Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime
The Q-switched pulse regime is demonstrated by integrating conductive graphene as passive saturable absorber producing relatively high instantaneous peak power and pulse energy. The fabricated conductive graphene is investigated using Raman spectroscopy. The single wavelength Q-switching operates at...
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doaj-3e8669186ab94a7eb8e911ef645698922020-11-24T21:12:03ZengElsevierResults in Physics2211-37972018-06-019371375Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regimeSiti Nur Fatin Zuikafly0Ali Khalifa1Fauzan Ahmad2Suhaidi Shafie3SulaimanWadi Harun4Malaysia-Japan Institute of Technology, Universiti Teknologi Malaysia, 54100 Kuala Lumpur, MalaysiaInstitute of Advanced Technology and Department of Electrical and Electronic Engineering, Faculty of Engineering, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, MalaysiaMalaysia-Japan Institute of Technology, Universiti Teknologi Malaysia, 54100 Kuala Lumpur, MalaysiaInstitute of Advanced Technology and Department of Electrical and Electronic Engineering, Faculty of Engineering, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia; Corresponding author.Department of Electrical Engineering, Faculty of Engineering, University of Malaya, 50603 Kuala Lumpur, MalaysiaThe Q-switched pulse regime is demonstrated by integrating conductive graphene as passive saturable absorber producing relatively high instantaneous peak power and pulse energy. The fabricated conductive graphene is investigated using Raman spectroscopy. The single wavelength Q-switching operates at 1558.28 nm at maximum input pump power of 151.47 mW. As the pump power is increased from threshold power of 51.6 mW to 151.47 mW, the pulse train repetition rate increases proportionally from 47.94 kHz to 67.8 kHz while the pulse width is reduced from 9.58 μs to 6.02 μs. The generated stable pulse produced maximum peak power and pulse energy of 32 mW and 206 nJ, respectively. The first beat node of the measured signal-to-noise ratio is about 62 dB indicating high pulse stability.http://www.sciencedirect.com/science/article/pii/S2211379717324713 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Siti Nur Fatin Zuikafly Ali Khalifa Fauzan Ahmad Suhaidi Shafie SulaimanWadi Harun |
spellingShingle |
Siti Nur Fatin Zuikafly Ali Khalifa Fauzan Ahmad Suhaidi Shafie SulaimanWadi Harun Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime Results in Physics |
author_facet |
Siti Nur Fatin Zuikafly Ali Khalifa Fauzan Ahmad Suhaidi Shafie SulaimanWadi Harun |
author_sort |
Siti Nur Fatin Zuikafly |
title |
Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime |
title_short |
Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime |
title_full |
Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime |
title_fullStr |
Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime |
title_full_unstemmed |
Conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in Q-switched regime |
title_sort |
conductive graphene as passive saturable absorber with high instantaneous peak power and pulse energy in q-switched regime |
publisher |
Elsevier |
series |
Results in Physics |
issn |
2211-3797 |
publishDate |
2018-06-01 |
description |
The Q-switched pulse regime is demonstrated by integrating conductive graphene as passive saturable absorber producing relatively high instantaneous peak power and pulse energy. The fabricated conductive graphene is investigated using Raman spectroscopy. The single wavelength Q-switching operates at 1558.28 nm at maximum input pump power of 151.47 mW. As the pump power is increased from threshold power of 51.6 mW to 151.47 mW, the pulse train repetition rate increases proportionally from 47.94 kHz to 67.8 kHz while the pulse width is reduced from 9.58 μs to 6.02 μs. The generated stable pulse produced maximum peak power and pulse energy of 32 mW and 206 nJ, respectively. The first beat node of the measured signal-to-noise ratio is about 62 dB indicating high pulse stability. |
url |
http://www.sciencedirect.com/science/article/pii/S2211379717324713 |
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