% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Ikonomov:57110,
author = {Ikonomov, J. and Starbova, K. and Giesen, M.},
title = {{M}easurements of {S}tep and {K}ink {E}nergies and of the
{S}tep {E}dge {S}tiffness from {I}sland {S}tudies on
{P}t(111)},
journal = {Physical review / B},
volume = {75},
number = {24},
issn = {1098-0121},
address = {College Park, Md.},
publisher = {APS},
reportid = {PreJuSER-57110},
pages = {245411},
year = {2007},
note = {Record converted from VDB: 12.11.2012},
abstract = {By using temperature-variable scanning tunneling
microscopy, we studied two-dimensional vacancy islands on
Pt(111) between 593 and 713 K. Due to the difference in the
step free energies of A and B steps, the equilibrium shape
of the vacancy islands has a threefold symmetry. From the
analysis of the equilibrium shape of the vacancy islands, we
calculate the angular dependence of the step free energy on
Pt(111). The absolute values for the step free energies per
atom of A and B steps are determined from the equilibrium
shape fluctuations to be beta(A)=348 +/- 16 meV/atom and
beta(B)=300 +/- 14 meV/atom, respectively. Furthermore, we
derive the temperature dependence of the step-edge stiffness
(beta) over tilde with (beta) over tilde (A) between 510 and
453 meV/atom and (beta) over tilde (B) between 1974 and 1104
meV/atom in the temperature range considered. From the
stiffness, we obtain the kink formation energies for A and B
steps, epsilon(A)=143 +/- 9 meV and epsilon(B)=206 +/- 9
meV, respectively.},
keywords = {J (WoSType)},
cin = {IBN-4},
ddc = {530},
cid = {I:(DE-Juel1)VDB802},
pnm = {Kondensierte Materie},
pid = {G:(DE-Juel1)FUEK414},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000247625000110},
doi = {10.1103/PhysRevB.75.245411},
url = {https://juser.fz-juelich.de/record/57110},
}