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At least 235 records · Page 13

Study of the Effect of Pr Doping on Structural, Morphological and Magnetic Properties of Nickel Ferrite

Praseodymium rare earth ion (Pr{sup 3+}) doped nickel ferrite (NiFe{sub 2−x}Pr{sub x}O{sub 4}, 0 < x< 0.1) nanocrystals (NFPO) were synthesized by hydrothermal method. The structural, morphological and magnetic properties of the prepared samples have been studied. The x-ray diffraction (XRD) and fourier transform infrared (FTIR) techniques confirmed the phase formation of the NFPO nanocrystals. The average crystallite size of NFPO nanoparticles found to be in the range 39 to 44 nm. The presence of Pr ions in NFPO was confirmed by energy-dispersive x-ray (EDX) analysis. It has been observed that after a certain amount of Pr doping, the morphology of the nanocrystals starts changing from nano-octahedrons to nanorods shape, as confirmed by transmission electron microscopy (TEM). Also, the magnetic properties of the prepared nanocrystals were measured using physical properties measurement system (PPMS) at 10 K and 300 K. The saturation magnetization (Ms) first decreases with the increasing loading amount of Pr ions up to (x = 0.025) and later it increases at both the temperatures. However, the value of coercivity shows an increasing trend with the increasing amount of Pr ions in NFPO at room temperature.

77 NANOSCIENCE AND NANOTECHNOLOGY↗

The Effects of La Doping on the Crystal Structure, Magnetic, and Microwave Absorption Properties of Nd{sub 2}Fe{sub 14}B Compound

The crystal structure, magnetic, and microwave absorption properties of the (Nd{sub 1−x}La{sub x}){sub 2}Fe{sub 14}B system have been investigated. The La{sub 2}Fe{sub 14}B compound was successfully synthesized and refined, giving a tetragonal structure, space group P4{sub 2}/mnm with the Nd{sub 2}Fe{sub 14}B-type structure. The crystal structure parameters of the (Nd{sub 1−x}La{sub x}){sub 2}Fe{sub 14}B compounds were determined by full-profile Rietveld refinements. The results revealed that all intermediate alloys form a continuous solid solution. The normalized lattice parameters of the (Nd{sub 1−x}La{sub x}){sub 2}Fe{sub 14}B compounds increase linearly with an increase of La concentration. Based on the results of DSC measurements and X-ray powder diffraction examinations, the phase diagram of the Nd{sub 2}Fe{sub 14}B-La{sub 2}Fe{sub 14}B system has been constructed. The remanence (M{sub r}) and coercivity (H{sub c}) of (Nd{sub 1−x}La{sub x}){sub 2}Fe{sub 14}B (x = 0.00, 0.10, 0.20, 0.30, and 0.40) gradually decrease. The highest reflection loss is − 29.8, − 27.4, − 24.1, − 18.6, and − 14.2 dB at 9.8, 8.9, 7.5, 6.9, and 6.5 GHz, respectively. The absorption peak shifts toward from higher frequency region to lower frequency region and the absorption bandwidth widens with the increase of the La substitution.

36 MATERIALS SCIENCE↗

Effect of Ca Doping on the Structure and Magnetic and Electronic Properties of La{sub 1 − x}Ca{sub x}Cr{sub 0.8}Cu{sub 0.2}O{sub 3} (x = 0~0.3)

A series of La{sub 1 − x}Ca{sub x}Cr{sub 0.8}Cu{sub 0.2}O{sub 3} samples were successfully prepared by sol-gel method, and their crystal structures were refined by using X-ray powder diffraction data. All samples had orthorhombic structure with a space group Pbnm. Two magnetic transitions were observed for all of samples, and the paramagnetism-antiferromagnetism transition temperature decreased, and the antiferromagnetism-ferromagnetism transition temperature increased with increasing Ca content. Moreover, Cu and Ca co-doping improved conductivity and active energy.

36 MATERIALS SCIENCE↗

Effects of Co doping on the structure and physicochemical properties of hausmannite (Mn 3 O 4 ) and its transformation during aging

Hausmannite is a common low-valence manganese oxide mineral with a distorted spinel structure in surficial sediments. Although natural Mn oxides often contain various transition metal (TM) impurities, few studies have addressed the substitution mechanisms of TMs, such as cobalt (Co), with hausmannite and induced changes in the mineral physicochemical properties. In this study, Co-doped hausmannites with final Co/Mn molar ratios of 0.05 and 0.11 were synthesized and characterized by wet chemical analysis, powder X-ray diffraction (XRD), Fourier transformed infrared spectra (FTIR), high resolution transmission electron microscope (HRTEM), X-ray photoelectron spectroscopy (XPS) and X-ray absorption fine structure spectroscopy (XAFS). Co-doped samples have larger crystallite sizes and smaller specific surface areas than those of the hausmannite without Co. The Co cations exist in a mixed-valence of +3 and + 2. Powder XRD and acid dissolution experiments indicate that Co incorporates into the mineral structures, and increases the mineral structural stability. Co K-edge extended X-ray adsorption fine structure (EXAFS) analysis demonstrates that Co likely substitutes for lattice Mn(III). After aging at room temperature for three years, 14.1 ± 1.9% of pure hausmannite is transformed to manganite while only 2.6 ± 0.7% of manganite appears in the aged Co-doped sample with an initial Co/Mn molar ratio of 0.10. Finally, these results provide new insights into the incorporation mechanisms of TMs into low valence Mn oxides, and the stability of these minerals in natural environments.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Effects of Selenium Doping in Zinc Telluride from First Principles

We report point defects and compensation in zinc telluride have been subjects of study for several decades due to the compound’s scientific/technological applications. Despite this, there remains some disagreement in the literature as to the fine details of its defect chemistry. Recently, it has also come under renewed interest due to the emerging Cd( 1–x )Zn x Te( 1–y )Se y material family, used in nuclear radiation detector applications. In this article, we use state-of-the-art computational tools to re-examine the native defect chemistry of ZnTe and explore how it changes upon addition of selenium using density functional theory with screened hybrid exchange–correlation functionals, thermochemical models of the equilibration environment, and statistical mechanics models of the point defect ensemble.

II-VI semiconductors↗