Y.-H. Yu et al. / Organic Electronics 12 (2011) 694–702
697
in 82% yield. 1H NMR (500 MHz, CDCl3): d = 2.24 (s, 12 H),
6.98–6.99 (d, J = 1.2 Hz, 16 H), 7.30–7.34 (m, 4H), 8.16–
8.19 (m, 4H); 13C NMR (125 MHz, CDCl3): d = 20.6, 120.1,
121.1, 126.6, 129.8, 130.3, 131.9, 137.5, 145.6; EI MS (m/
e): 568 (M+).
lower. The deposition rate was 1 Å/s for all organic films.
The LiF film, with thickness of 15 Å, was evaporated at a
rate of 0.1 Å/s. The Al cathode, with thickness of 200 nm,
was deposited at a rate of 5 Å/s.
2.2.4. N,N,N0,N0-tetrakis-(3,4-dimethyl-phenyl)-anthracene-
9,10-diamine (TmpAD)
3. Results and discussion
For the synthesis of TmpAD, the Bis-(3,4-dimethyl-phe-
nyl)-amine was first synthesized as the following proce-
dure: 4-Bromo-o-xylene (2 g, 10.8 mmol), Benzylamine
(2.54 g, 23.7 mmol), Pd2(dba)3 (0.1 g, 1 mol%), t-BuONa
(2.4 g, 2.3 equiv.) were weighted into a 250 ml double-
neck round-bottom flask connected with a condenser un-
der nitrogen. About 50 mL of toluene was added and then
stirred to give a homogeneous mixture. A solution of
5 mol% P(t-Bu)3 in toluene (2.6 mL) was then added to
the mixture and reacted at 130 °C. After overnight, the
resulting solution was cooled to room temperature, and
the solution was evaporated to dryness to afford a powder,
which was adsorbed onto 4 g of silica gel and chromato-
graphed with hexane to give 2 g (yield: 80%) of Benzyl-
bis-(3,4-dimethyl-phenyl)-amine as a red-brown liquid.
The as-prepared Benzyl-bis-(3,4-dimethyl-phenyl)-amine
was further reduced to form Bis-(3,4-dimethyl-phenyl)-
amine. A mixed solvent of ethanol and THF was added to
a 100 mL double-neck round-bottom flask which con-
3.1. Photo-physics studies
The photo-physics properties of as-synthesized methyl
groups substituted N-aryl anthracene-9,10-diamine deriv-
atives TAD, TmAD, TpAD and TmpAD were studied by UV–
visible and fluorescence spectrophotometer. The absorp-
tion and emission spectra as illustrated in Fig. 2a and Table
1 show that these compounds in form of solid film have
major absorption bands with wavelength maxima (kmax
)
within 258–268, 296–297, 360–380 and 470–490 nm.
The potoluminence (PL) emission band has kmax located
around 519–532 nm. As a result, compound TAD and
TmAD have similar emission spectra with kmax ꢂ 520 nm
in solid state, whereas there are obvious bathochromic
shift observed at kmax ꢂ 530 nm for compound TpAD and
TmpAD. The compound TmpAD, with methyl groups
substituted in both para/meta position, also has similar
emission spectra to that of TpAD. The result indicates the
methyl group substituted at the para position of aromatic
phenyl diamine has a greater electronic effect than meta
position on the anthracene moiety. There is a strong sol-
vent effect for these anthracene materials as illustrated
in Fig. 2b and Table 1. Basically the emission color of these
compounds exhibit a green color in non-polar solvents, i.e.,
toluene, and red shift to yellow-green color in polar sol-
vents, i.e., CH2Cl2, for compound with methyl substuents.
The solvent effect indicates there is an observable dipole
moment between phenyl diamine and anthracene moie-
ties. The dipole moment is strongly dependent on the posi-
tion of methyl groups at the phenyl diamine, especially for
the compound TpAD and TmpAD. The effects of methyl
substituents for the comparison of kem in solvent phase
showed the following sequence of TmpAD, TpAD and then
TmAD.
tained
Benzyl-bis-(3,4-dimethyl-phenyl)-amine
(2 g,
6.34 mmol) and Pd/C (0.025 g, 2 mol%) and stirred under
nitrogen. After the starting materials had dissolved, hydro-
gen gas was then bubbled into the solution and further re-
acted overnight. The reaction was monitored by thin-layer
chromatography. After the reaction had completed, the
resulting brown solution was evaporated to dryness to af-
ford 0.83 g (yield: 58%) of Bis-(3,4-dimethyl-phenyl)-
amine as a brown solid which was used as the starting
material for the synthesis of compound TmpAD. Compound
Benzyl-bis-(3,4-dimethyl-phenyl)-amine was identified by
1H NMR (400 MHz, CDCl3): d = 2.08–2.19 (m, 12 H), 4.30 (s,
2 H), 6.40–6.43 (q, J = 2.4 Hz, 2H), 6.49–6.50 (d, J = 2.0 Hz,
2H), 6.93–6.95 (d, J = 80 Hz, 2H), 7.25–7.38 (m, 5H). Com-
pound bis-(3,4-dimethyl-phenyl)-amine was identified by
1H NMR (400 MHz, CDCl3): d = 2.19–2.20 (d, 12 H), 5.43
(s, 1 H), 6.78–6.82 (m, 4 H), 6.99–7.01 (d, 2H).
From 9,10-Dibromoanthracence (5 g, 14.9 mmol) and
Bis-(3,4-dimethyl-phenyl)-amine (8.05 g, 35.7 mmol),
compound TmpAD was obtained as an orange solid. The
crude product was purified twice by sublimation to afford
compound TmpAD in 81% yield. 1H NMR (400 MHz, CDCl3):
d = 2.11 (s, 12 H), 2.15 (s, 12H), 6.77–6.80 (q, J = 2.4 Hz, 4
H), 6.91–6.93 (m, 8 H), 7.31–7.33 (q, J = 3.2 Hz, 4 H),
8.17–8.19 (q, J = 3.2 Hz, 4 H); 13C NMR (100 MHz, CDCl3):
d = 18.9, 20.1, 117.8, 121.4, 125.2, 126.4, 129.0, 130.2,
132.0, 137.2, 137.5, 145.96; EI MS (m/e): 624 (M+).
A photoelectron spectrometer was used to evaluate
the energy of the highest occupied molecular orbital
(HOMO). The energy gap (Eg) was calculated by the for-
mula: Eg (eV) = hc/konset = ꢂ1241/konset
,
where
h
is
Planck’s constant and c is speed of light. The wavelength
onset, konset, was obtained by absorption spectra as illus-
trated in Table 1. The lowest unoccupied molecular orbi-
tal (LUMO) was derivated from the values of HOMO and
Eg, and the data are listed in Table 1. The relative energy
diagram of materials used for devices fabrication is com-
pared in Fig. 1 The compound TmpAD has relatively the
smallest value of HOMO, i.e. 5.37 eV, due to its higher
donor ability than others. The delocalization degree of
anthracene relatively decreased along with the donor
ability of phenyl diamine moiety, and the energy band
gaps become smaller. The energy band gaps follow the
2.3. OLED fabrication
Indium tin oxide (ITO)-coated glass substrates were
thoroughly cleaned and treated with oxygen plasma.
OLEDs were fabricated by using a multiple source thermal
evaporation system at a base pressure of 2 ꢀ 10ꢁ5 Torr or
sequence:
compound
TAD > TmAD > TpAD > TmpAD,
where the Eg values are 2.46, 2.44, 2.39 and 2.36 eV,
respectively.