Ahmad Razif Muhammad

Dr. Ahmad Razif Muhammad

orcid

Research Focus & Metrics

Academic Career Length

13Years (2014-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 July 2020 in Optics & Laser Technology
Verified
Journal Article
Closed access
AJA.A.A. Jafry
A.A.A. Jafry
NKN. Kasim
N. Kasim
MRM.F.M. Rusdi
M.F.M. Rusdi
ARA.H.A. Rosol
A.H.A. Rosol
RYR.A.M. Yusoff
R.A.M. Yusoff
SHS.W. Harun
S.W. Harun

1 February 2017 in Optics & Laser Technology
Verified
Journal Article
Closed access
HHH. Haris
H. Haris
SHS.W. Harun
S.W. Harun
AMAhmad Razif Muhammad
Ahmad Razif Muhammad
CAC.L. Anyi
C.L. Anyi
TJtan sin jin
tan sin jin
HAH. Arof
H. Arof

1 March 2019 in Optical Fiber Technology
Verified
Journal Article
Closed access
HHH. Haris
H. Haris
HAH. Arof
H. Arof
AMAhmad Razif Muhammad
Ahmad Razif Muhammad
CAC.L. Anyi
C.L. Anyi
TJtan sin jin
tan sin jin
SHS.W. Harun
S.W. Harun

1 April 2022 in Crystals
Verified
Journal Article
Open access
PDF file
HHHazlihan Haris
Hazlihan Haris
MBMalathy Batumalay
Malathy Batumalay
TJtan sin jin
tan sin jin
AMArni Munira Markom
Arni Munira Markom
AMAhmad Razif Muhammad
Ahmad Razif Muhammad
ISI. Saad
I. Saad
Fiber lasers have long remained relevant for various applications worldwide in many industries. This paper presents a mode-locked ytterbium-doped fiber laser (YDFL) using our home-made topological insulator Bi2Se3 nanosheets (TI Bi2Se3) as the saturable absorber. The fabricated TI Bi2Se3 is transported to the end of the fiber ferrule using an optical deposition process, which is a key ingredient for initiating a pulsed fiber laser. With a pump power of 211.1 mW, the captured repetition rate and pulse width are 8.3 MHz and 6.2 ns, respectively. The length of the setup configuration is approximately 20 m, which corresponds to an output power measurement of 12.4 mW with a calculated pulse energy of 1.5 nJ. There are no significant Kelly sidebands, but the strong stability of the pulsed laser is defined by a high signal-to-noise ratio (SNR) of around 60.35 dB.

1 December 2020 in Optik
Verified
Journal Article
Closed access
AJAfiq Arif Aminuddin Jafry
Afiq Arif Aminuddin Jafry
NKNabilah Kasim
Nabilah Kasim
BNBilal Nizamani
Bilal Nizamani
AMAhmad Razif Muhammad
Ahmad Razif Muhammad
RYRabi’aTul Adawiyah Mat Yusoff
Rabi’aTul Adawiyah Mat Yusoff
PYPreecha Yupapin
Preecha Yupapin

1 March 2017 in Chinese Physics Letters
Verified
Journal Article
Closed access
PDF file
AMAhmad Razif Muhammad
Ahmad Razif Muhammad
MAM. T. Ahmad
M. T. Ahmad
RZR. Zakaria
R. Zakaria
HRH. R. A. Rahim
H. R. A. Rahim
SYS. F. A. Z. Yusoff
S. F. A. Z. Yusoff
S. W. HarunS. W. Harun
S. W. Harun
We demonstrate a passively Q-switched erbium-doped fiber laser (EDFL) using a copper nanoparticle (CuNP) thin film as the saturable absorber in a ring cavity. A stable Q-switched pulse operation is observed as the CuNP saturable absorber (SA) is introduced in the cavity. The pulse repetition rate of the EDFL is observed to be proportional to the pump power, and is limited to 101.2 kHz by the maximum pump power of 113.7 mW. On the other hand, the pulse width reduces from 10.19 μs to 4.28 μs as the pump power is varied from 26.1 mW to 113.7 mW. The findings suggest that CuNP SA could be useful as a potential saturable absorber for the development of the robust, compact, efficient and low cost Q-switched fiber laser operating at 1.5- μm region.