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Guguchia Z, Kerelsky A, Edelberg D, Banerjee S, von Rohr F, Scullion D, Augustin M, Scully M, Rhodes DA, Shermadini Z, Luetkens H, Shengelaya A, Baines C, Morenzoni E, Amato A, Hone JC, Khasanov R, Billinge SJL, Santos E, Pasupathy AN, Uemura YJ. Magnetism in semiconducting molybdenum dichalcogenides. Sci Adv 2018; 4:eaat3672. [PMID: 30588488 PMCID: PMC6303124 DOI: 10.1126/sciadv.aat3672] [Citation(s) in RCA: 19] [Impact Index Per Article: 3.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/19/2018] [Accepted: 11/19/2018] [Indexed: 05/30/2023]
Abstract
Transition metal dichalcogenides (TMDs) are interesting for understanding the fundamental physics of two-dimensional (2D) materials as well as for applications to many emerging technologies, including spin electronics. Here, we report the discovery of long-range magnetic order below T M = 40 and 100 K in bulk semiconducting TMDs 2H-MoTe2 and 2H-MoSe2, respectively, by means of muon spin rotation (μSR), scanning tunneling microscopy (STM), and density functional theory (DFT) calculations. The μSR measurements show the presence of large and homogeneous internal magnetic fields at low temperatures in both compounds indicative of long-range magnetic order. DFT calculations show that this magnetism is promoted by the presence of defects in the crystal. The STM measurements show that the vast majority of defects in these materials are metal vacancies and chalcogen-metal antisites, which are randomly distributed in the lattice at the subpercent level. DFT indicates that the antisite defects are magnetic with a magnetic moment in the range of 0.9 to 2.8 μB. Further, we find that the magnetic order stabilized in 2H-MoTe2 and 2H-MoSe2 is highly sensitive to hydrostatic pressure. These observations establish 2H-MoTe2 and 2H-MoSe2 as a new class of magnetic semiconductors and open a path to studying the interplay of 2D physics and magnetism in these interesting semiconductors.
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Affiliation(s)
- Z. Guguchia
- Department of Physics, Columbia University, New York, NY 10027, USA
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - A. Kerelsky
- Department of Physics, Columbia University, New York, NY 10027, USA
| | - D. Edelberg
- Department of Physics, Columbia University, New York, NY 10027, USA
| | - S. Banerjee
- Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY 10027, USA
| | - F. von Rohr
- Department of Chemistry, University of Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland
| | - D. Scullion
- School of Mathematics and Physics, Queen’s University Belfast, Belfast, UK
| | - M. Augustin
- School of Mathematics and Physics, Queen’s University Belfast, Belfast, UK
| | - M. Scully
- School of Mathematics and Physics, Queen’s University Belfast, Belfast, UK
| | - D. A. Rhodes
- Department of Mechanical Engineering, Columbia University, New York, NY 10027, USA
| | - Z. Shermadini
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - H. Luetkens
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - A. Shengelaya
- Department of Physics, Tbilisi State University, Chavchavadze 3, GE-0128 Tbilisi, Georgia
- Andronikashvili Institute of Physics of I. Javakhishvili Tbilisi State University, Tamarashvili str. 6, 0177 Tbilisi, Georgia
| | - C. Baines
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - E. Morenzoni
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - A. Amato
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - J. C. Hone
- Department of Mechanical Engineering, Columbia University, New York, NY 10027, USA
| | - R. Khasanov
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - S. J. L. Billinge
- Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY 10027, USA
- Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, NY 11973, USA
| | - E. Santos
- School of Mathematics and Physics, Queen’s University Belfast, Belfast, UK
| | - A. N. Pasupathy
- Department of Physics, Columbia University, New York, NY 10027, USA
| | - Y. J. Uemura
- Department of Physics, Columbia University, New York, NY 10027, USA
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Rhodes D, Chenet DA, Janicek BE, Nyby C, Lin Y, Jin W, Edelberg D, Mannebach E, Finney N, Antony A, Schiros T, Klarr T, Mazzoni A, Chin M, Chiu YC, Zheng W, Zhang QR, Ernst F, Dadap JI, Tong X, Ma J, Lou R, Wang S, Qian T, Ding H, Osgood RM, Paley DW, Lindenberg AM, Huang PY, Pasupathy AN, Dubey M, Hone J, Balicas L. Engineering the Structural and Electronic Phases of MoTe 2 through W Substitution. Nano Lett 2017; 17:1616-1622. [PMID: 28145719 DOI: 10.1021/acs.nanolett.6b04814] [Citation(s) in RCA: 20] [Impact Index Per Article: 2.9] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/17/2023]
Abstract
