X. Xu et al. / Bioorg. Med. Chem. Lett. 24 (2014) 1654–1656
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(a)
800
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0
425
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475
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575
0
200 400 600 800 1000 1200 1400 1600
Time / s
wavelength (nm)
Figure 1. Real-time emission intensity changes of FcPy (100 lM) at 505 nm upon
single-strand DNA (1 lM, 75 nt). kex = 396 nm.
900
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0
(b)
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(a)
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0
=
−
+
+
0
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g/ml)
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2500
RNA (
µ
Figure 3. (a) Changes in the emission spectrum of FcPy (5 lM) upon the different
450
500
550
600
650
concentrations (0–2.5 mg) of RNA in PBS. kex = 396 nm, kem = 420–575 nm. (b) Plot
of I/I0 À 1 at 470 nm versus the RNA concentration. I0 = emission intensity in the
absence of RNA.
wavelength (nm)
(b)
6
The results indicated that FcPy had almost no selectivity between
single and double strand DNA as the intensity of double strand
DNA was almost double of single strand DNA when interacted with
FcPy. Next, we used S1 nuclease to digest the DNA sequence and
recorded the fluorescence emission. From Figure S4 we can see that
the fluorescence intensity was nearly the same as control after
digesting with S1 nuclease. This is because that when the DNA
sequence is digested into nucleotides, the aggregated fluorescent
probes adhered to DNA sequence is also dispersed into the aqueous
solution. This also proved that FcPy has the property of AIE effect.
In order to study the kinetics of FcPy and nucleic acid interac-
tion, we recorded the real-time emission intensity of FcPy
5
4
3
2
1
=
−
+
+
0
0
5
10
15
20
25
30
ctDNA (µg/mL)
(100 lM) at 505 nm upon single-strand DNA (1 lM, 75 nt) with
excitation at 396 nm. The fluorescence intensity went to plateau
Figure 2. (a) Changes in the emission spectrum of FcPy (5
lM) upon the different
concentrations (0–30 g) of ctDNA in PBS. kex = 396 nm, kem = 420–600 nm. (b) Plot
l
at about 20 min (Fig. 1).
of I/I0 À 1 at 475 nm versus the ctDNA concentration. I0 = emission intensity in the
According to the results mentioned above, we tried to detect
natural DNA and RNA with FcPy. We chose ctDNA and RNA from
torula yeast as the target nucleic acid since they are cheap and easy
to obtain. FcPy was dissolved in phosphate-buffered saline (PBS)
solution (10 mM, pH 7.4), and the concentration of FcPy was
10 mM. The fluorescence intensity recorded at 475 nm is enhanced
quickly when the concentration of ctDNA is low, but it is gradually
saturated when the concentration of ctDNA becomes higher
(Fig. 2a). There is a gradual blueshift of the emission maximum
from 505 to 475 nm, this was elucidated by Park and coworkers.22
absence of ctDNA.
Firstly, we investigated the interaction of FcPy with nucleic acid
and single strand DNA sequences were chosen as the model. We
found that the fluorescence emission was brighter with increasing
length of the DNA sequences (Fig. S1). This was consistent with AIE
effect. As FcPy can be cations in aqueous media and DNA se-
quences have negative charges, the longer sequences have more
negative charges to be adhered with more FcPy.
Then we attempted to explore whether FcPy has an ability of
selectivity in the detection of double strand DNA and single strand
DNA. We tested the fluorescence emission of a single strand DNA
and its double strand DNA (Fig. S2) after interaction with FcPy.
This is because that there two forms of
in different situations. The change of (I/I0 À 1) versus ctDNA con-
centration (0–30 g/mL) was fitted well to the Boltzmann function
with an R2 value of 0.9738 as shown in Figure 2b. As the same as
p–p overlap of the molecule
l