-
1
-
-
0037138514
-
-
10.1016/S0039-6028(01)01805-2
-
A. Eichler, Surf. Sci. 498, 314 (2002). 10.1016/S0039-6028(01)01805-2
-
(2002)
Surf. Sci.
, vol.498
, pp. 314
-
-
Eichler, A.1
-
2
-
-
3743127068
-
-
10.1021/cr00035a012
-
R. Imbihl and G. Ertl, Chem. Rev. 95, 697 (1995). 10.1021/cr00035a012
-
(1995)
Chem. Rev.
, vol.95
, pp. 697
-
-
Imbihl, R.1
Ertl, G.2
-
4
-
-
0017504557
-
-
10.1007/BF00882473
-
H. Froitzheim, H. Hopster, H. Ibach, and S. Lehwald, Appl. Phys. (Berlin) 13, 147 (1977). 10.1007/BF00882473
-
(1977)
Appl. Phys. (Berlin)
, vol.13
, pp. 147
-
-
Froitzheim, H.1
Hopster, H.2
Ibach, H.3
Lehwald, S.4
-
8
-
-
0035837035
-
-
10.1021/jp002302t, and references herein.
-
P. J. Feibelman, B. Hammer, J. K. Norskov, F. Wagner, M. Scheffler, R. Stumpf, R. Watwe, and J. Dumesic, J. Phys. Chem. B 105, 4018 (2001) 10.1021/jp002302t
-
(2001)
J. Phys. Chem. B
, vol.105
, pp. 4018
-
-
Feibelman, P.J.1
Hammer, B.2
Norskov, J.K.3
Wagner, F.4
Scheffler, M.5
Stumpf, R.6
Watwe, R.7
Dumesic, J.8
-
9
-
-
0037115973
-
-
10.1103/PhysRevB.66.235409
-
P. van Beurden, H. G. J. Verhoeven, G. J. Kramer, and B. J. Thijsse, Phys. Rev. B 66, 235409 (2002). 10.1103/PhysRevB.66.235409
-
(2002)
Phys. Rev. B
, vol.66
, pp. 235409
-
-
Van Beurden, P.1
Verhoeven, H.G.J.2
Kramer, G.J.3
Thijsse, B.J.4
-
10
-
-
40849134058
-
-
10.1103/PhysRevB.77.085414
-
M. Alaei, H. Akbarzadeh, H. Gholizadeh, and S. de Gironcoli, Phys. Rev. B 77, 085414 (2008). 10.1103/PhysRevB.77.085414
-
(2008)
Phys. Rev. B
, vol.77
, pp. 085414
-
-
Alaei, M.1
Akbarzadeh, H.2
Gholizadeh, H.3
De Gironcoli, S.4
-
12
-
-
0030189250
-
-
10.1016/0039-6028(96)00590-0
-
M. L. Bocquet and P. Sautet, Surf. Sci. 360, 128 (1996). 10.1016/0039-6028(96)00590-0
-
(1996)
Surf. Sci.
, vol.360
, pp. 128
-
-
Bocquet, M.L.1
Sautet, P.2
-
13
-
-
0000544665
-
-
10.1016/S0009-2614(98)01318-9
-
M. Ø. Pedersen, M.-L. Bocquet, P. Sautet, E. Lægsgaard, I. Stensgaard, and F. Besenbacher, Chem. Phys. Lett. 299, 403 (1999). 10.1016/S0009-2614(98)01318-9
-
(1999)
Chem. Phys. Lett.
, vol.299
, pp. 403
-
-
Pedersen M.Ø1
Bocquet, M.-L.2
Sautet, P.3
Lægsgaard, E.4
Stensgaard, I.5
Besenbacher, F.6
-
14
-
-
0347477186
-
-
10.1063/1.1630383
-
O. Gurlu, O. A. O. Adam, H. J. W. Zandvliet, and B. Poelsema, Appl. Phys. Lett. 83, 4610 (2003). 10.1063/1.1630383
-
(2003)
Appl. Phys. Lett.
, vol.83
, pp. 4610
-
-
Gurlu, O.1
Adam, O.A.O.2
Zandvliet, H.J.W.3
Poelsema, B.4
-
15
-
-
33750008663
-
-
10.1016/j.susc.2006.07.055
-
N. Öncel, W. J. van Beek, J. Huijben, B. Poelsema, and H. J. W. Zandvliet, Surf. Sci. 600, 4690 (2006). 10.1016/j.susc.2006.07.055
-
(2006)
Surf. Sci.
