New electroluminescent bipolar compounds for balanced charge-transport and tuneable colour in organic light emitting diodes: triphenylamine– oxadiazole–fluorene triad molecules{ Kiran T. Kamtekar, a Changsheng Wang, a Sylvia Bettington, a Andrei S. Batsanov, a Igor F. Perepichka,{ a Martin R. Bryce,* a Jin H. Ahn, b Mohammad Rabinal b and Michael C. Petty* b Received 29th March 2006, Accepted 25th July 2006 First published as an Advance Article on the web 24th August 2006 DOI: 10.1039/b604543j This work describes bipolar 2,5-diaryl-1,3,4-oxadiazole–fluorene hybrids which incorporate triphenylamine or carbazole units within the p-electron system, viz. compounds 7, 8, 14 and 16.A related bipolar bis(oxadiazolyl)pyridine system 20 is reported. The syntheses of these five new materials are discussed, along with their optoelectronic absorption and emission properties, and their solution electrochemical redox properties. Anodic electropolymerisation of 20 was observed. Calculations using DFT (density functional theory) establish that they all possess a significantly higher HOMO energy level (by 0.60–1.02 eV) than 1,3-bis[2-(4-tert-butylphenyl)-1,3,4-oxadiazol- 5-yl]benzene (OXD-7) due to the presence of electron-rich amine moieties and increased conjugation lengths, thereby leading to more balanced charge-transport characteristics. Devices were fabricated by spin-coating techniques using the bipolar compounds as the emitters in the simple device architecture ITO:PEDOT-PSS:X:Ca/Al (X = 7, 8, 14, 16 or 20). The turn-on voltages were 2.9, 5.5, 3.6, 4.5 and 3.4 V for the devices incorporating 7, 8, 14, 16 and 20, respectively. The highest external quantum efficiency (EQE) was observed for compound 7: viz. EQE 0.36%; current efficiency 1.00 cd A 21 ; power efficiency 0.56 lm W 21 at 5.7 V. The EQE of the device fabricated from 8 was considerably lower than for devices using other materials due to low light emission. The EL emission peaked at l max 430, 487, 487 and 521 nm for 8, 14 and 16, and 7, respectively. For the 20 device l max = 521 nm and 564 nm. Thus the HOMO–LUMO gap has been modified, allowing the colour of the emitted light to vary from light blue through to green by the systematic chemical modification of the molecular subunits. The high chemical and thermal durability of these materials combined with the simplicity of the device structure and low turn-on voltages offers considerable potential for OLED applications. Introduction The discovery of electroluminescence (EL) in low molecular weight organic molecules 1 and in conjugated polymers, 2 has led to unabated intense interest in new materials for incorporation into organic light emitting diodes (OLEDs) for display applications, ranging from small portable devices to large area screens which consume much less power than current LCD materials. 3 The design and synthesis of materials which possess balanced hole-transport (HT) and electron- transport (ET) properties remain a major challenge. Most emissive polymers are predominantly hole-transporting (i.e. p-dopable), viz. derivatives of poly(p-phenylene vinylene) and poly(fluorene). In a device structure this creates an imbalance of electron injection (from the low work-function cathode) and hole injection (from the high work-function anode) with the consequence that charge recombination occurs near the polymer/cathode interface which lowers the EL efficiency due to quenching of excitons by the metal electrode. This problem can be overcome by using a lower work function metal (e.g. Ca) as the cathode. However, such metals are highly reactive and are unstable in the atmosphere. Alternatively, electron-deficient (n-type) polymeric or low molecular weight materials have been incorporated into devices in the following ways: (i) as an additional electron- transporting hole-blocking (ETHB) layer between the cathode and the emissive polymer; (ii) by covalently bonding the electron-deficient segments to the emissive polymer 4 or (iii) by blending the ET material into the emissive polymer prior to deposition. 