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@PHDTHESIS{Henneke:667469,
author = {Henneke, Caroline},
othercontributors = {Kumpf, Christian and Mayer zu Heringdorf, Frank and Mayer,
Joachim},
title = {{K}inetic and thermodynamic considerations on the formation
of heteromolecular layers on metal surfaces},
school = {RWTH Aachen University},
type = {Dissertation},
address = {Aachen},
reportid = {RWTH-2016-06249},
pages = {1 Online-Ressource (vii, 157, XIV Seiten) : Illustrationen,
Diagramme},
year = {2015},
note = {Veröffentlicht auf dem Publikationsserver der RWTH Aachen
University 2016; Dissertation, RWTH Aachen University, 2015},
abstract = {A systematic study of the growth of a heteromolecular
adsorbate system consisting of
3,4,9,10-perylenetetracarboxylic dianhydride (PTCDA) and
copper phthalocyanine (CuPc) on the substrates Ag(111) and
Cu(001) in the submonolayer regime is presented.The key
finding is the phase diagram of the PTCDA-CuPc system on
Ag(111) in the complete coverage regime up to 1 ML at 300 K.
It contains eight different regions with one or two
different crystalline phases which coexist with areas of a
disordered phase of both molecules. Only the disordered
phase is present on the surface in a ninth region. The
reason for this complicated phase diagram is the complex
interplay between energetic aspectsof the island formation
(adhesion energy) and the involved entropic effects which
are both investigated in detail.The phase formation is
strongly influenced by the deposition parameters for the
PTCDA-CuPc system on Cu(001). Heteromolecular phases only
grow when PTCDA is deposited on a submonolayer film of
CuPc, while the PTCDA islands remain unchanged for the
reversed deposition sequence when CuPc is deposited on a
submonolayer film of PTCDA. This is different on Ag(111).
PTCDA islands are transformed into three different
heteromolecular phases with increasing CuPc:PTCDA
stoichiometry during the deposition of CuPc on a
submonolayer film of PTCDA. It is found that the phases are
in thermodynamic equilibrium since they only depend on
coverage (of CuPc and PTCDA) and temperature, but (in
contrast to Cu(001)) not on other deposition parameters.
This allows the determination of the above mentioned phase
diagram. Its form can be explained by an ab-initio model
without any fit parameters. It is based on the model for an
intermetallic compound at 1 ML coverages and includes the
additional assumption that critical densities of CuPc in the
disordered phase must be exceeded for the growth of each
heteromolecular phase. The existence of such critical
densities of CuPc can be explained by the interplay between
the intermolecular PTCDA-CuPc interactions and the entropy
of the entire system. Both homomolecular systems were
characterized in a prefixed part of the work since their
understanding is essential for a successful analysis of the
heteromolecular system. Here, it is found that the strong
attractive intermolecular interaction dominates the growth
of PTCDA, while entropic effects can influence the growth
of CuPc molecules due to their weakly repulsive
interaction.The characterization of both homo- and
heteromolecular systems shows that an improved understanding
of the self-assembly of molecules on surfaces enables the
selective fabrication of heteromolecular thin films with
desired properties which potentially influences the
production of commercially used organic layers.},
cin = {139320 / 130000},
ddc = {530},
cid = {$I:(DE-82)139320_20140620$ / $I:(DE-82)130000_20140620$},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:hbz:82-rwth-2016-062498},
url = {https://publications.rwth-aachen.de/record/667469},
}