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Modelling of ‘sub-atomic’ contrast resulting from back-bonding on Si(111)-7×7

DOI:10.3762/bjnano.7.85 期刊:Beilstein Journal of Nanotechnology 出版年份:2016 更新时间:2025-09-23 15:22:29
摘要: It has recently been shown that ‘sub-atomic’ contrast can be observed during NC-AFM imaging of the Si(111)-7×7 substrate with a passivated tip, resulting in triangular shaped atoms [Sweetman et al. Nano Lett. 2014, 14, 2265]. The symmetry of the features, and the well-established nature of the dangling bond structure of the silicon adatom means that in this instance the contrast cannot arise from the orbital structure of the atoms, and it was suggested by simple symmetry arguments that the contrast could only arise from the backbonding symmetry of the surface adatoms. However, no modelling of the system has been performed in order to understand the precise origin of the contrast. In this paper we provide a detailed explanation for ‘sub-atomic’ contrast observed on Si(111)-7×7 using a simple model based on Lennard-Jones potentials, coupled with a flexible tip, as proposed by Hapala et al. [Phys. Rev. B 2014, 90, 085421] in the context of interpreting sub-molecular contrast. Our results show a striking similarity to experimental results, and demonstrate how ‘sub-atomic’ contrast can arise from a flexible tip exploring an asymmetric potential created due to the positioning of the surrounding surface atoms.
作者: Adam Sweetman,Samuel P. Jarvis,Mohammad A. Rashid
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To provide a detailed explanation for 'sub-atomic' contrast observed on Si(111)-7×7 using a simple model based on Lennard-Jones potentials and a flexible tip, and to understand the origin of the contrast.

The simulations demonstrate that 'sub-atomic' contrast on Si(111)-7×7 can arise from a flexible tip exploring an asymmetric potential created by the surrounding surface atoms, without needing to consider electronic orbital structure. The contrast is influenced by backbonding atoms and rest atoms, highlighting the role of multi-atom effects. However, the model cannot reproduce certain features like repulsive halos, requiring more sophisticated ab-initio modeling for full interpretation.

The model does not include chemical interactions or changes in chemical reactivity, which limits its accuracy at close tip-sample separations. It also assumes identical properties for all atoms, not accounting for known differences in chemical reactivity at different sites on the Si(111)-7×7 surface. Electrostatic forces are not included, and the tip termination is generic, not specific to the experimental setup.

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