Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber

Conventional Kelly sidebands soliton and dip-type sidebands soliton were observed with the employment of Bi2Te3 as saturable absorber (SA) in Erbium-Doped Fiber Laser (EDFL). The fabricated Bi2Te3 possessed the following characteristics: I-sat 102 MW/cm(2), modulation depth 41.4%, and non-saturable...

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Main Authors: Haris, H., Muhammad, A. R., Tan, S. J., Markom, A. M., Harun, Sulaiman Wadi, Hasnan, M. M. I. Megat, Saad, I
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Published: Elsevier 2022
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Online Access:http://eprints.um.edu.my/42903/
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spelling my.um.eprints.429032023-09-18T04:27:42Z http://eprints.um.edu.my/42903/ Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber Haris, H. Muhammad, A. R. Tan, S. J. Markom, A. M. Harun, Sulaiman Wadi Hasnan, M. M. I. Megat Saad, I TK Electrical engineering. Electronics Nuclear engineering Conventional Kelly sidebands soliton and dip-type sidebands soliton were observed with the employment of Bi2Te3 as saturable absorber (SA) in Erbium-Doped Fiber Laser (EDFL). The fabricated Bi2Te3 possessed the following characteristics: I-sat 102 MW/cm(2), modulation depth 41.4%, and non-saturable absorption at 10%. The Bi(2)Te3 solution was transferred to the end of the fiber ferrule by the optical deposition method. Conventional Kelly sidebands soliton was obtained with a fundamental repetition rate and pulse width of 24 MHz and 0.78 ps, respectively. The existing cavity length was extended and with the appropriate tuning of light polarization, dip peak intensity soliton sidebands with bunched pulses were observed. The oscillation trace revealed the repetition rate of dip-peak intensity sidebands soliton was ascertained at 13.5 MHz, which was in accordance with the cavity length. There was a total of 144 pulses in a single bunch envelope under the maximum available pump power. With the appropriate tuning of light polarization, constructive and destructive interference between soliton and dispersive waves took place in EDFL resulting in the formation of peak intensity (Kelly sidebands) and dip-peak intensity on the soliton spectrum. To the best of the author's knowledge, this is the first demonstration of dip-peak intensity sidebands soliton using Bi2Te3. Elsevier 2022-06 Article PeerReviewed Haris, H. and Muhammad, A. R. and Tan, S. J. and Markom, A. M. and Harun, Sulaiman Wadi and Hasnan, M. M. I. Megat and Saad, I (2022) Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber. Infrared Physics & Technology, 123. ISSN 1350-4495, DOI https://doi.org/10.1016/j.infrared.2022.104154 <https://doi.org/10.1016/j.infrared.2022.104154>. 10.1016/j.infrared.2022.104154
institution Universiti Malaya
building UM Library
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Malaya
content_source UM Research Repository
url_provider http://eprints.um.edu.my/
topic TK Electrical engineering. Electronics Nuclear engineering
spellingShingle TK Electrical engineering. Electronics Nuclear engineering
Haris, H.
Muhammad, A. R.
Tan, S. J.
Markom, A. M.
Harun, Sulaiman Wadi
Hasnan, M. M. I. Megat
Saad, I
Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
description Conventional Kelly sidebands soliton and dip-type sidebands soliton were observed with the employment of Bi2Te3 as saturable absorber (SA) in Erbium-Doped Fiber Laser (EDFL). The fabricated Bi2Te3 possessed the following characteristics: I-sat 102 MW/cm(2), modulation depth 41.4%, and non-saturable absorption at 10%. The Bi(2)Te3 solution was transferred to the end of the fiber ferrule by the optical deposition method. Conventional Kelly sidebands soliton was obtained with a fundamental repetition rate and pulse width of 24 MHz and 0.78 ps, respectively. The existing cavity length was extended and with the appropriate tuning of light polarization, dip peak intensity soliton sidebands with bunched pulses were observed. The oscillation trace revealed the repetition rate of dip-peak intensity sidebands soliton was ascertained at 13.5 MHz, which was in accordance with the cavity length. There was a total of 144 pulses in a single bunch envelope under the maximum available pump power. With the appropriate tuning of light polarization, constructive and destructive interference between soliton and dispersive waves took place in EDFL resulting in the formation of peak intensity (Kelly sidebands) and dip-peak intensity on the soliton spectrum. To the best of the author's knowledge, this is the first demonstration of dip-peak intensity sidebands soliton using Bi2Te3.
format Article
author Haris, H.
Muhammad, A. R.
Tan, S. J.
Markom, A. M.
Harun, Sulaiman Wadi
Hasnan, M. M. I. Megat
Saad, I
author_facet Haris, H.
Muhammad, A. R.
Tan, S. J.
Markom, A. M.
Harun, Sulaiman Wadi
Hasnan, M. M. I. Megat
Saad, I
author_sort Haris, H.
title Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
title_short Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
title_full Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
title_fullStr Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
title_full_unstemmed Generation of Kelly and dip type sidebands soliton employing Topological insulator (Bi2Te3) as saturable absorber
title_sort generation of kelly and dip type sidebands soliton employing topological insulator (bi2te3) as saturable absorber
publisher Elsevier
publishDate 2022
url http://eprints.um.edu.my/42903/
_version_ 1778161680061038592