multifluorophores with energy donorꢀacceptor architec-
tures can achieve large pseudo-Stokes shifts, meanwhile
affording simultaneous recorded ratio signals of two emis-
sion intensities at different wavelengths, which could pro-
vide a built-in correction for the environmental effects.
process could change the emission maximum of the
system from 535 nm (the characteristic peak of naphth-
alimide) to 577 nm (the characteristic peak of rhodamine).
This wavelength shift allows highly selective ratiometric
detection of Cu2þ both in acetonitrile/water solution and
in living cells.
To explore the mechanism, an RN1-Cu2þ complex was
detected by TOF mass spectrum analysis (Figure S14). A
peak at m/z 725.2745 corresponding to intermediate 6 was
observed after the addition of Cu2þ to RN1 aqueous
solution, which suggested that Cu2þ induces the hydrolysis
and opening of the spirolactam ring of the rhodamine
moiety.
RN1 was synthesized on the basis of the route shown in
Scheme 1. Compounds 4 and 3 were successfully linked
together by a Sonogashira reaction between terminal
alkynyl and bromine in the presence of PdCl2(PPh3)2,
PPh3, and CuI as the catalyst to afford 6 in 75% yield.
Finally, RN1 was obtained by refluxing 6 and hydrazine
hydrate for 6 h in ethanol with a yield of 74%. All the
new intermediates and RN1 were well characterized by
1H NMR, 13C NMR, and TOF-MS (Figures S9ꢀS24).
€
Forster Resonance Energy Transfer (FRET) is generally
the most adopted methodology for addressing this issue.
€
Forster Resonance Energy Transfer (FRET) is generally
the most adopted methodology for addressing this issue.
Normally, dyes based on FRET processes are usually
linked by a nonconjugated spacer, and the energy transfer
occurs through space. For FRET to be effective, a sub-
stantial spectral overlap for the donor emission and ac-
ceptor absorption bands is required, which sometimes
restrict the choice and the design of these kinds of probe
molecules. The dyesbasedon TBET(through-bondenergy
transfer) are the ones which have a donor connected to an
acceptor via electronically conjugated linkers which pre-
vent the donor and acceptor fragments from becoming
planar, and the energy transfer occurs through a bond. For
a TBET system there is no such prerequisite, thus it exhi-
bits fast energy transfer rates, large pseudo-Stokes shifts,
and flexibility in fluorophores.6 Actually, to the best of our
knowledge, there are a few fluorescent probes for Hg2þ
reported on TBET (naphthalimide appended rhodamine)7
and just only one for Cu2þ with two different approaches
which has not been applied in living cells.8 Thus, it is
important to develop ratiometric fluorescent probes for
Cu2þ with favorablechemicaland spectroscopicproperties
suitable for the imaging of Cu2þ in living cells.
As the fluorescence of the naphthalimide moiety was
often quenched probably due to the efficient photoinduced
electron transfer (PET) from the amide of rhodamine to
the naphthalimide fluorophore, the probes could not
exhibit any ratiometric fluorescence for metal ion detec-
tion. To solve this problem, herein, we report a ratiometric
fluorescent chemodosimeter RN1 for Cu2þ based on
TBET, in which (4-N,N-dimethylamino)-1,8-naphthalide
(energy donor) and rhodamine (energy acceptor) were
linked by a rigid and conjugated spacer 4-ethynylaniline
at the naphthalic anhydride position. A hydrazide func-
tional group was selected as the potential reaction site for
Figure 1. Fluorescence ratio of RN1 (5 μM) in response to the
presence of Cu2þ (0ꢀ20 equiv) in CH3CN/H2O (20:1, v/v)
buffered with Tris-HCl (pH 7.4, 10 mM). λex = 420 nm. Inset
showing the fluorescence before and after the addition of Cu2þ
.
Cu2þ 9
.
The absorption and emission properties (Figure S1) of
RN1 (5 μM) were investigated in CH3CN/Tris-HCl buffer
(v/v = 20:1, pH 7.4). In the absence of Cu2þ, RN1 showed
one absorption band at 431 nm due to the naphthalimide
moiety. On addition of Cu2þ (0ꢀ20 equiv), a new absorp-
tion band appeared at 546 nm corresponding to the
rhodamine acceptor. Such a large red shift (115 nm) in
absorption behavior changed the color of the solution
from yellow-green to pink, allowing colorimetric detection
of Cu2þ by the naked eye. Accordingly, as shown in Figure 1,
upon excitation at 420 nm, the free RN1 displays a single
emission band centered at 535 nm, attributed to the emis-
sion of the naphthalimide moiety. There is no TBET in the
free RN1, as the rhodamine acceptor is in a ring-closed
form. Addition of Cu2þ significantly decreases the fluo-
rescence intensity at around 535 nm, and simultaneously a
Fortunately, this connection efficiently prevented the
fluorescence quenching of naphthalimide. In the absence
of Cu2þ, the excited energy of the naphthalimide donor could
not be transferred to the rhodamine acceptor, as the rhoda-
mine acceptor is in the closed form. Thus, only the emission of
the dye naphthalimide is observed. A Cu2þ-induced
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Kaur, T. Org. Lett. 2011, 13, 1422. (b) Mahato, P.; Saha, S.; Suresh, E.;
Di Liddo, R.; Parnigotto, P. P.; Conconi, M. T.; Kesharwani, M. K.;
Ganguly, B.; Das, A. Inorg. Chem. 2012, 51, 1769. (c) Luxami, V.;
Verma, M.; Rani, R.; Paul, K.; Kumar, S. Org. Biomol. Chem. 2012, 10,
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Org. Lett. 2010, 12, 3852.
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