New soluble poly(2,3-diphenylphenylene vinylene) derivatives for
light-emitting diodes
Sheng-Hsiung Yang, Jiun-Tai Chen, An-Kuo Li, Chun-Hao Huang, Kuei-Bai Chen,
Bing-R. Hsieh, Chain-Shu Hsu*
Department of Applied Chemistry, National Chiao Tung University, Hsinchu 300, Taiwan
Abstract
Soluble poly(2,3-diphenylphenylene vinylene) (DP-PPV) derivatives, 5-(4-heptyloxy-4’-oxytrimethylenediphenyl)-phenylene vinylene) (P1), 5-[4-(4-pentylcyclohexyl)phenoxy]-propyl-p-5-(4-heptyloxy-4’-oxytrimethylenediphenyl)-phenylene vinylene) (P2) and poly(2,3-diphenyl-5-(2-(1, 4, 5-triphenyl-1H-2-imidazoloyl)-1-oxytrimethylene phenyl) phenylene vinylene) (P3), were synthesized. P1 and P2 contain liquid crystal side groups; while P3 contains a charge transport group. The polymers showed solid state UV–Visible absorption and photoluminescence in the range of 370–380 and 480–510 nm, corresponding to blue green emission. Similar to many other reported systems, the solution fluorescence spectra of P1 and P2 showed slight solvent dependency and blue-shifted with respect to those of the films. These were not the case for P3 which showed little solvent dependency and little blue shift in solution. Two-layer light-emitting devices with a simple ITO/PEDOT/polymer/Ca (Al) configuration were fabricated and characterized.
D 2004 Elsevier B.V. All rights reserved.
Keywords: Conjugated polymer; Poly(2,3-diphenylphenylene vinylene); Electroluminescent devices
0040-6090/$ - see front matterD 2004 Elsevier B.V. All rights reserved. doi:10.1016/j.tsf.2004.08.113
* Corresponding author.
E-mail address: [email protected] (C.-S. Hsu).
1. Introduction
Polymers based on poly(phenylene vinylene) and poly(dialkylfluorenes) show great promise for organic light-emitting diode (OLED) application [1–5]. We have been interested in poly(2,3-diphenylphenylene vinylene) (DP-PPV) derivatives, such as DP-PPV, DP6-, DP8-, and DP10-PPV shown below for the same application[6,7]. It has also been reported that DP-PPV derivatives (shown below) showed promising properties for organic laser application[8]. The advantages of this family of materials include (1) high glass transition temperatures, (2) high fluorescence efficiency (65–85%), (3) ease of monomer and polymer syntheses, and (4) broad molecular design latitudes[9].
The key synthetic step that enables the broad molecular design latitude is the Diels–Alder reaction shown below, wherein Ar is an aromatic group, PG and PGV are polymerizable groups, and R and RV are aliphatic or aromatic groups. Since there are numerous Ar, R and RV groups as well as many PG groups and PGV groups, numerous monomers can be prepared similarly. These monomers can be used for the synthesis of both conjugated and non-conjugated functional aromatic polymers via condensation or coupling polymerization. One design strategy is to select a long-chain aliphatic group for R and/or RV to
prevent insolubility problem generally associated with aromatic polymers, especially for conjugated polymers. Of course one can also incorporate solubilizing groups on Ar.
We have reported the synthesis of several DP-PPV derivatives[10]. Here we report the synthesis of three new DP-PPV derivatives (poly(2,3-diphenyl-5-(4-heptyloxy-4’-oxytrimethylenediphenyl)phenylene vinylene) (P1), poly(2,3-diphenyl-5-[4-(4-pentylcyclohexyl)phenoxy]-propyl-p-phenylene vinylene) (P2) and poly(2,3-diphenyl-5-(2-(1, 4, 5-triphenyl-1H-2-imidazoloyl)-1-oxytrimethylene phenyl) phenylene vinylene) (P3) see Scheme 2), their light emission properties, and other relevant physical properties. P1 and P2contain liquid crystal side groups; whileP3contains a charge transport group.
