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Novel Dynamical Magnetoelectric Effects in Multiferroic BiFeO_3

机译:多铁性BiFeO_3中的新型动态磁电效应

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摘要

An atomistic effective Hamiltonian scheme is employed within molecular dynamics simulations to investigate how the electrical polarization and magnetization of the multiferroic BiFeO3 respond to time-dependent ac magnetic fields of various frequencies, as well as to reveal the frequency dependency of the dynamical (quadratic) magnetoelectric coefficient. We found the occurrence of vibrations having phonon frequencies in both the time dependency of the electrical polarization and magnetization (for any applied ac frequency), therefore making such vibrations of electromagnonic nature, when the homogeneous strain of the system is frozen (case 1). Moreover, the quadratic magnetoelectric coupling constant is monotonic and almost dispersionless in the sub-THz range in this case 1. In contrast, when the homogeneous strain can fully relax (case 2), two additional low-frequency and strain-mediated oscillations emerge in the time-dependent behavior of the polarization and magnetization, which result in resonances in the quadratic magnetoelectric coefficient. Such additional oscillations consist of a mixing between acoustic phonons, optical phonons, and magnons, and reflect the existence of a new quasiparticle that can be coined an "electroacoustic magnon." This latter finding can prompt experimentalists to shape their samples to take advantage of, and tune, the magnetostrictive-induced mechanical resonance frequency, in order to achieve large dynamical magnetoelectric couplings.
机译:在分子动力学模拟中采用了原子有效的哈密顿方案,以研究多铁性BiFeO3的电极化和磁化如何响应各种频率随时间变化的交流磁场,并揭示动态(二次)磁电的频率依赖性。系数。我们发现,声子频率的振动与电极化和磁化强度的时间相关(对于任何施加的交流频率),因此,当系统的均匀应变被冻结时,这种振动具有电磁性质(案例1)。此外,在这种情况1下,二次磁电耦合常数在亚THz范围内是单调的,几乎是无色散的。相反,当均匀应变可以完全弛豫时(情况2),在磁场中出现了另外两个低频振荡和应变介导的振荡。极化和磁化的时间相关行为,导致二次磁电系数发生共振。这种额外的振荡包括声子,光学声子和磁振子之间的混合,并反映了可以被称为“电声磁振子”的新准粒子的存在。后一个发现可以促使实验家们利用它们的样品来形成形状。为了实现大的动态磁电耦合,对磁致伸缩引起的机械共振频率进行调整。

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  • 来源
    《Physical review letters》 |2019年第9期|097601.1-097601.6|共6页
  • 作者单位

    Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA|Univ Arkansas, Inst Nanosci & Engn, Fayetteville, AR 72701 USA|Univ Arkansas, Microelect Photon Program, Fayetteville, AR 72701 USA;

    Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA|Univ Arkansas, Inst Nanosci & Engn, Fayetteville, AR 72701 USA|Soochow Univ, Sch Phys Sci & Technol, Suzhou 215006, Jiangsu, Peoples R China;

    Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA|Univ Arkansas, Inst Nanosci & Engn, Fayetteville, AR 72701 USA|Southern Fed Univ, Inst Phys, Rostov Na Donu 344090, Russia|Southern Fed Univ, Dept Phys, Rostov Na Donu 344090, Russia;

    Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA|Univ Arkansas, Inst Nanosci & Engn, Fayetteville, AR 72701 USA|Univ Paris Saclay, Lab Struct Proprietes & Modelisat Solides, Cent Supelec, CNRS UMR 8580, F-91190 Gif Sur Yvette, France;

    Univ Arkansas, Dept Phys, Fayetteville, AR 72701 USA|Univ Arkansas, Inst Nanosci & Engn, Fayetteville, AR 72701 USA;

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