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Volumn 68, Issue 23, 2003, Pages

Topography and energy variation in physisorbed layers

Author keywords

[No Author keywords available]

Indexed keywords

ARGON; GRAPHITE; HELIUM; HYDROGEN; INERT GAS; KRYPTON; MAGNESIUM OXIDE;

EID: 0842321071     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.68.235420     Document Type: Article
Times cited : (6)

References (54)
  • 5
    • 85039030670 scopus 로고    scopus 로고
    • (private communication)
    • H. Hövel (private communication).
    • Hövel, H.1
  • 7
    • 85039025998 scopus 로고    scopus 로고
    • 2/MgO(001). This included the Beeby correction for an attractive well of depth 3 meV and an angle-factor following
    • 2/MgO(001). This included the Beeby correction for an attractive well of depth 3 meV and an angle-factor following
    • Traeger, F.1
  • 8
    • 0000032491 scopus 로고
    • h than on its attractive well. For some cautionary remarks on use of the eikonal analysis to estimate the topography of strongly corrugated systems
    • h than on its attractive well. For some cautionary remarks on use of the eikonal analysis to estimate the topography of strongly corrugated systems, see
    • (1975) Surf. Sci. , vol.48 , pp. 649
    • Garribaldi, U.1    Levi, A.C.2    Spadacini, R.3    Tommei, G.4
  • 21
    • 85039028932 scopus 로고    scopus 로고
    • The isotropic models used in the present work are chosen because they have been used in modeling of the monolayer solids and because it seems more consistent to include estimates of the effect of the substrate anisotropy on both the attractive and repulsive terms of the potential. This procedure has been discussed previously for the series He, Ne, and Kr on graphite:
    • The isotropic models used in the present work are chosen because they have been used in modeling of the monolayer solids and because it seems more consistent to include estimates of the effect of the substrate anisotropy on both the attractive and repulsive terms of the potential. This procedure has been discussed previously for the series He, Ne, and Kr on graphite:
  • 22
    • 0003864917 scopus 로고
    • H. Taub, G. Torzo, H. J. Lauter, and S. C. Fain, Jr. (Plenum, New York
    • L. W. Bruch, in Phase Transitions in Surface Films II, edited by H. Taub, G. Torzo, H. J. Lauter, and S. C. Fain, Jr. (Plenum, New York, 1991), p. 67.
    • (1991) Phase Transitions in Surface Films II , pp. 67
    • Bruch, L.W.1
  • 30
    • 0000986997 scopus 로고
    • 4He/graphite from band structure effects in selective adsorption resonance data
    • 4He/graphite from band structure effects in selective adsorption resonance data [M. W. Cole, D. R. Frankl, and D. L. Goodstein, Rev. Mod. Phys. 53, 199 (1981)].
    • (1981) Rev. Mod. Phys. , vol.53 , pp. 199
    • Cole, M.W.1    Frankl, D.R.2    Goodstein, D.L.3
  • 35
    • 85039021372 scopus 로고
    • Ph.D. thesis, University of Washington–Seattle
    • C. G. Shaw, Ph.D. thesis, University of Washington–Seattle, 1979.
    • (1979)
    • Shaw, C.G.1
  • 38
    • 85038973477 scopus 로고    scopus 로고
    • In this work, the substrate is treated as static. Although there is an adsorbate-substrate potential energy, there is no provision for the hybridization (Refs. 7 and 24) of adlayer and substrate dynamics that occurs close to the adlayer Brillouin zone center for some degrees of freedom
    • In this work, the substrate is treated as static. Although there is an adsorbate-substrate potential energy, there is no provision for the hybridization (Refs. 7 and 24) of adlayer and substrate dynamics that occurs close to the adlayer Brillouin zone center for some degrees of freedom.
  • 48
    • 85039014432 scopus 로고    scopus 로고
    • 2 molecules in the j = 1, m = ±1 state
    • 2 molecules in the j = 1, m = ±1 state.
  • 49
    • 85038978428 scopus 로고    scopus 로고
    • 2 in adsorption isotherms at about 18 K gives some evidence against this proposal
    • 2 in adsorption isotherms at about 18 K gives some evidence against this proposal.
  • 52
    • 85039027819 scopus 로고    scopus 로고
    • 2〉/2) and the force constant for ω0, is a weighted average of the contributions from the a and b sites of the HOC unit cell. The assumed exponential dependence is consistent with the large difference for the corrugation amplitudes of Xe/Cu at two values of g in Table I
    • ∥ is a weighted average of the contributions from the a and b sites of the HOC unit cell. The assumed exponential dependence is consistent with the large difference for the corrugation amplitudes of Xe/Cu at two values of g in Table I.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.