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2
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0032649994
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Surf. Sci.M. Kalff, P. Smilauer, G. Comsa, and T. Michely, 426, L447 (1999).
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Surf. Sci.
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Kalff, M.1
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Michely, T.4
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3
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0032070380
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C.-M. Zhang, M C. Bartelt, J.-M. Wen, C J. Jenks, J W. Evans, and P A. Thiel, Surf. Sci.406, 178 (1998);
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M, C.1
Bartelt, M.C.2
M, J.3
Jenks, C.J.4
Evans, J.W.5
Thiel, P.A.6
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4
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0001229243
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L. Bardotti, C R. Stoldt, C J. Jenks, M C. Bartelt, J W. Evans, and P A. Thiel, Phys. Rev. B57, 12 544 (1998).
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Phys. Rev. B
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Bardotti, L.1
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7
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0000697488
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K. Bormann, H. Brune, H. Röder, and K. Kern, Phys. Rev. Lett.75, 677 (1995).
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Bormann, K.1
Brune, H.2
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11
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85038287414
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A. Pimpinelli and J. Villain, (Cambridge University Press, Cambridge, England, 1998)
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A. Pimpinelli and J. Villain, Physics of Crystal Growth (Cambridge University Press, Cambridge, England, 1998).
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12
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85038328105
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T. Michely and J. Krug, (Springer, Berlin, 2003)
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T. Michely and J. Krug, Islands, Mounds and Atoms: Crystal Growth Far From Equilibrium (Springer, Berlin, 2003).
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13
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3643103938
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J. Jacobsen, K W. Jacobsen, P. Stoltze, and J K. Nørskov, Phys. Rev. Lett.74, 2295 (1995).
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17
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85038343767
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B. Poelsema and S. van Dijken, in, edited by M. Kotrla, N. I. Papanicolau, D. D. Vvedenski, and L. T. Wille (Kluwer Academic, Dordrecht, 2002), p. 165
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B. Poelsema and S. van Dijken, in Atomistic Aspects of Epitaxial Growth, edited by M. Kotrla, N. I. Papanicolau, D. D. Vvedenski, and L. T. Wille (Kluwer Academic, Dordrecht, 2002), p. 165.
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20
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85038272787
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When the ES length is large, we can neglect the term (formula presented) appearing in its general definition
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When the ES length is large, we can neglect the term (formula presented) appearing in its general definition.
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21
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85038321084
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With respect to our previous Refs., and, we have introduced the hopping rate (formula presented) rather than the diffusion constant (formula presented) in the expression (2) of the residence time. Therefore the new (formula presented) and (formula presented) are four times larger than the old ones
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With respect to our previous Refs. 5 and 6, we have introduced the hopping rate (formula presented) rather than the diffusion constant (formula presented) in the expression (2) of the residence time. Therefore the new (formula presented) and (formula presented) are four times larger than the old ones.
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22
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85038327259
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This is not true if the particle is initially confined to the edge of the terrace, but this case is not practically relevant
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This is not true if the particle is initially confined to the edge of the terrace, but this case is not practically relevant.
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23
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85038321744
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B. D. Hughes, (Clarendon, Oxford, 1995)
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B. D. Hughes, Random Walks and Random Environments (Clarendon, Oxford, 1995).
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25
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85038341609
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In Eq. (15) we are neglecting the existence of a kink between neighboring straight steps
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In Eq. (15) we are neglecting the existence of a kink between neighboring straight steps.
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27
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85038328672
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T. Michely (private communication)
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T. Michely (private communication).
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29
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85038291003
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Experimental data are (formula presented) as well, but they cannot be used in the present context, because (formula presented) for all observed islands
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Experimental data are available at (formula presented) as well, but they cannot be used in the present context, because (formula presented) for all observed islands.
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38
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85038314658
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Because of kinetic effects the number of kinks should decrease with increasing., Because of thermodynamical effects, it should increase, but (formula presented) is much smaller than the kink energy
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Because of kinetic effects the number of kinks should decrease with increasing T. Because of thermodynamical effects, it should increase, but (formula presented) is much smaller than the kink energy.
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41
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0000099859
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K. Morgenstern, G. Rosenfeld, E. Lægsgaard, F. Besenbacher, and G. Comsa, Phys. Rev. Lett.80, 556 (1998).
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(1998)
Phys. Rev. Lett.
, vol.80
, pp. 556
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Morgenstern, K.1
Rosenfeld, G.2
Lægsgaard, E.3
Besenbacher, F.4
Comsa, G.5
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