Huang Bevin, Cenker John, Zhang Xiaoou, Ray Essance L, Song Tiancheng, Taniguchi Takashi, Watanabe Kenji, McGuire Michael A, Xiao Di, Xu Xiaodong
Department of Physics, University of Washington, Seattle, WA, USA.
Department of Physics, Carnegie Mellon University, Pittsburgh, PA, USA.
Nat Nanotechnol. 2020 Mar;15(3):212-216. doi: 10.1038/s41565-019-0598-4. Epub 2020 Jan 6.
The coupling between spin and charge degrees of freedom in a crystal gives rise to magneto-optical effects with applications in the sensitive detection of local magnetic order, optical modulation and data storage. In two-dimensional magnets these effects manifest themselves in the large magneto-optical Kerr effect, spontaneous helical light emission from ferromagnetic (FM) monolayers and electric-field induced Kerr rotation and giant second-order non-reciprocal optical effects in antiferromagnetic (AFM) bilayers. Here we demonstrate the tuning of inelastically scattered light through symmetry control in atomically thin chromium triiodide (CrI). In monolayers, we found an extraordinarily large magneto-optical Raman effect from an A phonon mode due to the emergence of FM order. The linearly polarized, inelastically scattered light rotates by ~40°, more than two orders of magnitude larger than the rotation from the magneto-optical Kerr effect under the same experimental conditions. In CrI bilayers, the same phonon mode becomes Davydov-split into two modes of opposite parity, which exhibit divergent selection rules that depend on inversion symmetry and the underlying magnetic order. We demonstrate the magneto-electrical control over these selection rules by activating or suppressing Raman activity for the odd-parity phonon mode and the magneto-optical rotation of scattered light from the even-parity phonon mode. Our work underlines the unique opportunities provided by two-dimensional magnets to control the combined time-reversal and inversion symmetries to manipulate Raman optical selection rules and for exploring emergent magneto-optical effects and spin-phonon coupled physics.
晶体中自旋与电荷自由度之间的耦合会产生磁光效应,这些效应可应用于局部磁序的灵敏检测、光调制和数据存储。在二维磁体中,这些效应表现为大磁光克尔效应、铁磁(FM)单层的自发螺旋光发射以及反铁磁(AFM)双层中的电场诱导克尔旋转和巨大的二阶非互易光学效应。在此,我们展示了通过对原子级薄的三碘化铬(CrI)进行对称性控制来调节非弹性散射光。在单层中,由于FM序的出现,我们从一个A声子模式中发现了异常大的磁光拉曼效应。线偏振的非弹性散射光旋转了约40°,比在相同实验条件下磁光克尔效应引起的旋转大两个数量级以上。在CrI双层中,相同的声子模式发生达维多夫分裂,成为两个具有相反宇称的模式,它们表现出依赖于空间反演对称性和底层磁序的不同选择定则。我们通过激活或抑制奇宇称声子模式的拉曼活性以及偶宇称声子模式散射光的磁光旋转,展示了对这些选择定则的磁电控制。我们的工作强调了二维磁体提供的独特机会,即控制时间反演对称性和空间反演对称性的组合,以操纵拉曼光学选择定则,并探索新兴的磁光效应和自旋 - 声子耦合物理。