论文标题
在分层的抗fiferromagnet FEPS $ _3 $的高压调节
High pressure tuning of magnon-polarons in the layered antiferromagnet FePS$_3$
论文作者
论文摘要
磁性分层材料最近成为有前途的系统,可以在基于二维(2D)材料的结构中引入磁性,并在2D极限中研究外来磁接地态。在这项工作中,我们将高的静水压力施加到散装分层的抗fiferromagnet Feps $ _3 $上,以与磁激励(镁质)共鸣,以收集集体晶格激发(声子)。 Close to P = 4 GPa, the magnon-phonon resonance is achieved and the strong coupling between these collective modes leads to the formation of new quasi-particles, the magnon-polarons, evidenced in our low temperature Raman scattering experiments by a particular avoided crossing behavior between the phonon and the doubly degenerate antiferromagnetic magnon.在压力诱导的磁通共振下,出现了三种不同的耦合模式。由于它主要由内层特性定义,因此我们表明磁通的能量几乎与压力无关。另外,我们将高达B = 30 T的高磁场应用以充分识别和表征镁激发,并探索声子具有低于磁子的能量低,等于或更高的磁子的不同磁杆 - 果态。我们的实验数据的描述需要在实际计算中引入声子轴耦合。
Magnetic layered materials have emerged recently as promising systems to introduce magnetism in structures based on two-dimensional (2D) materials and to investigate exotic magnetic ground states in the 2D limit. In this work, we apply high hydrostatic pressures up to P = 8.7 GPa to the bulk layered antiferromagnet FePS$_3$ to tune the collective lattice excitations (phonons) in resonance with magnetic excitations (magnons). Close to P = 4 GPa, the magnon-phonon resonance is achieved and the strong coupling between these collective modes leads to the formation of new quasi-particles, the magnon-polarons, evidenced in our low temperature Raman scattering experiments by a particular avoided crossing behavior between the phonon and the doubly degenerate antiferromagnetic magnon. At the pressure-induced magnon-phonon resonance, three distinct coupled modes emerge. As it is mainly defined by intralayer properties, we show that the energy of the magnon is nearly pressure independent. We additionally apply high magnetic fields up to B = 30 T to fully identify and characterize the magnon excitations, and to explore the different magnon-polaron regimes for which the phonon has an energy lower-, equal to-, or higher- than the magnon energy. The description of our experimental data requires introducing a phonon-phonon coupling not taken into account in actual calculations.