903 research outputs found

    Magnetic properties of Hydrogenated Li and Co doped ZnO nanoparticles

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    The effect of hydrogenation on magnetic properties of Zn0.85Co0.05Li0.10O nanoparticles is presented. It was found that the sample hydrided at room temperature (RT) showed weak ferromagnetism (FM) while that hydrided at 400oC showed robust ferromagnetism at room temperature. In both cases reheating the sample at 400oC in air converts it back into paramagnetic state (P) completely. The characterization of samples by X-ray and electron diffraction (ED) showed that room temperature ferromagnetism observed in the samples hydrogenated at RT is intrinsic in nature whereas that observed in the samples hydrogenated at 400oC is partly due to the cobalt metal clusters.Comment: 10 pages, 3 figure

    Room temperature Ferromagnetism in Th1-xFexO2-d (x = 0.0, 0.05, 0.10, 0.15, 0.20 and 0.25) nanoparticles

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    Nanocrystalline (Th1-xFex)O2-d particles with different Fe concentrations (x = 0.0, 0.05, 0.10, 0.15, 0.20 and 0.25) have been prepared by a gel combustion method. Rietveld refinement analyses of X-ray diffraction data revealed the formation of an impurity free cubic type Th1-xFexO2-d structure up to x = 0.20. This observation is further confirmed from the detailed studies conducted on 10 at. percent Fe doped ThO2 using high-resolution transmission electron microscopy (HRTEM) imaging and indexing of the selected-area electron diffraction (SAED) patterns. DC Magnetization studies as a function field indicate that they are ferromagnetic with Curie temperature (Tc) well above room temperature.Comment: 10 pages, 5 figure

    Theory of Transition Temperature of Magnetic Double Perovskites

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    We formulate a theory of double perovskite coumpounds such as Sr2_2FeReO6_6 and Sr2_2FeMoO6_6 which have attracted recent attention for their possible uses as spin valves and sources of spin polarized electrons. We solve the theory in the dynamical mean field approximation to find the magnetic transition temperature TcT_c. We find that TcT_c is determined by a subtle interplay between carrier density and the Fe-Mo/Re site energy difference, and that the non-Fe same-sublattice hopping acts to reduce TcT_c. Our results suggest that presently existing materials do not optimize TcT_c

    Magnetic Behavior of Manganese-Doped ZnSe Quantum Dots

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    Magnetic properties of manganese-doped ZnSe quantum dots with the size of approximately 3.6 nm are investigated. The amount of Mn in the ZnSe quantum dots has been varied from 0.10% to 1.33%. The doping level in the quantum dots is much less than that used in the precursor. The co-ordination of Mn in the ZnSe lattice has been determined by electron paramagnetic resonance (EPR). Two different hyperfine couplings 67.3×10−4 and 60.9×10−4 cm−1 observed in the EPR spectrum imply that Mn atoms occupy two distinct sites; one uncoordinated (near the surface) and other having a cubic symmetric environment (nanocrystal core), respectively. Photoluminescence measurements also confirm the incorporation of Mn in ZnSe quantum dots. From the Curie-Weiss behavior of the susceptibility, the effective Mn-Mn antiferromagnetic exchange constant (J1) has been evaluated. The spin-glass behavior is observed in 1.33% Mn-doped ZnSe quantum dots, at low temperature. Magnetic behavior at a low temperature is discussed

    Dynamical Mean Field Theory of Double Perovskite Ferrimagnets

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    The dynamical mean field method is used to analyze the magnetic transition temperature and optical conductivity of a model for the ferrimagnetic double perovskites such as Sr2FeMoO6Sr_2FeMoO_6. The calculated transition temperatures and optical conductivities are found to depend sensitively on the band structure. For parameters consistent with local spin density approximation band calculations, the computed transition temperatures are lower than observed, and in particular decrease dramatically as band filling is increased, in contradiction to experiment. Band parameters which would increase the transition temperature are identified.Comment: Supercedes cond-mat/000628 (PRB64 024424/1-4 (2001

    Electronic structure study of double perovskites A2A_{2}FeReO6_{6} (A=Ba,Sr,Ca) and Sr2M_{2}MMoO6_{6} (M=Cr,Mn,Fe,Co) by LSDA and LSDA+U

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    We have implemented a systematic LSDA and LSDA+U study of the double perovskites A2A_{2}FeReO6_{6} (A=Ba,Sr,Ca) and Sr2_{2}MMMoO6_{6} (M=Cr,Mn,Fe,Co) for understanding of their intriguing electronic and magnetic properties. The results suggest a ferrimagnetic (FiM) and half-metallic (HM) state of A2A_{2}FeReO6_{6} (A=Ba,Sr) due to a pdd-π\pi coupling between the down-spin Re5+^{5+}/Fe3+^{3+} t2gt_{2g} orbitals via the intermediate O 2pπ2p_{\pi} ones, also a very similar FiM and HM state of Sr2_{2}FeMoO6_{6}. In contrast, a decreasing Fe t2gt_{2g} component at Fermi level (EFE_{F}) in the distorted Ca2_{2}FeReO6_{6} partly accounts for its nonmetallic behavior, while a finite pddpdd-σ\sigma coupling between the down-spin Re5+^{5+}/Fe3+^{3+} ege_{g} orbitals being present at EFE_{F} serves to stabilize its FiM state. For Sr2_{2}CrMoO6_{6} compared with Sr2_{2}FeMoO6_{6}, the coupling between the down-spin Mo5+^{5+}/Cr3+^{3+} t2gt_{2g} orbitals decreases as a noticeable shift up of the Cr3+^{3+} 3d levels, which is likely responsible for the decreasing TCT_{C} value and weak conductivity. Moreover, the calculated level distributions indicate a Mn2+^{2+}(Co2+^{2+})/Mo6+^{6+} ionic state in Sr2_{2}MnMoO6_{6} (Sr2_{2}CoMoO6_{6}), in terms of which their antiferromagnetic insulating ground state can be interpreted. While orbital population analyses show that owing to strong intrinsic pd covalence effects, Sr2M_{2}MMoO6_{6} (M=Cr,Mn,Fe,Co) have nearly the same valence state combinations, as accounts for the similar M-independent spectral features observed in them.Comment: 21 pages, 3 figures. to be published in Phys. Rev. B on 15th Se

    The structural and magnetic properties of (In1-xFex)2O3 (0.0 <= x <= 0.25) system : prepared by gel combustion method

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    (In1-xFex)2O3 polycrystalline samples with x = (0.0, 0.05, 0.10, 0.15, 0.20 and 0.25) have been synthesized by a gel combustion method. Reitveld refinement analysis of X raydiffraction data indicated the formation of single phase cubic bixbyite structure without any parasitic phases. This observation is further confirmed by high resolution transmission electron microscopy (HRTEM) imaging, and indexing of the selected-area electron diffraction (SAED) patterns, X-ray Absorption Spectroscopy (XAS) and Raman Spectroscopy. DC Magnetization studies as a function of temperature and field indicatethat they are ferromagnetic with Curie temperature (TC) well above room temperature.Comment: 9 pages 3 figure
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