Ligand-field helical luminescence in a 2D ferromagnetic insulator

Kyle L. Seyler, Ding Zhong, Dahlia R. Klein, Shiyuan Gao, Xiaoou Zhang, Bevin Huang, Efrén Navarro-Moratalla, Li Yang, David H. Cobden, Michael A. McGuire, Wang Yao, Di Xiao, Pablo Jarillo-Herrero, Xiaodong Xu

Research output: Contribution to journalArticlepeer-review

292 Scopus citations

Abstract

Bulk chromium tri-iodide (CrI 3 ) has long been known as a layered van der Waals ferromagnet 1 . However, its monolayer form was only recently isolated and confirmed to be a truly two-dimensional (2D) ferromagnet 2 , providing a new platform for investigating light-matter interactions and magneto-optical phenomena in the atomically thin limit. Here, we report spontaneous circularly polarized photoluminescence in monolayer CrI 3 under linearly polarized excitation, with helicity determined by the monolayer magnetization direction. In contrast, the bilayer CrI 3 photoluminescence exhibits vanishing circular polarization, supporting the recently uncovered anomalous antiferromagnetic interlayer coupling in CrI 3 bilayers 2 . Distinct from the Wannier-Mott excitons that dominate the optical response in well-known 2D van der Waals semiconductors 3 , our absorption and layer-dependent photoluminescence measurements reveal the importance of ligand-field and charge-transfer transitions to the optoelectronic response of atomically thin CrI 3 . We attribute the photoluminescence to a parity-forbidden d-d transition characteristic of Cr 3+ complexes, which displays broad linewidth due to strong vibronic coupling and thickness-independent peak energy due to its localized molecular orbital nature.

Original languageEnglish
Pages (from-to)277-281
Number of pages5
JournalNature Physics
Volume14
Issue number3
DOIs
StatePublished - Mar 1 2018

Funding

The authors thank D. Gamelin for insightful discussions on the optical response of CrI3, and A. Majumdar for testing the measurement system. Work at the University of Washington was mainly supported by the Department of Energy, Basic Energy Sciences, Materials Sciences and Engineering Division (DE-SC0018171), and University of Washington Innovation Award. Work at MIT has been supported by the Center for Integrated Quantum Materials under NSF grant DMR-1231319 as well as the Gordon and Betty Moore Foundation’s EPiQS Initiative through Grant GBMF4541 to P.J.-H. Device fabrication has been partly supported by the Center for Excitonics, an Energy Frontier Research Center funded by the US Department of Energy (DOE), Office of Science, Office of Basic Energy Sciences under Award Number DESC0001088. The contribution of D.H.C. is supported by DE-SC0002197. Work at CMU is supported by DOE BES DE-SC0012509. W.Y. is supported by the Croucher Foundation (Croucher Innovation Award), the RGC of Hong Kong (HKU17305914P), and the HKU ORA. Work at ORNL (M.A.M.) was supported by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. X.X. and D.X. acknowledge the support of a Cottrell Scholar Award. S.G. and L.Y. are supported by NSF grant no. DMR-1455346 and EFRI-2DARE-1542815. X.X. acknowledges the support from the State of Washington funded Clean Energy Institute and from the Boeing Distinguished Professorship in Physics. acknowledge the support of a Cottrell Scholar Award. S.G. and L.Y. are supported by NSF grant no. DMR-1455346 and EFRI-2DARE-1542815.

FundersFunder number
Center for Integrated Quantum Materials
DOE BESDE-SC0012509
Office of Basic Energy SciencesDESC0001088, DE-SC0002197
RGCHKU17305914P
State of Washington
US Department of Energy
National Science FoundationDMR-1455346, DMR-1231319, 1542815, EFRI-2DARE-1542815
U.S. Department of Energy
Gordon and Betty Moore FoundationGBMF4541
Office of Science
Basic Energy Sciences
Oak Ridge National Laboratory
University of Washington
Division of Materials Sciences and EngineeringDE-SC0018171
Croucher Foundation

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