5 Much work has concerned multilayer structures with electron-deficient 2,5-diaryl-1,3,4-oxadiazole (OXD) a Department of Chemistry and Centre for Molecular and Nanoscale Electronics, University of Durham, Durham, UK DH1 3LE. E-mail: [email protected]b School of Engineering and Centre for Molecular and Nanoscale Electronics, University of Durham, Durham, UK DH1 3LE. E-mail: [email protected]{ Electronic supplementary information (ESI) available: Synthesis of 11; cyclic voltammetry data for compounds 7, 8, 14, 16 and 20, X-ray crystallographic data for compounds 11, 12, 13 and 20 including diagrams and discussion of the structures; B3LYP/6-31G(d) optimised geometries (Figures and Tables of coordinates); orbital energy level diagrams and frontier orbital localisation for compounds 7a, 8a, 14a, 16a and 20; EL spectra of blended layer devices of MEH-PPV and compound 7. See DOI: 10.1039/b604543j { On leave from the L. M. Litvinenko Institute of Physical Organic and Coal Chemistry, National Academy of Sciences of Ukraine, R. Luxemburg Street 70, Donetsk 83114, Ukraine. PAPER www.rsc.org/materials | Journal of Materials Chemistry This journal is ß The Royal Society of Chemistry 2006 J. Mater. Chem., 2006, 16, 3823–3835 | 3823
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New electroluminescent bipolar compounds for balanced charge-transport and tuneable colour in organic light emitting diodes: triphenylamine?oxadiazole?fluorene triad molecules
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New electroluminescent bipolar compounds for balanced charge-transportand tuneable colour in organic light emitting diodes: triphenylamine–oxadiazole–fluorene triad molecules{
Kiran T. Kamtekar,a Changsheng Wang,a Sylvia Bettington,a Andrei S. Batsanov,a Igor F. Perepichka,{a
Martin R. Bryce,*a Jin H. Ahn,b Mohammad Rabinalb and Michael C. Petty*b
Received 29th March 2006, Accepted 25th July 2006
First published as an Advance Article on the web 24th August 2006
DOI: 10.1039/b604543j
This work describes bipolar 2,5-diaryl-1,3,4-oxadiazole–fluorene hybrids which incorporate
triphenylamine or carbazole units within the p-electron system, viz. compounds 7, 8, 14 and 16. A
related bipolar bis(oxadiazolyl)pyridine system 20 is reported. The syntheses of these five new
materials are discussed, along with their optoelectronic absorption and emission properties, and
their solution electrochemical redox properties. Anodic electropolymerisation of 20 was observed.
Calculations using DFT (density functional theory) establish that they all possess a significantly
higher HOMO energy level (by 0.60–1.02 eV) than 1,3-bis[2-(4-tert-butylphenyl)-1,3,4-oxadiazol-
5-yl]benzene (OXD-7) due to the presence of electron-rich amine moieties and increased
conjugation lengths, thereby leading to more balanced charge-transport characteristics. Devices
were fabricated by spin-coating techniques using the bipolar compounds as the emitters in the
simple device architecture ITO:PEDOT-PSS:X:Ca/Al (X = 7, 8, 14, 16 or 20). The turn-on
voltages were 2.9, 5.5, 3.6, 4.5 and 3.4 V for the devices incorporating 7, 8, 14, 16 and 20,
respectively. The highest external quantum efficiency (EQE) was observed for compound 7: viz.
EQE 0.36%; current efficiency 1.00 cd A21; power efficiency 0.56 lm W21 at 5.7 V. The EQE of
the device fabricated from 8 was considerably lower than for devices using other materials due to
low light emission. The EL emission peaked at lmax 430, 487, 487 and 521 nm for 8, 14 and 16,
and 7, respectively. For the 20 device lmax = 521 nm and 564 nm. Thus the HOMO–LUMO gap
has been modified, allowing the colour of the emitted light to vary from light blue through to
green by the systematic chemical modification of the molecular subunits. The high chemical and
thermal durability of these materials combined with the simplicity of the device structure and low
turn-on voltages offers considerable potential for OLED applications.
Introduction
The discovery of electroluminescence (EL) in low molecular
weight organic molecules1 and in conjugated polymers,2 has
led to unabated intense interest in new materials for
incorporation into organic light emitting diodes (OLEDs) for
display applications, ranging from small portable devices
to large area screens which consume much less power than
current LCD materials.3 The design and synthesis of materials
which possess balanced hole-transport (HT) and electron-
transport (ET) properties remain a major challenge. Most
emissive polymers are predominantly hole-transporting (i.e.
p-dopable), viz. derivatives of poly(p-phenylene vinylene) and
poly(fluorene). In a device structure this creates an imbalance
of electron injection (from the low work-function cathode) and
hole injection (from the high work-function anode) with the
consequence that charge recombination occurs near the
polymer/cathode interface which lowers the EL efficiency
due to quenching of excitons by the metal electrode. This
problem can be overcome by using a lower work function
metal (e.g. Ca) as the cathode. However, such metals are
highly reactive and are unstable in the atmosphere.
