...
首页> 外文期刊>Physical review, B >Electromagnon excitation in the field-induced noncollinear ferrimagnetic phase of Ba2Mg2Fe12O22 studied by polarized inelastic neutron scattering and terahertz time-domain optical spectroscopy
【24h】

Electromagnon excitation in the field-induced noncollinear ferrimagnetic phase of Ba2Mg2Fe12O22 studied by polarized inelastic neutron scattering and terahertz time-domain optical spectroscopy

机译:极化非弹性中子散射和太赫兹时域光谱学研究Ba2Mg2Fe12O22场致非共线亚铁磁性相中的电子磁振激发

获取原文
获取原文并翻译 | 示例
           

摘要

We have studied magnetic excitations in a field-induced noncollinear commensurate ferrimagnetic phase of Ba2Mg2Fe12O22 by means of polarized inelastic neutron scattering (PINS) and terahertz (THz) time-domain optical spectroscopy under magnetic field. A previous THz spectroscopy study reported that the field-induced phase exhibits electric-dipole-active excitations with energies of around 5 meV [Kida et al., Phys. Rev. B 83, 064422 (2011)]. In the present PINS measurements, we observed inelastic scattering signals around 5 meV at the zone center in the spin-flip channel. This directly shows that the electric-dipole-active excitations are indeed of magnetic origin, that is, electromagnons. In addition, the present THz spectroscopy confirms that the excitations have oscillating electric polarization parallel to the c axis. In terms of the spin-current model (Katsura-Nagaosa-Balatsky model), the noncollinear magnetic order in the field-induced phase can induce static electric polarization perpendicular to the c axis, but not dynamic electric polarization along the c axis. We suggest that the electromagnon excitations can be explained by applying the magnetostriction model to the out-of-phase oscillations of the magnetic moments, which is deduced from the present experimental results.
机译:我们已经通过极化非弹性中子散射(PINS)和太赫兹(THz)时域光谱在磁场下研究了Ba2Mg2Fe12O22场致非共线相称亚铁磁性相中的磁激发。先前的THz光谱研究报告说,场感应相表现出的电偶极子激发的能量约为5 meV [Kida等,Phys。 B 83,064422(2011)。在当前的PINS测量中,我们在自旋翻转通道的区域中心观察到了大约5 meV的非弹性散射信号。这直接表明,电偶极子激发确实是由磁性引起的,即电磁子。另外,当前的太赫兹光谱证实了激发具有平行于c轴的振荡电极化。就自旋电流模型(Katsura-Nagaosa-Balatsky模型)而言,场感应相中的非共线磁阶可以感应垂直于c轴的静态电极化,但不能沿c轴感应动态电极化。我们建议,可以通过将磁致伸缩模型应用于磁矩的异相振荡来解释电磁振子的激发,这是根据目前的实验结果推导出来的。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号