M.A. Shaz
Banaras Hindu University
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Publication
Featured researches published by M.A. Shaz.
Journal of Materials Chemistry | 2016
Ashish Bhatnagar; Sunita K. Pandey; Alok K. Vishwakarma; Sweta Singh; Vivek Shukla; Pawan K. Soni; M.A. Shaz; O.N. Srivastava
The present investigation describes the hydrogen sorption (de/absorption) behavior of MgH2 catalyzed by graphene sheet templated Fe3O4 nanoparticles (Fe3O4@GS). Hydrogen sorption studies reveal that MgH2 catalyzed by Fe3O4@GS (MgH2:Fe3O4@GS) offers improved hydrogen storage behavior as compared to stand-alone MgH2 catalyzed by graphene sheets (GS) (MgH2:GS) or Fe3O4 nanoparticles (MgH2:Fe3O4). The MgH2:Fe3O4@GS has an onset desorption temperature of ∼262 °C (∼142 °C lower than pristine MgH2), while MgH2:GS and MgH2:Fe3O4 have onset desorption temperatures of ∼275 °C and ∼298 °C respectively. In contrast to this, MgH2:GS absorbs 4.40 wt% and MgH2:Fe3O4 absorbs 5.50 wt% in 2.50 minutes at 290 °C under 15 atm hydrogen pressure. On the other hand, MgH2:Fe3O4@GS absorbs 6.20 wt% hydrogen in 2.50 minutes (which is considerably higher than recently studied catalyzed MgH2 systems) under identical temperature and pressure conditions. The MgH2 catalyzed with Fe3O4@GS shows negligible degradation of the storage capacity even after 25 cycles. Additionally, the desorption activation energy for MgH2:Fe3O4@GS has been found to be 90.53 kJ mol−1 (which is considerably lower as compared to metal/metal oxide catalyzed MgH2 and fluorographene catalyzed MgH2). The formation enthalpy for MgH2:Fe3O4@GS is 60.62 kJ per mole of H2 (13.44 kJ mol−1 lower than bulk MgH2). The catalytic effect of Fe3O4@GS has been described and discussed with the help of structural (X-ray diffraction (XRD)), micro structural (electron microscopy) and Raman spectroscopic studies.
Physical Review B | 2005
M.A. Shaz; Sander van Smaalen; Lukas Palatinus; M. Hoinkis; M. Klemm; S. Horn; R. Claessen
Temperature-dependent x-ray diffraction of the low-dimensional spin-
International Journal of Nanoscience | 2011
T.P. Yadav; Devinder Singh; N. K. Mukhopadhyay; M.A. Shaz; R. S. Tiwari; O.N. Srivastava
1∕2
International Journal of Hydrogen Energy | 2013
Rohit R. Shahi; Anand P. Tiwari; M.A. Shaz; O.N. Srivastava
quantum magnet TiOCl shows that the phase transition at
International Journal of Hydrogen Energy | 2011
Rohit R. Shahi; T.P. Yadav; M.A. Shaz; O.N. Srivastava; S. van Smaalen
{T}_{c2}=90\phantom{\rule{0.3em}{0ex}}\mathrm{K}
International Journal of Hydrogen Energy | 2014
Ashish Bhatnagar; Sunita K. Pandey; Viney Dixit; Vivek Shukla; Rohit R. Shahi; M.A. Shaz; O.N. Srivastava
corresponds to a lowering of the lattice symmetry. Below
International Journal of Hydrogen Energy | 2012
Rohit R. Shahi; Himanshu Raghubanshi; M.A. Shaz; O.N. Srivastava
{T}_{c1}=66\phantom{\rule{0.3em}{0ex}}\mathrm{K}
International Journal of Hydrogen Energy | 2015
Vivek Shukla; Ashish Bhatnagar; Sunita K. Pandey; Rohit R. Shahi; T.P. Yadav; M.A. Shaz; O.N. Srivastava
a twofold superstructure develops, that indicates the formation of spin-singlet pairs via direct exchange between neighboring Ti atoms, while the role of superexchange is found to be negligible. TiOCl thus is identified as a spin-Peierls system of pure one-dimensional chains of atoms. The first-order character of the transition at
International Journal of Hydrogen Energy | 2013
Rohit R. Shahi; Himanshu Raghubanshi; M.A. Shaz; O.N. Srivastava
{T}_{c1}
Applied Nanoscience | 2012
Rohit R. Shahi; Himanshu Raghubanshi; M.A. Shaz; O.N. Srivastava
is explained by the competition between the structurally deformed state below