C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber
We demonstrate a passively Q-switched erbium fiber laser using titanium dioxide (TiO2) as a saturable absorber. The TiO<sub>2</sub> saturable absorber was fabricated as a polymer composite film and sandwiched between fiber ferrules. Q-switched pulsing starts with the assistance of physic...
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doaj-5fac86c0148a4c489d3b6fd4857ea1ec2021-03-29T17:29:31ZengIEEEIEEE Photonics Journal1943-06552016-01-01811710.1109/JPHOT.2015.25061697348649C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable AbsorberH. Ahmad0Siti Aisyah Reduan1Zainal Abidin Ali2M. A. Ismail3N. E. Ruslan4C. S. J. Lee5R. Puteh6S. W. Harun7Photonics Research Centre, University of Malaya, Kuala Lumpur, MalaysiaPhotonics Research Centre, University of Malaya, Kuala Lumpur, MalaysiaDepartment of Physics, Faculty of Science, University of Malaya, Kuala Lumpur, MalaysiaPhotonics Research Centre, University of Malaya, Kuala Lumpur, MalaysiaPhotonics Research Centre, University of Malaya, Kuala Lumpur, MalaysiaPhotonics Research Centre, University of Malaya, Kuala Lumpur, MalaysiaDepartment of Physics, Faculty of Science, University of Malaya, Kuala Lumpur, MalaysiaDepartment of Electrical Engineering, Faculty of Engineering, University of Malaya, Kuala Lumpur, MalaysiaWe demonstrate a passively Q-switched erbium fiber laser using titanium dioxide (TiO2) as a saturable absorber. The TiO<sub>2</sub> saturable absorber was fabricated as a polymer composite film and sandwiched between fiber ferrules. Q-switched pulsing starts with the assistance of physical disturbance of the laser cavity (by lightly tapping the cavity to induce instability) at 140 mW and lasts until 240 mW. The repetition rate increases with the pump power from 80.28 to 120.48 kHz. On the other hand, the pulsewidth decreases from 2.054 μs until it reaches a plateau at 1.84 μs. The Q-switched fiber laser exhibits two competing modes: at 1558.1 and 1558.9 nm as the pump power increases. A high signal-tonoise ratio of 49.65 dB is obtained.https://ieeexplore.ieee.org/document/7348649/Q-switchedTiO <sub xmlns:ali="http://www.niso.org/schemas/ali/1.0/" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">2</sub> |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
H. Ahmad Siti Aisyah Reduan Zainal Abidin Ali M. A. Ismail N. E. Ruslan C. S. J. Lee R. Puteh S. W. Harun |
spellingShingle |
H. Ahmad Siti Aisyah Reduan Zainal Abidin Ali M. A. Ismail N. E. Ruslan C. S. J. Lee R. Puteh S. W. Harun C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber IEEE Photonics Journal Q-switched TiO <sub xmlns:ali="http://www.niso.org/schemas/ali/1.0/" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">2</sub> |
author_facet |
H. Ahmad Siti Aisyah Reduan Zainal Abidin Ali M. A. Ismail N. E. Ruslan C. S. J. Lee R. Puteh S. W. Harun |
author_sort |
H. Ahmad |
title |
C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber |
title_short |
C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber |
title_full |
C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber |
title_fullStr |
C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber |
title_full_unstemmed |
C-Band Q-Switched Fiber Laser Using Titanium Dioxide (TiO 2) As Saturable Absorber |
title_sort |
c-band q-switched fiber laser using titanium dioxide (tio 2) as saturable absorber |
publisher |
IEEE |
series |
IEEE Photonics Journal |
issn |
1943-0655 |
publishDate |
2016-01-01 |
description |
We demonstrate a passively Q-switched erbium fiber laser using titanium dioxide (TiO2) as a saturable absorber. The TiO<sub>2</sub> saturable absorber was fabricated as a polymer composite film and sandwiched between fiber ferrules. Q-switched pulsing starts with the assistance of physical disturbance of the laser cavity (by lightly tapping the cavity to induce instability) at 140 mW and lasts until 240 mW. The repetition rate increases with the pump power from 80.28 to 120.48 kHz. On the other hand, the pulsewidth decreases from 2.054 μs until it reaches a plateau at 1.84 μs. The Q-switched fiber laser exhibits two competing modes: at 1558.1 and 1558.9 nm as the pump power increases. A high signal-tonoise ratio of 49.65 dB is obtained. |
topic |
Q-switched TiO <sub xmlns:ali="http://www.niso.org/schemas/ali/1.0/" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">2</sub> |
url |
https://ieeexplore.ieee.org/document/7348649/ |
work_keys_str_mv |
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