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A-Site Cation Size Effect on Structure and Magnetic Properties of Sm(Eu,Gd)Cr 0.2 Mn 0.2 Fe 0.2 Co 0.2 Ni 0.2 O 3 High-Entropy Solid Solutions.

Denis A VinnikVladimir E ZhivulinEvgeny A TrofimovSvetlana A GudkovaAlexander Yu PundaAzalia N ValiulinaMaksim GavrilyakOlga V ZaitsevaSergey V TaskaevMayeen Uddin KhandakerAmal AlqahtaniDavid A BradleyMohammad Ibrahim AbualsayedVitaliy A TurchenkoAlexey V TrukhanovSergei V Trukhanov
Published in: Nanomaterials (Basel, Switzerland) (2021)
Three high-entropy Sm(Eu,Gd)Cr 0.2 Mn 0.2 Fe 0.2 Co 0.2 Ni 0.2 O 3 perovskite solid solutions were synthesized using the usual ceramic technology. The XRD investigation at room temperature established a single-phase perovskite product. The Rietveld refinement with the FullProf computer program in the frame of the orthorhombic Pnma (No 62) space group was realized. Along with a decrease in the V unit cell volume from ~224.33 Å 3 for the Sm-based sample down to ~221.52 Å 3 for the Gd-based sample, an opposite tendency was observed for the unit cell parameters as the ordinal number of the rare-earth cation increased. The average grain size was in the range of 5-8 μm. Field magnetization was measured up to 30 kOe at 50 K and 300 K. The law of approach to saturation was used to determine the M s spontaneous magnetization that nonlinearly increased from ~1.89 emu/g (Sm) up to ~17.49 emu/g (Gd) and from ~0.59 emu/g (Sm) up to ~3.16 emu/g (Gd) at 50 K and 300 K, respectively. The M r residual magnetization and H c coercive force were also determined, while the SQR loop squareness, k magnetic crystallographic anisotropy coefficient, and H a anisotropy field were calculated. Temperature magnetization was measured in a field of 30 kOe. ZFC and FC magnetization curves were fixed in a field of 100 Oe. It was discovered that the T mo magnetic ordering temperature downward-curve decreased from ~137.98 K (Sm) down to ~133.99 K (Gd). The spin glass state with ferromagnetic nanoinclusions for all the samples was observed. The <D> average and D max maximum diameter of ferromagnetic nanoinclusions were calculated and they were in the range of 40-50 nm and 160-180 nm, respectively. The mechanism of magnetic state formation is discussed in terms of the effects of the A-site cation size and B-site poly-substitution on the indirect superexchange interactions.
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