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@ARTICLE{Soubatch:19536,
author = {Soubatch, S. and Kröger, I. and Kumpf, C. and Tautz, F.S.},
title = {{S}tructure and growth of tetracene on {A}g(111)},
journal = {Physical review / B},
volume = {84},
number = {19},
issn = {1098-0121},
address = {College Park, Md.},
publisher = {APS},
reportid = {PreJuSER-19536},
pages = {195440},
year = {2011},
note = {We thank M. Sokolowski (University of Bonn), B. Voigtlander
(Forschungszentrum Julich), G. Meyer (IBM Research, Zurich),
and S. Folsch (Paul-Drude-Institute, Berlin) for helpful
discussion. This work was partially supported by the
Deutsche Forschungsgemeinschaft (DFG) via priority program
1121 "Organic field effect transistors: structural and
dynamic properties" and the project TA244.},
abstract = {The structure of the tetracene/Ag(111) interface in the
coverage range theta = 0 to 2.4 ML is studied with scanning
tunneling microscopy (STM) at 8 K and with low energy
electron diffraction (LEED) at T = 300 ... 100 K. For theta
less than or similar to 0.01 ML, one-dimensional (1D)
diffusion of single molecules along < 01 (1) over bar
>-directions is observed even at 8 K. For 0.1 ML < theta <
0.5 ML molecules are homogeneously distributed over the
surface forming a disordered phase (static at T = 8 K,
dynamic at T = 25 K), indicating a repulsive intermolecular
interaction (delta-phase). For theta greater than or similar
to 0.5 ML, local ordering in the commensurate gamma-phase is
observed. Further increase of the coverage yields a
compressed monolayer (ML) phase (theta = 1 ML) with
point-on-line registry (alpha-phase). The interaction
between molecules has been calculated with the force-field
approach to rationalize the molecular packing motifs in the
various phases. Under most circumstances molecule-molecule
interactions are repulsive, in agreement with experimental
findings. A simulation of the adsorption up to theta = 1 ML
according to the random sequential adsorption (RSA)
algorithm shows that the disorder-to-order transition from
the delta- to gamma-phase occurs close to random close
packing (RCP), theta = 0.5-0.6 ML. Since tetracene molecules
are a two-dimensional (2D) representation of Onsager's hard
rod model, this suggests that this phase transition is
driven both energetically and entropically. For theta
approximate to 2.23 ML a metastable bilayer phase with
point-on-line coincidence is observed (beta-phase). The
basic structural unit of this phase is a triplet of
molecules that are tilted along the long molecular axis
against each other; at least one of these molecules is
tilted out of the surface plane. Within the beta-phase a
superstructure of alternating rotation domains is observed.
This superstructure has a period of 7.4 nm. The molecular
packing in the beta-phase resembles the packing in the bulk
crystal structure of tetracene, its formation can therefore
be interpreted as incipient pseudomorphic growth of
tetracene on Ag(111). However, pseudomorphic growth cannot
be continued beyond the beta-phase.},
keywords = {J (WoSType)},
cin = {PGI-3 / JARA-FIT},
ddc = {530},
cid = {I:(DE-Juel1)PGI-3-20110106 / $I:(DE-82)080009_20140620$},
pnm = {Grundlagen für zukünftige Informationstechnologien},
pid = {G:(DE-Juel1)FUEK412},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000296866000012},
doi = {10.1103/PhysRevB.84.195440},
url = {https://juser.fz-juelich.de/record/19536},
}