Partha Hajra
Indian Association for the Cultivation of Science
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Publication
Featured researches published by Partha Hajra.
Bulletin of Materials Science | 2014
Shilpi Banerjee; Partha Hajra; Anindya Datta; Asim Bhaumik; Mykanth Reddy Mada; Sri Bandyopadhyay; D. Chakravorty
Composites comprising of nanoparticles of Ni0∙5Zn0∙5Fe2O4 (NZF) and BaTiO3 (BT), respectively were synthesized by a chemical method. The particles had diameters in the range of 15–31 nm. NZF was prepared by a coprecipitation technique. This was soaked in a sol containing BT. Compositions synthesized were xNZF-(1 – x) BT, where x = 0∙7, 0∙5 and 0∙3, respectively. The composites showed ferromagnetic hysteresis loops due to NZF phase. The analysis of coercivity variation as a function of temperature gave blocking temperatures in the range of 306–384 K depending on the diameter of the ferrite nanoparticles. This implied that superparamagnetic interactions are above these temperatures. The nanocomposites also exhibited ferroelectric behaviour arising due to the presence of BT. The remanent polarization of the samples was small. This was adduced to the nanosize of BT. The specimens showed magneto-dielectric (MD) effect in the magnetic field range 0–0∙7 Tesla. The MD parameter measured at the maximum magnetic field was around 2%. This was one order of magnitude higher than that reported so far in similar composite systems. This was explained on the basis of a two-phase inhomogeneous medium model with an interface between them, the phases possessing drastically different electrical conductivities.
SOLID STATE PHYSICS: Proceedings of the 56th DAE Solid State Physics Symposium 2011 | 2012
Dhriti Ranjan Saha; Partha Hajra; Mykanth Reddy Mada; Philip Boughton; Sri Bandyopadhyay; D. Chakravorty
Nanoindentation of CuO-lithia silica nanoglass (CuO-NG) composite was studied and compared with only CuO nanoparticles (CuO). Youngs Modulus (E) and hardness (H) of the composite was found to be greater in comparison with CuO nanoparticles. Creep measurements showed that Creep strain rate (CSR) is lower for composite material than only CuO. This is due to decrease of copper diffusion through nanoglass phase in composite sample.
Journal of Magnetism and Magnetic Materials | 2011
Partha Hajra; S. Dutta; P. Brahma; D. Chakravorty
Journal of Magnetism and Magnetic Materials | 2012
Partha Hajra; P. Brahma; S. Dutta; Sourish Banerjee; D. Chakravorty
Materials Letters | 2012
Shilpi Banerjee; Partha Hajra; Asim Bhaumik; D. Chakravorty
Journal of Magnetism and Magnetic Materials | 2013
Shilpi Banerjee; Partha Hajra; Mykanth Reddy Mada; Asim Bhaumik; Sri Bandyopadhyay; D. Chakravorty
Materials Letters | 2012
Partha Hajra; R.P. Maiti; D. Chakravorty
Chemical Physics Letters | 2012
Shilpi Banerjee; Partha Hajra; Asim Bhaumik; Sri Bandyopadhyay; D. Chakravorty
Materials Science and Engineering A-structural Materials Properties Microstructure and Processing | 2014
Partha Hajra; Dhriti Ranjan Saha; Mykanth Reddy Mada; S. Dutta; P. Brahma; Philip Boughton; Sri Bandyopadhyay; D. Chakravorty
Journal of the American Ceramic Society | 2011
R. Venkata Ram Naidu; Partha Hajra; Anindya Datta; Santanu Bhattacharya; D. Chakravorty