Giant nonreciprocal second-harmonic generation from antiferromagnetic bilayer CrI<sub>3</sub>.

Sun, Zeyuan; Yi, Yangfan; Song, Tiancheng; Clark, Genevieve; Huang, Bevin; Shan, Yuwei; Wu, Shuang; Huang, Di et al. · Nature · 2019

basic_science · Level V

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Abstract

Layered antiferromagnetism is the spatial arrangement of ferromagnetic layers with antiferromagnetic interlayer coupling. The van der Waals magnet chromium triiodide (CrI<sub>3</sub>) has been shown to be a layered antiferromagnetic insulator in its few-layer form<sup>1</sup>, opening up opportunities for various functionalities<sup>2-7</sup> in electronic and optical devices. Here we report an emergent nonreciprocal second-order nonlinear optical effect in bilayer CrI<sub>3</sub>. The observed second-harmonic generation (SHG; a nonlinear optical process that converts two photons of the same frequency into one photon of twice the fundamental frequency) is several orders of magnitude larger than known magnetization-induced SHG<sup>8-11</sup> and comparable to the SHG of the best (in terms of nonlinear susceptibility) two-dimensional nonlinear optical materials studied so far<sup>12,13</sup> (for example, molybdenum disulfide). We show that although the parent lattice of bilayer CrI<sub>3</sub> is centrosymmetric, and thus does not contribute to the SHG signal, the observed giant nonreciprocal SHG originates only from the layered antiferromagnetic order, which breaks both the spatial-inversion symmetry and the time-reversal symmetry. Furthermore, polarization-resolved measurements reveal underlying C<sub>2h</sub> crystallographic symmetry-and thus monoclinic stacking order-in bilayer CrI<sub>3</sub>, providing key structural information for the microscopic origin of layered antiferromagnetism<sup>14-18</sup>. Our results indicate that SHG is a highly sensitive probe of subtle magnetic orders and open up possibilities for the use of two-dimensional magnets in nonlinear and nonreciprocal optical devices.