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Realization of an intrinsic ferromagnetic topological state in MnBi8Te13

Journal Article · · Science Advances
 [1];  [2];  [3];  [4];  [5];  [3];  [3];  [5];  [6];  [1];  [1];  [5];  [7];  [4];  [7];  [8];  [8];  [9];  [6];  [2] more »;  [10];  [11];  [1] « less
  1. Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, Los Angeles, CA 90095, USA.
  2. Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA.
  3. Department of Physics, University of Colorado, Boulder, CO 80309, USA.
  4. Department of Physics, Indian Institute of Technology-Kanpur, Kanpur 208016, India.
  5. Department of Physics, National Cheng Kung University, Tainan 701, Taiwan.
  6. Institute of Physics, Academia Sinica, Taipei 11529, Taiwan.
  7. Department of Physics, Northeastern University, Boston, MA 02115, USA.
  8. Physical and Computational Sciences Directorate, Pacific Northwest National Laboratory, Richland, WA 99352, USA.
  9. Department of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02138, USA.
  10. Department of Physics, National Cheng Kung University, Tainan 701, Taiwan., Center for Quantum Frontiers of Research & Technology (QFort), Tainan 701, Taiwan., Physics Division, National Center for Theoretical Sciences, Hsinchu, Taiwan.
  11. Department of Physics, University of Colorado, Boulder, CO 80309, USA., Center for Experiments on Quantum Materials, University of Colorado, Boulder, CO 80309, USA.
Novel magnetic topological materials pave the way for studying the interplay between band topology and magnetism. However, an intrinsically ferromagnetic topological material with only topological bands at the charge neutrality energy has so far remained elusive. Using rational design, we synthesized MnBi8Te13, a natural heterostructure with [MnBi2Te4] and [Bi2Te3] layers. Thermodynamic, transport, and neutron diffraction measurements show that despite the adjacent [MnBi2Te4] being 44.1 Å apart, MnBi8Te13 manifests long-range ferromagnetism below 10.5 K with strong coupling between magnetism and charge carriers. First-principles calculations and angle-resolved photoemission spectroscopy measurements reveal it is an axion insulator with sizable surface hybridization gaps. Our calculations further demonstrate the hybridization gap persists in the two-dimensional limit with a nontrivial Chern number. Therefore, as an intrinsic ferromagnetic axion insulator with clean low-energy band structures, MnBi8Te13 serves as an ideal system to investigate rich emergent phenomena, including the quantized anomalous Hall effect and quantized magnetoelectric effect.
Research Organization:
Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States). National Energy Research Scientific Computing Center (NERSC); Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR); SLAC National Accelerator Laboratory, Menlo Park, CA (United States). Stanford Synchrotron Radiation Lightsource (SSRL)
Sponsoring Organization:
Council of Scientific & Industrial Research (CSIR); National Science Foundation (NSF); Taiwan Ministry of Science and Technology (MOST); USDOE Office of Science (SC), Basic Energy Sciences (BES). Materials Sciences & Engineering Division
Grant/Contract Number:
AC02-05CH11231; AC02-76SF00515; AC05-00OR22725; SC0011978; SC0019275
OSTI ID:
1641878
Alternate ID(s):
OSTI ID: 1649161
Journal Information:
Science Advances, Journal Name: Science Advances Journal Issue: 30 Vol. 6; ISSN 2375-2548
Publisher:
AAASCopyright Statement
Country of Publication:
United States
Language:
English

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