Dynamically induced magnetism in KTaO3

被引:29
|
作者
Geilhufe, R. Matthias [1 ,2 ]
Juricic, Vladimir [1 ,2 ,3 ]
Bonetti, Stefano [4 ,5 ]
Zhu, Jian-Xin [6 ,7 ]
Balatsky, Alexander, V [1 ,2 ,8 ,9 ]
机构
[1] KTH Royal Inst Technol, NORDITA, Roslagstullsbacken 23, S-10691 Stockholm, Sweden
[2] Stockholm Univ, Roslagstullsbacken 23, S-10691 Stockholm, Sweden
[3] Univ Tecn Federico Santa Maria, Dept Fis, Casilla 110, Valparaiso, Chile
[4] Stockholm Univ, Dept Phys, S-10691 Stockholm, Sweden
[5] Ca Foscari Univ Venice, Dept Mol Sci & Nanosyst, I-30172 Venice, Italy
[6] Los Alamos Natl Lab, Theoret Div, Los Alamos, NM 87545 USA
[7] Los Alamos Natl Lab, Ctr Integrated Nanotechnol, Los Alamos, NM 87545 USA
[8] Univ Connecticut, Dept Phys, Storrs, CT 06269 USA
[9] Univ Connecticut, Inst Mat Sci, Storrs, CT 06269 USA
来源
PHYSICAL REVIEW RESEARCH | 2021年 / 3卷 / 02期
基金
瑞典研究理事会; 欧洲研究理事会;
关键词
PHASE-TRANSITION; PHONON;
D O I
10.1103/PhysRevResearch.3.L022011
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Dynamical multiferroicity features entangled dynamic orders: fluctuating electric dipoles induce magnetization. Hence, the material with paraelectric fluctuations can develop magnetic signatures if dynamically driven. We identify the paraelectric KTaO3 (KTO) as a prime candidate for the observation of the dynamical multiferroicity. We show that when a KTO sample is exposed to a circularly polarized laser pulse, the dynamically induced ionic magnetic moments are of the order of 5% of the nuclear magneton per unit cell. We determine the phonon spectrum using ab initio methods, and we identify T-1u as relevant phonon modes that couple to the external field and induce magnetic polarization. We also predict a corresponding electron effect for the dynamically induced magnetic moment, which is enhanced by several orders of magnitude due to the significant mass difference between electron and ionic nucleus.
引用
收藏
页数:5
相关论文
共 50 条
  • [41] Striped electron fluid on (111) KTaO3
    Arribi, P. Villar
    Paramekanti, A.
    Norman, M. R.
    PHYSICAL REVIEW B, 2021, 103 (03)
  • [42] THE HYPER-RAMAN SPECTRUM OF KTAO3
    UWE, H
    VOGT, H
    FERROELECTRICS, 1984, 55 (1-4) : 755 - 758
  • [43] Thermoluminescence of nominally pure KTaO3 crystals
    Potucek, Z
    Bryknar, Z
    Schulz, HJ
    RADIATION EFFECTS AND DEFECTS IN SOLIDS, 2002, 157 (6-12): : 1021 - 1024
  • [44] Electric-field-induced orientation of iron tetragonal centers in KTaO3
    Sochava, LS
    Bursian, VÉ
    Razdobarin, AG
    PHYSICS OF THE SOLID STATE, 2000, 42 (09) : 1640 - 1642
  • [45] FE-3+ AXIAL CENTERS IN KTAO3
    LAGUTA, VV
    GLINCHUK, MD
    KARMAZIN, AA
    BYKOV, IP
    SYRNIKOV, PP
    FIZIKA TVERDOGO TELA, 1985, 27 (07): : 2211 - 2214
  • [46] Electron density and atomic displacements in KTaO3
    Zhurova, EA
    Ivanov, Y
    Zavodnik, V
    Tsirelson, V
    ACTA CRYSTALLOGRAPHICA SECTION B-STRUCTURAL SCIENCE CRYSTAL ENGINEERING AND MATERIALS, 2000, 56 : 594 - 600
  • [47] SURFACE BARRIER DIODES ON SEMICONDUCTING KTAO3
    WEMPLE, SH
    KAHNG, D
    BRAUN, HJ
    JOURNAL OF APPLIED PHYSICS, 1967, 38 (01) : 353 - &
  • [48] FIELD-INDUCED SPLITTING OF THE OH-STRETCH ABSORPTION-LINE IN KTAO3 AND KTAO3LI
    JOVANOVIC, A
    WOHLECKE, M
    KAPPHAN, S
    RADIATION EFFECTS AND DEFECTS IN SOLIDS, 1991, 119 : 785 - 790
  • [49] AnomalousMetallicStateDrivenbyMagneticFieldattheLaAlO3/KTaO3(111)Interface
    张子涛
    乔宇杰
    邵婷娜
    赵强
    陈星宇
    陈美慧
    朱芳慧
    窦瑞芬
    刘海文
    熊昌民
    聂家财
    Chinese Physics Letters, 2023, 40 (03) : 52 - 59
  • [50] RHOMBIC FE-3+ CENTERS IN KTAO3
    PECHENYI, AP
    GLINCHUK, MD
    ANTIMIROVA, TV
    KLEEMANN, W
    PHYSICA STATUS SOLIDI B-BASIC RESEARCH, 1992, 174 (02): : 325 - 333