Communications
transitions to the upper excitonic level. The excited state was
Control of fluorescence emission by an excitonic inter-
action was also evident when the target was RNA. Several
colored nucleotides exhibited a shift of the absorption bands
and the switching of fluorescence intensity upon hybridization
with the complementary RNA strands. However, inefficient
exciton control was observed in some nucleotides. The shift of
the absorption bands was minimal for nucleotides with
hemicyanine dyes (D539, D570, and D590). The absorption
bands occurred at relatively short wavelengths for both the
hybrid and the nonhybrid form, in contrast to the absorption
behavior of nucleotides in Figure 2. The DNA-binding ability
of hemicyanines is known to be inherently lower than that of
thiazole orange dyes.[12] The small shift in the absorption band
suggests that the dissociation of the dye aggregate is
inefficient in the hybrid with RNA, and that it is difficult
for the dyes to bind independently to the hybrid structure.
Similarly, D640 and D660, which have relatively larger con-
jugated systems, showed low efficiency of dye-aggregate
dissociation upon hybrid formation with RNA. The ratio of
the fluorescence intensity of the hybrid to that of the
nonhybrid in these nucleotides was not as high as for other
nucleotides that were controlled well by an excitonic inter-
action.
rapidly transferred to the lower level, but the path from this
energy level to the ground state was not emissive. The
fluorescence from the fluorescent ODNs was suppressed by
an interdye excitonic interaction in the nonhybridized state.
Fluorescence quenching was much more effective than for
probes labeled with one dye unit.[5,10] Hybridization with the
target nucleic acid resulted in a great enhancement of
emission with dissociation of the aggregate. This exciton-
controlled fluorescence behavior was also observed for
doubly labeled ODNs with other sequences (see Table S2 in
the Supporting Information).
However, among the twelve colored nucleotides consid-
ered, only the D410-containing ODN showed relatively strong
emission, even when the ODN was in the nonhybridized state.
In this case, the blue-shifted absorption spectrum suggested
the existence of an interdye excitonic interaction. The
excitation spectra revealed two peaks, and the absorption
bands of the aggregate and the non-aggregate overlapped.
These spectra are quite different from the excitation spectra
of the D514 probe, for which only one signal corresponding to
the non-aggregate was observed (Figure 3). Furthermore, the
excitation and emission spectra showed that excitation at a
shorter wavelength (aggregate) corresponded to emission at a
longer wavelength, while excitation at a longer wavelength
(non-aggregate) corresponded to emission at a shorter wave-
length. This result suggested that the dyes of the D410
nucleotide were inclined with respect to one another, and
that the emission from the lower excitonic state after
excitation to the upper excitonic state was not completely
forbidden.[9,11]
The appropriate design of dye aggregation in the non-
hybridized state is the key point that determines the ability of
doubly labeled ODNs to function as hybridization-sensitive
fluorescent probes. We developed a series of hybridization-
sensitive fluorescent probes that cover the excitation-wave-
length range 400–700 nm. From this series, we can select the
probe that is most suitable for the nature and number of
nucleic acids, and the filter type of the detector.
We believed that these doubly labeled ODNs
might be useful for multicolor RNA imaging. The
development of chemical methods for imaging the
dynamic and static behavior of RNA in a living cell is
essential for increasing our understanding of cell life:
a key goal of life scientists.[13] Although many
methods for RNA detection have been developed,
such as molecular beacons,[14] MS2-GFP fusion
proteins,[15] GFP reconstitution,[16] quenched autoli-
gation probes,[17] and dye-binding aptamers,[18] there
are various associated problems, including the low
availability of many color probes, limitations in
sequence design, slow response in terms of reactivity
or conformation change, high background fluores-
cence, or low fluorescence reversibility. Our new
hybridization-sensitive probes may offer solutions to
these issues and provide advantages.
We next designed a model experiment with a
series of probes for RNA imaging in a living cell. The
probes capable of binding to the polyA tail of
mRNA, 5’-d(T6DnnnT6)-3’, were transfected to HeLa
cells with the common transfection reagent Lip-
ofectamine 2000. After incubation for 1 h and wash-
ing, fluorescence emission from the cells was
observed at the wavelength expected for each Dnnn
(Figure 4a). The fluorescence from the cells
decreased upon competitive hybridization of a dT
70-mer (dT70) DNA molecule. This fluorescence
Figure 3. Excitation and emission spectra of the single-stranded D410 and D514
probes 5’-d(TACCAGDnnnCACCAT)-3’, and a model of molecule orientation and
transition dipole interactions in H aggregates. D410: excitation spectra for emis-
sion at 426 (red) and 480 nm (black), and emission spectra at 410 (red) and
360 nm (black); D514: excitation spectra for emission at 537 (red) and 600 nm
(black), and emission spectra at 516 (red) and 480 nm (black). M is the transition
dipole moment; m+ and mÀ are the excitonic states.
ꢀ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2009, 48, 6480 –6484