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35949011121
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19
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85038347993
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The energy barriers for ad-dimer diffusion along and across dimer rows are (formula presented) and (formula presented) respectively (see Refs., and, For adatom diffusion, they are (formula presented) and (formula presented) (Refs., and, For DV diffusion, they are 1.4–1.6 eV and (formula presented) (Refs., and
-
The energy barriers for ad-dimer diffusion along and across dimer rows are (formula presented) and (formula presented) respectively (see Refs. 20 and 21). For adatom diffusion, they are (formula presented) and (formula presented) (Refs. 22 and 23). For DV diffusion, they are 1.4–1.6 eV and (formula presented) (Refs. 24 and 25).
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22
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3342968424
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Y. Mo, J. Kleiner, M B. Webb, and M G. Lagally, Phys. Rev. Lett.66, 1998 (1991).
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Kleiner, J.2
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0026859649
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24
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12044254794
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Z. Zhang, H. Chen, B. Bolding, and M. Lagally, Phys. Rev. Lett.71, 3677 (1993).
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0037544054
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following paper
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G J. Xu, K S. Nakayama, B R. Trenhaile, C M. Aldao, and J H. Weaver, following paper, Phys. Rev. B67, 125321 (2003).
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Weaver, J.H.5
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27
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85038289325
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Images obtained for new areas and for small areas that were scanned dozens of times to follow reaction, image by image, gave no evidence of tip-induced changes for negative sample bias. See, however, Ref., for tunneling-electron-induced Br hopping for positive bias above 0.8 V
-
Images obtained for new areas and for small areas that were scanned dozens of times to follow reaction, image by image, gave no evidence of tip-induced changes for negative sample bias. See, however, Ref. 28 for tunneling-electron-induced Br hopping for positive bias above 0.8 V.
-
-
-
-
30
-
-
85038296410
-
-
B. S. Swartzentruber (private communication)
-
B. S. Swartzentruber (private communication).
-
-
-
-
31
-
-
85038337915
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-
E. Graugnard, K. S. Nakayama, and J. H. Weaver (unpublished)
-
E. Graugnard, K. S. Nakayama, and J. H. Weaver (unpublished).
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-
-
-
33
-
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85038318189
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-
Line profiles along AVLs showed that the distance between adjacent valleys or peaks was (formula presented) The positions of valleys or peaks in a line profile in a filled-state image were offset by (formula presented) compared to those in an empty-state image
-
Line profiles along AVLs showed that the distance between adjacent valleys or peaks was (formula presented) The positions of valleys or peaks in a line profile in a filled-state image were offset by (formula presented) compared to those in an empty-state image.
-
-
-
-
35
-
-
85038286371
-
-
Changes from (formula presented) to (formula presented) have also been observed, but this is a rare event
-
Changes from (formula presented) to (formula presented) have also been observed, but this is a rare event.
-
-
-
-
36
-
-
85038342302
-
-
The (formula presented) structure has never been observed for a clean Si(100) surface because these out-of-phase dimer rows are energetically unfavorable due to back bond stress
-
The (formula presented) structure has never been observed for a clean Si(100) surface because these out-of-phase dimer rows are energetically unfavorable due to back bond stress.
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-
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-
37
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-
0037179363
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-
reported that second-layer Si dimers in AVLs were Cl terminated. This would be surprising since Cl should impede the dynamic conversion between AVLs and DVLs. To confirm this we reexposed the sample to chlorine to saturate the surface. This quenched any further conversion
-
C F. Herrmann, D. Chen, and J J. Boland, Phys. Rev. Lett.89, 096102 (2002), reported that second-layer Si dimers in AVLs were Cl terminated. This would be surprising since Cl should impede the dynamic conversion between AVLs and DVLs. To confirm this we reexposed the sample to chlorine to saturate the surface. This quenched any further conversion.
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Phys. Rev. Lett.
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, pp. 96102
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Herrmann, C.F.1
Chen, D.2
Boland, J.J.3
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