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Microwave response of the chiral helimagnetic MnNb_3S_6

机译:手性直升机MNNB_3S_6的微波反应

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摘要

Chiral magnetic soliton (CMS), an isolated topological kink consisting of spins, has potential applications in spintronics. In this work, the microwave response of layered MnNb_3S_6, which is suggested as a candidate for CMS, is investigated by the electronic spin resonance (ESR). Angle-dependent ESR spectra show that the microwave response is strong for H⊥c while it is weak for H//c, where c is the c-axis of the single crystal. When H⊥c, two resonance lines are observed, which are marked as H_(r1) for the higher field and H_(r2) for the lower field. It is determined that H_(r1) originates from the ferromagnetic resonance of forced ferromagnetic moments, which evolves into paramagnetic resonance above T_c. Meanwhile, H(r2) existing only below T_c fulfills the Goldstone excitation of CMS. The microwave response of MnNb_3S_6 supports the existence of CMS in MnNb_3S_6, and is proved to be an effective means for modulating and investigating CMS.
机译:手性磁性孤子(CMS),由旋转组成的隔离拓扑扭结,具有闪光灯的潜在应用。在这项工作中,通过电子旋转共振(ESR)研究了分层MNNB_3S_6的微波响应,其被提出为CMS的候选者。角度依赖的ESR光谱表明,对于H⊥C,微波响应对于H = H // C弱,其中C是单晶的C轴。当H⊥C时,观察到两个共振线,其标记为下场的高场和H_(R2)的H_(R1)。确定H_(R1)起源于强制铁磁性矩的铁磁共振,这在T_C中发展成顺磁共振。同时,仅存在于T_C的H(R2)满足CMS的Goldstone激励。 MNNB_3S_6的微波响应支持MNNB_3S_6中的CMS存在,并且被证明是用于调制和调查CMS的有效手段。

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  • 来源
    《Applied Physics Letters》 |2020年第2期|022410.1-022410.4|共4页
  • 作者单位

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China State Key Laboratory of Advanced Special Steel Shanghai University Shanghai 200444 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China University of Science and Technology of China Hefei 230026 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China University of Science and Technology of China Hefei 230026 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China University of Science and Technology of China Hefei 230026 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China University of Science and Technology of China Hefei 230026 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China Hefei National Laboratory for Physical Sciences at the Microscale University of Science and Technology of China Hefei 230026 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China State Key Laboratory of Advanced Special Steel Shanghai University Shanghai 200444 China;

    Anhui Key Laboratory of Condensed Matter Physics at Extreme Conditions High Magnetic Field Laboratory Chinese Academy of Sciences Hefei 230031 China Hefei National Laboratory for Physical Sciences at the Microscale University of Science and Technology of China Hefei 230026 China;

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