2. Synthesis and characterization of P1–P3
The synthetic sequences of P1, P2andP3are shown in
Schemes 1 and 2. Scheme 1 shows the synthesis of functional acetylene compounds 3, 5 and 7. 4,4V-Biphenol (1) is monoalkylated to give 2 which is alkylated with 5-chloro-1-pentyne to give 3. Similar alkylation of 4 gives 5. Compound 6, which was prepared from condensation of salicyladehyde, benzil and aniline under acidic con-dition, is also similarly alkylated to give 7. As shown in
Scheme 2, 3, 5, and 7 undergo Diels-Alder reaction with 2,5-Bis(ethoxycarbonyl)-3,4-diphenylcyclopentadie-none (8) to give 9a-c, respectively. In order to improve the reactivity of Diels–Alder reaction of 3, 5 and 7 with cyclopentadienone, the reaction uses solvent-free condition and melts the mixture under 120 8C stirring for 12 h.
These are reduced with LiAlH4 to give the
respective 10a–c which then react with thionyl chloride to give monomers 11a–c. Normally, the reduction of diesters with LiAlH4 can be accomplished with stirring
at room temperature for several hours as was found for the reduction of 2,5-diphenylterphthalate. However, the sterically hindered diesters (9a–c) had to be refluxed overnight to reduce both ester groups to the alcohol. All substituted DP monomers were identified by NMR and elemental analysis. Polymerization of
11a, 11b, and 11c in the presence of large excess of potassium tert-butoxide (t-BuOK) gives P1, P2 and P3, respectively.
In order to find out the amount of base needed to eliminate HCl completely, we experimented with 8, 12, and 16 equivalents of t-BuOK. From 1H-NMR spectra, we found that polymers prepared from 8 and 12 equivalents of base still gave peaks at 4.3–4.4 ppm, which can readily be assigned to the proton signal for –CHCl. These polymers also showed weight loss during TGA measurement at about 190 8C, which is the typical cleavage temperature of C–Cl bond. With 16 equivalents of base, we were able to obtain polymers free from the –CHCl peak and without weight loss. All the results above show that 16 equiv of t-BuOK is the best amount used to carry out polymer-ization. No gelation is observed during polymerpolymer-ization. The polymers were isolated by precipitation in MeOH, followed by purification by redissolving in CHCl3 and
precipitating into methanol three times. The polymers were then dialyzed successively in acetone, water and methanol for 2 days each. The polymers were highly soluble in common organic solvents such as THF, chloroform, dichloromethane, and toluene. All polymers possess high molecular weights and narrow molecular weight distribution. The weight-average molecular weight (Mw) and polydispersity (PD) for polymers P1, P2 and
P3 are 226 K, 1.53, 401 K, 1.97 and 418 K, 2.91, respectively.
3. Mesomorphic behaviors
The thermotropic liquid crystalline phase of P1 and P2
was investigated by differential scanning calorimetry (DSC) and a polarized optical microscope (POM). The glass transition temperature (Tg) of P1 and P2 are 172 and 156
8C, respectively. An apparent endothermic peak at 290 8C is assigned to the melting point (Tm) of P1and we cannot see
it of P2 up to 300 8C in DSC diagram. Typical nematic textures of the polymers are shown in Fig. 1. A stable mesophase with a threaded texture and large domains was observed for P1at 200 8C. Similarly, a mesophase with a very fine treaded texture was observed forP2at 190 8C. The optical texture of the sample was almost unchanged after it was quenched to room temperature. This is advantageous for our further application in rubbing alignment process.
4. Optical properties
Absorption and emission spectra were measured in THF, CHCl3, Toluene, and in the solid state. Fig. 2 shows the
UV–Vis absorption and fluorescence spectra of these polymers as solid film and in THF. The wavelengths of absorption and emission maxima are listed in Table 1. The film of P1 has an absorption maximum (kmax) at 381 nm,
which is about 70 and 35 nm blue-shifted as compared to PPV and DP-PPV, respectively. This can be attributed to the bulky substituents of the two phenyl rings and the pendant alkyl groups that interrupt the planarity of the main chain and thus reduce the degree of conjugation. The kmaxof P1at
339 nm in chloroform, 348 nm in THF, and 378 nm in toluene, is blue-shifted with respect to that of the film. Similar results were obtained forP2andP3. The absorption maxima of the films are slightly red-shifted as compared to those in solutions, consistent with other poly(p-phenylene vinylene)-related polymers [11].
