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Y. Liu et al. / Dyes and Pigments 92 (2012) 909e915
a big change from 0.44 in the absence of Hg2þ to 28.7 when the
fluorescence and absorption changes (Fig. 8, inset). In addition,
because the excess of Cu2þ can partly quenches the fluorescence of
4 þ Hg2þ due to its paramagnetic property, thus, only 1 equiv of
Cu2þ was used in the selectivity experiment.
amount of Hg2þ ions added reached 1 equiv of 4. A good linear
working range from 2 to 10 mM was observed in the titration
experiment. In addition, we also measured the sensitivity of 4 for
monitoring the lower concentration of Hg2þ by changing the slit
size. When 4 was employed at 1
20 nm, the good linear working range from 0.3 to 1
(Fig. 4b). Further, when 4 was employed at 0.1 M with the same slit
size (20 nm/20 nm), the good linear working range from 0.03 to
m
M with the slit size being 20 nm/
4. Conclusions
mM is obtainable
m
In summary, we have developed a new ratiometric fluorescent
probe 4 for Hg2þ based on an intramolecular FRET with an excellent
selectivity over other metal ions. It exhibits a clear Hg2þ-induced
change in the intensity ratio of the two emission bands of naph-
thalimide and rhodamine. The selective absorption and fluores-
cence response of 4 is due to the Hg2þ-promoted desulfurization of
the thiocarbonyl moiety, leading to the ring-opening of rhodamine
B moiety of 4. We expect that the method will serve as practical tool
for environmental samples analysis and biological studies.
0.08 mM can still be obtained (Fig. 4c), suggesting a lower level of
Hg2þ can be detected using the system.
It was clear that the FRET process was switched on by Hg2þ ions
as excitation of 1,8-naphthalimide at 400 nm resulted in the
emission of rhodamine with a maximum of 585 nm. This can also
be corroborated by the excitation spectra of the ring-opened
product 5. The excitation spectra obtained by collecting emission
data of 5 at 585 nm shows both the donor and the acceptor bands
with good correspondence with the absorption spectra (Fig. 5),
indicating that both the two transitions participate in the emission
process, and an efficient energy transfer can occur from the 1,8-
naphthalimide donor to the rhodamine acceptor. The efficiency of
energy transfer (EET) was calculated to be 86.3% based on the
Acknowledgments
We would like to thank the Natural Science Foundation of China
(NSFC Nos. 20772073 and 21072121) and the Natural Science
Foundation of Shanxi Province (2008011015-2) for financial
support.
equation [52]: hEET ¼ 1 ꢁ FF(donor in FRET system)
/FF(free donor), in which
hEET is the efficiency of energy transfer, FF(donor in FRET system) is the
fluorescence quantum yields of the donor part in FRET system (1,8-
naphthalimide part in 5 in this investigation), and FF(free donor) is the
fluorescence quantum yields of the donor when not connected to
the acceptor (1,8-naphthalimide part in 4 in this investigation).
Further, to evaluate the role of the 1,8-naphthalimide donor
moiety, a control compound 6 (with the 1,8-naphthalimide group
in 4 being replaced by a phenyl group) was synthesized (Scheme 1)
and its fluorescent response performances were investigated and
compared with that of 4 in the same conditions. The free 6 dis-
played no any emission when excited at 400 nm (excitation of 1,8-
naphthalimide). Upon addition of 1 equiv Hg2þ, only a weaker
emission compared with 4 þ Hg2þ was observed at 585 nm (Fig. 6).
Obviously, the 1,8-naphthalimide donor plays an important role for
FRET of 4 þ Hg2þ. The property is especially important because
a large Stokes shift (185 nm) can be realized in this system, which
can eliminate any influence of excitation backscattering effects on
the fluorescence assay and facilitate the practical application.
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