fluorescence changes.9 The latter, very convenient method,
is intriguingly attractive for sensing as it exhibits great
sensitivity at very low analyte concentrations down to the
micromolar scale,9b which is required for detection of
physiological fluoride3c as well as fluoride in drinking
water.4,8c However, most of the fluorescence-based sensory
materials employed rely on changes in the emission intensi-
ties that are less reliable than the detection of a new emission
at a different wavelength.9,10
δ ) 29.0 ppm. The blue luminescent compound 2 exhibits
pronounced optoelectronic properties with a maximum
wavelength of absorption at 376 nm, an emission at 419 nm,
and a very high photoluminescence (PL) quantum yield
efficiency of φPL ) 0.6113 that is typical for dithienophos-
pholes.12 Compared to the nonfunctionalized dithienophos-
phole 1 (λex ) 346 nm; λem ) 424 nm),12b the value for
absorption experiences a red shift of about 30 nm, supporting
the electron-accepting properties of the boryl groups, whereas
the emission is almost not affected.
An ideal sensory material for the fluoride ion at the parts
per million scale could therefore combine the strong affinity
of boron centers to fluoride with the generation of a new
fluorescence emission upon exposure. With respect to
stability under environmental conditions, the use of boronic
esters would be particularly favorable. Known fluorescence-
based sensor systems that utilize boron-fluoride interactions
are sensitive toward oxygen and moisture,8a,9d or they are
based on boronic acids, which involve complicated equilibria
through the formation of various fluoroborate species.10c
Boronic esters such as pinacole borane, on the other hand,
provide the necessary stability as well as selectivity toward
one fluoride ion only.11 The use of a π-conjugated material
with very favorable optoelectronic properties as central
fluorophore would also be very helpful for the successful
design of an appropriate sensor.7 In the context of our work
on materials for molecular electronics and optoelectronics,
we have established the novel dithieno[3,2-b:2′,3′-d]phos-
phole moiety that exhibits very promising photophysical
properties in terms of wavelength, intensity, and tunability.12
This system was expected to be an excellent fluorescent relay
for a corresponding boron-based sensory material. The
desired 5,5′-bis(pinacoleboryl) functionalized system can be
accessed by a newly developed general procedure via
lithiation of the unsubstituted dithienophosphole 1 with LDA
followed by the addition of 2 equiv of isopropoxy(pinacole)-
borane (iPrOB(pin)) at -78 °C in THF (Scheme 1). The
However, to gain the necessary stability at environmental
conditions, we targeted an oxidized phosphole species that
has been found to fulfill these requirements before.12 The
oxidized bis(boryl)dithienophosphole 3 is accessible in a
manner similar to that described for 2 followed by in situ
oxidation of the functionalized phosphole intermediate with
aqueous tert-butylhydroperoxide to give the air- and moisture-
stable product 3. Analysis by 31P NMR spectroscopy clearly
supports the oxidation of the dithienophosphole moiety with
a resonance at δ ) 16.5 ppm (δ 11B ) 28.5 ppm).
The fluorescence spectrum of the strongly blue luminesc-
ing 3 shows a maximum wavelength for absorption at λex
398 nm that is red shifted about 20 nm from the one for 2,
whereas the maximum wavelength for emission at λem
)
)
452 nm shows a red shift of about 30 nm supporting the
successful oxidation.12 The oxidized boryl-substituted species
3 also exhibits a very good PL quantum yield efficiency of
φPL ) 0.53.13
Treatment of a 1 × 10-4 M or 1 × 10-5 M undegassed
CH2Cl2 solution of 3 with a stoichiometric amount of
Bu4NF results in a significant red shift of the maximum
wavelengths for absorption and emission with λex ) 415 nm
and λem ) 485 nm, now displaying a blue-green emission
with a photoluminescence quantum yield of φPL ) 0.5513
(Figure 1, top). Owing to the formation of the ionic species
4 (δ 31P ) 17.9; δ 11B ) 5.8; δ 19F ) -132.2 ppm), the
intensities for absorption and emission, as observed by
fluorescence spectroscopy, drop to some extent but still
remain significantly strong. It is important to note that the
observed change in the fluorescence emission in a solution
of 3 toward the fluoro-substituted borate 4 can even be
detected, for the first time for B-F interactions,10c at the
micromolar (ppm) scale (see Supporting Information), which
is attributed to the extraordinary optoelectronic properties
of the dithienophosphole moiety. By contrast, addition of
Bu4NCl, Bu4NBr, or Bu4NI does not affect the fluorescence
properties of 3 at all, resulting in fluorescence spectra similar
to the one observed for genuine 3, supporting the high
selectivity of the boryl-functionalized dithienophosphole
toward fluoride ions. Slight differences from the spectrum
Scheme 1. Synthesis of Boryl-Functionalized
Dithieno[3,2-b:2′,3′-d]phospholes and Reaction with Fluoride
(10) (a) Kim, T.-H.; Swager, T. M. Angew. Chem., Int. Ed. 2003, 42,
4803. (b) Liu, B.; Tian, H. J. Mater. Chem. 2005, 15, 2681. (c) Badugu,
R.; Lakowicz, J. R.; Geddes, C. D. Sens. Actuators, B 2005, 104, 103.
(11) Aldridge, S.; Bresner, C.; Fallis, I. A.; Coles, S. J.; Hursthouse, M.
B. Chem Commun. 2002, 740.
(12) (a) Baumgartner, T.; Bergmans, W.; Ka´rpa´ti, T.; Neumann, T.;
Nieger, M.; Nyula´szi, L. Chem. Eur. J. 2005, 11, 4687. (b) Baumgartner,
T.; Neumann T.; Wirges, B. Angew. Chem., Int. Ed. 2004, 43, 6197.
(13) Relative to quinine sulfate (0.1 M H2SO4 solution). See: Demas,
N. J.; Crosby, G. A. J. Chem. Phys. 1971, 75, 991.
multinuclear NMR data support the successful functional-
ization of the dithienophosphole unit showing a 31P NMR
resonance at δ ) -24.3 ppm and a 11B NMR resonance at
496
Org. Lett., Vol. 8, No. 3, 2006