Alternatively, electron-deficient (n-type) polymeric or low
molecular weight materials have been incorporated into
devices in the following ways: (i) as an additional electron-
transporting hole-blocking (ETHB) layer between the cathode
and the emissive polymer; (ii) by covalently bonding the
electron-deficient segments to the emissive polymer4 or (iii) by
blending the ET material into the emissive polymer prior to
deposition.5 Much work has concerned multilayer structures
with electron-deficient 2,5-diaryl-1,3,4-oxadiazole (OXD)
aDepartment of Chemistry and Centre for Molecular and NanoscaleElectronics, University of Durham, Durham, UK DH1 3LE.E-mail: [email protected] of Engineering and Centre for Molecular and NanoscaleElectronics, University of Durham, Durham, UK DH1 3LE.E-mail: [email protected]{ Electronic supplementary information (ESI) available: Synthesis of11; cyclic voltammetry data for compounds 7, 8, 14, 16 and 20, X-raycrystallographic data for compounds 11, 12, 13 and 20 includingdiagrams and discussion of the structures; B3LYP/6-31G(d) optimisedgeometries (Figures and Tables of coordinates); orbital energy leveldiagrams and frontier orbital localisation for compounds 7a, 8a, 14a,16a and 20; EL spectra of blended layer devices of MEH-PPV andcompound 7. See DOI: 10.1039/b604543j{ On leave from the L. M. Litvinenko Institute of Physical Organicand Coal Chemistry, National Academy of Sciences of Ukraine, R.Luxemburg Street 70, Donetsk 83114, Ukraine.
PAPER www.rsc.org/materials | Journal of Materials Chemistry
This journal is � The Royal Society of Chemistry 2006 J. Mater. Chem., 2006, 16, 3823–3835 | 3823
derivatives6 or Alq3 [tris(8-hydroxyquinoline)aluminium]7
serving as the ET material. While this strategy can lead to
very bright devices (sometimes requiring additional transport
layers to provide tri- and tetra-layer structures)8 there are
limitations in their practical applicability. Notably, multilayer
devices require more complex fabrication procedures than
single-layer devices and exciplex formation at the interface of
the organic layers can reduce operating lifetimes and lead to
broad red-shifted emission.9
Our strategy has been to develop single-layer devices
(sometimes with an additional PEDOT-PSS layer) fabricated
using solution-based processes which offer advantages to
commercialisation by such techniques as ink-jet printing. We
have chemically tailored functional molecules for balanced
charge-injection and charge-transport. For example, new
OXD derivatives, e.g. 1, enhance electron injection in single-
layer devices as blends with poly[2-(2-ethylhexyloxy)-5-meth-
oxy-1,4-phenylenevinylene] (MEH-PPV) as the emissive
material.10 The modest increase in efficiency for the same
device when Al was replaced by a Ca/Al cathode suggests that,
for some combinations of materials, the two methods of
enhancing electron injection into the MEH-PPV emitter are
mutually exclusive, with blended layers offering an attractive
alternative to using Ca electrodes, which are highly reactive
and are unstable in the atmosphere.11
We have now extended these studies by combining OXD,
triarylamine and fluorene units in the same molecule to serve
as ET, HT and emitter segments, respectively. Bipolar triad
molecules of this type are largely unexplored, although diads
comprising ET and HT moieties have been studied. For
example, Adachi and co-workers combined 1,3,4-oxadiazole
with triphenylamine moieties in small molecules.12 More
recently, Zhang et al. reported a luminescent PPV-type
polymer containing 1,3,4-oxadiazole and triphenylamine
units in the main chain.13 Thomas et al. synthesised various
combinations of oxadiazole and quinoxaline as ET segments,
with carbazole and triarylamine as HT segments,14 including
the fluorene-containing system 2. Vacuum deposition techni-
ques were used to fabricate multilayer OLEDs incorporating 2
and additional HT or ET layers. An OXD–spirobifluorene–
triphenylamine hybrid has been reported but no device
studies were mentioned.15 The EL properties of the blue-green
emitting dye 3 as a blend with poly(9-vinylcarbazole) in the
single-layer device ITO/PVK:3/Ca/Al have been reported.16
An analogue of 7 (with octyl chains instead of hexyl) has been
used by Antoniadis et al. as a component of vapour-deposited
OLEDs with a very complicated device structure involving
several additional hole-transport and electron-transport
layers.17 Rapid degradation of these devices was ascribed
to a combination of exciplex formation at the HTL/ETL
interfaces and instability of the excited state of the fluorene–
oxadiazole hybrid.
In this article we present the synthesis of the new
compounds 7, 8, 14 and 16 which comprise varying juxtaposi-
tions of OXD, fluorene and triphenylamine units along with a
related bipolar bis(oxadiazolyl)pyridine system 20. We discuss
their optoelectronic properties and their applications as
emitters in OLEDs fabricated using simple spin-coating
techniques. In particular, we have established that within this
series of molecules the colour of the emitted light is tuned from
light blue through to green. These materials exhibit good
durability, unlike the analogue of 7 studied by Antoniadis et al.
which was reported to show instability in the excited state.17
Results and discussion
Synthesis
The route to compounds 7 and 8 is shown in Scheme 1. The
known dihydrazide 4 (obtained in three high yielding steps
from readily available 2,7-dibromo-9,9-dihexylfluorene)10 was
condensed with 4-iodobenzoyl chloride to give derivative 5
(90% yield) which undergoes dehydrative cyclisation18 in
phosphorus oxychloride to give compound 6 (86% yield).
