M. R. Dousti
Universiti Teknologi Malaysia
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Featured researches published by M. R. Dousti.
Optics Express | 2013
Raja J. Amjad; Md. Rahim Sahar; M. R. Dousti; Sib Krishna Ghoshal; M. N. A. Jamaludin
We report significant enhancements in Er(3+) luminescence as well as in Raman intensity in silver nanoparticles embedded zinc-tellurite glass. Surface enhanced Raman scattering effect is highlighted for the first time in tellurite glass containing silver NPs resulting in an enhanced Raman signal (~10 times). SAED manifest the growth of Ag(0) nanoparticles along the (111) and (200) crystallographic planes having average diameter in the range 14-36 nm. Surface plasmon resonance bands are observed in the range 484-551 nm. Furthermore, four prominent photoluminescence bands undergo significant enhancements up to 3 times. The enhancement is majorly attributed to the local field effect of silver NPs.
Chinese Optics Letters | 2013
Fakhra Nawaz; Md. Rahim Sahar; Sib Krishna Ghoshal; Raja; J. Amjad; M. R. Dousti; Asmahani Awang
Sm 3+ /Yb 3+ co-doped tellurite glasses are prepared by melt-quenching technique. The density of the glasses varies between 4.65 and 4.84 g/cm 3 . The optical absorption spectra consist of eight bands in the wavelength range of 350-2 000 nm, which correspond to the transitions from ground level 6 H 5/2 to the various excited states of the Sm 3+ ion. Energy band gaps vary in the range of 2.73-2.91 eV, and the Urbach energy ranges from 0.21 to 0.27. Emission spectra exhibit four peaks originating from the 4 G 5/2 energy level centered at 576, 613, 657, and 718 nm. Quenches in emission bands may be due to the energy transfer from the Sm 3+ to Yb 3+ ions.
Chinese Physics Letters | 2012
Raja J. Amjad; Md. Rahim Sahar; Sib Krishna Ghoshal; M. R. Dousti; Saira Riaz; Bashir Ahmed Tahir
Samarium doped lead-zinc-phosphate glasses having composition (60−x)P2O5-20PbO-20ZnO-xSm2O3 where x=0, 0.5, 1.0, 3.0mol% were prepared by using the melt quenching technique. The Archimedes method was used to measure their densities, which are used to calculate the molar volumes. The values of densities lie in the range 3.698–4.090 gm/cm3 whereas those of molar volume lie in the range of 37.24–40.00 cm−3. UV-vis-NIR absorption spectroscopy in the wavelength range 200–2000 nm was carried out. Absorption spectra consist of seven absorption peaks corresponding to the transitions from the 6H5/2 ground state to various excited energy levels. The energy band gap measured from the optical absorbance is found to be in the range of 3.88-4.43 eV and 3.68-4.33 eV for direct and indirect transitions, respectively. In addition, the photoluminescence spectrum shows four prominent emission bands centered at 560, 597, 642 and 700 nm corresponding to the 4G5/2−6HJ (J=5/2, 7/2, 9/2, 11/2) transitions respectively and the intensity of all the bands are enhanced as the concentration of Sm3+ ions increases.
Chinese Physics Letters | 2013
Raja J. Amjad; Md. Rahim Sahar; Sib Krishna Ghoshal; M. R. Dousti; Saira Riaz; Alireza Samavati; M. N. A. Jamaludin; Shahzad Naseem
The melt quenching method is used to prepare erbium-doped silver nanoparticle (NP) embedded phosphate glass. The effect of annealing on the glass on the formation of silver NPs produced by the reduction of silver (Ag+ →Ag°) is studied. The glass samples are characterized by x-ray diffraction, UV-vis-NIR absorption, photoluminescence spectroscopy and transmission electron microscopy (TEM) imaging. The absorption spectra reveal not only the peaks due to Er3+ ions, but also the surface plasmon resonance band of silver NPs located around ~442 nm. The TEM imaging shows the homogeneous distribution of silver NPs of almost spherical shape with an average diameter of ~5 nm. Upconversion luminescence spectra show two major emissions at 550 and 638 nm, originating from the 4S3/2 and 4F9/2 energy levels of the Er3+ ions, respectively. The enhancement in the luminescence intensity of both the green and red bands is found to be due to the effective local field of the silver NPs as well as the energy transfer from the nanoclusters, comprised of centers with silver ions bound to silver atoms in dimers or trimers to Er3+ ions, whereas quenching occurred due to the energy transfer from erbium ions to silver NPs (Er3+ →Ag°).
Chinese Physics Letters | 2012
Alireza Samavati; Zulkafli Othaman; Sib Krishna Ghoshal; M. R. Dousti; Raja J. Amjad
Controlled growth, synthesis, and characterization of a high density and large-scale Ge nanostructure by an easy fabrication method are key issues for optoelectronic devices. Ge quantum dots (QDs) having a density of ~1011 cm−2 and a size as small as ~8 nm are grown by radio frequency magnetron sputtering on Si (100) substrates under different heat treatments. The annealing temperature dependent structural and optical properties are measured using AFM, XRD, FESEM, EDX, photoluminescence (PL) and Raman spectroscopy. The effect of annealing is found to coarsen the Ge QDs from pyramidal to dome-shaped structures as they grow larger and transform the nanoislands into relatively stable and steady state configurations. Consequently, the annealing allows the intermixing of Si into the Ge QDs and thereby reduces the strain energy that enhances the formation of larger nanoislands. The room temperature PL spectra exhibits two strong peaks at ~2.87 eV and ~3.21 eV attributed to the interaction between Ge, GeOx and the possibility of the presence of QDs core-shell structure. No reports so far exist on the red shift ~0.05 eV of the strongest PL peak that results from the effect of quantum confinement. Furthermore, the Raman spectra for the pre-annealed QDs that consist of three peaks at around ~305.25 cm−1, 409.19 cm−1 and 515.25 cm−1 are attributed to Ge-Ge, Ge-Si, and Si-Si vibration modes, respectively. The Ge-Ge optical phonon frequency shift (~3.27 cm−1) associated with the annealed samples is assigned to the variation of shape, size distribution, and Ge composition in different QDs. The variation in the annealing dependent surface roughness and the number density is found to be in the range of ~0.83 to ~2.24 nm and ~4.41 to ~2.14 × 1011 cm−2, respectively.
Optical Materials | 2013
Raja J. Amjad; Md. Rahim Sahar; Sib Krishna Ghoshal; M. R. Dousti; Ramli Arifin
Materials Letters | 2013
Zahra Ashur Said Mahraz; Md. Rahim Sahar; Sib Krishna Ghoshal; M. R. Dousti; Raja J. Amjad
Journal of Luminescence | 2013
Raja J. Amjad; Md. Rahim Sahar; Sib Krishna Ghoshal; M. R. Dousti; Saira Riaz; Alireza Samavati; Ramli Arifin; Shahzad Naseem
Journal of Luminescence | 2014
Alireza Samavati; Zulkafli Othaman; Sib Krishna Ghoshal; M. R. Dousti
Indian Journal of Pure & Applied Physics | 2012
Sib Krishna Ghoshal; Md. Rahim Sahar; M. R. Dousti; Sunita Sharma; Md. Supar Rohani; Ramli Arifin; K. Hamzah