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Atomically thin half-van der Waals metals enabled by confinement heteroepitaxy.
Briggs, Natalie; Bersch, Brian; Wang, Yuanxi; Jiang, Jue; Koch, Roland J; Nayir, Nadire; Wang, Ke; Kolmer, Marek; Ko, Wonhee; De La Fuente Duran, Ana; Subramanian, Shruti; Dong, Chengye; Shallenberger, Jeffrey; Fu, Mingming; Zou, Qiang; Chuang, Ya-Wen; Gai, Zheng; Li, An-Ping; Bostwick, Aaron; Jozwiak, Chris; Chang, Cui-Zu; Rotenberg, Eli; Zhu, Jun; van Duin, Adri C T; Crespi, Vincent; Robinson, Joshua A.
Affiliation
  • Briggs N; Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Bersch B; Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, USA.
  • Wang Y; 2-Dimensional Crystal Consortium, The Pennsylvania State University, University Park, PA, USA.
  • Jiang J; Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Koch RJ; Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, USA.
  • Nayir N; Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, USA.
  • Wang K; 2-Dimensional Crystal Consortium, The Pennsylvania State University, University Park, PA, USA.
  • Kolmer M; Department of Physics, The Pennsylvania State University, University Park, PA, USA.
  • Ko W; Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California, USA.
  • De La Fuente Duran A; The Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California, USA.
  • Subramanian S; 2-Dimensional Crystal Consortium, The Pennsylvania State University, University Park, PA, USA.
  • Dong C; Department of Mechanical Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Shallenberger J; Materials Research Institute, The Pennsylvania State University, University Park, PA, USA.
  • Fu M; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Zou Q; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Chuang YW; Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Gai Z; Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Li AP; Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, USA.
  • Bostwick A; Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
  • Jozwiak C; Center for 2-Dimensional and Layered Materials, The Pennsylvania State University, University Park, PA, USA.
  • Chang CZ; Materials Research Institute, The Pennsylvania State University, University Park, PA, USA.
  • Rotenberg E; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Zhu J; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • van Duin ACT; Department of Physics, The Pennsylvania State University, University Park, PA, USA.
  • Crespi V; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
  • Robinson JA; Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, TN, USA.
Nat Mater ; 19(6): 637-643, 2020 Jun.
Article in En | MEDLINE | ID: mdl-32157191
Atomically thin two-dimensional (2D) metals may be key ingredients in next-generation quantum and optoelectronic devices. However, 2D metals must be stabilized against environmental degradation and integrated into heterostructure devices at the wafer scale. The high-energy interface between silicon carbide and epitaxial graphene provides an intriguing framework for stabilizing a diverse range of 2D metals. Here we demonstrate large-area, environmentally stable, single-crystal 2D gallium, indium and tin that are stabilized at the interface of epitaxial graphene and silicon carbide. The 2D metals are covalently bonded to SiC below but present a non-bonded interface to the graphene overlayer; that is, they are 'half van der Waals' metals with strong internal gradients in bonding character. These non-centrosymmetric 2D metals offer compelling opportunities for superconducting devices, topological phenomena and advanced optoelectronic properties. For example, the reported 2D Ga is a superconductor that combines six strongly coupled Ga-derived electron pockets with a large nearly free-electron Fermi surface that closely approaches the Dirac points of the graphene overlayer.

Full text: 1 Database: MEDLINE Language: En Journal: Nat Mater Journal subject: CIENCIA / QUIMICA Year: 2020 Type: Article Affiliation country: United States

Full text: 1 Database: MEDLINE Language: En Journal: Nat Mater Journal subject: CIENCIA / QUIMICA Year: 2020 Type: Article Affiliation country: United States