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Issue 1, March 2001
Engineering & Applied Sciences
Aryl Substituted Tetraazaphenanthrenes as Electron Transport Material for EL-Devices
Naoki Matsumoto1, Hideo Une2, Hideki Gorohmaru2, Thies Thiemann3, Shuntaro Mataka3*, Akihiro Seno-o4, Kazunori Ueno4
1 Faculty of
Engineering, Kyushu University, Hakozaki, Higashi-ku, Fukuoka 812-8581,
Japan
2 Graduate School of Engineering, Kyushu University, 6-1,
Kasuga-koh-en, Kasuga-shi, Fukuoka 816-8580, Japan
3 Institute of Advanced Material Study, Kyushu University,
6-1, Kasuga-koh-en, Kasuga-shi, Fukuoka 816-8580, Japan
4 Electrophotography Research Center, Canon Inc., 30-2
Shimomaruko 3-Chome, Ohta-ku, Tokyo 146-8501, Japan
Abstract
Aryl substituted
tetraazaphenanthrenes (9) were synthesized as electron transport material
for electroluminescent-devices (EL-devices). Their synthesis and their
physical properties are discussed. The results of an experimental
EL-device using tetraphenyltetraazaphenanthrene (9a) as an electron
transport material are presented.
Introduction
With the fast growing
array of electronic equipment, a demand for novel types of displays
has arisen over the last few years. These range from small, flat
panel displays, useful for mobile telephones and for the ‘back-rest'
movie and entertainment screens recently installed in certain aircraft,
to large full-color displays for new generations of televisions,
video players and perhaps even cinema viewing screens. The characteristics
required of such displays are manifold, but difficult to achieve:
long life-time, high brightness, high resolution, fast response
time, low operating voltage. Anybody who has worked with flat panel
displays realizes that a wide viewing angle is of great importance.
Against this background, the discovery of electroluminescence in
non-crystalline organic material (in both ‘low-weight' and polymeric
material) was propitious. While light-emitting diodes (LEDs) based
on inorganic solids have been known for some time, it was shown
in the 1960s that single crystals of anthracene sandwiched between
two electrodes exhibit electroluminescence (Helfrich 1965, Pope
1963). The underlying principle of this is the injection of electrons
into the semiconducting material from one electrode and a concomitant
creation of migrating ‘positive' holes at the other electrode. The
capture of the electron by the hole (recombination) is associated
with the emission of radiative energy, produced by the so-called
excited electron-hole state (exciton). Over 25 years later, Tang
and Van Slyke demonstrated that organic polymers could be used in
making LEDs (Tang 1987). These devices consisted of a hole-transporting
layer of an aromatic diamine and an emissive layer of (8)-hydroxyquinoline
aluminum (Alq3). Although the quantum efficiency of the
devices was on the order of 0.05% and the driving voltage was >
10 V, the potential advantages associated with organic materials
versus inorganic materials in the variability of compounds that
can be used and the processability of these materials to form uniform,
thin layered coatings, made the use of organic compounds in LEDs
an attractive alternative. Another 15 years have passed since then.
The research effort devoted to organic luminescent material has
been tremendous. (For a review of organic materials in modern display
technology, see Ziemelis 1999, Friend 1999). Last year, a number
of products were announced which feature electroluminescent displays
based on organic materials (Philipps, Pioneer). Today, the research
in this area is an interplay of chemistry (designing of new organic
compounds), physics and engineering. In order to achieve a balanced
injection and transport of electrons and holes into the emissive
layer, additional organic layers have been introduced into the device
structure, providing for the crucial separation of the emissive
layer from the electrodes. Thus, much higher quantum efficiencies
and much lower driving voltages have been achieved. The research,
however, is far from over. The development of improved full-color
LEDs is one of the major targets in the next few years.
For the fabrication of high-performance LEDs, hole and electron-transporting
material, as well as light emitting material, are required. The
aim of our work is the synthesis of electron-transporting material.
Important for this type of material is a strong electron acceptor
characteristic and the ability to form amorphous films. Pyrazino-annelated
benzenes are known to accept an electron relatively easily. Thus,
1,4,5,8,9,12-hexaazatriphenylene (HAT) (see also: Nasielski-Hinkens
1981) has been studied extensively in our laboratory. Previously,
it had been reported to be a strong electron acceptor. Albeit it
crystallizes easily and has a high melting point. Hexaphenyl-HAT
is also expected to be a good electron-acceptor. Moreover, due to
the phenyl groups, hexaphenyl-HAT crystallizes less easily, thus
a better result was expected for the formation of an amorphous film
incorporating this material. Its preparation was carried out via
hexaaminobenzene (2) as the key intermediate, using a known procedure.
The synthesis of hexaaminobenzene (2) had been described via reduction
of 1,3,5-triamino-2,4,6-trinitrobenzene (1) (Rogers 1986). As this
compound is explosive, a new route had been devised, which takes
the advantage of the reducability of nitrobenzothiadiazoles, e.g.
(6) and (7), to the corresponding polyaminobenzenes (Mataka 1989).
In a method similar to this route, it was also possible to prepare
1,4,5,8-tetraazaphenanthrene. In the following text, the synthesis
and the physical properties of some substituted 1,4,5,8-tetraazaphenanthrenes
(9) are described, with attention to the fact that substituents
are needed to tailor the electronic properties and to facilitate
the formation of amorphous films with this material at a later stage.
