The magnetoelectric properties of A- or B-site-doped PbVO3 films: A first-principles study

We employ first-principles calculations to study the magnetic and ferroelectric properties of PbVO3 with A (XA = Ca, Sr, Bi, Ba, and La) or B (XB = Ti, Cr, Mn, Fe, Co, Ni, and Cu) site dopants, with the aim of ascertaining a large ferroelectric polarization and a long magnetic order, or even a macro...

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Published in中国物理B:英文版 no. 8; pp. 641 - 647
Main Author 陈星源 陈丽娟 赵宇军
Format Journal Article
LanguageEnglish
Published 01.08.2013
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ISSN1674-1056
2058-3834
DOI10.1088/1674-1056/22/8/087703

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Summary:We employ first-principles calculations to study the magnetic and ferroelectric properties of PbVO3 with A (XA = Ca, Sr, Bi, Ba, and La) or B (XB = Ti, Cr, Mn, Fe, Co, Ni, and Cu) site dopants, with the aim of ascertaining a large ferroelectric polarization and a long magnetic order, or even a macro fen'i/ferromagnetism, which is critical to their potential applications in magnetoelectronic devices. It is found that PbTXAVsO24 (XA =Ca, Sr, and Ba,) are inclined to maintain the spin glass and large ferroelectric polarization. The degenerated G- and C-antiferromagnetic (AFM) couplings in the ideal PbVO3 are broken up, accompanied by the loss of ferroelectric properties, when La or Bi is doped at the A site. In contrast, the above-mentioned 3d transition elements doped at the B site of PbVO3 could induce remnant magnetic moments and preserve the large ferroelectric polarization, except for Ni and Cu. The Fe or Cr at the B site clearly remove the degenerated G- and C-AFM coupling, but the nonmagnetic Ti cannot do so. For the Mn, Co, Ni, or Cu doped at the B sites, even the two-dimensional AFM ordering in PbVO3 is destabilized. The various doping effects are further discussed with inner strain and charge transfer.
Bibliography:We employ first-principles calculations to study the magnetic and ferroelectric properties of PbVO3 with A (XA = Ca, Sr, Bi, Ba, and La) or B (XB = Ti, Cr, Mn, Fe, Co, Ni, and Cu) site dopants, with the aim of ascertaining a large ferroelectric polarization and a long magnetic order, or even a macro fen'i/ferromagnetism, which is critical to their potential applications in magnetoelectronic devices. It is found that PbTXAVsO24 (XA =Ca, Sr, and Ba,) are inclined to maintain the spin glass and large ferroelectric polarization. The degenerated G- and C-antiferromagnetic (AFM) couplings in the ideal PbVO3 are broken up, accompanied by the loss of ferroelectric properties, when La or Bi is doped at the A site. In contrast, the above-mentioned 3d transition elements doped at the B site of PbVO3 could induce remnant magnetic moments and preserve the large ferroelectric polarization, except for Ni and Cu. The Fe or Cr at the B site clearly remove the degenerated G- and C-AFM coupling, but the nonmagnetic Ti cannot do so. For the Mn, Co, Ni, or Cu doped at the B sites, even the two-dimensional AFM ordering in PbVO3 is destabilized. The various doping effects are further discussed with inner strain and charge transfer.
multiferroic, magnetism, ferroelectric, doping
11-5639/O4
Chen Xing-Yuan, Chen Li-Juan and Zhao Yu-Junt Department of Physics and State Key Laboratory of Luminescent Mate15als and Devices, South China University of Technology, Guangzhou 510640, China
ISSN:1674-1056
2058-3834
DOI:10.1088/1674-1056/22/8/087703