Giant nonreciprocal second-harmonic generation from antiferromagnetic bilayer CrI3

Zeyuan Sun, Yangfan Yi, Tiancheng Song, Genevieve Clark, Bevin Huang, Yuwei Shan, Shuang Wu, Di Huang, Chunlei Gao, Zhanghai Chen, Michael McGuire, Ting Cao, Di Xiao, Wei Tao Liu, Wang Yao, Xiaodong Xu, Shiwei Wu

Research output: Contribution to journalArticlepeer-review

363 Scopus citations

Abstract

Layered antiferromagnetism is the spatial arrangement of ferromagnetic layers with antiferromagnetic interlayer coupling. The van der Waals magnet chromium triiodide (CrI3) has been shown to be a layered antiferromagnetic insulator in its few-layer form1, opening up opportunities for various functionalities2–7 in electronic and optical devices. Here we report an emergent nonreciprocal second-order nonlinear optical effect in bilayer CrI3. 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 SHG8–11 and comparable to the SHG of the best (in terms of nonlinear susceptibility) two-dimensional nonlinear optical materials studied so far12,13 (for example, molybdenum disulfide). We show that although the parent lattice of bilayer CrI3 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 C2h crystallographic symmetry—and thus monoclinic stacking order—in bilayer CrI3, providing key structural information for the microscopic origin of layered antiferromagnetism14–18. 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.

Original languageEnglish
Pages (from-to)497-501
Number of pages5
JournalNature
Volume572
Issue number7770
DOIs
StatePublished - Aug 22 2019

Funding

Acknowledgements We thank Y.-R. Shen for discussions and W. Han for providing the Cr2O3 crystals. The work at Fudan University was supported by the National Natural Science Foundation of China (11427902), the National Basic Research Program of China (2014CB921601) and the National Key Research and Development Program of China (2016YFA0301002). The work at the University of Washington and Carnegie Mellon University was mainly supported by the Department of Energy, Basic Energy Sciences, Materials Sciences and Engineering Division (DE-SC0012509). Device fabrication was partially supported by NSF-DMR-1708419. X.X. acknowledges support from the Clean Energy Institute (funded by the State of Washington) and from a Boeing Distinguished Professorship in Physics. Crystal growth at Oak Ridge National Laboratory was supported by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. W.Y. acknowledges support from the Research Grants Council of Hong Kong Special Administrative Region (17303518P). W.-T.L. acknowledges support from the National Natural Science Foundation of China (11622429), the National Program for Support of Top-Notch Young Professionals and the Shu Guang Program.

FundersFunder number
National Program for Support of Top-notch Young Professionals
Research Grants Council of Hong Kong Special Administrative Region17303518P, 11622429
State of Washington
US Department of Energy
National Science Foundation1708419
U.S. Department of Energy
Office of Science
Basic Energy Sciences
Clean Energy Institute
Division of Materials Sciences and EngineeringDE-SC0012509, NSF-DMR-1708419
National Natural Science Foundation of China11427902
Fudan University
National Basic Research Program of China (973 Program)2014CB921601, 2016YFA0301002

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