Role of A Cation Vacancy in the Exchange-Biased LaFeO3 Multiferroic Nanocrystals

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作者
M. M. Arman
M. A. Ahmed
S. I. El-Dek
机构
[1] Cairo University,Materials Science Lab (1), Physics Department, Faculty of Science
[2] Beni-Suef University,Materials Science and Nanotechnology Department, Faculty of Postgraduate Studies for Advanced Sciences (PSAS)
关键词
Multiferroic; Magnetic; Ferroelectric; Exchange bias; Vacancy;
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摘要
Multiferroic samples with the chemical formula La1−x□x\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$_{1-x}\square _{x}$\end{document}FeO3 (0.0 ≤ x ≤ 0.03) were successfully prepared in nanoscale by citrate nitrate combustion method. XRD data reveals crystallized single-phase orthorhombic symmetry for the prepared nanopowder. All measured magnetic parameters point to the antiferromagnetic character with weak ferromagnetic moment. The value of the molar magnetic susceptibility (χM) for La0.99□0.01\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$_{\mathrm {0.99}}\square _{\mathrm {0.01}}$\end{document}FeO3 reaches 3.5 times that of the undoped sample. The saturation magnetization of the samples La0.99□0.01\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$_{\mathrm {0.99}}\square _{\mathrm {0.01}}$\end{document}FeO3 and La0.97□0.03\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$_{\mathrm {0.97}}\square _{\mathrm {0.03}}$\end{document}FeO3 increased two times as compared with that of the parent one. The exchange bias (EB) effect was observed for 1st time at room temperature and originated from antiferromagnetic–ferromagnetic (AFM-FM) interface effect. Ferroelectric hysteresis loop was observed at room temperature for the samples which highlighted the presence of the ferroelectric ordering. A huge enhancement in the saturation (Ps), the remnant polarization (Pr), and the coercive electric field (Ec) of the sample La0.98□0.02\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$_{\mathrm {0.98}}\square _{\mathrm {0.02}}$\end{document}FeO3 by 7.5, 24, and 12 times, respectively, when compared with the parent sample LaFeO3. Based on the obtained results, the investigated samples are categorized in type I multiferroics.
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页码:1867 / 1879
页数:12
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