Imperfection of the clustered perovskite structure, phase transitions, and magnetoresistive properties of ceramic La0.6Sr0.2Mn1.2 − x Ni x O3 ± δ (x = 0–0.3)

Abstract

Ceramic samples of lanthanum strontium manganite perovskites La 0.6 Sr 0.2 Mn 1.2 -x Ni x O 3 ± δ (0 ≤ x ≤ 0.3) have been investigated using the X ray diffraction, magnetic (χ ac ), 55 Mn NMR, resistive, and magnetoresistive methods. The specific features of the influence of the composition on the structure and properties of nonstoichiometric manganite perovskites have been established. It has been found that the rhombohedrally ( ) distorted perovskite structure contains cation and anion vacancies, as well as nano structured clusters with Mn 2+ ions in the A positions. The substitution of Ni 3+ ions (r = 0.74 Å) for Mn 3+ ions (r = 0.785 Å) leads to a decrease in the lattice parameter a, the ferromagnetic-paramagnetic phase transition temperature T C , and the metal-semiconductor phase transition temperature T ms due to the disturbance of the superexchange interactions between heterovalent manganese ions Mn 3+ and Mn 4+ . The observed anom alous magnetic hysteresis at 77 K has been explained by the antiferromagnetic effect of the unidirectional exchange anisotropy of the ferromagnetic matrix structure on the magnetic moments of the superstoichio metric manganese Mn 2+ ions located in nanostructured planar clusters. An analysis of the asymmetrically broadened 55 Mn NMR spectra of the compounds has revealed a high frequency electronic superexchange of the ions Mn 3+ O 2-Mn 4+ ; a local heterogeneity of their surrounding by other ions, vacancies, and clusters; and a partial localization of Mn 4+ ions. The local hyperfine interaction fields on 55 Mn nuclei have been determined. The concentration dependences of the activation energy and charge hopping frequency have confirmed that the Ni ions decrease the electrical conductivity due to the weakening of the electronic superexchange Mn 3+ O 2-Mn 4+ . Two types of magnetoresistive effects have been found: one effect, which is observed near the phase transition temperatures T C and T ms , is caused by scattering at intracrystalline nanostructured heterogeneities, and the other effect, which is observed in the low temperature range, is induced by tunneling through intercrystalline mesostructured boundaries. The phase diagram has demon strated that there is a strong correlation between magnetic and electrical properties in rare earth manganites.

Smart magnetic nanopowder based on the manganite perovskite for local hyperthermia

“…Using equation: It should be also noted that there are two 55 Mn and 139 La centers of the NMR signal in the synthesized smart magnetic La 0.6 Ag 0.2 Mn 1.2 O 3 nanopowder. In the FM state at T < T C (42 C), the formation of the NMR spectrum on 55 Mn nuclei (the gyromagnetic ratio g Mn ¼ 10.560 MHz/T) 65 occurs under the inuence of the hyperne interaction eld H HIF ¼ 34-38 T. 36 The eld on 139 La nuclei (g La ¼ 6.014 MHz/T) 66 has a dipole-dipole character and is in the range H dd ¼ 2.3-3.7 T. 65,67 In the PM state (T > T C ), during MRI studies, the eld on the 55 Mn and 139 La NMR nuclei decreases to $1.5 T of the tomograph eld. Such a variety of magnetic resonance properties of the synthesized La 0.6 Ag 0.2 Mn 1.2 O 3 nanopowder operating at the intracellular level additionally opens up great prospects for its use as novel MRI contrast agents for tumor theranostics, which combine the properties of both therapeutic and diagnostic agents.…”