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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...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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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. |
format | Online Article Text |
id | pubmed-10180442 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
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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