Synthetic Metals 159 (2009) 1014–1018
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Synthetic Metals
journal homepage: www.elsevier.com/locate/synmet
Phenoxazine and N-phenyl-1-naphtylamine-based enamines as
hole-transporting glass-forming materials
R. Paspirgelyte
a
, J.V. Grazulevicius
a,∗
, S. Grigalevicius
a,∗
, V. Jankauskas
b
a
Department of Organic Technology, Kaunas University of Technology, Radvilenu Plentas 19, LT50254, Kaunas, Lithuania
b
Department of Solid State Electronics, Vilnius University, Sauletekio Aleja 9, LT10222, Vilnius, Lithuania
article info
Article history:
Received 1 November 2008
Received in revised form 20 December 2008
Accepted 12 January 2009
Available online 6 February 2009
Keywords:
Electro-active material
Enamine
Hole drift mobility
Ionization potential
abstract
New aromatic enamines were synthesized by condensation of the commercially available phenoxazine
and N-phenyl-1-naphtylamine with 2,2-diphenylacetaldehyde or 2-phenylpropionaldehyde. The materi-
als were examined by various techniques including differential scanning calorimetry, UV and fluorescence
spectrometry, electron photoemission and time of flight techniques. The electron photoemission spectra
of the layers of the amorphous materials showed the ionization potentials of 5.42–5.61eV. Hole drift
mobilities in the layers of 33–50% solid solutions of the derivatives in bisphenol Z polycarbonate range
from 10
-5
to 3.4 × 10
-4
cm
2
/V s at high electric fields.
© 2009 Elsevier B.V. All rights reserved.
1. Introduction
Low-molar-mass organic compounds that readily form stable
glasses receive growing attention both in terms of academic inter-
est and technological applications [1–3]. Some of these derivatives
belong to the classes of organic electro-active materials and are
known for various applications such as organic light-emitting
diodes, photovoltaic cells, electro-photographic photoreceptors
[4–7].
Among organic semiconductors materials transporting positive
charges are so far much wider synthesized, studied and applied. For
various fields of application the hole-transporting materials with
the certain complex of properties are required. No reliable theo-
ries for the design of organic semiconductors having an optimal
combination of the required properties have yet been developed.
Consequently, such materials need to be discovered experimen-
tally. Different electrophores are used in the design and synthesis
of organic hole-transporting compounds. In this work, we have
designed and synthesised new electro-active materials having phe-
noxazine and N-phenyl-1-naphtylamine fragments. These building
blocs were used for the preparation of aromatic enamines. The
materials demonstrate promising optoelectronic properties, how-
ever their synthesis and properties are little studied [8,9].
∗
Corresponding author.
E-mail addresses: juozas.grazulevicius@ktu.lt (J.V. Grazulevicius),
saulius.grigalevicius@ktu.lt (S. Grigalevicius).
2. Experimental
2.1. Instrumentation
1
H NMR spectra were recorded using Varian Unity Inova
(300 MHz) apparatus. Mass spectra were obtained on a Waters ZQ
2000 spectrometer. FT-IR spectra were recorded using PerkinElmer
FT-IR system. UV spectra were measured with a Spectronic
Genesys
TM
8 spectrometer. Fluorescence (FL) spectra were recorded
with a Hitachi MPF-4 spectrometer.
Differential scanning calorimetry (DSC) measurements were
carried out using a Bruker Reflex II thermo-system. Thermogravi-
metric analysis (TGA) was performed on a Netzsch STA 409. The
TGA and DSC curves were recorded in a nitrogen atmosphere at a
heating rate of 10
◦
C/min.
The ionization potentials of the layers of the compounds syn-
thesized were measured by the electron photoemission method in
air, which was described earlier [10]. The measurement method
was, in principle, similar to that demonstrated by Miyamoto et al.
[11]. The samples for the ionisation potential measurement were
prepared as reported previously [12]. The materials were dissolved
in THF and were coated on Al plates pre-coated with ∼0.5 m
thick methylmethacrylate and methacrylic acid copolymer (MKM)
adhesive layer. The function of this layer was not only to improve
adhesion, but also to eliminate the electron photoemission from
Al layer. In addition, the MKM layer is conductive enough to avoid
charge accumulation on it during the measurements. The thickness
of the layers was 0.5–1 m.
0379-6779/$ – see front matter © 2009 Elsevier B.V. All rights reserved.
doi:10.1016/j.synthmet.2009.01.015