/articles/PMC10180442/ /pubmed/37177083 http://dx.doi.org/10.3390/nano13091538 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Communication
Haris, Hazlihan
Jin, Tan Sin
Batumalay, Malathy
Muhammad, Ahmad Razif
Sampe, Jahariah
Markom, Arni Munira
Zain, Huda Adnan
Harun, Sulaiman Wadi
Hasnan, Megat Muhammad Ikhsan Megat
Saad, Ismail
Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title_full Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title_fullStr Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title_full_unstemmed Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title_short Single and Bunch Soliton Generation in Optical Fiber Lasers Using Bismuth Selenide Topological Insulator Saturable Absorber
title_sort single and bunch soliton generation in optical fiber lasers using bismuth selenide topological insulator saturable absorber
topic Communication
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10180442/
https://www.ncbi.nlm.nih.gov/pubmed/37177083
http://dx.doi.org/10.3390/nano13091538
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