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Non-equilibrium induction of tin in germanium: towards direct bandgap Ge1−xSnx nanowires

Author

Listed:
  • Subhajit Biswas

    (Materials Chemistry & Analysis Group, Tyndall National Institute, University College Cork)

  • Jessica Doherty

    (Materials Chemistry & Analysis Group, Tyndall National Institute, University College Cork)

  • Dzianis Saladukha

    (Tyndall National Institute, University College Cork
    CAPPA, Cork Institute of Technology)

  • Quentin Ramasse

    (SuperSTEM Laboratory, SciTech Daresbury Campus)

  • Dipanwita Majumdar

    (Bose Institute)

  • Moneesh Upmanyu

    (Group for Simulation and Theory of Atomic-Scale Material Phenomena (stAMP), Northeastern University)

  • Achintya Singha

    (Bose Institute)

  • Tomasz Ochalski

    (Tyndall National Institute, University College Cork
    CAPPA, Cork Institute of Technology)

  • Michael A. Morris

    (AMBER, CRANN, Trinity College Dublin)

  • Justin D. Holmes

    (Materials Chemistry & Analysis Group, Tyndall National Institute, University College Cork
    AMBER, CRANN, Trinity College Dublin)

Abstract

The development of non-equilibrium group IV nanoscale alloys is critical to achieving new functionalities, such as the formation of a direct bandgap in a conventional indirect bandgap elemental semiconductor. Here, we describe the fabrication of uniform diameter, direct bandgap Ge1−xSnx alloy nanowires, with a Sn incorporation up to 9.2 at.%, far in excess of the equilibrium solubility of Sn in bulk Ge, through a conventional catalytic bottom-up growth paradigm using noble metal and metal alloy catalysts. Metal alloy catalysts permitted a greater inclusion of Sn in Ge nanowires compared with conventional Au catalysts, when used during vapour–liquid–solid growth. The addition of an annealing step close to the Ge-Sn eutectic temperature (230 °C) during cool-down, further facilitated the excessive dissolution of Sn in the nanowires. Sn was distributed throughout the Ge nanowire lattice with no metallic Sn segregation or precipitation at the surface or within the bulk of the nanowires. The non-equilibrium incorporation of Sn into the Ge nanowires can be understood in terms of a kinetic trapping model for impurity incorporation at the triple-phase boundary during growth.

Suggested Citation

  • Subhajit Biswas & Jessica Doherty & Dzianis Saladukha & Quentin Ramasse & Dipanwita Majumdar & Moneesh Upmanyu & Achintya Singha & Tomasz Ochalski & Michael A. Morris & Justin D. Holmes, 2016. "Non-equilibrium induction of tin in germanium: towards direct bandgap Ge1−xSnx nanowires," Nature Communications, Nature, vol. 7(1), pages 1-12, September.
  • Handle: RePEc:nat:natcom:v:7:y:2016:i:1:d:10.1038_ncomms11405
    DOI: 10.1038/ncomms11405
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    Cited by:

    1. Youngmin Kim & Simone Assali & Hyo-Jun Joo & Sebastian Koelling & Melvina Chen & Lu Luo & Xuncheng Shi & Daniel Burt & Zoran Ikonic & Donguk Nam & Oussama Moutanabbir, 2023. "Short-wave infrared cavity resonances in a single GeSn nanowire," Nature Communications, Nature, vol. 14(1), pages 1-7, December.

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