APS Logo

Atomic imaging of edge structure and growth of a two-dimensional hexagonal ice

ORAL

Abstract

The formation and growth of water ice layers on surfaces and of low-dimensional ice under confinement are common occurrences. While structured water adlayers and 2D ice have been imaged, capturing metastable or intermediate edge structures involved in their growth is extremely challenging due to their fragile and short-lived nature.
Here we show that noncontact atomic force microscopy with a CO-terminated tip allows real-space imaging of the edge structures of a 2D bilayer of hexagonal ice grown on an Au(111) surface. We find a new edge type that coexists with the zigzag edge commonly observed in 2D hexagonal crystals, and freeze samples during growth to identify intermediate structures.
When combined with MD simulations, these allow us to reconstruct growth processes that in the case of the zigzag edge involve addition of water molecules to the existing edge and a collective bridging mechanism. Armchair edge growth, in contrast, involves local seeding and edge reconstruction and thus is in stark contrast to conventional views of ice growth. The growth mechanism we have uncovered might also occur at the surface of bilayer hexagonal ice and might support a bilayer-on-bilayer ice growth to 3D ice transformation.

Presenters

  • Runze Ma

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

Authors

  • Runze Ma

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Duanyun Cao

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Chongqin Zhu

    Department of Earth and Environmental Sciences, University of Pennsylvania, Department of Chemistry and Department of Chemical & Biomolecular Engineering and Department of Mechanical & Materials Engineering, University of Nebraska–Lincoln, Lincoln, N

  • Ye Tian

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Jinbo Peng

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Jing Guo

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Ji Chen

    School of Physics, Peking University, School of Physics, Peking University, Beijing 100871, P. R. China

  • Xin-Zheng Li

    Peking Univ, School of Physics, Peking University, School of Physics, Peking University, Beijing 100871, P. R. China

  • Joseph S Francisco

    Department of Earth and Environmental Sciences, University of Pennsylvania, Department of Earth and Environmental Sciences, University of Pennsylvania, Philadelphia, Pennsylvania 19104, USA

  • Xiao Cheng Zeng

    Department of Physics, University of Nebraska–Lincoln, Department of Chemistry and Department of Chemical & Biomolecular Engineering and Department of Mechanical & Materials Engineering, University of Nebraska–Lincoln, Lincoln, N

  • Limei Xu

    International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University

  • Enge Wang

    School of Physics, Peking Universiry, International Center for Quantum Materials, Peking University, University of Chinese Academy of Sciences, Beijing 100190, P. R. China, CAS Center for Excellence in Topological Quantum Computation

  • Ying Jiang

    Peking Univ, International Center for Quantum Materials, Peking University, International Center for Quantum Materials, School of Physics, Peking University, Physics, Peking University