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| Home > Publications database > Size-dependent magnetic transitions in CoFe$_0.1$Cr$_1.9$O$_4$ nanoparticles studied by magnetic and neutron-polarization analysis > print |
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| 100 | 1 | _ | |a Kumar, D. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Size-dependent magnetic transitions in CoFe$_0.1$Cr$_1.9$O$_4$ nanoparticles studied by magnetic and neutron-polarization analysis |
| 260 | _ | _ | |a Bristol |c 2016 |b IOP Publ. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a Multiferroic, CoCr2O4 bulk material undergoes successive magnetic transitions such as a paramagnetic to collinear and non-collinear ferrimagnetic state at the Curie temperature (T C) and spiral ordering temperature (T S) respectively and finally to a lock-in-transition temperature (T l). In this paper, the rich sequence of magnetic transitions in CoCr2O4 after mixing the octahedral site with 10% of iron are investigated by varying the size of the particle from 10 to 50 nm. With the increasing size, while the T C increases from 110 to 119 K which is higher than the T C (95 K) of pure CoCr2O4, the T S remains unaffected. In addition, a compensation of magnetization at 34 K and a lock-in transition at 10 K are also monitored in 50 nm particles. Further, we have examined the magnetic-ordering temperatures through neutron scattering using a polarized neutron beam along three orthogonal directions after separating the magnetic scattering from nuclear-coherent and spin-incoherent contributions. While a sharp long-range ferrimagnetic ordering down to 110 K and a short-range spiral ordering down to 50 K are obtained in 50 nm particles, in 10 nm particles, the para to ferrimagnetic transition is found to be continuous and spiral ordering is diffused in nature. Frequency-dependent ac susceptibility (χ) data fitted with different phenomenological models such as the Neel–Arrhenius, Vogel–Fulcher and power law, while ruling out the canonical spin-glass, cluster-glass and interacting superparamagnetism, reveal that both particles show spin-glass behavior with a higher relaxation time in 10 nm particles than in 50 nm. The smaller spin flip time in 50 nm particles confirms that spin dynamics does not slow down on approaching the glass transition temperature (T g). |
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| 700 | 1 | _ | |a Banerjee, A. |0 P:(DE-HGF)0 |b 2 |
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| 700 | 1 | _ | |a Rath, Chandana |0 P:(DE-HGF)0 |b 5 |e Corresponding author |
| 773 | _ | _ | |a 10.1088/0957-4484/27/17/175702 |g Vol. 27, no. 17, p. 175702 - |0 PERI:(DE-600)1362365-5 |n 17 |p 175702 1-10 |t Nanotechnology |v 27 |y 2016 |x 1361-6528 |
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