磁场诱导的TmFeO<sub>3</sub>单晶

None Wang Ning, None Huang Feng, None Chen Ying, None Zhu Guofeng, None Su Haobin, None Guo Cuixia, None Wang Xiangfeng
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引用次数: 0

摘要

TmFeO< sub> 3 & lt; / sub>它具有磁光效应、多铁性和自旋取向等丰富的物理性质,在凝聚态物理和材料科学中具有重要的研究价值。在本研究中,我们利用时域太赫兹磁光光谱系统研究了TmFeO<sub>3</sub>在0-7 T外磁场作用下,温度为T=1.6 K的单晶。样品在光学浮区炉中生长,用钨靶背向反射Laue x射线照相法测定其晶体取向。测量装置为自建时域太赫兹磁光光谱系统,磁场范围为0-7 T,温度范围为1.6-300 K,光谱范围为0.2-2.0 THz。利用一对1mm厚的ZnTe非线性晶体,通过光学整流和电光采样技术产生和检测太赫兹信号。该系统的可变温度和磁场由超导磁体控制。实验中,线极化太赫兹波垂直入射样品表面,其磁分量H<sub>THz</sub>与样品表面平行。通过旋转样品,可以调节宏观磁矩M与H<sub>THz</sub>之间的角度q,实现两种模式的选择性激励,即q- afm模式q=0, q- fm模式q= 90°。太赫兹吸收光谱结果表明,随着磁场的增大,TmFeO<sub>3</sub>单晶向高频偏移,准反铁磁共振(q-AFM)在低临界磁场(2.2 ~ 3.6 T)向q-FM转变,通过磁结构分析和理论拟合,证实单晶磁矩经历了磁场诱导自旋重定向。本研究有助于更深入地了解外磁场和温度场共同作用下稀土铁氧体内部磁性结构的调控机制,以及相关自旋电子器件的开发。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Magnetic-Field-Induced Spin Reorientation in TmFeO<sub>3</sub> Single Crystals
TmFeO3 exhibits rich physical properties such as the magneto-optical effect, multiferroicity, and spin reorientation, making it of significant research value in condensed matter physics and materials science. In this study, we utilized a time-domain terahertz magneto-optical spectroscopy system to investigate the change in spin resonance frequency of TmFeO3 single crystals at T=1.6 K under external magnetic fields 0-7 T. The TmFeO3 sample was grown in an optical floating zone furnace and its crystallographic orientation was determined using back-reflection Laue X-ray photography with a tungsten target. The measurement setup is a self-built time-domain terahertz magneto-optical spectroscopy system, with a magnetic field range of 0-7 T, a temperature range of 1.6-300 K, and a spectral range of 0.2-2.0 THz. A pair of 1mm-thick ZnTe nonlinear crystals were used to generate and detect terahertz signals through optical rectification and electro-optic sampling techniques. The system's variable temperature and magnetic field are controlled by a superconducting magnet. In experiments, a linearly polarized terahertz wave is incident perpendicularly to the sample surface, and its magnetic component HTHz is parallel to the sample surface. By rotating the sample, the angle (q) between macroscopic magnetic moment M and HTHzcan be tuned, achieving selective excitations of the two modes, that is, q=0 for q-AFM mode or 90° for q-FM mode. Terahertz absorption spectroscopy results indicate that as the magnetic field increases, the quasi-ferromagnetic resonance (q-FM) of TmFeO3 single crystal shifts towards high frequencies, and quasi-antiferromagnetic resonance (q-AFM) transitions to q-FM at low critical magnetic fields (2.2-3.6 T). Through magnetic structure analysis and theoretical fitting, it is confirmed that the magnetic moment of the single crystal undergoes magnetic field induced spin reorientation. This study contributes to a deeper understanding of the regulatory mechanism of the internal magnetic structure of rare earth ferrite under the combined effects of external magnetic field and temperature field, and the development of related spin electronic devices.
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