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Dive into the research topics where M. H. M. Ahmed is active.

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Featured researches published by M. H. M. Ahmed.


Chinese Physics Letters | 2016

Q-Switched Ytterbium-Doped Fiber Laser Using Black Phosphorus as Saturable Absorber

A. H. H. Al-Masoodi; M. H. M. Ahmed; A. A. Latiff; Hamzah Arof; S. W. Harun

We demonstrate a Q-switched ytterbium-doped fiber laser (YDFL) using a newly developed multi-layer black phosphorous (BP) saturable absorber (SA). The BP SA is prepared by mechanically exfoliating a BP crystal and sticking the acquired BP flakes onto a scotch tape. A small piece of the tape is then placed between two ferrules and incorporated in a YDFL cavity to achieve a stable Q-switched operation in a 1.0μm region. The laser has a pump threshold of 55.1 mW, a pulse repetition rate that is tunable from 8.2 to 32.9 kHz, and the narrowest pulse width of 10.8 μs. The highest pulse energy of 328 nJ is achieved at the pump power of 97.6mW. Our results show that multi-layer BP is a promising SA for Q-switching laser operation.


Laser Physics Letters | 2016

Ultrafast erbium-doped fiber laser mode-locked with a black phosphorus saturable absorber

M. H. M. Ahmed; A. A. Latiff; Hamzah Arof; S. W. Harun

We experimentally demonstrate a passive mode-locked erbium-doped fiber laser (EDFL) using a multi-layer black phosphorus saturable absorber (BPSA). The BPSA is fabricated by mechanically exfoliating a BP crystal and sticking the acquired BP flakes onto scotch tape. A small piece of the tape is then placed between two ferrules and integrated into an EDFL cavity to achieve a self-started soliton mode-locked pulse operation at 1560.7 nm wavelength. The 3 dB bandwidth, pulse width, and repetition rate of the laser are 6.4 nm, 570 fs, and 6.88 MHz, respectively. The average output power is 5.1 mW at pump power of 140 mW and thus, the pulse energy and peak power are estimated at 0.74 nJ and 1.22 kW, respectively. The BPSA was constructed in a simple fabrication process and has a modulation depth of 7% to successfully produce the stable mode-locked fiber laser.


Journal of Modern Optics | 2017

Passively Q-switched erbium-doped fibre laser using cobalt oxide nanocubes as a saturable absorber

A. Nady; M. H. M. Ahmed; Arshid Numan; S. Ramesh; A. A. Latiff; C. H. R. Ooi; Hamzah Arof; S. W. Harun

Abstract We demonstrate a Q-switched Erbium-doped fibre laser (EDFL) utilizing cobalt oxide (Co3O4) nanocubes film based saturable absorber (SA) as a passive Q-switcher. Co3O4 nanocubes are embedded into a polyethylene oxide film to produce a high nonlinear optical response, which is useful for SA application. It has saturation intensity and modulation depth of 3 MW/cm2 and 0.35%, respectively. The proposed laser cavity successfully generates a stable pulse train where the pulse repetition rate is tunable from 29.8 to 70.92 kHz and the pulse-width reduces from 10.9 to 5.02 μs as the 980 nm pump power increases. This result indicates that the Co3O4 is excellent for constructing an SA that can be used in producing a passively Q-switched fibre laser operating at a low pump intensity. To the best of our knowledge, this is the first demonstration of Co3O4 film based fibre laser.


Journal of Modern Optics | 2018

Nickel oxide nanoparticles thin film saturable absorber for 1-micron pulsed all-fibre lasers operation

A. H. H. Al-Masoodi; M. H. M. Ahmed; Anas Abdul Latiff; Hamzah Arof; S. W. Harun

Abstract A passive Q-switched and mode-locked ytterbium-doped fibre laser (YDFL) pulse generation using a nickel oxide thin film as a saturable absorber is reported. The nickel oxide nanoparticle thin film was fabricated by a simple processing technique, and it has a modulation depth of 39% and saturation intensity of 0.04 MW/cm2. The saturable absorber was constructed by inserting a small piece of the film between two fibre ferrules. Then it was integrated in a YDFL cavity. The Q-switching operation started at a threshold pump power of 117.73 mW with an initial wavelength of 1073.5 nm. When the pump power was raised from 117.73 to 133 mW, the repetition rate grew from 9.5 to 15.8 kHz. The pulses had a maximum pulse energy of 478 nJ. Furthermore, a stable self-started mode-locked pulse was also succesfully generated at the threshold pump power of 97.3 mW. The central wavelength and repetition rate of the laser were 1037.72 nm and 23 MHz, respectively. The maximum pulse energy of 0.56 nJ and a peak power of 26.4 W were recorded at a pump power of 137.5 mW.


