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    Formation and properties of the Bi (3×3)R30∘ wetting layer on Ge(111)

    Kevin Vonk1,*, Ying Wang1, Montserrat Navarro Espino2, Andrés R. Botello Mendez2, Zeila Zanolli2, and Harold J. W. Zandvliet1,†

    • 1Physics of Interfaces and Nanomaterials, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, 7500AE Enschede, The Netherlands
    • 2Chemistry Department, Debye Institute for Nanomaterials Science and ETSF, Utrecht University, P.O. Box 80.000, 3508TA Utrecht, The Netherlands

    • *Contact author: k.vonk@utwente.nl
    • †Contact author: h.j.w.zandvliet@utwente.nl

    Phys. Rev. B 112, 205422 – Published 18 November, 2025

    DOI: https://doi.org/10.1103/3ws2-w84r

    Abstract

    Owing to the broken inversion symmetry at the surface, thin Bi films are expected to exhibit interesting electronic and topological properties stemming from its large spin-orbit coupling. Furthermore, the properties of Bi thin films are also governed by the coupling to the underlying substrate. In this work, we scrutinize the formation and properties of the (3×3)R30∘ Bi wetting layer on Ge(111) using scanning tunneling microscopy and first-principles simulations. The deposition of Bi on Ge(111) leads to the de-reconstruction of the c(2×8) adatom structure of Ge(111) and the formation of Ge islands. The unreconstructed Ge terraces and islands are covered by a semiconducting (3×3)R30∘ Bi wetting layer. The elementary building block of the Bi wetting layer is a Bi trimer, which is located on a T4 site of the underlying Ge(111) substrate. This Bi trimer has a well-defined electronic state at −0.4eV. The edges of the small Bi covered Ge islands, which are slightly metallic, are mainly of the armchair edge configuration. The most abundant defects in the Bi wetting layer are antiphase boundaries and single Bi trimer vacancies. Our work lays the foundation to investigate the topological nature of the Bi trimer wetting layer and any layers grown on top.

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