MoTe2 is an exfoliable transition metal dichalcogenide (TMD) that crystallizes in three symmetries: the semiconducting trigonal-prismatic 2H- or α-phase, the semimetallic and monoclinic 1T'- or β-phase, and the semimetallic orthorhombic γ-structure. The 2H-phase displays a band gap of ∼1 eV making it appealing for flexible and transparent optoelectronics. The γ-phase is predicted to possess unique topological properties that might lead to topologically protected nondissipative transport channels. Recently, it was argued that it is possible to locally induce phase-transformations in TMDs, through chemical doping, local heating, or electric-field to achieve ohmic contacts or to induce useful functionalities such as electronic phase-change memory elements. The combination of semiconducting and topological elements based upon the same compound might produce a new generation of high performance, low dissipation optoelectronic elements. Here, we show that it is possible to engineer the phases of MoTe2 through W substitution by unveiling the phase-diagram of the Mo1-xWxTe2 solid solution, which displays a semiconducting to semimetallic transition as a function of x. We find that a small critical W concentration xc ∼ 8% stabilizes the γ-phase at room temperature. This suggests that crystals with x close to xc might be particularly susceptible to phase transformations induced by an external perturbation, for example, an electric field. Photoemission spectroscopy, indicates that the γ-phase possesses a Fermi surface akin to that of WTe2.
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Affiliation(s)
- D Rhodes
- National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States
- Department of Physics, Florida State University , Tallahassee, Florida 32306, United States
| | - D A Chenet
- Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States
| | - B E Janicek
- Department of Materials Science and Engineering, University of Illinois Urbana-Champaign , Urbana, Illinois 61801, United States
| | - C Nyby
- Department of Chemistry, Stanford University , Stanford, California 94305-4401, United States
| | | | | | | | - E Mannebach
- Department of Materials Science and Engineering, Stanford University , Stanford, California 94305, United States
| | - N Finney
- Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States
| | - A Antony
- Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States
| | - T Schiros
- Materials Research Science and Engineering Center, Columbia University , New York, New York 10027 United States
- Department of Science and Mathematics, SUNY Fashion Institute of Technology , New York, New York 10001 United States
| | - T Klarr
- Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States
| | - A Mazzoni
- Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States
| | - M Chin
- Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States
| | - Y-C Chiu
- National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States
- Department of Physics, Florida State University , Tallahassee, Florida 32306, United States
| | - W Zheng
- National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States
- Department of Physics, Florida State University , Tallahassee, Florida 32306, United States
| | - Q R Zhang
- National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States
- Department of Physics, Florida State University , Tallahassee, Florida 32306, United States
| | - F Ernst
- Department of Applied Physics, Stanford University , Stanford, California 94305-4090, United States
- Stanford PULSE Institute, SLAC National Accelerator Laboratory , Menlo Park, California 94025, United States
| | - J I Dadap
- Department of Electrical Engineering, Columbia University , New York, New York 10027, United States
| | - X Tong
- Center for Functional Nanomaterials, Brookhaven National Laboratory , Upton, New York 11973-5000, United States
| | - J Ma
- Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China
| | - R Lou
- Department of Physics, Renmin University of China , Beijing 100872, China
| | - S Wang
- Department of Physics, Renmin University of China , Beijing 100872, China
| | - T Qian
- Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China
| | - H Ding
- Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China
| | - R M Osgood
- Department of Electrical Engineering, Columbia University , New York, New York 10027, United States
| | | | - A M Lindenberg
- Department of Materials Science and Engineering, Stanford University , Stanford, California 94305, United States
- Stanford PULSE Institute, SLAC National Accelerator Laboratory , Menlo Park, California 94025, United States
- Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory , Menlo Park, California 94025, United States
| | - P Y Huang
- Department of Mechanical Science and Engineering, University of Illinois Urbana-Champaign , Urbana, Illinois 61801, United States
| | | | - M Dubey
- Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States
| | - J Hone
- Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States
| | - L Balicas
- National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States
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