Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Symposium Organic and Hybrid Systems for Future Electronics Donnerstag<br />
Fachsitzungen<br />
– Haupt-, Fach-, Kurzvorträge und Posterbeiträge –<br />
SYOH 1 Geometric Organic Structures on Surfaces<br />
Zeit: Donnerstag 14:00–14:45 Raum: H37<br />
SYOH 1.1 Do 14:00 H37<br />
Self-assembled molecular architectures — •Elena Mena-<br />
Osteritz and Peter Baeuerle — Organic Chemistry II. University<br />
of Ulm. Albert-Einstein-allee 11 89081 ULM<br />
Well-defined pi-conjugated macrocycles are of interest as modular<br />
building blocks for the assembly of new materials and supramolecular<br />
chemistry. They will play an essential role as key components for coming<br />
nanoelectronic devices. However, the assembly of molecular materials<br />
in nanoscale architectures will be a crucial step for the future molecular<br />
scale electronics. On the other side due to their toroidal structure,<br />
p-conjugated macrocycles could represent intriguing molecular circuits<br />
which would additionally include sites for recognition and selective complexation.<br />
Two years ago our group successfully achieved the synthesis of the first<br />
class of fully conjugated macrocycles: the cyclo[n]thiophene. In this contribution<br />
we will present the different 2D-arrangements of the macrocycles<br />
at the liquid/HOPG interface re-vealed by in-situ scanning tunnelling<br />
macroscopy (STM). The data will be analysed with the help of theoretical<br />
conformational and MO analyses. By means of STM, we also investigated<br />
epitaxy and interactions of C60-fullerenes with 2D crystalline monolayers<br />
of cyclo[12]thiophene resulting in perfectly ordered 1:1 complexes.<br />
STM-analyses of the nature, specificity and dynamics of the processes<br />
taking place at the surface, supported by theoretical calculations, will be<br />
discussed.<br />
SYOH 1.2 Do 14:15 H37<br />
Growth of perylene films on Cu(110) — •Kathrin Hänel, Sandra<br />
Söhnchen, Thomas Strunskus, Gregor Witte, Alexander<br />
Birkner, and Christof Wöll — Lehrstuhl für Physikalische Chemie<br />
I, Ruhr Universität Bochum, Universitätstr. 150, 44780 Bochum<br />
Organic semiconductors such as polycyclic hydrocarbons have attracted<br />
a considerable amount of attention because of their promising<br />
potential for electronic and optoelectronic devices. Of particular interest<br />
for the fabrication of such devices is the molecular microstructure in het-<br />
SYOH 2 Spectroscopy<br />
erostructures of thin organic films deposited on inorganic substrates. Here<br />
we present a comprehensive study of perylene (C20H12) films grown under<br />
UHV conditions on Cu(110). The growth and structure of the films<br />
were characterized by means of STM, LEED, HAS, TDS, XPS, NEX-<br />
AFS. While the perylene molecules form an ordered monolayer with an<br />
almost planar orientation, they continue to grow in an upright orientation<br />
without a preferential azimuthal ordering. The multilayer films<br />
reveal a pronounced tendency for dewetting leading to the formation of<br />
descrete islands. The terrace structure of such islands could be imaged<br />
by non contact AFM measurements under ambient condition and reveals<br />
the presence of molecular steps.<br />
SYOH 1.3 Do 14:30 H37<br />
Spectro-microscopic study of organic film growth: PTCDA/<br />
Ag(111) — •Th. Schmidt 1 , U. Groh 1 , H. Marchetto 2 , R. Fink 3 ,<br />
and E. Umbach 1 for the SMART collaboration — 1 Exp. Physik II,<br />
Universität Würzburg, 97074 Würzburg — 2 Fritz-Haber-Institut, 14195<br />
Berlin — 3 Phys. Chemie II, Univ. Erlangen, 91058 Erlangen<br />
We report on first dynamic growth studies of PTCDA on Ag(111) using<br />
a PEEM with photon excitation by either UV-light or polarized monoenergetic<br />
synchrotron radiation. The PEEM instrument is the SMART<br />
spectro-microscope in the actual version, an energy-filtered, but not yet<br />
aberration-corrected microscope. At elevated temperatures between 350<br />
and 450 K we observe the layer-by-layer growth of two to three layers, followed<br />
