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Volumn 64, Issue 7, 2001, Pages

Metal homoepitaxial growth at very low temperatures: Lattice-gas models with restricted downward funneling

Author keywords

[No Author keywords available]

Indexed keywords

ADSORPTION; ARTICLE; CRYSTAL STRUCTURE; CRYSTALLIZATION; DIFFUSION; DRY DEPOSITION; FILM; GEOMETRY; LOW TEMPERATURE PROCEDURES;

EID: 0035881477     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.075401     Document Type: Article
Times cited : (22)

References (42)
  • 2
    • 85038894372 scopus 로고    scopus 로고
    • Another misconception (see Ref. is that smoother growth at low, is simply due to the presence of smaller islands from which deposited atoms can more easily descend
    • Another misconception (see Ref. 1) is that smoother growth at low T is simply due to the presence of smaller islands from which deposited atoms can more easily descend.
  • 7
    • 0345103245 scopus 로고    scopus 로고
    • Long-range correlations have been attributed to intralayer “clumping” of atoms deposited nearby other adatoms, facilitated by low-barrier edge diffusion processes. See, and
    • Long-range correlations have been attributed to intralayer “clumping” of atoms deposited nearby other adatoms, facilitated by low-barrier edge diffusion processes. See M C. Bartelt and J W. Evans, Surf. Sci.423, 189 (1999);
    • (1999) Surf. Sci. , vol.423 , pp. 189
    • Bartelt, M.C.1    Evans, J.W.2
  • 9
    • 85038945410 scopus 로고    scopus 로고
    • (unpublished)
    • M. Breeman (unpublished).
    • Breeman, M.1
  • 13
    • 0004199617 scopus 로고
    • S. Y. Tong, M. A. Van Hove, K. Takayanagi, X. D. Xie, Springer, Berlin, and, in, edited by, and
    • D E. Sanders and J W. Evans, in Structure of Surfaces III, edited by S. Y. Tong, M. A. Van Hove, K. Takayanagi, and X. D. Xie (Springer, Berlin, 1991);
    • (1991) Structure of Surfaces III
    • Sanders, D.E.1    Evans, J.W.2
  • 17
    • 0000566005 scopus 로고
    • See the Appendix in,) which normalized (formula presented) to the number of atoms in a complete layer. Here, we normalize to the number of columns (twice as large), hence the extra factor of 2 relating, ’s and θ’s
    • See the Appendix in J W. Evans, Phys. Rev. B39, 5655 (1989) which normalized (formula presented) to the number of atoms in a complete layer. Here, we normalize to the number of columns (twice as large), hence the extra factor of 2 relating P’s and θ’s.
    • (1989) Phys. Rev. B , vol.39 , pp. 5655
    • Evans, J.W.1
  • 18
    • 85038909057 scopus 로고    scopus 로고
    • If (formula presented) and (formula presented) then (formula presented) (formula presented) (formula presented) (formula presented) and similarly with, even. If expressions in parentheses approximate an integral with error (formula presented) then (formula presented)
    • If (formula presented) and (formula presented) then (formula presented) (formula presented) (formula presented) (formula presented) and similarly with j even. If expressions in parentheses approximate an integral with error (formula presented) then (formula presented)
  • 22
    • 85038902977 scopus 로고    scopus 로고
    • P. Meakin, (Cambridge University Press, Cambridge, 1998). See Fig. 55.8b for an alternative realization of DF in (formula presented)
    • P. Meakin, Fractals, Scaling and Growth Far From Equilibrium (Cambridge University Press, Cambridge, 1998). See Fig. 55.8b for an alternative realization of DF in (formula presented)
  • 23
    • 85038938761 scopus 로고    scopus 로고
    • Our nonsymmetric choice of (formula presented) for (formula presented) dimensions, atoms at the top (formula presented) and at the bottom (formula presented) of saw-tooth profiles are not weighted equally. A symmetric choice with (formula presented) would produce modified behavior, perhaps more like in sc geometries
    • Our nonsymmetric choice of (formula presented) for (formula presented) dimensions, atoms at the top (formula presented) and at the bottom (formula presented) of saw-tooth profiles are not weighted equally. A symmetric choice with (formula presented) would produce modified behavior, perhaps more like in sc geometries.
  • 26
    • 85038944374 scopus 로고    scopus 로고
    • We have checked that behavior of a modified RDF model with only 4\0, 3\0, and 2\1 trap sites is similar to that of the RDF model analyzed here
    • We have checked that behavior of a modified RDF model with only 4\0, 3\0, and 2\1 trap sites is similar to that of the RDF model analyzed here.
  • 27
    • 85038936799 scopus 로고    scopus 로고
    • For the (formula presented) ballistic deposition (single-step) model (Ref. reaches about 0.7 (-1.3), and, reaches about 0.3 (0.3) at (formula presented) These models have KPZ scaling
    • For the (formula presented) ballistic deposition (single-step) model (Ref. 12), κ reaches about 0.7 (-1.3), and Q reaches about 0.3 (0.3) at (formula presented) These models have KPZ scaling.
  • 30
    • 0000151371 scopus 로고    scopus 로고
    • in Ref., estimate 0.13 eV for the (formula presented) pair bond energy. For refined estimates, see, and
    • J W. Evans and M C. Bartelt, in Ref. 1 estimate 0.13 eV for the (formula presented) pair bond energy. For refined estimates, see K A. Fichthorn and M. Scheffler, Phys. Rev. Lett.84, 5371 (2000).
    • (2000) Phys. Rev. Lett. , vol.84 , pp. 5371
    • Evans, J.W.1    Bartelt, M.C.2    Fichthorn, K.A.3    Scheffler, M.4


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.