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Engineering the Structural and Electronic Phases of MoTe2 through W Substitution.
Rhodes, D; Chenet, D A; Janicek, B E; Nyby, C; Lin, Y; Jin, W; Edelberg, D; Mannebach, E; Finney, N; Antony, A; Schiros, T; Klarr, T; Mazzoni, A; Chin, M; Chiu, Y-C; Zheng, W; Zhang, Q R; Ernst, F; Dadap, J I; Tong, X; Ma, J; Lou, R; Wang, S; Qian, T; Ding, H; Osgood, R M; Paley, D W; Lindenberg, A M; Huang, P Y; Pasupathy, A N; Dubey, M; Hone, J; Balicas, L.
Afiliação
  • Rhodes D; National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States.
  • Chenet DA; Department of Physics, Florida State University , Tallahassee, Florida 32306, United States.
  • Janicek BE; Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States.
  • Nyby C; Department of Materials Science and Engineering, University of Illinois Urbana-Champaign , Urbana, Illinois 61801, United States.
  • Lin Y; Department of Chemistry, Stanford University , Stanford, California 94305-4401, United States.
  • Finney N; Department of Materials Science and Engineering, Stanford University , Stanford, California 94305, United States.
  • Antony A; Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States.
  • Schiros T; Department of Mechanical Engineering, Columbia University , New York, New York 10027, United States.
  • Klarr T; Materials Research Science and Engineering Center, Columbia University , New York, New York 10027 United States.
  • Mazzoni A; Department of Science and Mathematics, SUNY Fashion Institute of Technology , New York, New York 10001 United States.
  • Chin M; Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States.
  • Chiu YC; Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States.
  • Zheng W; Sensors and Electronic Devices Directorate, United States Army Research Laboratory , Adelphi, Maryland 20723, United States.
  • Zhang QR; National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States.
  • Ernst F; Department of Physics, Florida State University , Tallahassee, Florida 32306, United States.
  • Dadap JI; National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States.
  • Tong X; Department of Physics, Florida State University , Tallahassee, Florida 32306, United States.
  • Ma J; National High Magnetic Field Laboratory, Florida State University , Tallahassee, Florida 32310, United States.
  • Lou R; Department of Physics, Florida State University , Tallahassee, Florida 32306, United States.
  • Wang S; Department of Applied Physics, Stanford University , Stanford, California 94305-4090, United States.
  • Qian T; Stanford PULSE Institute, SLAC National Accelerator Laboratory , Menlo Park, California 94025, United States.
  • Ding H; Department of Electrical Engineering, Columbia University , New York, New York 10027, United States.
  • Osgood RM; Center for Functional Nanomaterials, Brookhaven National Laboratory , Upton, New York 11973-5000, United States.
  • Paley DW; Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China.
  • Lindenberg AM; Department of Physics, Renmin University of China , Beijing 100872, China.
  • Huang PY; Department of Physics, Renmin University of China , Beijing 100872, China.
  • Pasupathy AN; Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China.
  • Dubey M; Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China.
  • Hone J; Department of Electrical Engineering, Columbia University , New York, New York 10027, United States.
Nano Lett ; 17(3): 1616-1622, 2017 03 08.
Article em En | MEDLINE | ID: mdl-28145719
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 ß-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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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article