Table 1. Summary of Physical Measurements of OFn-EG, n ) 1-3, and EG-H
f
λabs a/nm (ꢀ‚105/M-1cm-1
)
λem a,b/nm
Φa,c
ETEa,d/%
HOMOe/eV
E1/2e/V
Eg /eV
Tgg/°C
Tdech/°C
max
max
OF1-EG
OF2-EG
OF3-EG
EG-H
347 (1.31)
348 (1.49)
356 (1.66)
324 (0.65)
404
436
436
396
<0.01
0.31
0.38
78
68
69
5.18
5.19
5.19
5.17
0.38, 0.71
0.39, 0.69
0.39, 0.68
0.40, 0.75
2.08
2.17
2.20
1.87
192
225
254
124
596
601
601
565
<0.01
a Measured in CHCl3. b Excited at the absorption maxima. c Using quinine sulfate monohydrate (Φ313 ) 0.48) as a standard. d Energy-transfer efficiency
e
is determined by comparing the absorption maximium of the dendritic wedges of the absorption and fluorescence excitation spectra. E1/2 vs Fc+/Fc estimated
by CV method using platinum disk electrode as a working electrode, platinum wire as a counter electrode, and SCE as a reference electrode with an agar
salt bridge connecting to the oligomer solution. All of the potentials were calibrated with ferrocene, E1/2 (Fc/Fc+) ) 0.45 V vs SCE. f Estimated from the
edge of electronic absorption spectra. g Determined by differential scanning calorimeter from remelt after cooling with a heating rate of 10 °C/min under N2.
h Determined by thermal gravimetric analyzer with a heating rate of 10 °C/min under N2.
and 356 nm, respectively, and were generally structureless
and blue shifted (∼30 nm) relative to the corresponding
diphenylamino end-capped oligofluorenes4b (Figure 1a and
triarylamine to the fluorene core. The energy transfer
efficiency (ETE) of this dendritic wedge is approximately
70% as estimated by comparing the difference in intensity
at the absorption maximum of the dendritic wedges of the
absorption spectrum and the fluorescence excitation spec-
trum. The fluorescence quantum yields (ΦPL) measured in
chloroform using quinine sulfate monohydrate as a standard
are less than 0.01, 0.31, and 0.38, respectively, and increase
as the core chain length increases, indicating the longer
homologue has better coplanarity in the excited state than
the shorter one; however, these ΦPL values are quite smaller
than those (∼0.90) of the corresponding analogues only end-
capped with diphenylamino groups,4b suggesting that intro-
duction of dendrons onto the oligofluorene skeleton perturbs
the planarity and alters the fluorescent nature of oligofluorene
core.
Figure 1. (a) Absorption and fluorescence spectra of OFn-EG
and EG-H, measured in CHCl3. (b) Cyclic voltammograms of OFn-
EG and EG-H, measured in CH2Cl2.
The electrochemical behaviors of these newly synthesized
dendrimers are tabulated in Table 1 and Figure 1b. In contrast
to the triaryldiamine,4b,c the new dendrimers OFn-EG exhibit
an electrochemical behavior similar to that of the triary-
lamine- and carbazole-based dendron EG-H, in which one
reversible four-electron anodic redox couples (E1/2 ∼ 0.38
eV), corresponding to removal of electrons from the periph-
eral arylamino group of the dendrons, and another reversible
two-electron anodic redox couple (E1/2 ∼ 0.70 eV), corre-
sponding to removal of electrons from the interior carbazole
moieties forming radical tetracations and hexylcations,
respectively (Figure 1b). Both first oxidation potentials and
second oxidation potentials are essentially unaffected by the
length and structure of the oligofluorene core as the oxidation
occurs only at the wedges; however, both first oxidation
potential values and second oxidation potential values of
OFn-EGs are a bit smaller than those of EG-H (E1/2: 0.40
and 0.75 eV, respectively) (Table 1), indicating that the
incorporation of dendron EG makes the resulting dendrimers
more susceptible for electrochemical oxidation. In general,
with an incorporation of triarylamine-based dendritic end-
caps, the HOMO energy level of oligofluorenes moves up
to ∼5.20 eV (relative to the vacuum level) as estimated by
the electrochemical method. Such a high HOMO energy level
greatly reduces the energy barrier for the hole injection from
ITO (φ ) 5.0 eV) to the emissive oligofluorenes. As a result,
OFn-EGs can also be used as hole transport/injection
materials.
Table 1). There is a substantial red-shift of the absorption
maxima (λmax) of oligofluorenes (∆ 25-54 nm) upon
incorporation of strongly electron-donating diphenylamino
group(s) which is attributed to the asymmetric destabilization
of the HOMO and the LUMO levels leading to the decrease
in the energy gap;9 however, the introduction of dendrons
onto the oligofluorene backbone causes the resulting mol-
ecule less planar than the analogues end-capped with
diphenylamino groups in their electronic ground state leading
to a blue shift in λabs
(∆ 30-54 nm).10 The absorption
max
maxima (λabsmax) and molar absorptivities (ꢀmax) of OFn-EGs
increase sequentially as the core chain length increases
(Figure 1a and Table 1). Surprisingly, the emission maxima
(λemmax: 404, 436, and 436 nm, respectively) of these
dendrimers first red-shifted (∆ 5 nm) and then remained
fairly constant at 436 nm (Figure 1a and Table 1). Upon
excitation either at 324 nm attributed to the nfπ* transition
of triarylamine- and carbazole-based dendron or at 350 nm
corresponding to the πfπ* transition of oligofluorene core,
the emission spectra obtained are identical, suggesting that
energy or exciton can efficiently transfer from the peripheral
(9) Wong, M. S.; Li, Z. H. Pure Appl.Chem. 2004, 76, 1409.
(10) (a) Berlman, I. B.; J. Phys. Chem. 1970, 74, 3085. (b) Nijegorodov,
N. I.; Downey, W. S. J. Phys. Chem. 1994, 98, 5639.
Org. Lett., Vol. 8, No. 7, 2006
1501