Table 1 Summary of fluorescence, molar absorptivity and quantum
yield F
Entry Excitation/nm Emission/nm ha
Fb
p - p*
n - p*
I
II
423
390
450
405
6.5 Â 104 3.4 Â 104 0.46
1.4 Â 105 5.5 Â 104 0.36
a
Molar absorptivity I: p–p* 350 nm, n–p* 422 nm; II: p–p* 390 nm,
b
n–p* 422 nm. Quantum yields are calculated based on quinine
sulfate.
This observation lends evidence against any excimer formation
as being responsible for the panchromatic features.10 As
shown in Table 1, both dyes exhibit high fluorescence quantum
yields. In addition, the optical spectra for these dyes indicate
high molar absorptivities. We tentatively assign the shortwave
and more intense absorption as p–p* and the long wavelength
less intense absorption as n–p*.11
In conclusion, we have synthesized two dual fluorescent
2,3-NI dyes using vicarious nucleophilic substitution at the
aromatic C–H bond to deliver the required Diels–Alder synthons.
Our hypothesis that 2,3-NI dyes would exhibit similar photo-
physics as symmetry related 1,8-NI proved to be a correct one
with the added advantage that the 5-ring carboximide/6-ring
N-aryl juncture permits broader fluorescence emission than
the more restrictive 6-ring carboximide/6-ring N-aryl juncture
of 1,8 NI. In addition these dyes exceeded our goals prescribed
earlier such as water solubility, reduced chromophore size and
molecular weight as well as a synthetic path that allows
synthetic diversity of substituents within the 2,3-NI frame-
work. Plans to utilize this synthetic approach for a variety of
panchromatic fluorophores are currently underway. Lastly,
experiments involving solid state optical properties using
electroluminescence are planned in the near future.
Fig. 1 The emission spectra of 20 mM compound I in water with
0.10% DMSO at different excitation wavelengths 390 nm, 423 nm and
450 nm, corresponding to blue, white and green photographs, respec-
tively. Colored light of cuvette is due to output of excitation light.
Fig. 2 Excitation–emission matrix of 20 mM compound I in DMSO
with 0.25% phosphate buffer (35 mM, pH 7).
Notes and references
states.8 An excitation–emission matrix of I in DMSO are
shown in Fig. 2. This figure shows broad spectrum of
wavelengths from 450 nm to 700 nm.
1 (a) Y. Xu, J. Jiang, W. Xu, W. Yang and Y. Cao, Appl. Phys. Lett.,
2005, 87, 193502; (b) H. Bolink, F. De Angelis, E. Baranoff,
C. Klien, S. Fantacci, E. Coronado, M. Sessolo,
K. Kalyanasundaram, M. Gratzel and K. Md. Nazeeruddin,
Chem. Commun., 2009, 4672–4674; (c) Y. Yang, M. Lowry,
M. C. Schowalter, J. T. Fakayode, R. F. Fronczek,
M. I. Warner and M. R. Strongin, J. Am. Chem. Soc., 2006, 128,
14081–14092; (d) S. Park, E. J. Kwon, H. S. Kim, J. Seo,
K. Chung, Y.-S. Park, J.-D. Jang, B. Medina, J. Gieschner and
K. S. Park, J. Am. Chem. Soc., 2009, 131, 14043–14049;
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A. W. Goddard, J. Am. Chem. Soc., 2005, 127, 15994.
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2008, 27, 231–242; (b) M. Sibrian-Vasquez and R. Strongin,
Supramol. Chem., 2009, 21, 107–110.
When we measured the fluorescence spectra at different
concentrations (Fig. 3), the peak profiles and lmax values
did not change over a 100 fold increase in concentration.
3 H. Bolink, F. De Angelis, E. Baranoff, C. Klien, S. Fantacci,
E. Coronado, M. Sessolo, K. Kalyanasundaram, M. Gratzel and
K. Md. Nazeeruddin, Chem. Commun., 2009, 4672–4674.
4 Y. Yang, M. Lowry, C. M. Schowalter, T. J. Fakayode,
F. R. Fronczek, I. M. Warner and R. M. Strongin, J. Am. Chem.
Soc., 2006, 128, 14081–14092.
5 S. Park, J. E. Kwon, S. H. Kim, J. Seo, K. Chung, S. Y. Park,
D. J. Jang, B. Medina, J. Gieschner and S. K. Park, J. Am. Chem.
Soc., 2009, 14043–14049.
6 Y. Liu, M. Nishiura, Y. Wang and Z. Hou, J. Am. Chem. Soc.,
2006, 128, 5592–5593.
7 G. A. S. Baker, S. Baker and T. M. McClesky, Chem. Commun.,
2003, 2932–2933.
Fig. 3 Fluorescence spectra of I at different concentrations (1 Â 10À5
,
6 Â 10À5 and 1 Â 10À3 M in water with 0.10% DMSO). The excitation
wavelength was 423 nm.
c
This journal is The Royal Society of Chemistry 2010
Chem. Commun., 2010, 46, 8002–8004 8003