Experimental Procedure
A mixture of 1,2,3,4-tetraaminobenzene bishydrochloride (8) (211
mg, 1.0 mmol) and 1,2-bis-(4-chlorophenyl)-1,2-diketone (560 mg,
2.0 mmol) in ethanol (10 mL) and acetic acid (3 mL) was heated under
reflux for 15 hours under an argon atmosphere. Thereafter the cooled
reaction mixture was poured into water (xx mL) and the formed precipitate
was filtered off. The precipitate was dried and purified by column
chromatography (silica gel, eluant CHCl3) and recrystallised
from ethanol to give 2,3,6,7-tetrakis-(4-chlorophenyl)-1,4,5,8-tetraazaphenanthrene
(9e) (150 mg, 24%) as yellow needles; mp > 300°C; IR (KBr/cm-1)
u 1594, 1492, 1365, 1250, 1097, 1014;
1H NMR (270 MHz, CDCl3) d
7.36 - 7.41 (m, 8H), 7.58 - 7.67 (m, 8H), 8.36 (s, 2H).
Synthesis of 2,3,6,7-tetraaryl substituted 1,4,5,8-tetraazaphenanthrenes
(9)
The
key intermediate in the synthesis of the substituted tetraazaphenanthrenes
is the 1,2,3,4,-tetraaminobenzene bishydrochloride (8). Starting
from o-phenylenediamine (4), which is reacted with thionyl chloride
in the presence of pyridine to give 2,1,3-benzothiadiazole (5),
5-amino-4-nitro-2,1,3-benzothiadiazole (7) can be prepared in four
steps as shown in Scheme 2. (7) can be reduced with ease to (8)
with tin-hydrochloric acid in dioxane.
(8) was reacted with a number of substituted 1,2-diaryl-1,2-diketones
(benzils). The reaction has not been optimized as of yet. Nevertheless,
it can be noted that unsubstituted benzil gave the best yield. Furthermore,
electron-acceptor substituted benzils gave better yields than the
corresponding electron-donor substituted substances. This is not surprising
as the carbonyl ‘reactivity' of the former is higher than that of
the latter. While the melting point of most compounds could be reduced
relatively to the parent compound, especially in the case of the methoxy-substituted
tetraazaphenanthrenes (9c) and (9d), the fluoro-substituted tetraazaphenanthrene
(9f) showed a remarkably high melting point. The crystallizability
of the compounds was investigated by multiple TG/DTA scans. The tetrakis
(trimethoxyphenyl) tetraaza-phenanthrene (9d) clearly showed amorphous
behaviour upon cooling (after melting the sample). Tetraphenyltetraazaphenanthrene
(9a) formed an amorphous thin layer after vacuum deposition (see experimental
EL-device, below).
Physical properties
UV data
All the tetraazaphenanthrenes synthesized are colored materials.
For the most part, they are yellow. The UV data of the TAP derivatives
are listed in Table 1. Substituting tetraphenylazaphenanthrenes
with electron withdrawing moities such as with fluoro, or chloro
groups induces a hypochromic shift in the wavelength of the absorption
maximum, when compared with molecules having one or more electron
donors on the phenyl groups (e.g., methoxy-(9c), or trimethoxy-(9d)).
Nevertheless, all substituted tetraphenylazaphenanthrenes experience
a bathochromic shift in relation to the unsubstituted tetraphenylazaphenanthrene.
This is in reasonable agreement with the expected data.
CV data
Cyclic voltammetry (CV) of the TAP derivatives was carried out in
dichloromethane using a glassy carbon electrode as the working electrode.
The results can be found in Table 2. The potentials are given versus
Ag/AgCl as reference electrode. The CV data holds no surprises insofar
as the substances substituted with electron-withdrawing groups (i.e.,
relatively electron poor tetraazaphenanthrenes) are reduced at comparatively
lower half potentials than the corresponding electron-donor substituted
tetraazaphenanthrenes (i.e., relatively electron-rich tetraazaphenanthrenes).
Thus, the gradation di-o-F-Ph < p-Cl-Ph
< Ph < p-Me-Ph < p-MeO-Ph
would be expected from the electron-donor capability of the substituents
and is in accordance with the Hammett parameters (where it is known
that o-fluoro substituents areusually
not well reflected). The only TAP derivative that does not seem to
fit is the trimethoxy derivative (9d), which reduces at a half wave
potential comparable to that of the unsubstituted tetraphenyltetraazaphenanthrene
(9a). The reason for this may be due to steric overfreighting within
the perimeter of the phenyl groups. Thus, the methoxy groups may effect
a deviation from planarity of the phenyl groups with concurrent loss
of some p-p interaction with the tetraazaphenanthrene
core unit.
An EL-device [ITO/0.1%FL-03(Spin-coated; Canon hole transport material)/Alq3
(600 A; luminescent layer)/tetraphenyltetraazaphenanthrene
(9a) (50 A or 200 A; electron transport layer)/Al-electrode 1500 A]
was built and tested. It was noted that at higher driving voltages
the use of tetraphenyltetraazaphenanthrene was beneficial as compared
to using no added layer of electron transport carrier or to using
hexaphenyl-HAT in the electron transport layer.
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Journal of Young
Investigators. 2001. Volume Three.
Copyright © 2001 by Naoki Matsumoto and JYI. All rights reserved.
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