R.N. Dubey
Maulana Azad National Institute of Technology
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Featured researches published by R.N. Dubey.
Radiation Effects and Defects in Solids | 2008
Suchinder K. Sharma; Shreyas S. Pitale; M.M. Malik; R.N. Dubey; M.S. Qureshi
Black light source (360 nm) is used to undertake detailed kinetic analysis of strontium aluminate (Sr4Al14O25:Eu2+) with a long-lasting afterglow. Thermally stimulated luminescence studies were carried out to obtain different trapping parameters such as order of kinetics, frequency factor(s) and activation energy (E). The non-shifting T m property in the measured glow curves is used to describe the order of kinetics. Decay studies are also used to verify the order of kinetics. Double peak structure is obtained with peaks at 487 and 423 K. Glow curve deconvolution function using a computerized package is applied to find the associated trapping parameters. McKeevers T m–T stop method is applied to determine the trap distribution and to approximate energies. The depth of the traps is found to be varying within 0.50 and 1.36 eV. Photoluminescence studies reveal the emission characteristics and mechanism. The emission peak is obtained at 487 nm.
INTERNATIONAL CONFERENCE ON PHYSICS OF EMERGING FUNCTIONAL MATERIALS (PEFM-2010) | 2010
Bhakti V. Raigaonkar; Lajna P. Vijayan; R.N. Dubey; M.S. Qureshi
Anthracene doped emeraldine base polyaniline (EB‐PAni) compounds were prepared through emulsion polymerization reaction. The difference of two orders of magnitude was observed in room temperature conductivity (σ) of bare and doped EB‐PAni. For bare EB‐PAni σ = 1.13×10−3 Sm−1 and σ = 15.0×10−5 Sm−1 for doped EB‐PAni with highest dopant concentration. UV‐VIS absorption studies indicate that with increasing dopant concentration the intensity of absorption at 600 nm increases. This is attributed to the change in population of quinoid imine units in the polymer backbone. Two significant changes were observed in the FTIR spectrum of bare and doped EB‐PAni. First is appearance of a peak at 1140.0 cm−1 in doped compounds, attributed to vibration mode of the ‐NH+= structure. It suggests oxidation of polymer backbone. And second is decrease in intensity in the peak at 1294.8 cm−1 in doped EB‐PAni, which is attributed to decrease in π electron delocalization across the polymer backbone. Therefore doping of anthracen...
Journal of Alloys and Compounds | 2009
Suchinder K. Sharma; Shreyas S. Pitale; M.M. Malik; M.S. Qureshi; R.N. Dubey
Journal of Luminescence | 2009
Suchinder K. Sharma; Shreyas S. Pitale; M.M. Malik; R.N. Dubey; M.S. Qureshi
Physica B-condensed Matter | 2010
Suchinder K. Sharma; Shreyas S. Pitale; M.M. Malik; R.N. Dubey; M.S. Qureshi; Siddharth Ojha
Optical Materials | 2009
Shreyas S. Pitale; Suchinder K. Sharma; R.N. Dubey; M.S. Qureshi; M.M. Malik
Optical Materials | 2010
Shreyas S. Pitale; Suchinder K. Sharma; R.N. Dubey; M.S. Qureshi; M.M. Malik
Journal of Luminescence | 2010
Suchinder K. Sharma; Shreyas S. Pitale; M.M. Malik; T.K. GunduRao; Santa Chawla; M.S. Qureshi; R.N. Dubey
Journal of Luminescence | 2008
Shreyas S. Pitale; Suchinder K. Sharma; R.N. Dubey; M.S. Qureshi; M.M. Malik
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2008
Shreyas S. Pitale; Suchinder K. Sharma; R.N. Dubey; M.S. Qureshi; M.M. Malik