Abstract
Breaking time-reversal symmetry by introducing magnetic order, thereby opening a gap in the topological surface state bands, is essential for realizing useful topological properties such as the quantum anomalous Hall and axion insulator states. In this work, a novel topological antiferromagnetic (AFM) phase is created at the interface of a sputtered, c-axis-oriented, topological insulator/ferromagnet heterostructure—Bi2Te3/Ni80Fe20 because of diffusion of Ni in Bi2Te3 (Ni-Bi2Te3). The AFM property of the Ni-Bi2Te3 interfacial layer is established by observation of spontaneous exchange bias in the magnetic hysteresis loop and compensated moments in the depth profile of the magnetization using polarized neutron reflectometry. Analysis of the structural and chemical properties of the Ni-Bi2Te3 layer is carried out using selected-area electron diffraction, electron energy loss spectroscopy, and X-ray photoelectron spectroscopy. These studies, in parallel with first-principles calculations, indicate a solid-state chemical reaction that leads to the formation of Ni−Te bonds and the presence of topological antiferromagnetic (AFM) compound NiBi2Te4 in the Ni-Bi2Te3 interface layer. The Neél temperature of the Ni-Bi2Te3 layer is ≈63 K, which is higher than that of typical magnetic topological insulators (MTIs). The presented results provide a pathway toward industrial complementary metal−oxide−semiconductor (CMOS)-process-compatible sputtered-MTI heterostructures, leading to novel materials for topological quantum devices.
Original language | English |
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Article number | 2108790 |
Journal | Advanced Materials |
Volume | 34 |
Issue number | 15 |
DOIs | |
State | Published - Apr 14 2022 |
Funding
This work was partially supported by the U.S Army under grant no. W911NF20P0009, the NIH Award UF1NS107694, and the NSF TANMS ERC Award 1160504. The work of D.H. and A.F. was partially supported by the National Science Foundation grant DMR-1905662 and the Air Force Office of Scientific Research award FA9550-20-1-0247. The work of M.M. and A.B. was supported by the US Department of Energy (DOE), Office of Science, Basic Energy Sciences Grant No. DE-SC0019275 and of R.M. by DOE grant number DE-FG02-07ER46352, and benefited from Northeastern University's Advanced Scientific Computation Center and the Discovery Cluster, and the National Energy Research Scientific Computing Center through DOE Grant No. DE-AC02-05CH11231. The work of K.M. was supported by Air Force Research Laboratory under AFRL/NEMO contract: FA8650-19-F-5403 TO3. Studies employing the Titan 60–300 TEM were performed at the Center for Electron Microscopy and Analysis (CEMAS) at The Ohio State University with support through Air Force contract FA8650-18-2-5295. The work at TIFR Mumbai was supported by the Department of Atomic Energy of the Government of India under Project No. 12-R&D-TFR-5.10-0100. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The authors thank Charles Settens and Libby Shaw (MIT, Materials Research Laboratory) for help with XRD and XPS measurements. Certain commercial equipments are identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by Northeastern University, AFRL, ORNL, NIST, and TIFR. Note: the National Science Foundation grant number was corrected on April 14, 2022, after initial publication online. This work was partially supported by the U.S Army under grant no. W911NF20P0009, the NIH Award UF1NS107694, and the NSF TANMS ERC Award 1160504. The work of D.H. and A.F. was partially supported by the National Science Foundation grant DMR‐1905661 and the Air Force Office of Scientific Research award FA9550‐20‐1‐0247. The work of M.M. and A.B. was supported by the US Department of Energy (DOE), Office of Science, Basic Energy Sciences Grant No. DE‐SC0019275 and of R.M. by DOE grant number DE‐FG02‐07ER46352, and benefited from Northeastern University's Advanced Scientific Computation Center and the Discovery Cluster, and the National Energy Research Scientific Computing Center through DOE Grant No. DE‐AC02‐05CH11231. The work of K.M. was supported by Air Force Research Laboratory under AFRL/NEMO contract: FA8650‐19‐F‐5403 TO3. Studies employing the Titan 60–300 TEM were performed at the Center for Electron Microscopy and Analysis (CEMAS) at The Ohio State University with support through Air Force contract FA8650‐18‐2‐5295. The work at TIFR Mumbai was supported by the Department of Atomic Energy of the Government of India under Project No. 12‐R&D‐TFR‐5.10‐0100. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The authors thank Charles Settens and Libby Shaw (MIT, Materials Research Laboratory) for help with XRD and XPS measurements. Certain commercial equipments are identified in this paper to foster understanding. Such identification does not imply recommendation or endorsement by Northeastern University, AFRL, ORNL, NIST, and TIFR.
Funders | Funder number |
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Charles Settens and Libby Shaw | |
Materials Research Laboratory | |
National Science Foundation | 1160504, DMR-1905662, DMR‐1905661 |
National Institutes of Health | UF1NS107694 |
U.S. Department of Energy | |
National Institute of Standards and Technology | |
Air Force Office of Scientific Research | FA9550‐20‐1‐0247 |
Office of Science | |
Basic Energy Sciences | DE‐SC0019275, DE‐FG02‐07ER46352 |
Oak Ridge National Laboratory | |
Air Force Research Laboratory | FA8650‐19‐F‐5403 TO3 |
U.S. Army | W911NF20P0009 |
U.S. Air Force | FA8650-18-2-5295 |
Massachusetts Institute of Technology | |
Ohio State University | |
Northeastern University | |
National Energy Research Scientific Computing Center | DE‐AC02‐05CH11231 |
Tata Institute of Fundamental Research | |
Department of Atomic Energy, Government of India | 12‐R&D‐TFR‐5.10‐0100 |
Keywords
- ferromagnets
- interface
- magnetic topological insulators
- topological insulators
- van der Waals materials