메뉴 건너뛰기




Volumn 57, Issue 3, 1998, Pages 1896-1907

Adatom dynamics and diffusion in a model of O/W(110)

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000044712     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.57.1896     Document Type: Article
Times cited : (47)

References (86)
  • 2
  • 49
    • 0001270233 scopus 로고
    • G.-C. Wang, T.-M. Lu, and M. G. Lagally, J. Chem. Phys. 69, 479 (1978).
    • (1978) J. Chem. Phys. , vol.69 , pp. 479
    • Lagally, M.1
  • 62
    • 0000088280 scopus 로고
    • J.-R. Chen and R. Gomer, Surf. Sci. 79, 413 (1979).
    • (1979) Surf. Sci. , vol.79 , pp. 413
    • Gomer, R.1
  • 64
    • 0000214844 scopus 로고    scopus 로고
    • A generalization of the approach for a case where the binding energies at different adsorption sites may vary will be presented elsewhere. Such a situation is realized, e.g., on stepped surfaces [J. Merikoski and S. C. Ying, Phys. Rev. B 56, 2166 (1997); (unpublished).
    • (1997) Phys. Rev. B , vol.56 , pp. 2166
    • Merikoski, J.1    Ying, S.2
  • 77
    • 0019712678 scopus 로고
    • The order-disorder transition for the present case belongs to the universality class of the 2D (Formula presented) model with a cubic anisotropy field [M. Schick, Prog. Surf. Sci. 11, 245 (1981).
    • (1981) Prog. Surf. Sci. , vol.11 , pp. 245
    • Schick, M.1
  • 78
    • 13044268246 scopus 로고
    • We expect [J. M. Kosterlitz (private communication)] the compressibility to behave as (Formula presented), where (Formula presented) leading to the observed weak cusplike behavior (see the inset of Fig. 77)
    • J. V. José, L. P. Kadanoff, S. Kirckpatrick, and D. R. Nelson, Phys. Rev. B 16, 1217 (1977)], for which the critical exponents are nonuniversal. This implies that the critical behavior in corresponding systems is affected by local properties such as the coverage and the interaction strengths and is therefore system dependent. We expect [J. M. Kosterlitz (private communication)] the compressibility to behave as (Formula presented), where (Formula presented) leading to the observed weak cusplike behavior (see the inset of Fig. 77).
    • (1977) Phys. Rev. B , vol.16 , pp. 1217
    • José, J.1    Kadanoff, L.2    Kirckpatrick, S.3    Nelson, D.4
  • 80
    • 0001226745 scopus 로고
    • In a complex many-particle system like the one studied here, the instantaneous activation barrier (Formula presented) may naturally change due to jumps of the neighboring particles while the tagged particle is waiting for a successful jump to occur. Also, right after a jump, the site left behind is more likely to be vacant than other neighboring sites [K. W. Kehr, R. Kutner, and K. Binder, Phys. Rev. B 23, 4931 (1981)].
    • (1981) Phys. Rev. B , vol.23 , pp. 4931
    • Kehr, K.1    Kutner, R.2    Binder, K.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.