Lattice expansion and non-collinear to collinear ferrimagnetic order in MnCrO nanoparticle
arXiv:cond-mat/0510814 · doi:10.1103/PhysRevB.73.144413
Abstract
We report magnetic behaviour of MnCrO, which belongs to a special class of spinel, known as chromite. Bulk MnCrO shows a sequence of magnetic states, which follows paramagnetic (PM) to collinear ferrimagnetic (FM) state below T 45 K and collinear FM state to non-collinear FM state below T 18 K. The non-collinear spin structure has been modified on decreasing the particle size, and magnetic transition at T decreases in nanoparticle samples. However, ferrimagnetic order is still dominating in nanoparticles, except the observation of superparamagnetic like blocking and decrease of spontaneous magnetization for nanoparticle. This may, according to the core-shell model of ferrimagnetic nanoparticle, be the surface disorder effect of nanoparticle. The system also show the increase of T in nanoparticle samples, which is not consistent with the core-shell model. The analysis of the M(T) data, applying spin wave theory, has shown an unusual Bloch exponent value 3.35 for bulk MnCrO, which decreases and approaches to 1.5, a typical value for any standard ferromagnet, with decreasing the particle size. MnCrO has shown a few more unusual behaviour. For example, lattice expansion in nanoparticle samples. The present work demonstrates the correlation between a systematic increase of lattice parameter and the gradual decrease of B site non-collinear spin structure in the light of magnetism of MnCrO nanoparticles.
References in corpus (2)
Cited by in corpus (5)
- Evidence of Ferrimagnetism in Ferromagnetic La0_{67}Ca0_{33}MnO_3 nanoparticle
- Spinel Cu-Mn-Cr Oxide Nanoparticle-Pigmented Solar Selective Coatings Maintaining >94% Efficiency at 750 degrees C
- Low temperature ferromagnetism, surface paramagnetism and exchange bias effect in nano-grained alpha-Fe1.4Ga0.6O3 oxide
- Temperature evolution of the effective magnetic anisotropy in the MnCrO spinel
- Rare-earth-free noncollinear metallic ferrimagnets Mn4-xZxN with compensation at room temperature