Fiber and Integrated Optics | 2018

Multi-Wavelength Q-Switched Ytterbium-Doped Fiber Laser with Multi-Walled Carbon Nanotubes

A. H. H. Al-Masoodi; M. H. M. Ahmed; Hamzah Arof; S. W. Harun

ABSTRACT We demonstrate a passively multi-wavelength Q-switched Ytterbium-doped fiber laser (YDFL) based on a multi-wall carbon nanotubes embedded in polyethylene oxide film as saturable absorber. The YDFL generates a stable multi-wavelength with spacing of 1.9 nm as the 980 nm pump power is fixed within 62. 4 mW and 78.0 mW. The repetition rate of the laser is tunable from 10.41 to 29.04 kHz by increasing the pump power from the threshold power of 62.4 mW to 78 mW. At 78 mW pump power, the maximum pulse energy of 38 nJ and the shortest pulse width of 8.87 µs are obtained.


Optical Engineering | 2017

Q-switched ytterbium-doped fiber laser with topological insulator-based saturable absorber

A. H. H. Al-Masoodi; Fauzan Ahmad; M. H. M. Ahmed; Hamzah Arof; S. W. Harun

Abstract. A stable passive Q-switched ytterbium-doped fiber laser (YDFL) operating at 1057.4 and 1044.5 nm is demonstrated using two types of topological insulator-based saturable absorbers (SAs): bismuth (III) selenide (Bi2Se3) and bismuth (III) telluride (Bi2Te3). These materials are embedded in polyvinyl alcohol film and incorporated in the YDFL cavity. Using Bi2Se3 SA, the YDFL obtains a stable train of pulses with a repetition rate that is tunable from 48.83 to 102 kHz. Meanwhile, the corresponding pulse width decreases from 8.9 to 3.48  μs as the pump power increases from 67.6 to 88.3 mW. For the Bi2Te3-based Q-switched YDFL, the repetition rate grows from 43.25 to 93.63 kHz and the pulse width shrinks from 5.65 to 2.01  μs as the 980-nm pump power rises from 72.8 to 98.4 mW. The maximum pulse energy is obtained with the Bi2Te3 SA at 29.95 nJ.


Optics and Laser Technology | 2015

Q-switched erbium doped fiber laser based on single and multiple walled carbon nanotubes embedded in polyethylene oxide film as saturable absorber

M. H. M. Ahmed; N. M. Ali; Z.S. Salleh; A. A. Rahman; S. W. Harun; Mazani Manaf; Hamzah Arof


Laser Physics | 2017

Nickel oxide nanoparticles as a saturable absorber for an all-fiber passively Q-switched erbium-doped fiber laser

A Nady; M. H. M. Ahmed; A. A. Latiff; A Numan; C. H. Raymond Ooi; S. W. Harun


Optics and Laser Technology | 2016

Femtosecond mode-locked erbium-doped fiber laser based on MoS2–PVA saturable absorber

M. H. M. Ahmed; A. A. Latiff; Hamzah Arof; H. Ahmad; S. W. Harun


Optik | 2015

Passively Q-switched fiber lasers using a multi-walled carbon nanotube polymer composite based saturable absorber

S.M. Azooz; M. H. M. Ahmed; Fauzan Ahmad; Belal Ahmed Hamida; Sheroz Khan; H. Ahmad; S. W. Harun

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H. Ahmad

University of Malaya

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Anas Abdul Latiff

Universiti Teknikal Malaysia Melaka

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Fauzan Ahmad

Universiti Teknologi Malaysia

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M. Yasin

Airlangga University

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