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Field induced crossover in critical behaviour and direct measurement of the magnetocaloric properties of La(0.4)Pr(0.3)Ca(0.1)Sr(0.2)MnO(3)

La(0.4)Pr(0.3)Ca(0.1)Sr(0.2)MnO(3) has been investigated as a potential candidate for room temperature magnetic refrigeration. Results from X-ray powder diffraction reveal an orthorhombic structure with Pnma space group. The electronic and chemical properties have been confirmed by X-ray photoelectr...

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Detalles Bibliográficos
Autores principales: Ghorai, Sagar, Skini, Ridha, Hedlund, Daniel, Ström, Petter, Svedlindh, Peter
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7655858/
https://www.ncbi.nlm.nih.gov/pubmed/33173113
http://dx.doi.org/10.1038/s41598-020-76321-w
Descripción
Sumario:La(0.4)Pr(0.3)Ca(0.1)Sr(0.2)MnO(3) has been investigated as a potential candidate for room temperature magnetic refrigeration. Results from X-ray powder diffraction reveal an orthorhombic structure with Pnma space group. The electronic and chemical properties have been confirmed by X-ray photoelectron spectroscopy and ion-beam analysis. A second-order paramagnetic to ferromagnetic transition was observed near room temperature (289 K), with a mean-field like critical behaviour at low field and a tricritical mean-field like behaviour at high field. The field induced crossover in critical behaviour is a consequence of the system being close to a first-order magnetic transition in combination with a magnetic field induced suppression of local lattice distortions. The lattice distortions consist of interconnected and weakly distorted pairs of Mn-ions, where each pair shares an electron and a hole, dispersed by large Jahn–Teller distortions at Mn(3+) lattice sites. A comparatively high value of the isothermal entropy-change (3.08 J/kg-K at 2 T) is observed and the direct measurements of the adiabatic temperature change reveal a temperature change of 1.5 K for a magnetic field change of 1.9 T.