Roughening of vicinal surfaces and step—step interactions: application to Cu(1,1,11) by means of statistical analysis of STM images

1996 ◽  
Vol 345 (1-2) ◽  
pp. 197-212 ◽  
Author(s):  
L. Barbier ◽  
L. Masson ◽  
J. Cousty ◽  
B. Salanon
1994 ◽  
Vol 317 (1-2) ◽  
pp. L1115-L1119 ◽  
Author(s):  
L. Masson ◽  
L. Barbier ◽  
J. Cousty ◽  
B. Salanon

2020 ◽  
Vol 20 (11) ◽  
pp. 7246-7259
Author(s):  
Hristina Popova ◽  
Filip Krzyżewski ◽  
Magdalena A. Załuska-Kotur ◽  
Vesselin Tonchev

1999 ◽  
Vol 06 (01) ◽  
pp. 27-34 ◽  
Author(s):  
MARGRET GIESEN ◽  
GEORG SCHULZE ICKING-KONERT

We have measured the terrace width distribution on copper (111) vicinal surfaces with (100) steps. For all surfaces, the distribution is well fitted by a Gaussian. The width of the Gaussian scales with the mean terrace width L, which is indicative of a repulsive 1/L2 interaction potential between steps. We determine an interaction strength of the potential of 3.2± 0.2 meV per atom length. From the temperature-dependent analysis of the step–step distance distribution, we find a kink formation energy for (100) steps of 0.12± 0.03 eV, which is consistent with previous measurements of the kink energy on copper (100) vicinal surfaces.


2001 ◽  
Vol 482-485 ◽  
pp. 1413-1418 ◽  
Author(s):  
F Raouafi ◽  
C Barreteau ◽  
M.C Desjonquères ◽  
D Spanjaard
Keyword(s):  

2001 ◽  
Vol 175-176 ◽  
pp. 62-68 ◽  
Author(s):  
T.L Einstein ◽  
Howard L Richards ◽  
Saul D Cohen ◽  
O Pierre-Louis ◽  
M Giesen

1993 ◽  
Vol 07 (24n25) ◽  
pp. 1547-1566 ◽  
Author(s):  
H.J.W. ZANDVLIET ◽  
H.B. ELSWIJK

The morphology of monatomic step edges on vicinal Si (001) surfaces is briefly reviewed. With increasing miscut angle, the Si (001) surface exhibits an interesting sequence of phase transitions. For a miscut angle smaller than about 0.03°, a hilly structure with step loops is found, whereas a phase of wavy steps coexisting with a phase of straight steps is observed in the range of 0.03°–0.1°. If the miscut angle lies in the range of 0.1° up to about 3°, two types, one much straighter than the other, of monatomic step edges develop. For even larger miscut angles, a phase of straight biatomic step edges is found. The fundamental energetic parameters, like kink formation energies, step edge energies and step-step interactions, which govern the thermodynamic behavior are determined using Scanning Tunneling Microscopy (STM) images of 0.5° misoriented Si (001). Despite the weak strength of energetic and entropic step-step interactions as compared to the interactions along the step edge, i.e. the kink formation and step edge energies, they have a profound effect on the meandering of the step edges. Both entropic and energetic step-step interactions are proportional to L−2 (where L is the average terrace length). The behavior of the step edges at temperatures above room temperature will be addressed with the aid of a high-temperature STM. The freeze-out temperature, T f , of the monatomic step edges is estimated to be higher than 600–700 K. The temperature T f is significantly above the roughening temperature, Tr, of the step edges. This means that at room temperature, the monatomic step edges on vicinal Si (001) are always rough.


1996 ◽  
Vol 54 (24) ◽  
pp. 17850-17857 ◽  
Author(s):  
J. Trost ◽  
T. Zambelli ◽  
J. Wintterlin ◽  
G. Ertl

2017 ◽  
Vol 2017 ◽  
pp. 1-10 ◽  
Author(s):  
Noriko Akutsu

The height profile of a macrostep on a vicinal surface near equilibrium is studied numerically using a restricted solid-on-solid model with a point-contact-type step-step attraction (p-RSOS model). We calculate the surface tension of vicinal surfaces around the (001) surface inclined towards the111direction using the density-matrix-renormalization group method. We also calculate the height profiles of vicinal surfaces using the Monte Carlo method and study the connection between the height profile of the macrostep near equilibrium and the discontinuous surface tension. We find that the height profile of a macrostep on a vicinal surface near equilibrium can be classified depending on the zone in the faceting diagram where the system exists. We also find finite size effects both for the height profile and for the inhibition of the macrostep motion in the relaxation process to the equilibrium state.


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