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Effects of sodium doping on physical properties of La0.75Sr0.25-xNaxCoO3 (0≤X≤0.2) cobaltites

Identifieur interne : 000152 ( France/Analysis ); précédent : 000151; suivant : 000153

Effects of sodium doping on physical properties of La0.75Sr0.25-xNaxCoO3 (0≤X≤0.2) cobaltites

Auteurs : M. Koubaa [Tunisie] ; W. Cheikhrouhou-Koubaa [Tunisie] ; A. Cheikhrouhou [Tunisie, France] ; L. Ranno [France]

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RBID : Pascal:09-0024147

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English descriptors

Abstract

The effects of Na doping on the crystallographic, magnetic, electrical and magnetocaloric properties of La0.75Sr0.25-xNaxCoO3 (0≤X≤0.2) samples, elaborated using the solid-state reaction method at high temperature, have been investigated. X-ray powder diffraction studies reveal that all our synthesized samples crystallize in the rhombohedral structure (R3c space group). Na substitution leads to an enhancement of the Co-O bond length and a reduction in the Co-O-Co bond angle and consequently to a weakening of the double exchange interaction between Co3+ and Co4+ ions. The zero field cooled (ZFC) and field cooled (FC) magnetization curves at 50 mT show thermomagnetic irreversibility. At low temperatures, with increasing Na amount, the samples change from ferromagnetic-like behavior (x = 0, 0.05 and 0.1) to spin-glass one (X=0.15 and 0.2). The ferromagnetic-paramagnetic transition temperature decreases with increasing Na amount from 235 to 200 K (x = 0.1). The critical exponent value, associated to the spontaneous magnetization, increases with increasing Na amount from 0.37 for x = 0 to 0.57 for x = 0.1. The temperature dependence of the electrical resistivity reveals three different regimes as a function of Na content: (i) for x = 0, a metallic behavior is observed in the whole temperature range, (ii) for x = 0.05, a metal-semiconducting transition is observed around 80 K and (iii) for x≥0.1, we observe a semiconducting behavior in the whole temperature range. The parent compound (x = 0) exhibits a maximum entropy change |ΔSMAXM| of 0.84 J kg-1 K-1 at 220 K in a magnetic applied field of2T. |ΔSMAXM| decreases to 0.47 J kg-1 K-1 at 185 K forx = 0.1 in the same field magnitude. Well above Tc, |ΔSMAXM| shows a linear dependence as a function of H2 indicating the existence of spin fluctuations inside ferromagnetic clusters.


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<title xml:lang="en" level="a">Effects of sodium doping on physical properties of La
<sub>0.75</sub>
Sr
<sub>0.25-x</sub>
Na
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CoO
<sub>3</sub>
(0≤X≤0.2) cobaltites</title>
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<title xml:lang="en" level="a">Effects of sodium doping on physical properties of La
<sub>0.75</sub>
Sr
<sub>0.25-x</sub>
Na
<sub>x</sub>
CoO
<sub>3</sub>
(0≤X≤0.2) cobaltites</title>
<author>
<name sortKey="Koubaa, M" sort="Koubaa, M" uniqKey="Koubaa M" first="M." last="Koubaa">M. Koubaa</name>
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<term>Bond angle</term>
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<term>Cobalt Lanthanum Sodium Strontium Oxides Mixed</term>
<term>Double exchange</term>
<term>Ferromagnetic materials</term>
<term>Ferromagnetic-paramagnetic transitions</term>
<term>Magnetic cluster</term>
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<term>Diffraction RX</term>
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<term>Longueur liaison</term>
<term>Angle liaison</term>
<term>Fluctuation spin</term>
<term>Double échange</term>
<term>Amas magnétique</term>
<term>Cobalt Lanthane Sodium Strontium Oxyde Mixte</term>
<term>Réseau rhomboédrique</term>
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<term>Matériau ferromagnétique</term>
<term>Cobaltite</term>
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<front>
<div type="abstract" xml:lang="en">The effects of Na doping on the crystallographic, magnetic, electrical and magnetocaloric properties of La
<sub>0.75</sub>
Sr
<sub>0.25-x</sub>
Na
<sub>x</sub>
CoO
<sub>3</sub>
(0≤X≤0.2) samples, elaborated using the solid-state reaction method at high temperature, have been investigated. X-ray powder diffraction studies reveal that all our synthesized samples crystallize in the rhombohedral structure (R3c space group). Na substitution leads to an enhancement of the Co-O bond length and a reduction in the Co-O-Co bond angle and consequently to a weakening of the double exchange interaction between Co
<sup>3+</sup>
and Co
<sup>4+</sup>
ions. The zero field cooled (ZFC) and field cooled (FC) magnetization curves at 50 mT show thermomagnetic irreversibility. At low temperatures, with increasing Na amount, the samples change from ferromagnetic-like behavior (x = 0, 0.05 and 0.1) to spin-glass one (X=0.15 and 0.2). The ferromagnetic-paramagnetic transition temperature decreases with increasing Na amount from 235 to 200 K (x = 0.1). The critical exponent value, associated to the spontaneous magnetization, increases with increasing Na amount from 0.37 for x = 0 to 0.57 for x = 0.1. The temperature dependence of the electrical resistivity reveals three different regimes as a function of Na content: (i) for x = 0, a metallic behavior is observed in the whole temperature range, (ii) for x = 0.05, a metal-semiconducting transition is observed around 80 K and (iii) for x≥0.1, we observe a semiconducting behavior in the whole temperature range. The parent compound (x = 0) exhibits a maximum entropy change |ΔS
<sup>MAX</sup>
<sub>M</sub>
| of 0.84 J kg
<sup>-1</sup>
K
<sup>-1</sup>
at 220 K in a magnetic applied field of2T. |ΔS
<sup>MAX</sup>
<sub>M</sub>
| decreases to 0.47 J kg
<sup>-1</sup>
K
<sup>-1</sup>
at 185 K forx = 0.1 in the same field magnitude. Well above Tc, |ΔS
<sup>MAX</sup>
<sub>M</sub>
| shows a linear dependence as a function of H
<sup>2</sup>
indicating the existence of spin fluctuations inside ferromagnetic clusters.</div>
</front>
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