Reaction of 6 with diphenylamine or carbazole under copper-
catalysed C–N bond-forming conditions19 gave the desired
products 7 and 8 in 83 and 85% yields, respectively.
The route to compounds 14 and 16 is shown in Scheme 2.
We have previously shown that the fluorene derivative 9,
containing a trimethylsilyl substituent, is a versatile reagent
which is readily synthesised from 2,7-dibromofluorene.20 The
boronic ester 10 was readily obtained by lithiation followed by
reaction with 2-isopropyl-4,4,5,5-tetramethyl-1,3,2-dioxaboro-
lane (69% yield from 2,7-dibromofluorene). Cross-coupling of
10 with the 2,5-diaryl-1,3,4-oxadiazole derivative 1121 under
for reversible processes. c Electrochemical band gap estimated from the onsets of oxidation and reduction processes. d Optical band gapestimated from the red edge of absorption spectra in chloroform (Fig. 7). e HOMO–LUMO gap from DFT calculations (Fig. 2).
Fig. 3 Cyclic voltammogram of compound 14 in benzonitrile, 0.1 M
Bu4NPF6 at 100 mV s21 (Eox11=2 = 0.60 V, DEox1
pa{pc = 60 mV, Eox2pa =
1.24 V). Inset shows the deconvoluted CV.
Fig. 4 Cyclic voltammograms of compound 7 in benzonitrile, 0.1 M
Bu4NPF6 at different scan rates. CV at scan rate of 100 mV s21 is
normalised to that for scan rate of 2000 mV s21 at Eoxpa (by multiplying
ipa 63.53). Eoxpa = +0.88 V, Eox
pc = +0.77 V, Epolympc = +0.62 V
(100 mV s21); Eoxpa = +0.89 V, Eox
pc = +0.78 V (2000 mV s21).
This journal is � The Royal Society of Chemistry 2006 J. Mater. Chem., 2006, 16, 3823–3835 | 3827
ca. +(0.65–0.7) V corresponds to a partial electropolymerisa-
tion process for 20.
More detailed studies of the anodic electropolymerisation of
20 were performed in potentiodynamic conditions by scanning
the potentials for a solution of 20 in benzonitrile between 0
and +0.9 V. Cycling resulted in the growth of a new peak (at
ca. 0.65–0.70 V, inset in Fig. 6) of a polymer film on the Pt
electrode (yellow film). After rinsing the electrode with
acetonitrile, the CV recorded in monomer-free acetonitrile
(with 0.1 M Bu4NPF6 as electrolyte) showed the electroactivity
towards both p- and n-doping, with high stability on cycling
(Fig. 6). The electroactivity of poly(20) towards p-doping (at
ca. 0.6–0.8 V) demonstrated a good linear dependence on the
scan rate in the range of 10 to 200 mV s21 proving that an
electrochemical process occurs in the film deposited on the
electrode (Fig. S9, ESI{). The formation of poly(20) is
represented in Scheme 4; it is a non-conjugated polymer.
Couplings at triphenylamine units will increase the extent of
conjugation at these sites (at which the HOMO is located,
see Fig. S20, ESI{) resulting in a lowering of the HOMO
energy and a cathodic shift of its oxidation wave by y0.15–
0.2 V (cf. Fig. 5 and 6). Reduction of both 20 and poly(20)
occurred at almost the same potentials, which is under-
standable considering the similar localisation of their LUMOs
(Fig. S20, ESI{) and the interrupted conjugation in poly(20)
(cf. Fig. 5 and 6).
Fig. 5 Cyclic voltammogram of compound 20 in benzonitrile, 0.1 M
Bu4NPF6 at scan rate 100 mV s21, 4 consecutive scans (starting at
21.2 V, scan to negative): Eredpc = 21.79 V, Ered
pa = 21.73 V, Eoxpa =
+0.89 V, Eoxpc = +0.78 V. Inset: deconvoluted CV for the oxidation
process. Arrows show electrodeposition of the polymer on the Pt
electrode after the first oxidation scan.
Fig. 6 Cyclic voltammogram of a film of poly(20) on Pt disk,
4224 unique, Rint = 0.031, R(F) = 0.055 [3572 data with F2¢
2s(F2)], wR(F2) = 0.166 (all data), CCDC 602979.
Acknowledgements
This work was funded by EPSRC (K.T.K., C.S.W. and
improvements to the X-ray instrumentation), Durham County
Council under the Science and Technology for Business and
Enterprise Programme SP/082, and CENAMPS (S.L.B.) and
the Postdoctoral Fellowship Programme of Korea Science
and Engineering Programme (KOSEF) (for J.H.A.). We thank
Professor J. A. K. Howard for the use of X-ray facilities.
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