Y. Qu et al. / Tetrahedron Letters 54 (2013) 4942–4944
4943
HOMO
LUMO
LUMO+1
1
Scheme 1. Structures of 1 and 1-CN.
1-CN
which can be confirmed by 1H NMR, 13C NMR, HRMS, and IR spec-
tra (Figs. S2–S5).
Figure 2. Electron density maps of the frontier molecular orbitals of 1 and 1-CN.
Fluorescent properties of sensor 1 were also studied by adding
CNÀ to a pure water solution of 1 (2.5
lM) at room temperature. As
shown in Figure 1B, the emission 1 at 612 nm (kex = 465 nm) de-
creased rapidly upon the addition of CNÀ. When 2.4 equiv CNÀ
was added to the solution of 1 (Uf = 0.16, pH 7, Fig. S1), a fivefold
(F0/F) decrease in fluorescence intensity at 612 nm was observed.
These facts indicate that 1 can serve as a ‘naked-eye’ sensor for
CNÀ.
This is further supported through TD-DFT calculations on 1 and
1-CN compounds. The molecular orbitals of these compounds are
presented in Figure 2. The HOMO orbital of 1 is localized on the en-
tire molecule including the donor and acceptor. The LUMO orbital
is concentrated on the acceptor side of dicyano-vinyl and LUMO+1
is on the pyridine groups, thus resulting in a charge transfer from
triphenylamine to dicyano-vinyl and pyridine. Interestingly, the
electron density of 1-CN compound is significantly contributed to
the cyanation of the anionic species at the HOMO level, but the
LUMO state stretches out to the pyridine moiety. However, the
electron density of the phenyl group connected with the cyanine
anion is low. ICT process in sensor 1 is also weak. Furthermore,
we also calculated the lowest excitation energies of 1 and 1-CN
(Table 1). Calculation results indicated the absorbance at short
wavelength became stronger than that at long wavelength in 1-
CN, which is close to the experimental results (Table 1). Although
the computational absorption spectra underestimated the experi-
mental absorption maxima in general as shown in Table 2, analo-
gous spectroscopic behaviors were reproduced qualitatively.
Moreover, absorption band at 471 nm in 1-CN is close to the exper-
imental results (465 nm).
To better evaluate the cyanide-selective nature of 1, fluores-
cence changes caused by the addition of other anions, including
FÀ, ClÀ, BrÀ, IÀ, CO32À, HCOÀ3 , SO23À, H2POÀ, HPO2À, PO43À, SCNÀ,
4
4
NOÀ2 , S2O8À, AcOÀ, S2À and N3À were investigated. A pure water solu-
tion of 1 (2.5 lM), containing 40 equiv of each of these anions,
were maintained for 20 min at room temperature and then sub-
jected to fluorescence analysis. As shown in Figure 3, anions other
Table 1
Calculated TD-DFT (MPW1K) excitation energies for the lowest transition (eV, nm),
oscillator strengths (f), and composition in terms of molecular orbital contributions,
and experimental absorption maxima
State
Compositiona
E (nm)
f
Exp. (nm)c
1
S1
S2
S1
S2
94% H ? L
88% H ? L+1
98% H ? L
414.15
309.95
471.62b
419.19b
1.2040
0.7433
0.0083
0.0152
465
360
465
360
1-CN
83% H ? L+1
a
b
c
H = HOMO, L = LUMO, L+1 = LUMO+1.
TD-DFT calculation in vacuo.
In H2O.
Figure 1. (A) Absorption titration of 1 (2.5
1.2, 1.6, 2.0, 2.4, 2.8, 3.2, 3.6, 4.0, 4.4, 4.8, and 5.2
l
M) with the addition of CNÀ (0, 0.4, 0.8,
M) in water at room temperature
Figure 3. Various anions selectivity profiles of 1 (2.5
lM) in the presence of various
l
anions in water (pH 7): (black bars) emission ratios of (F0 À F)/F0 at 612 nm in the
(inset: the color change images of 1). (B) Emission titration of 1 (kex = 465 nm) with
presence of 40 equiv of FÀ, ClÀ, BrÀ, IÀ, CO23À, HCO3À, SO23À, H2POÀ, HPO2À, PO34À
,
4 4
addition of CNÀ (0, 0.4, 0.8, 1.2, 1.6, 2.0, 2.4, 2.8, 3.2, 3.6, 4.0, 4.4, 4.8, and 5.2
lM) in
SCNÀ, NO2À, S2OÀ8 , AcOÀ, S2À and NÀ3 ; (blue bars) fluorescence intensity in the
presence of various anions, followed by 4.0 equiv of CNÀ.
water at room temperature (inset: the fluorescent change images of 1).