C O MMU N I C A T I O N S
Figure 2. (a) TR emission intensity for PFP/ss-DNA-TR and (b) PFPB/
ss-DNA-TR in water (λexc ) 380 nm, [ss-DNA-TR] ) 2.0 × 10-8 M, TR
intensity is corrected to reflect the difference in optical density for the two
polymers).
Figure 3. Normalized fluorescence in water of (a) PFPB/PNA-Cy5, (b)
PFPB/DNAn+PNA-Cy5, and (c) PFPB/DNAc/PNA-Cy5 ([PNA-Cy5] )
2.0 × 10-8 M, [RU] ) 1.6 × 10-7 M, (λexc ) 380 nm).
TGG GTG CT), [ss-DNA] varies from 0 M to 2.7 × 10-8 M). The
isosbestic point at 492 nm highlights the transition from blue to
green emission with increasing [ssDNA].
polymer segments and encourages energy migration to low-energy
emissive sites (BT in the case of PFPB). With the aid of PNA-C*
probe strands, one obtains three different colors, depending on the
solution content: (1) blue, in the absence of DNA, (2) green, when
noncomplementary ssDNA is present, (3) and red, when the
complementary ssDNA is found. Fine-tuning of these electrostatic
and optical events could lead to multicolor biosensor schemes that
take advantage of the fluorescence amplification characteristic of
conjugated polymers.
Acknowledgment. We are grateful to the NIH (GM62958-01)
and the NSF (DMR-0097611) for financial support.
Supporting Information Available: Details for the synthesis of
PFPB and FRET experiments (PDF). This material is available free
Figure 1B shows the emission spectra of PFP, and the absorption
and emission of ss-DNA-TR (TR ) Texas Red dye and ssDNA-
TR ) 5′-TR-ATC TTG ACT ATG TGG GTG CT). Note that the
spectral overlap between the absorption of TR and the green
emission band of PFPB/ss-DNA is substantially larger than that
with the PFP emission. Therefore, we anticipated a larger value
for the overlap integral in the Fo¨rster equation and more efficient
fluorescence resonance energy transfer (FRET) with PFPB.19
Indeed, as shown in Figure 2, the TR emission intensity as a
function of polymer concentration, is greater when PFPB is excited,
relative to PFB (the value of Φ for TR is the same in the two
solutions). The spectra in Figure 2 were measured by excitation at
380 nm, which selectively creates polymer-based excited states.
On the basis of the mechanistic information above, we postulated
that PFPB could be used in a three-color DNA assay by using a
PNA-C* strand.6 PNA serves to provide a base sequence that
searches complementary ssDNA. However, because PNA is neutral,
it is possible to use water without buffer or other ions that are
required to screen the negatively charged phosphate backbone
during duplex formation.20 Since PNA-TR is not available com-
mercially, we used PNA-Cy5 (5′-Cy5-CAGTCCAGTGATACG)
as the PNA-probe instead. The absorption and emission of Cy5
(λabs ) 648 nm, λem ) 681 nm) are similar to those of TR
(Supporting Information). Hybridization of PNA-Cy5 with a
complementary ss-DNA (ss-DNAc ) 5′-CGTATCACTGGACTG)
endows the ss-DNAc/PNA-Cy5 duplex with multiple negative
charges. Complexation of ss-DNAc/PNA-Cy5 by electrostatic forces
to the positively charged PFPB allows for energy transfer from
the polymer to Cy5 and should lead to red emission. In the case of
a noncomplementary ss-DNA (ss-DNAn ) 5′-ACTGACGATA-
GACTG), electrostatic complexation occurs only between PFPB
and the ss-DNAn, which should give rise to emission from the BT
units.
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Figure 3 shows the different emission colors that are observed
in this detection scheme. In water (pH ) 7.0), a solution of PFPB
([RU] ) 1.6 × 10-7 M) and PNA-Cy5 emits blue. For the
noncomplementary situation ss-DNAn+PNA-Cy5 (annealing pro-
tocols are done independently), green emission is predominant.
Under similar conditions, when ss-DNAc/PNA-Cy5 is used, only
red emission from the Cy5 units takes place. These data indicate
that FRET from PFPB to the Cy5 signaling chromophore is
essentially complete.
In summary, we report design guidelines for water-soluble
conjugated polymer structures that change emission color as a result
of conformational and aggregation changes. Complexation with
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