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@ARTICLE{Krieger:1055123,
author = {Krieger, Ina and Sokolowski, Moritz and Haags, Anja and
Bredow, Thomas and Kumpf, Christian and Tautz, F. Stefan and
Held, Georg},
title = {{S}tructure analysis of {PTCDA}/{A}g(100) by low-energy
electron diffraction and density functional theory},
journal = {Physical review / B},
volume = {113},
number = {7},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2026-01872},
pages = {075425},
year = {2026},
abstract = {The adsorption geometry of the planar 3, 4, 9,
10-perylene-tetracarboxylic-dianhydride (PTCDA) moleculein
the commensurate c(8 × 8) structure on Ag(100) was
determined from the analysis of the intensities in
low-energy electron diffraction (LEED-IV). Using data from
different angles of incidence and optimized computercode, we
were able to overcome earlier challenges given by the
limitations of the experimental data set and thecalculation
times required for the large unit cell with many atoms.
Testing of different structures confirmed theon-top
adsorption site for the center of the perylene core. The
final Pendry R factor of RP = 0.180 for the on-topposition
is significantly lower than the one for the fourfold hollow
position (minimum RP = 0.369) that is henceexcluded. The
molecule shows archlike deformation with a downshift of the
terminal carboxylic groups. Boththe molecular structure and
the adsorption height are in very good agreement with
results from an earlier normalincidence x-ray standing wave
(NIXSW) experiment and new density functional theory (DFT)
calculations,which we performed in parallel for 0 K and in
addition for 300 K. The LEED-IV analysis demonstrates that
thePTCDA induces a relaxation (−0.08 versus −0.04 Å of
the clean surface) and buckling (0.33 Å) of the topmostAg
layer. Special attention was given to the Ag atom below the
central ring of the PTCDA. The IV analysiswas rather
insensitive to its vertical position, and a small R factor,
close to the minimal, was also obtainedwhen this Ag atom was
moved upward (RP = 0.185) or even an Ag vacancy site (RP =
0.171) was assumed.However, these structures could be
excluded on the basis of DFT calculations. The vacancy
structure has afree adsorption energy that is 0.18 eV larger
compared to the favored geometry where this central Ag atom
ispushed downward, partly due to the energy cost for the
vacancy formation. The discussion of
adsorbate-inducedformation of vacancy sites is important
because it was reported for C60 on Ag(111). The up- and
downwarddisplacements of the first-layer Ag atoms support
the understanding of the chemical bond of the PTCDA tothe Ag
substrate and reveal how the originally planar π system is
locally distorted. Our analysis proves thatLEED-IV is a
powerful technique for surface crystallography of large
organic adsorbates.},
cin = {PGI-3},
ddc = {530},
cid = {I:(DE-Juel1)PGI-3-20110106},
pnm = {5213 - Quantum Nanoscience (POF4-521)},
pid = {G:(DE-HGF)POF4-5213},
typ = {PUB:(DE-HGF)16},
doi = {10.1103/gxh1-b3w4},
url = {https://juser.fz-juelich.de/record/1055123},
}