-
1
-
-
33751299299
-
-
10.1103/PhysRevLett.97.215501
-
A. T. N'Diaye, S. Bleikamp, P. J. Feibelman, and T. Michely, Phys. Rev. Lett. 97, 215501 (2006). 10.1103/PhysRevLett.97.215501
-
(2006)
Phys. Rev. Lett.
, vol.97
, pp. 215501
-
-
N'Diaye, A.T.1
Bleikamp, S.2
Feibelman, P.J.3
Michely, T.4
-
2
-
-
42449143086
-
-
10.1103/PhysRevB.77.165419
-
P. J. Feibelman, Phys. Rev. B 77, 165419 (2008). 10.1103/PhysRevB.77. 165419
-
(2008)
Phys. Rev. B
, vol.77
, pp. 165419
-
-
Feibelman, P.J.1
-
3
-
-
10644250257
-
-
10.1103/PhysRev.136.B864
-
P. Hohenberg and W. Kohn, Phys. Rev. 136, B864 (1964). 10.1103/PhysRev.136.B864
-
(1964)
Phys. Rev.
, vol.136
, pp. 864
-
-
Hohenberg, P.1
Kohn, W.2
-
4
-
-
0042113153
-
-
10.1103/PhysRev.140.A1133
-
W. Kohn and L. J. Sham, Phys. Rev. 140, A1133 (1965). 10.1103/PhysRev.140.A1133
-
(1965)
Phys. Rev.
, vol.140
, pp. 1133
-
-
Kohn, W.1
Sham, L.J.2
-
5
-
-
0003754095
-
-
edited by P. Ziesche and H. Eschrig (Akademie Verlag, Berlin
-
J. P. Perdew, in Electronic Structure of Solids '91, edited by, P. Ziesche, and, H. Eschrig, (Akademie Verlag, Berlin, 1991)
-
(1991)
Electronic Structure of Solids '91
-
-
Perdew, J.P.1
-
6
-
-
23244460838
-
-
10.1103/PhysRevB.46.6671;
-
J. P. Perdew, J. A. Chevary, S. H. Vosko, K. A. Jackson, M. R. Pederson, D. J. Singh, and C. Fiolhais, Phys. Rev. B 46, 6671 (1992) 10.1103/PhysRevB.46. 6671
-
(1992)
Phys. Rev. B
, vol.46
, pp. 6671
-
-
Perdew, J.P.1
Chevary, J.A.2
Vosko, S.H.3
Jackson, K.A.4
Pederson, M.R.5
Singh, D.J.6
Fiolhais, C.7
-
7
-
-
0001622167
-
-
10.1103/PhysRevB.48.4978.2
-
J. P. Perdew, J. A. Chevary, S. H. Vosko, K. A. Jackson, M. R. Pederson, D. J. Singh, and C. Fiolhais, Phys. Rev. B 48, 4978 (1993). 10.1103/PhysRevB.48. 4978.2
-
(1993)
Phys. Rev. B
, vol.48
, pp. 4978
-
-
Perdew, J.P.1
Chevary, J.A.2
Vosko, S.H.3
Jackson, K.A.4
Pederson, M.R.5
Singh, D.J.6
Fiolhais, C.7
-
9
-
-
26144450583
-
-
as parametrized by 10.1103/PhysRevB.23.5048
-
as parametrized by J. P. Perdew and A. Zunger, Phys. Rev. B 23, 5048 (1981). 10.1103/PhysRevB.23.5048
-
(1981)
Phys. Rev. B
, vol.23
, pp. 5048
-
-
Perdew, J.P.1
Zunger, A.2
-
10
-
-
12844286241
-
-
10.1103/PhysRevB.47.558;
-
G. Kresse and J. Hafner, Phys. Rev. B 47, 558 (1993) 10.1103/PhysRevB.47. 558
-
(1993)
Phys. Rev. B
, vol.47
, pp. 558
-
-
Kresse, G.1
Hafner, J.2
-
11
-
-
27744460065
-
-
10.1103/PhysRevB.49.14251
-
G. Kresse and J. Hafner, Phys. Rev. B 49, 14251 (1994). 10.1103/PhysRevB.49.14251
-
(1994)
Phys. Rev. B
, vol.49
, pp. 14251
-
-
Kresse, G.1
Hafner, J.2
-
14
-
-
25744460922
-
-
10.1103/PhysRevB.50.17953
-
P. E. Blöchl, Phys. Rev. B 50, 17953 (1994). 10.1103/PhysRevB.50. 17953
-
(1994)
Phys. Rev. B
, vol.50
, pp. 17953
-
-
Blöchl, P.E.1
-
15
-
-
0011236321
-
-
10.1103/PhysRevB.59.1758
-
G. Kresse and D. Joubert, Phys. Rev. B 59, 1758 (1999). 10.1103/PhysRevB.59.1758
-
(1999)
Phys. Rev. B
, vol.59
, pp. 1758
-
-
Kresse, G.1
Joubert, D.2
-
18
-
-
70349447769
-
-
The "hcp region" of the moiré is where the C atoms reside close to directly atop either a surface layer Ir atom or an fcc threefold hollow. Accordingly, subsurface Ir atoms (colored red in Figs. 1 2) can be seen through C-atom hexagons in the hcp region. Similarly, third-layer Ir adatoms (colored green in Figs. 1 2) are seen through C-atom hexagons in the "fcc region" of the moiré, and surface Ir adatoms are visible through the C-atom hexagons in the "atop region." According to Ref., Ir islands on graphene/Ir(111) equilibrate in the hcp region of the moiré.
-
The "hcp region" of the moiré is where the C atoms reside close to directly atop either a surface layer Ir atom or an fcc threefold hollow. Accordingly, subsurface Ir atoms (colored red in Figs. 1 2) can be seen through C-atom hexagons in the hcp region. Similarly, third-layer Ir adatoms (colored green in Figs. 1 2) are seen through C-atom hexagons in the "fcc region" of the moiré, and surface Ir adatoms are visible through the C-atom hexagons in the "atop region." According to Ref., Ir islands on graphene/Ir(111) equilibrate in the hcp region of the moiré.
-
-
-
-
19
-
-
12044253536
-
-
For a perspective on kinetically driven transitions from 2D to 3D island growth in homoepitaxy, see, e.g., 10.1103/PhysRevLett.72.266
-
For a perspective on kinetically driven transitions from 2D to 3D island growth in homoepitaxy, see, e.g., J. Tersoff, A. W. Denier van der Gon, and R. M. Tromp, Phys. Rev. Lett. 72, 266 (1994). 10.1103/PhysRevLett.72.266
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 266
-
-
Tersoff, J.1
Van Der Gon, A.W.D.2
Tromp, R.M.3
-
22
-
-
0033750166
-
-
10.1016/S0079-6816(00)00017-4
-
T. T. Tsong, Prog. Surf. Sci. 64, 199 (2000), Table 2 quotes an excess barrier, relative to terrace diffusion, of about 0.2 eV to descend a step on pure Ir(111). 10.1016/S0079-6816(00)00017-4
-
(2000)
Prog. Surf. Sci.
, vol.64
, pp. 199
-
-
Tsong, T.T.1
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