论文标题
在2D磁铁ERBR3中的狄拉克点处的偶极自旋波和可调频带隙
Dipolar spin-waves and tunable band gap at the Dirac points in the 2D magnet ErBr3
论文作者
论文摘要
拓扑镁绝缘子构成了一个不断增长的研究领域,因为它们的潜在用作信息载体而无需散热。我们报告了磁态和范围二维蜂窝磁铁ERBR3中磁化态和激发的实验和理论研究。我们表明,该化合物的磁性完全由偶极相互作用控制,偶极相互作用会在蜂窝状晶格上连续退化,并在平面上旋转旋转。我们发现,当地面中的磁矩与单层石墨烯中与浆果相πas相关的时间反转和反转对称性相关时,镁色散表现出类似狄拉克的锥。当偶极子从该状态旋转时,一个镁带隙会打开,在K和K'DIRAC点附近需要有限的浆果曲率。我们的结果表明,蜂窝晶格上偶极子的自旋分散体可以从带有狄拉克锥的磁相转化为具有非平凡山谷Chern号的拓扑抗铁磁绝缘子。
Topological magnon insulators constitute a growing field of research for their potential use as information carriers without heat dissipation. We report an experimental and theoretical study of the magnetic ground-state and excitations in the van der Waals two-dimensional honeycomb magnet ErBr3. We show that the magnetic properties of this compound are entirely governed by the dipolar interactions which generate a continuously degenerate non-collinear ground-state on the honeycomb lattice with spins confined in the plane. We find that the magnon dispersion exhibits Dirac-like cones when the magnetic moments in the ground-state are related by time-reversal and inversion symmetries associated with a Berry phase πas in single-layer graphene. A magnon band gap opens when the dipoles are rotated away from this state, entailing a finite Berry curvature in the vicinity of the K and K' Dirac points. Our results illustrate that the spin-wave dispersion of dipoles on the honeycomb lattice can be reversibly controlled from a magnetic phase with Dirac cones to a topological antiferromagnetic insulator with non-trivial valley Chern number.