Aromatic organic molecules exhibit a conjugated
π-electron system giving rise to delocalized electrons which on the
one hand can be excited by illumination of visible light and on the
other hand can emit light in the visible energy range. This makes
these molecules interesting for optoelectronic applications, such as
OLEDs or organic solar cells. The typical absorption and emission
processes are depicted in Fig. 1 as transitions between the singlet
electronic ground state (S0, also
called HOMO,
highest occupied molecular orbital) and the first electronic excited
state (S1, also
called LUMO,
lowest unoccupied molecular orbital). |
Due to a different charge
distribution between the HOMO and the LUMO electronic excitations or
relaxations lead to spatial deformations of the molecule that result
in additional vibronic excitations. This deformation is represented
by a change of the configuration coordinate Q in Fig. 2, which is in
the simplest case of a diatomic molecule the distance between the
nuclei. The bonding between the nuclei can be described by some
potential as depicted in Fig. 2 from which the vibronic states,
represented by the wavefunctions ψ, can be calculated for each
electronic state S0 and S1. |
Due to interactions in molecular aggregates, such as thin films or single crystals, the optical properties are modified. Compared to inorganic materials these interactions are small, mainly governed by the van-der-Waals interaction. Various effects, which are related to the structural properties of the aggregate system, such as
The optical spectra of thin films give therefore insight into the intermolecular coupling, which is relevant for transport properties and thus important for device applications. A further aspect is to monitor and control the film growth in order to obtain desired film properties. Optical methods are very well suited to study these properties in situ and in real-time to observe possible changes, such as:
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For the optical characterization we employ different experimental setups:
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[1] Birks Photophysics of aromatic molecules, Wiley (1970)
[2] R. Scholz, Organic Semiconductors, Encyclopedia of
Condensed Matter Physics (2005)
[3] A. S. Davydov, The theory of molecular excitons, Soviet
Physics (1964)
[4] U. Heinemeyer, R. Scholz, L. Gisslen, M. I. Alonso,
J. O. Osso, M. Garriga, A. Hinderhofer, M. Kytka, S. Kowarik,
A. Gerlach, and F. Schreiber. Exciton-phonon coupling in
diindenoperylene thin films Phys. Rev. B 78 (2008) 085210
For our recent work on the optical properties of organic thin films, see list of publications.