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Volumn 4, Issue 4, 1998, Pages 401-404

Logarithmic islanding in submonolayer epitaxial growth

Author keywords

36.40.Sx Diffusion and dynamics of clusters; 66.30.Fq Self diffusion in metals, semimetals, and alloys; 68.35.Fx Diffusion; interface formation

Indexed keywords


EID: 0347809947     PISSN: 14346028     EISSN: None     Source Type: Journal    
DOI: 10.1007/s100510050395     Document Type: Article
Times cited : (28)

References (22)
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    • Morgenstern, K.1    Rosenfeld, G.2    Poelsema, B.3    Comsa, G.4
  • 4
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    • K. Morgenstern, G. Rosenfeld, B. Poelsema, G. Comsa, Phys. Rev. Lett. 74, 2058 (1995); J.M. Wen, J.W. Evans, M.C. Bartelt, J.W. Burnett, P.A. Thiel, Phys. Rev. Lett. 76, 652 (1996); W.W. Pai, A.K. Swan, Z. Zhang, J.F. Wendelken, Phys. Rev. Lett. 79, 3210 (1997).
    • (1996) Phys. Rev. Lett. , vol.76 , pp. 652
    • Wen, J.M.1    Evans, J.W.2    Bartelt, M.C.3    Burnett, J.W.4    Thiel, P.A.5
  • 5
    • 0001718659 scopus 로고    scopus 로고
    • K. Morgenstern, G. Rosenfeld, B. Poelsema, G. Comsa, Phys. Rev. Lett. 74, 2058 (1995); J.M. Wen, J.W. Evans, M.C. Bartelt, J.W. Burnett, P.A. Thiel, Phys. Rev. Lett. 76, 652 (1996); W.W. Pai, A.K. Swan, Z. Zhang, J.F. Wendelken, Phys. Rev. Lett. 79, 3210 (1997).
    • (1997) Phys. Rev. Lett. , vol.79 , pp. 3210
    • Pai, W.W.1    Swan, A.K.2    Zhang, Z.3    Wendelken, J.F.4
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    • edited by L. Pietronero, E. Tosatti Elsevier, Amsterdam
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    • The inclusion of this logarithmic factor ultimately leads to the flux rescaling F → F ln(1/F) in our primary results given in equations (8) (P.L. Krapivsky, J.F.F. Mendes, S. Redner, in preparation)
    • The inclusion of this logarithmic factor ultimately leads to the flux rescaling F → F ln(1/F) in our primary results given in equations (8) (P.L. Krapivsky, J.F.F. Mendes, S. Redner, in preparation).
  • 14
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    • Similar rate equations describe the model of mobile adatoms and immobile islands, leading to somewhat similar island mass distribution. See e.g., N.V. Brilliantov, P.L. Krapivsky, J. Phys. A 24, 4787 (1991); J.A. Blackman, A. Wielding, Europhys. Lett. 16, 115 (1991); M.C. Bartelt, J.W. Evans, Phys. Rev. B 46, 12675 (1992).
    • (1991) J. Phys. A , vol.24 , pp. 4787
    • Brilliantov, N.V.1    Krapivsky, P.L.2
  • 15
    • 84956259961 scopus 로고
    • Similar rate equations describe the model of mobile adatoms and immobile islands, leading to somewhat similar island mass distribution. See e.g., N.V. Brilliantov, P.L. Krapivsky, J. Phys. A 24, 4787 (1991); J.A. Blackman, A. Wielding, Europhys. Lett. 16, 115 (1991); M.C. Bartelt, J.W. Evans, Phys. Rev. B 46, 12675 (1992).
    • (1991) Europhys. Lett. , vol.16 , pp. 115
    • Blackman, J.A.1    Wielding, A.2
  • 16
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    • Similar rate equations describe the model of mobile adatoms and immobile islands, leading to somewhat similar island mass distribution. See e.g., N.V. Brilliantov, P.L. Krapivsky, J. Phys. A 24, 4787 (1991); J.A. Blackman, A. Wielding, Europhys. Lett. 16, 115 (1991); M.C. Bartelt, J.W. Evans, Phys. Rev. B 46, 12675 (1992).
    • (1992) Phys. Rev. B , vol.46 , pp. 12675
    • Bartelt, M.C.1    Evans, J.W.2
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    • Note, however, that within the point-island description, the submonolayer regime is defined by the less stringent criterion N ≪ 1. This means that relatively long simulations are still within the submonolayer regime (Fig. 1)
    • Note, however, that within the point-island description, the submonolayer regime is defined by the less stringent criterion N ≪ 1. This means that relatively long simulations are still within the submonolayer regime (Fig. 1).
  • 21
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    • J. Villain, A. Pimpinelli, D.E. Wolf, Comments Cond. Mat. Phys. 16, 1 (1992); I. Furman, O. Biham, Phys. Rev. B 55, 7917 (1997).
    • (1997) Phys. Rev. B , vol.55 , pp. 7917
    • Furman, I.1    Biham, O.2


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