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 language | English |
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Pages (from-to) | 497-501 |
Number of pages | 5 |
Journal | Nature |
Volume | 572 |
Issue number | 7770 |
DOIs | |
State | Published - 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.
Funders | Funder number |
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National Program for Support of Top-notch Young Professionals | |
Research Grants Council of Hong Kong Special Administrative Region | 17303518P, 11622429 |
State of Washington | |
US Department of Energy | |
National Science Foundation | 1708419 |
U.S. Department of Energy | |
Office of Science | |
Basic Energy Sciences | |
Clean Energy Institute | |
Division of Materials Sciences and Engineering | DE-SC0012509, NSF-DMR-1708419 |
National Natural Science Foundation of China | 11427902 |
Fudan University | |
National Basic Research Program of China (973 Program) | 2014CB921601, 2016YFA0301002 |