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@ARTICLE{Sttele:907590,
author = {Sättele, Marie S. and Windischbacher, Andreas and
Greulich, Katharina and Egger, Larissa and Haags, Anja and
Kirschner, Hans and Ovsyannikov, Ruslan and Giangrisostomi,
Erika and Gottwald, Alexander and Richter, Mathias and
Soubatch, Serguei and Tautz, F. Stefan and Ramsey, Michael
G. and Puschnig, Peter and Koller, Georg and Bettinger,
Holger F. and Chassé, Thomas and Peisert, Heiko},
title = {{H}exacene on {C}u(110) and {A}g(110): {I}nfluence of the
{S}ubstrate on {M}olecular {O}rientation and {I}nterfacial
{C}harge {T}ransfer},
journal = {The journal of physical chemistry / C},
volume = {126},
number = {10},
issn = {1932-7447},
address = {Washington, DC},
publisher = {Soc.},
reportid = {FZJ-2022-02096},
pages = {5036 - 5045},
year = {2022},
abstract = {Hexacene, composed of six linearly fused benzene rings, is
an organic semiconductor material with superior electronic
properties. The fundamental understanding of the electronic
and chemical properties is prerequisite to any possible
application in devices. We investigate the orientation and
interface properties of highly ordered hexacene monolayers
on Ag(110) and Cu(110) with X-ray photoemission spectroscopy
(XPS), photoemission orbital tomography (POT), X-ray
absorption spectroscopy (XAS), low-energy electron
diffraction (LEED), scanning tunneling microscopy (STM), and
density functional theory (DFT). We find pronounced
differences in the structural arrangement of the molecules
and the electronic properties at the metal/organic
interfaces for the two substrates. While on Cu(110) the
molecules adsorb with their long molecular axis parallel to
the high symmetry substrate direction, on Ag(110), hexacene
adsorbs in an azimuthally slightly rotated geometry with
respect to the metal rows of the substrate. In both cases,
molecular planes are oriented parallel to the substrate. A
pronounced charge transfer from both substrates to different
molecular states affects the effective charge of different C
atoms of the molecule. Through analysis of experimental and
theoretical data, we found out that on Ag(110) the LUMO of
the molecule is occupied through charge transfer from the
metal, whereas on Cu(110) even the LUMO+1 receives a charge.
Interface dipoles are determined to a large extent by the
push-back effect, which are also found to differ
significantly between 6A/Ag(110) and 6A/Cu(110).},
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},
UT = {WOS:000776247200034},
doi = {10.1021/acs.jpcc.2c00081},
url = {https://juser.fz-juelich.de/record/907590},
}