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反铁磁RuO₂中的手性磁振子

Chiral Magnons in Altermagnetic RuO_{2}.

作者信息

Šmejkal Libor, Marmodoro Alberto, Ahn Kyo-Hoon, González-Hernández Rafael, Turek Ilja, Mankovsky Sergiy, Ebert Hubert, D'Souza Sunil W, Šipr Ondřej, Sinova Jairo, Jungwirth Tomáš

机构信息

Institut für Physik, Johannes Gutenberg Universität Mainz, D-55099 Mainz, Germany.

Institute of Physics, Czech Academy of Sciences, Cukrovarnická 10, 162 00 Praha 6, Czech Republic.

出版信息

Phys Rev Lett. 2023 Dec 22;131(25):256703. doi: 10.1103/PhysRevLett.131.256703.

Abstract

Magnons in ferromagnets have one chirality, and typically are in the GHz range and have a quadratic dispersion near the zero wave vector. In contrast, magnons in antiferromagnets are commonly considered to have bands with both chiralities that are degenerate across the entire Brillouin zone, and to be in the THz range and to have a linear dispersion near the center of the Brillouin zone. Here we theoretically demonstrate a new class of magnons on a prototypical d-wave altermagnet RuO_{2} with the compensated antiparallel magnetic order in the ground state. Based on density-functional-theory calculations we observe that the THz-range magnon bands in RuO_{2} have an alternating chirality splitting, similar to the alternating spin splitting of the electronic bands, and a linear magnon dispersion near the zero wave vector. We also show that, overall, the Landau damping of this metallic altermagnet is suppressed due to the spin-split electronic structure, as compared to an artificial antiferromagnetic phase of the same RuO_{2} crystal with spin-degenerate electronic bands and chirality-degenerate magnon bands.

摘要

铁磁体中的磁振子具有一种手性,通常处于吉赫兹频率范围,并且在零波矢附近具有二次色散。相比之下,反铁磁体中的磁振子通常被认为具有在整个布里渊区简并的两种手性的能带,处于太赫兹频率范围,并且在布里渊区中心附近具有线性色散。在此,我们从理论上证明了在一种具有基态补偿反平行磁序的典型d波交替磁体RuO₂上存在一类新型磁振子。基于密度泛函理论计算,我们观察到RuO₂中太赫兹频率范围的磁振子能带具有交替的手性分裂,类似于电子能带的交替自旋分裂,并且在零波矢附近具有线性磁振子色散。我们还表明,总体而言,与具有自旋简并电子能带和手性简并磁振子能带的相同RuO₂晶体的人工反铁磁相相比,这种金属交替磁体的朗道阻尼由于自旋分裂的电子结构而受到抑制。

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