Chemistry Letters Vol.34, No.7 (2005)
901
Table 2. Optical properties of the polymers 2
emitting core in poly(carbazol-2,7-ylene) by introducing the aryl
group enhanced quantum efficiency in comparison with poly-
(N-alkylcarbazol-2,7-ylene)s (ꢂ ꢃ 0:8).2 The branched 2-ethyl-
hexyl side chain effectively worked disturbing formation of
excimers. The polymerization of 1 by Zn with the Ni catalyst
(method B) was enough to obtain the polymer with good optical
properties, which had a merit without using the hazardous
Ni(cod)2. Furthermore, preliminary manufacturing of PLED
device with 2 (method A) composing of ITO/PEDOT(PSS)/2/
Ca–Al realized the blue emission the same to the PL spectra in
the solid state at a low turn on voltage (ꢃ3 V) with a maximum
luminance (about 2000 cd/m2) and an efficiency ðꢃcÞ > 0:2 cd/
A at 10 V, which was superior to those of poly(N-alkylcarbazol-
2,7-ylene)s. The bridged triphenylamine structure might affect a
hole transporting ability of 2, which resulted in an appropriate
bipolar valance of the device.
Solution ꢁmax (nm) Thin solid ꢁmax (nm)
Polymer
(method)
ꢂfd
abs.
Emc
abs.
em.
2a (A)a
2b (A)a
2b (B)a
2b (B)b
380
379
384
372
418
420
417
415
418
381
389
373
(441) 467
432
433
0.87
ꢃ1
ꢃ1
428
0.80
aPrepared from 2,7-dichlorocarbazole monomers (1a and 1b).
bPrepared from 2,7-dibromocarbazole 1c. cThe polymer concen-
tration was about 10ꢁ6 mol/dm3. dFluorescence quantum yields
(ꢂf) were determined in CHCl3 against 9,10-diphenylanthracene
in cyclohexane (ꢂf ¼ 0:9) as the standard.
This work was partially supported from Promotion of
Creative Interdisciplinary Materials Science for Novel Functions
by The 21st Century COE Program. We thank to Fujitsu Lab.
Ltd. for making and evaluation of the PLED devices, and the
Chemical Analysis Center, University of Tsukuba, for NMR
spectroscopic and elemental analysis data.
References and Notes
1
D. Y. Kim, H. N. Cho, and C. Y. Kimm, Prog. Polym. Sci., 25,
1089 (2000); A. Kraft, A. C. Grimsdate, and A. B. Holmes,
Angew. Chem., Int. Ed., 37, 402 (1998); R. H. Friend, R. W.
Gymer, A. B. Holmes, J. H. Burroughes, R. N. Marks, C.
300
400
500
600
Wavelength/ nm
´
Taliani, D. D. C. Bradley, D. A. Dos Santos, J. L. Bredas,
M. Logdlund, and W. R. Salaneck, Nature, 397, 121 (1999).
Figure 1. UV–vis absorption and fluorescence spectra of 2b in
CHCl3 (solid line) and in the solid state (broken line).
¨
2
J.-F. Morin and M. Leclerc, Macromolecules, 34, 4680 (2001);
G. Zotti, G. Schiavon, S. Zecchin, J.-F. Morin, and M. Leclerc,
Macromolecules, 35, 2122 (2002); J.-F. Morin and M. Leclerc,
By contrast, 2b having the branched 2-ethylhexyl (EH) side
chain showed the absorption ꢁmax, both in the solution and in
the solid state, was around 380 nm (Figure 1). This suggests that
2b has very similar conformations in both states. From the ab-
sorption edge observed in the thin-film samples, HOMO–LUMO
energy gap (Eg) is estimated to be 2.80 eV for 2a and 2.90 eV for
2b, respectively. The HOMO level is also determined by electro-
chemical method,8 being about ꢁ5:8 eV.
´
Macromolecules, 35, 8413 (2002); J.-F. Morin, S. Beaupre,
M. Leclerc, I. Levesque, and M. D’lorio, Appl. Phys. Lett.,
80, 341 (2002); J.-F. Morin, P.-L. Boudreault, and M. Leclerc,
Macromol. Rapid Commun., 23, 1032 (2002).
´
`
ˆ ´
3
4
J.-F. Briere and M. Cote, J. Phys. Chem. B, 108, 3123 (2004).
S. Abe, Y. Nagasaki, and M. Kijima, Synth. Met., 135–136,
123 (2003).
PL spectra of 2b, which was symmetrical with a vibronic
fine structure to the absorption spectra, showed a maximum
emission (ꢁmax) around 420 nm in CHCl3 and 430 nm in the
solid state (Figure 1). Almost the same and narrow shape of
the emission spectra with slight difference of fluorescence
ꢁmax suggests that the emission is essentially the same both in
solution and in the solid state without formation of excimer. The
degree of polymerization and the terminal residue influence the
optical properties. On the other hand, 2a showed wider spectrum
than 2b in the solid state, and the emission ꢁmax shifted longer in
wavelength (Table 1). The symmetrical Gaussian fitting of the
fluorescence spectrum for 2a suggests that the spectrum is com-
posed of three peaks at 434, 461, 493 (shoulder) nm. The peak
around 430 nm may be formed by the radiative singlet exciton
decay with the Stokes’ shift of 50 nm and the most intense peak
around 465 nm may be attributed to the radiative decay of exci-
mer. The Stokes’ shifts are small within about 40 nm in solution
and 50 nm in the solid state. The fluorescence quantum efficien-
cy of 2 in CHCl3 is almost quantitative.
5
6
7
A. Klapars, J. C. Antilla, X. Huang, and S. L. Buchwald, J. Am.
Chem. Soc., 123, 7727 (2001).
F. Dierschke, A. C. Grinsdale, and K. Mullen, Synthesis, 2003,
¨
2470.
NMR data for 2a:1H NMR in CDCl3; ꢄ (ppm) 0.88 (3H, t,
CH3), 1.27–1.85 (20H, CH2), 4.05 (2H, t, OCH2–), 6.93–
8.13 (10H, carbazole, Ph); 13C NMR in CDCl3, 14.6 (CH3),
23.1, 26.5, 29.8, 29.87, 29.93, 30.11, 30.14, 32.4 (CH2), 68.8
(OCH2–), 109.1, 120.9, 122.5, 128.9, 140.7, 142.9, 158.7
(carbazole), 115.2, 116.1, 130.3, 159.0 (Ph), and for 2b:
1H NMR in CDCl3; ꢄ (ppm) 0.92, 0.99 (6H, CH3), 1.34–1.80
(8H, CH2), 3.95 (2H, OCH2–), 6.95, 7.58 (4H, phenyl), 7.10,
7.49, 8.15 (6H, carbazole); 13C NMR in CDCl3, 11.6, 14.6
(CH3), 23.5, 24.4, 29.6, 31.0, (CH2), 39.9 (CH), 71.3
(OCH2–), 109.1, 116.1, 122.5, 129.1, 130.3, 142.9 (carbazole),
115.2, 120.8, 140.7, 159.2 (Ph).
8
S. Gauvin, F. Santerre, J. P. Dodelet, Y. Ding, A. R. Hill, A. S.
Hay, J. Anderson, N. R. Armstrong, T. C. Gorjanc, and
M. D’Iorio, Thin Solid Films, 353, 218 (1999).
In conclusions, increase of rigidity at the absorption and
Published on the web (Advance View) May 28, 2005; DOI 10.1246/cl.2005.900