, vol.600
, pp. 4690
-
-
Öncel, N.1
Van Beek, W.J.2
Huijben, J.3
Poelsema, B.4
Zandvliet, H.J.W.5
-
17
-
-
50049103972
-
-
10.1103/PhysRevB.78.085421
-
G. Sclauzero, A. Dal Corso, A. Smogunov, and E. Tosatti, Phys. Rev. B 78, 085421 (2008). 10.1103/PhysRevB.78.085421
-
(2008)
Phys. Rev. B
, vol.78
, pp. 085421
-
-
Sclauzero, G.1
Dal Corso, A.2
Smogunov, A.3
Tosatti, E.4
-
20
-
-
0001382287
-
-
10.1016/S0368-2048(97)00124-2
-
K. Fukutani, T. T. Magkoev, Y. Murata, M. Matsumoto, T. Kawauchi, T. Magome, Y. Tezuka, and S. Shin, J. Electron Spectrosc. Relat. Phenom. 88-91, 597 (1998). 10.1016/S0368-2048(97)00124-2
-
(1998)
J. Electron Spectrosc. Relat. Phenom.
, vol.8891
, pp. 597
-
-
Fukutani, K.1
Magkoev, T.T.2
Murata, Y.3
Matsumoto, M.4
Kawauchi, T.5
Magome, T.6
Tezuka, Y.7
Shin, S.8
-
22
-
-
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
-
23
-
-
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
-
24
-
-
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
-
28
-
-
77956313222
-
-
The NW at the edge of a NW array next to bare β terrace, just like a solitary NW, does not present the 4×1 periodicity typical for NWs in a NW array. It was argued in Ref. that these edge NWs might have the same geometry as the solitary NWs. The latter could be understood to be an extreme case of a NW array, i.e., one only consisting of its edge. Because of this, we will refer to both solitary and edge NWs as solitary NWs while array NWs refers to the none-edge NWs of a NW array.
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The NW at the edge of a NW array next to bare β terrace, just like a solitary NW, does not present the 4 × 1 periodicity typical for NWs in a NW array. It was argued in Ref. that these edge NWs might have the same geometry as the solitary NWs. The latter could be understood to be an extreme case of a NW array, i.e., one only consisting of its edge. Because of this, we will refer to both solitary and edge NWs as solitary NWs while array NWs refers to the none-edge NWs of a NW array.
-
-
-
-
29
-
-
43849108614
-
-
10.1016/j.susc.2008.01.040
-
A. van Houselt, T. Gnielka, J. M. J. Aan de Brugh, N. Öncel, D. Kockmann, R. Heid, K. P. Bohnen, B. Poelsema, and H. Zandvliet, Surf. Sci. 602, 1731 (2008). 10.1016/j.susc.2008.01.040
-
(2008)
Surf. Sci.
, vol.602
, pp. 1731
-
-
Van Houselt, A.1
Gnielka, T.2
Aan De Brugh, J.M.J.3
Öncel, N.4
Kockmann, D.5
Heid, R.6
Bohnen, K.P.7
Poelsema, B.8
Zandvliet, H.9
-
31
-
-
0013457036
-
-
10.1103/PhysRevB.66.155438
-
R. Hirschl, F. Delbecq, P. Sautet, and J. Hafner, Phys. Rev. B 66, 155438 (2002). 10.1103/PhysRevB.66.155438
-
(2002)
Phys. Rev. B
, vol.66
, pp. 155438
-
-
Hirschl, R.1
Delbecq, F.2
Sautet, P.3
Hafner, J.4
-
32
-
-
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Two surface unit cells are shown in Fig. .
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Two surface unit cells are shown in Fig..
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34
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77956313942
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Ph.D. thesis University of Twente
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N. Öncel, Ph.D. thesis, University of Twente, 2007.
-
(2007)
-
-
Öncel, N.1
-
35
-
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The computational cost to calculate diffusion barriers between these intermediate steps is, due to the system size, too large, so no diffusion barriers were calculated.
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The computational cost to calculate diffusion barriers between these intermediate steps is, due to the system size, too large, so no diffusion barriers were calculated.
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36
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77956313751
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In our limited surface cell the NW dimers could not spread further before colliding with periodic copies, limiting the width of the depression to ∼8 Å
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In our limited surface cell the NW dimers could not spread further before colliding with periodic copies, limiting the width of the depression to ∼ 8 Å
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