Effects of non-magnetic Ti4+ ion doping on the structural, magnetic and magnetocaloric properties of La0.65Dy0.05Sr0.3Mn1−xTixO3 compounds

Perovskite manganites have many prospective applications as magnetic solids, however, their synthesis remains challenging of a high purity and a high crystallinity. Herein, a solid state method has been successfully employed for the synthesis of the La 0.65 Dy 0.05 Sr 0.3 Mn 1−x Ti x O 3 (x = 0.05 a...

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Veröffentlicht in:Journal of materials science. Materials in electronics 2019-07, Vol.30 (13), p.12426-12436
Hauptverfasser: Felhi, R., Omrani, H., Koubaa, M., Cheikhrouhou Koubaa, W., Cheikhrouhou, A.
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Sprache:eng
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Zusammenfassung:Perovskite manganites have many prospective applications as magnetic solids, however, their synthesis remains challenging of a high purity and a high crystallinity. Herein, a solid state method has been successfully employed for the synthesis of the La 0.65 Dy 0.05 Sr 0.3 Mn 1−x Ti x O 3 (x = 0.05 and x = 0.10) materials. Moreover, the impact of the Mn by Ti ion substitution on the structural, magnetic and magnetocaloric properties has fully been looked into. The Rietveld refinement technique showed that all the compounds crystallize in the orthorhombic structure with Pbnm space group and that the Mn 4+ by Ti 4+ substitution causes the increase of the unit cell volume. Magnetization versus temperature measurements shows a large ferromagnetic–paramagnetic transition with decreasing temperature. The Curie temperature T C fall with the rise of titanium content from 175 K for x = 0.05 to 114 K for x = 0.10. An analysis of both Banerjee criteria and Landau theory revealed a second-order magnetic phase transition at T C for the current manganites. The magnetocaloric impact is calculated through the measurement of initial isothermal magnetization versus magnetic applied field at various temperatures. The maximum magnetic entropy change Δ S M max , which is calculated on the basis of isothermal magnetization curves under magnetic field change of 5 T is found to be 1.79 J kg −1 K −1 and 1.49 J kg −1 K −1 for x = 0.05 and 0.10, respectively. The relative cooling power (RCP) rose to 239 J kg −1 and 211 J kg −1 at 5 T for x = 0.05, 0.10, respectively. In fact, our results match those about some other doped manganites, which imply that these materials may be appropriate candidates as working substances in magnetic cooling applications. Furthermore, by normalizing the Δ S M ( T , μ 0 H ) curves to their respective Δ S ′ = Δ S M T / Δ S M Max values, we noticed that all the obtained curves drop to a universal master curve. The combination of experiment data and theory analysis is favorable for a better understanding of manganite properties.
ISSN:0957-4522
1573-482X
DOI:10.1007/s10854-019-01602-8