S. R. Barman
Max Planck Society
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Featured researches published by S. R. Barman.
Applied Physics Letters | 2005
C. Biswas; R. Rawat; S. R. Barman
5% negative magnetoresistance (MR) at room temperature has been observed in bulk Ni2+xMn1−xGa. This indicates the possibility of using Ni2+xMn1−xGa as magnetic sensors. We have measured MR in the ferromagnetic state for different compositions (x=0–0.2) in the austenitic, premartensitic, and martensitic phases. MR is found to increase with x. While MR for x=0 varies almost linearly in the austenitic and premartensitic phases, in the martensitic phase it shows a cusplike shape. This has been explained by the changes in twin and domain structures in the martensitic phase. In the austenitic phase, which does not have twin structure, MR agrees with theory based on s-d scattering model.
Applied Physics Letters | 2009
Aparna Chakrabarti; S. R. Barman
Using density functional theory, we show that in Mn2NiIn a phase transition from cubic to tetragonal structure results in a lowering of the total energy, indicating occurrence of martensitic phase transition. The structural phase transition is nearly volume conserving, which is a characteristic of a shape memory alloy. The magnetic ground state is ferrimagnetic with antiparallel Mn spin moments and the total spin magnetization is 0.51μB in the martensitic phase. Thus, we predict that Mn2NiIn would behave like a magnetic shape memory alloy. The electronic structure and magnetic properties are explained by the spin polarized density of states.
EPL | 2007
S. R. Barman; S. Banik; A. K. Shukla; C. Kamal; Aparna Chakrabarti
The electronic structure of Mn2NiGa has been studied using density functional theory and photoemission spectroscopy. The lower-temperature tetragonal martensitic phase with c/a= 1.25 is more stable compared to the higher-temperature austenitic phase. Mn2NiGa is ferrimagnetic in both phases. The calculated valence band spectrum, the optimized lattice constants and the magnetic moments are in good agreement with experiment. The majority-spin Fermi surface (FS) expands in the martensitic phase, while the minority-spin FS shrinks. FS nesting indicates occurrence of phonon softening and modulation in the martensitic phase.
Physical Review B | 2008
S. R. Barman; Aparna Chakrabarti; Sanjay Singh; S. Banik; S. Bhardwaj; P. L. Paulose; B. A. Chalke; A K Panda; A Mitra; A. M. Awasthi
We predict the existence of a ferromagnetic shape memory alloy
Applied Physics Letters | 1997
S. A. Ding; S. R. Barman; Karsten Horn; Hui Yang; B. Yang; Oliver Brandt; Klaus H. Ploog
{\text{Ga}}_{2}\text{MnNi}
Physical Review B | 2005
Aparna Chakrabarti; C. Biswas; S. Banik; R. S. Dhaka; A. K. Shukla; S. R. Barman
using density-functional theory. The martensitic start temperature
Physical Review B | 2008
S. Banik; R. Rawat; P. K. Mukhopadhyay; B. L. Ahuja; Aparna Chakrabarti; P. L. Paulose; Sanjay Singh; Akhilesh Kumar Singh; Daya Shankar Pandey; S. R. Barman
({T}_{M})
Physical Review B | 2013
K. R. Priolkar; P. A. Bhobe; D. N. Lobo; S. W. D'Souza; S. R. Barman; Aparna Chakrabarti; S. Emura
is found to be approximately proportional to the stabilization energy of the martensitic phase
Journal of Applied Physics | 2009
S. Banik; Sanjay Singh; Rajeev Rawat; P. K. Mukhopadhyay; B. L. Ahuja; A. M. Awasthi; S. R. Barman; E. V. Sampathkumaran
(\ensuremath{\delta}{E}_{\text{tot}})
Journal of Physics: Condensed Matter | 2013
Sanjay Singh; J. Nayak; Abhishek Rai; Parasmani Rajput; Adrian H. Hill; S. R. Barman; Dhananjai Pandey
for different shape memory alloys. Experimental studies performed to verify the theoretical results show that