-
3
-
-
77956694634
-
-
For higher temperatures, where evaporation of atoms from a step edge is active, this assumption needs to be critically checked, see below
-
For higher temperatures, where evaporation of atoms from a step edge is active, this assumption needs to be critically checked, see below.
-
-
-
-
21
-
-
77956673402
-
-
In contrast to [15] and [16, we do not treat the density of nuclei as an independent parameter, but we have eliminated the diffusion constant and deposition rate by using equation 5
-
In contrast to [15] and [16], we do not treat the density of nuclei as an independent parameter, but we have eliminated the diffusion constant and deposition rate by using equation (5).
-
-
-
-
22
-
-
77956660354
-
-
i+2], where η is the function given in Figure 6 of [17].
-
i+2], where η is the function given in Figure 6 of [17].
-
-
-
-
23
-
-
77956677918
-
-
k (i) = ((i + 2; k)) {dot operator} frac(sqrt(π) / 2, 2 i + 6 - k), where the ((i + 2; k)) are the binomial, coefficients.
-
k (i) = ((i + 2; k)) {dot operator} frac(sqrt(π) / 2, 2 i + 6 - k), where the ((i + 2; k)) are the binomial, coefficients.
-
-
-
-
24
-
-
77956683347
-
-
From Ref. [17], η=0.21 (0.23) at a coverage of 0.1 for i=1 (2).
-
From Ref. [17], η=0.21 (0.23) at a coverage of 0.1 for i=1 (2).
-
-
-
-
27
-
-
0040400869
-
-
and references therein
-
and references therein. Henzler M. Surf. Sci. 298 (1993) 369
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Esch S. PhD-thesis (1996), University of Bonn
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77956666051
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The entire high temperature layer-by-layer growth regime in Henzler's work is exclusively defined by two experiments at a single temperature. There is reason to suspect that these results are caused by artefacts see discussion in [51].
-
The entire high temperature layer-by-layer growth regime in Henzler's work is exclusively defined by two experiments at a single temperature. There is reason to suspect that these results are caused by artefacts (see discussion in [51].
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