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氧化镍(II)中的相互自旋-声子驱动效应和声子本征向量重整化

Mutual spin-phonon driving effects and phonon eigenvector renormalization in nickel (II) oxide.

作者信息

Sun Qiyang, Wei Bin, Su Yaokun, Smith Hillary, Lin Jiao Y Y, Abernathy Douglas L, Li Chen

机构信息

Department of Mechanical Engineering, University of California, Riverside, CA 92521.

Henan Key Laboratory of Materials on Deep-Earth Engineering, School of Materials Science and Engineering, Henan Polytechnic University, Jiaozuo 454000, China.

出版信息

Proc Natl Acad Sci U S A. 2022 Jul 19;119(29):e2120553119. doi: 10.1073/pnas.2120553119. Epub 2022 Jul 12.

Abstract

The physics of mutual interaction of phonon quasiparticles with electronic spin degrees of freedom, leading to unusual transport phenomena of spin and heat, has been a subject of continuing interests for decades. Despite its pivotal role in transport processes, the effect of spin-phonon coupling on the phonon system, especially acoustic phonon properties, has so far been elusive. By means of inelastic neutron scattering and first-principles calculations, anomalous scattering spectral intensity from acoustic phonons was identified in the exemplary collinear antiferromagnetic nickel (II) oxide, unveiling strong spin-lattice correlations that renormalize the polarization of acoustic phonon. In particular, a clear magnetic scattering signature of the measured neutron scattering intensity from acoustic phonons is demonstrated by its momentum transfer and temperature dependences. The anomalous scattering intensity is successfully modeled with a modified magneto-vibrational scattering cross-section, suggesting the presence of spin precession driven by phonon. The renormalization of phonon eigenvector is indicated by the observed "geometry-forbidden" neutron scattering intensity from transverse acoustic phonon. Importantly, the eigenvector renormalization cannot be explained by magnetostriction but instead, it could result from the coupling between phonon and local magnetization of ions.

摘要

声子准粒子与电子自旋自由度的相互作用物理,导致了自旋和热的异常输运现象,几十年来一直是人们持续关注的课题。尽管自旋 - 声子耦合在输运过程中起着关键作用,但迄今为止,其对声子系统,特别是声学声子性质的影响仍不明确。通过非弹性中子散射和第一性原理计算,在典型的共线反铁磁氧化镍(II)中发现了声学声子的反常散射谱强度,揭示了使声学声子极化重整化的强自旋 - 晶格相关性。特别是,通过其动量转移和温度依赖性,证明了从声学声子测量的中子散射强度具有明显的磁散射特征。利用修正的磁振散射截面成功地模拟了反常散射强度,表明存在由声子驱动的自旋进动。从横向声学声子观察到的“几何禁戒”中子散射强度表明了声子本征矢量的重整化。重要的是,本征矢量重整化不能用磁致伸缩来解释,相反,它可能是由声子与离子的局部磁化之间的耦合引起的。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5946/9304033/a667f9a28a8e/pnas.2120553119fig01.jpg

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