Differences between the multiferroic properties of hexagonal and orthorhombic ion-doped YFeO3 nanoparticles

被引:2
作者
Apostolov, A. T. [1 ]
Apostolova, I. N. [2 ]
Wesselinowa, J. M. [3 ]
机构
[1] Univ Architecture Civil Engn & Geodesy, Hristo Smirnenski Blvd 1, Sofia 1046, Bulgaria
[2] Univ Forestry, Kl Ohridski Blvd 10, Sofia 1756, Bulgaria
[3] Univ Sofia, J Bourchier Blvd 5, Sofia 1164, Bulgaria
来源
INTERNATIONAL JOURNAL OF MODERN PHYSICS B | 2023年 / 37卷 / 21期
关键词
h- and o-YFeO3 nanoparticles; ion doping; magnetization; bandgap; polarization; dielectric constant; microscopic model; DIELECTRIC-PROPERTIES; MAGNETIC-PROPERTIES; OPTICAL-PROPERTIES; NANOCRYSTALLINE; PEROVSKITE; ORIGIN; PURE;
D O I
10.1142/S0217979223502016
中图分类号
O59 [应用物理学];
学科分类号
摘要
The multiferroic properties of ion-doped hexagonal and orthorhombic YFeO3 (YFO) nanoparticles (NPs) are studied theoretically. The magnetization M-s in h-YFO NPs increases, whereas for o-YFO NPs it decreases with decreasing NP size. In the dielectric constant (DC) both h- and o-YFO have a peak around T-C1 similar to 450 and 460 K, respectively, but only in h-YFO an anomaly appears at T-C2 similar to 300 K in the DC and the polarization which could be connected with a possible P6(3)mc-P63cm phase transition. The polarization in pure and Bi-doped o-YFO NPs increases with increasing magnetic field. M-s(x) is studied by doping of a o-YFO NP with Ti4+ ions at the octahedral Fe3+ sites. M-s(T) in undoped YFO shows a small kink at TC1 similar to 450 K, whereas in the doped YFO it shows at similar to 480 K. By different ion doping on the Y or Fe sites in YFO there is a transformation from the h- to the o-phase or vice versa. In M-n-doped o-YFO a spin-reorientation transition appears. The bandgap of h-YFO is smaller compared to that of o-YFO.
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页数:13
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