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Atomic and electronic structure of doped Si(111)(2 root 3 x 2 root 3)R30 degrees-Sn interfacesopen access

Authors
Yi, SehoMing, FangfeiHuang, Ying-TzuSmith, Tyler S.Peng, XiyouTu, WeisongMulugeta, DanielDiehl, Renee D.Snijders, Paul C.Cho, Jun HyungWeitering, Hanno H.
Issue Date
May-2018
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW B, v.97, no.19, pp.1 - 15
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW B
Volume
97
Number
19
Start Page
1
End Page
15
URI
https://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/150093
DOI
10.1103/PhysRevB.97.195402
ISSN
2469-9950
Abstract
The hole-doped Si(111)(2 root 3 x 2 root 3) R30 degrees-Sn interface exhibits a symmetry- breaking insulator-insulator transition below 100 K that appears to be triggered by electron tunneling into the empty surface-state bands. No such transition is seen in electron-doped systems. To elucidate the nature and driving force of this phenomenon, the structure of the interface must be resolved. Here we report on an extensive experimental and theoretical study, including scanning tunneling microscopyand spectroscopy (STM/STS), dynamical low-energy electron diffraction (LEED) analysis, and density functional theory (DFT) calculations, to elucidate the structure of this interface. We consider six different structure models, three of which have been proposed before, and conclude that only two of them can account for the majority of experimental data. One of them is the model according to Tornevik et al. [C. Tornevik et al., Phys. Rev. B 44, 13144 (1991)] with a total Sn coverage of 14/12 monolayers (ML). The other is the "revised trimer model" with a total Sn coverage of 13/12 ML, introduced in this work. These two models are very difficult to discriminate on the basis of DFT or LEED alone, but STS data clearly point toward the Tornevik model as the most viable candidate among the models considered here. The STS data also provide additional insights regarding the electron-injection-driven phase transformation. Similar processes may occur at other metal/semiconductor interfaces, provided they are nonmetallic and can be doped. This could open up a new pathway toward the creation of novel surface phases with potentially very interesting and desirable electronic properties.
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