Interaction of UV light with
amorphous small-molecule organic thin films
There is an ongoing interest in organic materials
due to their application in various organic
electronic devices. However stability of organic
materials limits their potential use. They are prone
to degradation both during the working life and
storage. One of the main causes is extrinsic
degradation, under the influence of oxygen and
moisture. This problem can be solved by
encapsulation of devices. However no encapsulation
is perfect.
We study interaction of thin
films of small-molecule organic blue-emitter
materials, such as
N,N′-bis(3-methylphenyl)-N,N′-bis(phenyl)benzidine
(TPD) and 4,4′-bis(2,2-diphenylvinyl)-1,1′-biphenyl
(DPVBi), with UV light. Films are stable in vacuum,
but readily degrade in the presence of oxygen. Thus,
the necessary condition for interaction
(degradation) is the simultaneous presence of UV
light and oxygen. These impurities are responsible
for increased morphological stability of irradiated
films and quenching of photoluminescence (PL).
In general, there are two possible pathways for
chemical reaction of films and oxygen: (1) excited
singlet molecule gives an electron to ground-state
oxygen molecule to form radical cation and the
superoxide anion, which can further react chemically
to form new species; (2) host molecule in excited
triplet state acts as a sensitizer and transfers its
energy to ground-state triplet oxygen to form
singlet oxygen and ground-state host molecule. The
energy needed for singlet oxygen formation is 0.97
eV. Singlet oxygen is very reactive and may further
interact with host molecules to form photo-oxidized
species. Only small amount of
impurities, less than 0.5%, causes 50% decrease of
PL. This implies a non-trivial mechanism of
quenching. The necessary condition for quenching is
that the distance between impurities is smaller or
equal to exciton diffusion length, which is
fulfilled in our films.
Following mechanism of PL
quenching is proposed: exciton diffuses by hopping
form one host molecule to another through Förster
resonant energy transfer in a random walk manner.
If, during its lifetime, it comes to proximity of an
impurity, a PL quenching process occurs. Even a
small amount of oxygen that penetrates a blue
emitter layer would impair luminescence efficiency
of a device. Moreover, the absorption of its own
radiation would additionally contribute to the rate
of degradation of a device.

a) Photoluminescence IPL/IPL0 at 458 nm and b)
absorbance A/A0 at 355 nm vs. t of 190 nm thick
DPVBi films irradiated with 3mWcm-2 recorded in
vacuum (10−4 Pa, open downward triangles), nitrogen
at 100 kPa (open upward triangles), different oxygen
pressures (solid symbols) and air at 100 kPa (solid
stars). In a) top x-axis (in minutes) refers to
measurements in vacuum and nitrogen (open symbols
and indicated by arrow), while bottom x-axis (in
seconds) refers to measurements in different oxygen
pressures and air. Curves obtained in air and at
oxygen pressure of 24 kPa have similar rates due to
the fact that the partial pressure of oxygen in air
is around 20 kPa. Micro-rods of
oxidized pentacene Pentacene is
hole-type semiconductor used in organic electronic
devices, well-known for its high charge carrier
mobility as high as 35 cm2V-1s-1 at room
temperature. Performance of devices made from
organic thin films strongly depends on their
morphology and it is often limited by the presence
of molecular disorder and grain boundaries, which
reduce mobility of charge carriers of a material.
To improve charge transport properties thermal
annealing could be used. Prolonged annealing of
pentacene films leads to surprising result: nano-
and micro-scale rod-shaped structures are forming on
film surface. Based on scanning electron microscopy
measurements, it is supposed that these structures
are crystalline. Their UV-vis absorbance indicates
that they are composed of more than one species of
oxidized pentacene molecules, including
6,13-pentacenequinone.

Images of crystal-like structures (micro-rods and
micro-crystals) formed on the surface of pentacene
films obtained by a), d) optical and b), c) scanning
electron microscopes.
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