by the growth of three-dimensional islands (Stranski-Krastanov).<br />
At room temperature a transition from Stranski-Krastanov to layer-bylayer<br />
growth (Franck-van der Merwe) occurs. By laterally resolved NEX-<br />
AFS spectroscopy and by switching the linear polarization of the light<br />
one can clearly derive the molecular orientation as flat-lying in both, the<br />
islands and the bilayer. Additionally, the circular polarization reveals a<br />
natural circular dichroism for the PTCDA crystallites, which is unique<br />
and unexpectedly large for these planar and non-chiral molecules. Funded<br />
by BMBF under contract no. 05-KS1WW2-0.<br />
Zeit: Donnerstag 14:45–15:45 Raum: H37<br />
SYOH 2.1 Do 14:45 H37<br />
Relation between optical transition energies and the transport<br />
gap in α-PTCDA — •Reinhard Scholz and Thorsten U Kampen<br />
— Institut für Physik, Technische Universität Chemnitz<br />
Recently, the slowest photoluminescence (PL) channels in α-PTCDA<br />
were assigned to pairs of oppositely charged molecules [1]. Based on detailed<br />
model calculations of molecular dimers with time-dependent density<br />
functional theory, we can determine the Stokes shift arising from the<br />
internal deformation of the ionized molecules, resulting in an improved estimate<br />
for the energy of the charge transfer states in the periodic crystal.<br />
These findings are compared with the results of high-resolution photoemission<br />
spectroscopy and electrical characterization techniques applied<br />
to PTCDA films grown on n-doped GaAs(100) substrates. Depending<br />
on the substrate treatment, the ionization potential of the GaAs surfaces<br />
varies by more than 1 eV, resulting in a sign change of the interface dipole<br />
within this interval. From a linear fit of the interface dipole vs. the electron<br />
affinity of the substrate, an electron affinity of 4.12 ± 0.10 eV can<br />
be deduced for the organic layer. This procedure allows for an estimate<br />
of the energy offset between the LUMO of PTCDA and the conduction<br />
band minimum of the substrate, and the resulting HOMO-LUMO gap of<br />
2.44 - 2.55 eV is in agreement with the lower limit estimated from the<br />
electrical measurements. The energetic difference between the observed<br />
PL energy and the transport gap can be related to the energy required<br />
for the separation of the two opposite charges to infinite distance.<br />
[1] A. Yu. Kobitski, R. Scholz, H. P. Wagner, and D. R. T. Zahn, Phys.<br />
Rev. B 68, 155201 (2003).<br />
SYOH 2.2 Do 15:00 H37<br />
Femtosecond near-field spectroscopy of semiconducting polymers<br />
— •Kerstin Müller 1 , Christoph Lienau 1 , Dario Polli 2 ,<br />
Giulio Cerullo 2 , and Guglielmo Lanzani 2 — 1 Max-Born-Institut<br />
für Nichtlineare Optik und Kurzzeitspektroskopie, 12489 Berlin —<br />
2 Politecnico di Milano, Dipartimento di Fisica, 20133 Milano, Italy<br />
During recent years, ultrafast spectroscopy has provided a wealth of<br />
new insight into the dynamics of optical excitations of semiconducting<br />
polymers and thus into the function of polymer-based optoelectronic devices.<br />
So far from these studies little is known about spatial inhomogeneities<br />
of optical nonlinearities in such systems. Such information is<br />
crucial, however, for a detailed microscopic understanding of the optolectronic<br />
properties of polymers, which are strongly influenced by effects<br />
of disorder, e.g, fluctuations in size and orientation of polymer chains<br />
on nanoscopic and mesoscopic length scales. Here, we introduce a novel<br />
technique, femtosecond near-field pump-probe spectroscopy, for spatially<br />
mapping the temporal dynamics of polymer optical nonlinearities on a<br />
100 nm length scale with sub-picosecond resolution. We report first experimental<br />
studies of the time- and space-resolved photo-induced absorption<br />
of thin films of methyl-substituted poly(para-phenylene) ladder-type<br />
polymers (m-LPPP) and of mixed phase segregated polyfluorene/dye