The new DP-PPV polymers are highly fluorescent in the solid state as well as in dilute solution. As shown in
Fig. 2 and Table 1, PL spectra of P1 and P2 in low polarity solvent, such as toluene and in the solid state are red-shifted with respect to those in polar solvents, suggest-ing that polymer aggregation is relatively strong in the non-polar solvents and solid state. Comparing with other PPVs such as MEH-PPV and polyfluorene where large PL peak wavelength difference of 40–60 nm between solid state and dilute solution was reported[8,12–14,17], we have the same PL wavelength-shifted tendency, but red-shifts are much
Fig. 1. Optical textures of (a) polymer P1 at 200 8C and (b) polymer P2at 190 8C.
Table 1
Optical properties of the polymers
Polymer Absorption Fluorescence
In THF In CHCl3 In toluene Films In THF In CHCl3 In toluene Films
kmax(nm) kmax(nm) kmax(nm) kmax(nm) kmax(nm) kmax(nm) kmax(nm) kmax(nm)
P1 348 339 378 381 473 475 502 503
P2 NAa 357 NAa 381 NAa 476 NAa 494
P3 358 360 358 375 477 477 474 483
PPV NAb NAb NAb 440 NAb NAb NAb 565
DP-PPV NAb NAb NAb 405 NAb NAb NAb 505
a Slight soluble in THF and toluene. b Insoluble in organic solvents.
smaller for the DP-PPVs. This is most apparent for P3, its emission peak remains relatively unchanged in the solid state and in solutions. The fluorescence quantum yields (Ufl)
of the polymers in THF were estimated by comparing with the standard of quinine sulfate (ca. 110 5M solution in 0.1 M H2SO4, having a fluorescence quantum yield of
55%). The Uflof P1,P2 and P3 are 0.57, 0.53 and 0.65,
respectively. The results demonstrate that high PL yield polymers can be achieved by the introduction of the bulky side groups, since separation of the polymer backbones partially can prevent interchain exciton transfer.[12,15].
5. Polarized photoluminescent
We aligned P1 and P2by a rubbing treatment at the LC state to give polarized optical properties. The UV dichroism measurement was performed in the presence of a polarizer inserted in parallel or in perpendicular (with respect to the rubbing direction) between the sample and the light source. As shown in Fig. 3, a significantly larger absorption ascribed to a k–k* transition can be seen at the perpendic-ular polarized direction for P1. Rubbing-induced chain alignment of P1 was also detected by a polarized PL measurement. The dichroic PL spectra ofP1are also shown inFig. 3, indicating that the light emitted from the rubbed film was preferentially polarized perpendicular to the rubbing direction. This is because rubbing at thermotropic liquid crystalline phase induces alignment of the LC side groups along the rubbing direction and the alignment of the polymer backbones perpendicular to the rubbing direction (Fig. 4). As a result, relatively large absorption and emission are observed in the orthogonal direction with respect to the rubbing direction. The dichroic ratio, defined as the perpendicular to parallel fluorescence intensity, was 2.1 which was better than dialkoxy side chain liquid crystalline PPVs and PTVs (1.2–1.4) [16]. However, we did not see large difference in peak intensity between rubbed and unrubbed films. This suggests that alignment may occur only at the top surface and not in the bulk film.
6. Electrochemical study
The cyclic voltammograms of compound 6 and P1– P3(Fig. 5) absorbed on a Pt wire from toluene solution were performed in an electrochemical cell with a Pt counter electrode and a Hg reference electrode. From the different onset potentials, and the band gaps calculated from the onsets of UV absorption, the band diagrams were determined [17,18] and displayed in Fig. 6. It can be
Fig. 3. Polarized optical absorption spectra and PL spectra of polymer P1. Fig. 2. UV–Vis and PL spectra of all polymers in solid state (solid square)
seen that all DP polymers show similar HOMO-LUMO levels suggesting that the pendant groups do not change the electronic state of the polymer significantly, although they may help the charge transport and injection. This resembles the molecularly doped system. The cyclic voltagram of 6 shown in the inset of Fig. 5c suggests that it is a one-electron transport material that can be easily reduced. The oxidation potential for imidazole is 0.52 V, corresponding to a HOMO level of 4.92 eV. This suggests that removal of electrons from 6 to ITO can readily occur. However, the effect of the imidazole group cannot readily be seen from Fig. 6.
