-
2
-
-
3342968424
-
-
Y W. Mo, J. Kleiner, M B. Webb, M G. Lagally, Phys. Rev. Lett.66, 1998 (1991).
-
(1991)
Phys. Rev. Lett.
, vol.66
, pp. 1998
-
-
Mo, Y.W.1
Kleiner, J.2
Webb, M.B.3
Lagally, M.G.4
-
6
-
-
4043180426
-
-
R Q. Hwang, J. Schroder, C. Gunther, and R J. Behm, Phys. Rev. Lett.67, 3279 (1991)
-
(1991)
Phys. Rev. Lett.
, vol.67
, pp. 3279
-
-
Hwang, R.Q.1
Schroder, J.2
Gunther, C.3
Behm, R.J.4
-
9
-
-
0027558079
-
-
E. Kopatzki, S. Gunther, W. Nichtl-Pecher, and R J. Behm, Surf. Sci.284, 154 (1993).
-
(1993)
Surf. Sci.
, vol.284
, pp. 154
-
-
Kopatzki, E.1
Gunther, S.2
Nichtl-Pecher, W.3
Behm, R.J.4
-
10
-
-
3342882885
-
-
G. Rosenfeld, R. Servaty, C. Teichert, B. Poelsema, and G. Comsa, Phys. Rev. Lett.71, 895 (1993).
-
(1993)
Phys. Rev. Lett.
, vol.71
, pp. 895
-
-
Rosenfeld, G.1
Servaty, R.2
Teichert, C.3
Poelsema, B.4
Comsa, G.5
-
16
-
-
4243241445
-
-
F. Tsui, J. Wellman, C. Uher, and R. Clarke, Phys. Rev. Lett.76, 3164 (1996).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 3164
-
-
Tsui, F.1
Wellman, J.2
Uher, C.3
Clarke, R.4
-
17
-
-
3442879159
-
-
T R. Linderoth, S. Horch, E. Laegsgaard, I. Stensgaard, and F. Besenbacher, Phys. Rev. Lett.78, 4978 (1997).
-
(1997)
Phys. Rev. Lett.
, vol.78
, pp. 4978
-
-
Linderoth, T.R.1
Horch, S.2
Laegsgaard, E.3
Stensgaard, I.4
Besenbacher, F.5
-
33
-
-
0001378388
-
-
C. Ratsch, A. Zangwill, P. Smilauer, and D D. Vvedensky, Phys. Rev. Lett.72, 3194 (1994).
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 3194
-
-
Ratsch, C.1
Zangwill, A.2
Smilauer, P.3
Vvedensky, D.D.4
-
38
-
-
11544344891
-
-
M C. Bartelt, A K. Schmid, J W. Evans, and R Q. Hwang, Phys. Rev. Lett.81, 1901 (1998).
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 1901
-
-
Bartelt, M.C.1
Schmid, A.K.2
Evans, J.W.3
Hwang, R.Q.4
-
50
-
-
85038303531
-
-
The exact term to account for the monomer-monomer collision rate in Eqs. (678) is (formula presented) that leads to a nonlinear diffusion equation which may be solved numerically (see Ref. In order to obtain a linear equation the mean-field approximation (formula presented) is used (see also Ref
-
The exact term to account for the monomer-monomer collision rate in Eqs. (678) is (formula presented) that leads to a nonlinear diffusion equation which may be solved numerically (see Ref. 41). In order to obtain a linear equation the mean-field approximation (formula presented) is used (see also Ref. 20).
-
-
-
-
53
-
-
85038273475
-
-
The, dependence of (formula presented) can be neglected because it is much smaller than that due to the terms depending on (formula presented)
-
The A dependence of (formula presented) can be neglected because it is much smaller than that due to the terms depending on (formula presented)
-
-
-
-
55
-
-
0001601882
-
-
Phys. Rev. BM C. Bartelt, C R. Stoldt, C J. Jenks, P A. Thiel, and J W. Evans, 59, 3125 (1999).
-
(1999)
Phys. Rev. B
, vol.59
, pp. 3125
-
-
Bartelt, M.C.1
Stoldt, C.R.2
Jenks, C.J.3
Thiel, P.A.4
Evans, J.W.5
-
56
-
-
85038305903
-
-
Coalescence effects (see Fig. 22) are also important starting at coverages around 0.18. While the KMC simulations naturally include coalescence, the rate equations do not include terms to account for such effects
-
Coalescence effects (see Fig. 22) are also important starting at coverages around 0.18. While the KMC simulations naturally include coalescence, the rate equations do not include terms to account for such effects.
-
-
-
-
57
-
-
85038305772
-
-
The condition (formula presented) is required by the definition of the average capture number along with the normalization of the island-size distribution function
-
The condition (formula presented) is required by the definition of the average capture number along with the normalization of the island-size distribution function.
-
-
-
-
58
-
-
85038324275
-
-
A decreasing value of (formula presented) with increasing coverage for irreversible growth of extended islands has been seen previously experimentally (Ref. as well as in KMC simulations. (Ref
-
A decreasing value of (formula presented) with increasing coverage for irreversible growth of extended islands has been seen previously experimentally (Ref. 3) as well as in KMC simulations. (Ref. 16).
-
-
-
-
59
-
-
85038298417
-
-
Summing Eq. (36) over all (formula presented), without any correction to ensure that the normalization condition (formula presented) is satisfied, one obtains (formula presented), where (formula presented) is the Heaviside step function. While this distribution satisfies the normalization condition (formula presented), it has very little resemblance to the correct Voronoi-area distribution and leads to a divergent average Voronoi area
-
Summing Eq. (36) over all (formula presented), without any correction to ensure that the normalization condition (formula presented) is satisfied, one obtains (formula presented), where (formula presented) is the Heaviside step function. While this distribution satisfies the normalization condition (formula presented), it has very little resemblance to the correct Voronoi-area distribution and leads to a divergent average Voronoi area.
-
-
-
|