S. Wu et al. / Tetrahedron Letters xxx (2016) xxx–xxx
3
Subsequently, fluorescence titration of FBB by increasing
amounts of Fꢀ ions was examined (Fig. 6). Upon excitation at
320 nm, the free sensor showed an intense emission at 539 nm,
however, the addition of the Fꢀ led to a drastic decrease at
539 nm and simultaneous appearance of a new emission band at
435 nm.
Inset in Figure 5 shows a near-linear correlation of FBB between
intensity ratios of absorbance at 363 nm to those at 422 nm
(A363/A422) vs concentrations of Fꢀ in the range from 0 to 150
lM
(0–3.0 equiv) in THF. The linear equation was found to be
y = 0.70 ꢂ 105x + 0.73 (R2 = 0.9984) (Fig. S1), where
y is the
absorbance at 363 nm measured at a given Fꢀ concentration and
x represents the concentration (10ꢀ5 mol/L) of F ꢀ. According to
IUPAC, the detection limit was determined from three times the
standard deviation of the blank signal (3d) as 0.12 lM. This also
demonstrated the potential utility of probe FBB for calibrating
and determining fluoride ion concentration in THF. Furthermore,
a
corresponding correlation between emission ratiometric
Figure 4. Fluorescent spectra of probe FBB solution (5 ꢂ 10ꢀ5 M) in the absence
and ꢀpresence of 5.0 equiv of various anions (Fꢀ, Clꢀ, Brꢀ, Iꢀ, HSO4ꢀ, H2PO4ꢀ, OAcꢀ,
response of FBB at 539 nm and 435 nm (I435/I539) and fluoride
ion concentration in THF (Fig. 6, inset). Thus, FBB could also serve
as a ratiometric fluorescent probe for Fꢀ. As a result, the probe pro-
vided a ‘on–off–on’ colorimetric (A363/A422) and ratiometric fluo-
rescent response (I435/I539) to Fꢀ.
NO3
, a photograph showing the colour change of FBB
CNꢀ) in THF. Inset:
(1 ꢂ 10ꢀ4 M) under a UV lamp (at 365 nm) in THF without or with addition of
5.0 equiv of TBAF.
On the basis of the above experiments, we hypothesized that
the affinity of Fꢀ to boron centre led to the cleavage of B and N,
and the phenolic O–H and benzylic N engaged in strong hydrogen
bonds with fluoride. The change promoted both the photo-induced
electron-transfer (PET) and the intramolecular charge transfer
(ICT) effects30, as shown in Scheme 2. To confirm this assumption,
the titrations of 1H NMR (Fig. 7a), 19F NMR (Fig. 7b) and 11B NMR
(Fig. S2) were adapted. From the 1H NMR titration spectra, the Ha
shifted to the low field due to the deshielding effect induced by
the combination of Fꢀ and Ha. The peak position of Hb in 1H NMR
illustrated by the addition of Fꢀ, the first cleavage of B–N led to
the slight movement of Hb’s chemical shift to the upfield. When
the Fꢀ concentration became higher, the deshielding effect was
created due to the strong affinity between B and Fꢀ and the pheno-
lic O–H and benzylic N engaging in strong hydrogen bonds with
fluoride, thus, the position of Hb moved to the low field in the spec-
trum. The intramolecular hydrogen bond effect caused the chemi-
cal shift of Hc changing to the downfield. In the 19F NMR, the three
group of peaks of different fluorine ions found in the spectra with
the addition of Fꢀ could illustrate that the Fꢀ from the TBAF formed
the complex with the probe molecules.31 In the process of the 19F
NMR titration, the distance of Fa and Fb in the chemical shift was
Figure 5. UV–vis absorption spectra of FBB (5 ꢂ 10ꢀ5 M) in THF upon addition of
0–5.0 equiv of TBAF. Inset: plot of the absorbance ratio of FBB between 363 nm and
422 nm (A363 nm/A422 nm) versus concentration of Fꢀ in THF.
H2PO4ꢀ, OAcꢀ, NO3ꢀ, CNꢀ, to investigate the selectivity (Figs. 3 and
4). Free FBB displayed a maximum absorption at 422 nm. nBu4NF
(TBAF) as a fluoride source was added to a THF solution of the
probe FBB, the peak at 422 nm was decreased along with a new
peak at 363 nm appeared. However, the addition of other anions
caused little changes in the absorption (Fig. 3). The similar phe-
nomena occurred on the fluorescence with the addition of anions.
Upon addition of 5.0 equiv of Fꢀ ions to FBB solution, the emission
at 539 nm was decreased, accompanied with the appearance of a
strong emission band at 435 nm and a remarkable hypochromatic
shift of 104 nm, while other anions induced little quenching effect
at 539 nm without any new bank emerged (Fig. 4). Thus, FBB has
good sensitivity and selectivity for Fꢀ ions.
To get insight into the mode of probe FBB with the fluoride ions,
UV–vis absorption and fluorescence emission spectra were investi-
gated. In the absence of anions, the maximum absorption wave-
length of FBB was at about 422 nm. Upon progressive addition of
TBAF, the peak at 422 nm decreased gradually, and a large blue
shift of the maximum could be observed and increased,
meanwhile, a new band at 363 nm was developed with a clear
isosbestic point at 396 nm, which indicated the formation of the
new compound (Fig. 5).
Figure 6. Emission spectra of FBB (5 ꢂ 10ꢀ5 M) in THF (kex = 320 nm) upon the
addition of 0–5.0 equiv of TBAF. Inset: plot of the emission intensity ratio of FBB
between 435 nm and 539 nm (I435 nm/I539 nm) versus concentration of Fꢀ in THF.