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3
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-
0031077199
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S. Song et al., Surf. Sci. 372, 37 (1997).
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(1997)
Surf. Sci.
, vol.372
, pp. 37
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-
Song, S.1
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4
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-
0032136175
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M. Yoon et al., Surf. Sci. 411, 70 (1998).
-
(1998)
Surf. Sci.
, vol.411
, pp. 70
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-
Yoon, M.1
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7
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-
0034188497
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K. Sudoh et al., Surf. Sci. 452, L287 (2000);
-
(2000)
Surf. Sci.
, vol.452
, pp. L287
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-
Sudoh, K.1
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17
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-
85038994284
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-
Ab initio studies to capture the elastic interactions between steps on the (113) surfaces would require prohibitive amounts of computational resources
-
Ab initio studies to capture the elastic interactions between steps on the (113) surfaces would require prohibitive amounts of computational resources.
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-
-
-
22
-
-
85038983050
-
-
This potential (T3) was used in the coupling scheme because its elastic constants are close to the tight-binding values (Ref. 13)
-
This potential (T3) was used in the coupling scheme because its elastic constants are close to the tight-binding values (Ref. 13).
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-
-
-
23
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-
0001018655
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-
Implementation details of this multiscale procedure will be reported elsewhere. A similar coupling scheme, though not self-consistent, was used by, to compute the formation energy of the dimer vacancies on Si(001)
-
Implementation details of this multiscale procedure will be reported elsewhere. A similar coupling scheme, though not self-consistent, was used by J. Wang et al., Phys. Rev. B 47, 10 497 (1993) to compute the formation energy of the dimer vacancies on Si(001).
-
(1993)
Phys. Rev. B
, vol.47
, pp. 10 497
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-
Wang, J.1
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24
-
-
85038982399
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b is the tight-binding cohesive energy, which was chosen as the common scale for expressing the total energy
-
b is the tight-binding cohesive energy, which was chosen as the common scale for expressing the total energy.
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-
-
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26
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0000319431
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[JETP 52, 129 (1980)].
-
(1980)
JETP
, vol.52
, pp. 129
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-
-
27
-
-
85039013553
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(Formula presented) (see Fig. 11) is the projected surface energy of Si(114)
-
(Formula presented) (see Fig. 11) is the projected surface energy of Si(114).
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-
-
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29
-
-
85038991255
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1 < 10. Beyond this range, the theory developed in Ref. 7 shows that the periodicity of the bunch structures exceeds the experimental observations (100–1000 Å) (Refs. 1 and 2) by nearly 2 orders of magnitude
-
1 < 10. Beyond this range, the theory developed in Ref. 7 shows that the periodicity of the bunch structures exceeds the experimental observations (100–1000 Å) (Refs. 1 and 2) by nearly 2 orders of magnitude.
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-
-
-
30
-
-
85038974268
-
-
n is closely related to the edge energy (Ref. 7), and should not depend on the number of steps within the bunch
-
n is closely related to the edge energy (Ref. 7), and should not depend on the number of steps within the bunch.
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