7. Electroluminescence
Double-layer LED devices ITO/PEDOT:PSS/Polymer/ Ca(Al) were fabricated by spin coating the polymer solution onto ITO-coated glass substrates. The coating thickness of PEDOT and polymers was about 1000 2, and the active areas were 0.09 cm2. The EL spectra of the polymers are shown in Fig. 7. All polymers showed bluish-green emission at around 490 nm, in good agreement with the PL emission peaks. These results suggest that EL and PL come from similar excited states. The current–voltage–luminance characteristics of three polymers are shown in Fig. 8. The turn-on voltage of the P1 device is 11 V with a maximum brightness of 420 cd/m2and maximum EL yield of 0.79 cd/ A at 16 V. The turn-on voltage of the P2device is 10 V with a maximum brightness of 70 cd/m2and maximum EL yield of 0.33 cd/A at 24 V. The turn-on voltage of the P3device is 8 V with a maximum brightness of 22 cd/m2 and maximum EL yield of 0.11 cd/A at 12 V. The lower turn-on voltage of P3 may be due to the introduction of imidazole charge transport side group, which results in an increase of charge transport properties. However, the three polymers still did not show reduced driving voltage as compared with the unsubstituted DP-PPV. This suggests that the DP-PPV polymer backbone controls the funda-mental electro-optical properties of this series polymer.
Although the present polymers have high PL quantum efficiency, they did not show high electroluminescent as other substituted PPV polymers such as MEH-PPV did.
Fig. 5. Cyclic voltammograms of polymer films dip-coated on platinum plate electrodes in acetontrile containing 0.1 M Bu4NBF4. Platinum wire as
the counter electrode. The potentials reference against Ag/0.1M AgNO3in
acetonitrile. Scan rate: 50 mV/s. Fig. 4. Alignment of LC side groups and polymer backbones due to rubbing
This may be attributable to the very order packing of DP-PPV backbones which was proved by X-ray diffrac-tions[19].
8. Summary
We synthesized three substituted DP-PPV derivatives, and the PL and EL properties were characterized. The three bulky substituents make the polymer chain rotation, forming cis-and trans-structures, and non-aggregation. The three things make our polymers show blue shift and high PL efficiency with respect to the traditional PPV. An improvement of the emission properties compared with traditional DP-PPVs was obtained from the three polymers as the double layer devices of the type ITO/PEDOT:PSS/Polymer/Ca(Al). Device fabricated by P1 turn on at 11 V and a maximum luminance of 433 cd/m2could be observed at 17 V applied voltage. This is the brightest DP-PPV EL device so far. We
also showed clear evidence of nematic LC phases in the polymers P1 and P2. The polymers can be aligned by traditional rubbing treatment to give linearly dichroic PL with a dichroic ratio of 2.1. The decrease of the driving voltage of P3 is due to the introduction of imidazole group to decrease the band offset between polymer and hole injection electrode. In this result, we successfully could obtain a low driving voltage electroluminescent
Fig. 8. Current–voltage–luminescence characteristics of ITO/PEDOT/ polymers/Ca(Al).
Fig. 7. Electroluminescence spectra of the polymers P1 (n), P2(E), and P3(o).
Fig. 6. Band diagram of 6, DP6-PPV, P1, P2, andP3used in this study. The position of the valence band (HOMO) is estimated from electrochemical studies, and the band gap (HOMO-LUMO) from the onset of optical absorption.
DP-PPV polymer by adopting the charge transport side group.
Acknowledgements
The authors are grateful to the National Science Council of the Republic of China (NSC90-2216-E-009-019) for its financial support of this work.
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