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Volumn 55, Issue 23, 1997, Pages 15643-15651

Si(110)-16×2 and Si(110)-5×1 surface reconstructions: Stretched-hexagon face-centered adatom model

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EID: 0001746259     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.55.15643     Document Type: Article
Times cited : (58)

References (18)
  • 5
    • 0028444784 scopus 로고
    • Y. Yamamoto, Surf. Sci. 313, 155 (1994) tabulates reconstructions observed by various authors on the Si(110) surface. Seealso M. A. Lutz, R. M. Feenstra and J. O. Chu, Surf. Sci. 328, 215 (1995), and references therein.
    • (1994) Surf. Sci. , vol.313 , pp. 155
    • Yamamoto, Y.1
  • 10
    • 0006200017 scopus 로고
    • Our images are calibrated against LEED data for the distance of 50.2 Å between two stripes, from which a 13.3-Å zigzag period is determined. The lattice constant a is taken to be 5.43 Å. See, for example, S. Miura, K. Kato, T. Ide and T. Ichinokawa, Surf. Sci. 191, 259 (1987) and Ref. 6. These calibrated values are fully consistent with the STM data. The magnitude of the uncertainty in lengths determined exclusively by STM is typically <10%.
    • (1987) Surf. Sci. , vol.191 , pp. 259
    • Miura, S.1    Kato, K.2    Ide, T.3    Ichinokawa, T.4
  • 11
    • 0006276022 scopus 로고
    • Y. Yamamoto, Phys. Rev. B 50, 8534 (1994) has proposed another 16×2 model, which features trimers of Si, dimerization of adjacent atoms along a chain, rumpling of the surface, and no adatoms. Our data (Fig. 1) are inconsistent with his model.
    • (1994) Phys. Rev. B , vol.50 , pp. 8534
    • Yamamoto, Y.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.