Structural, magnetic, and electrical characteristics of manganites in the system La3+0.7Sr2+0.3Mn3+0.6–x-2γMn4+0.3+x+2γFe3+0.1–x Mg2+xO2-3+γ (0 ≤ x ≤ 0.1) synthesized by solid-state reactions are presented. Sintering was performed in air at 1423 K. Samples with stoichiometric… Click to show full abstract
Structural, magnetic, and electrical characteristics of manganites in the system La3+0.7Sr2+0.3Mn3+0.6–x-2γMn4+0.3+x+2γFe3+0.1–x Mg2+xO2-3+γ (0 ≤ x ≤ 0.1) synthesized by solid-state reactions are presented. Sintering was performed in air at 1423 K. Samples with stoichiometric oxygen content (γ = 0) were obtained by annealing at 1223 K and a partial oxygen pressure of 0.1 Pa. All studied manganites have a rhombohedral structure. With an increase in the magnesium content, the volume of the unit cell decreases, and annealed samples have a larger cell volume than the initial, sintered manganites containing over-stoichiometric oxygen. The ratio c/a of lattice parameters is practically unchanged. Curie point of manganites decreases in general with an increase in the magnesium content, showing a weakly expressed plateau in the region of 0.025 < x < 0.075. Magnetization and “metal-semiconductor” transition temperature have maximum values at x = 0, then change non-monotonically, and at x > 0.075 fall sharply. Manganite, which contains the largest amount of magnesium, has the highest resistance at temperatures below 180 K and is characterized by the largest width of the temperature interval of “ferromagnetic-paramagnetic” transition, which indicates the existence of magnetic inhomogeneities. The electromagnetic parameters of the initial and annealed samples differ slightly. A number of effects and competing factors that determine complicated dependencies of electromagnetic characteristics of the manganites of this system on the composition are considered.
               
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