Communication
The efficiency of energy transfer (E), was calculated using
Equation (1):
F
F0
ð1Þ
E ¼ 1 À
where F and F0 are the fluorescence intensity of donor (pyrene
chromophore) in the tetraplex form (with the influence of ac-
ceptor) and in the single strand form (without the influence of
acceptor), respectively. The energy transfer efficiency (E) from
donor to acceptor was found as 66%, 55%, and 39% for ODN
1, 2, and 3, respectively. Thus, the FRET efficiency decreases
with increase in G-quartet units and ODN 3 showed the lowest
FRET efficiency among all three ODNs upon conformational
change from a single strand to an anti-parallel G-quadruplex.
The Fçrster radius (R0) for this system was calculated using
Equation (2):
Figure 3. Absorption and emission spectra of PyA and PerA chromophore.
Shaded area shows spectral overlap of FRET pair. Bold lines are extracted
from dotted lines. Blue, green, and red dotted lines denote absorption of
ssODN 1, emission of ssODN 1, and emission of GQ 1, respectively.
close proximity for energy transfer. The fluorescence spectra of
the ODNs exhibited two emission bands at around 450 and
520 nm for pyrene and perylene chromophores, respectively.
The excitation wavelength was chosen as 385 nm to measure
the fluorescence spectroscopy and thereby FRET. In the unfold-
ed single strand form, the emission band intensity at around
450 nm dominates over the emission band intensity at around
520 nm for ODN 1, 2, and 3. It is noteworthy that, in ODN 1,
the emission intensity at around 520 nm is slightly higher than
the other two ODN 2 and 3 and this may be because of little
energy transfer due to the smaller distance between donor
and acceptor (see Figures 1 and 4). Interesting fluorescence
1=6
R0 ¼ 0:2108½JðlÞk2nÀ4FD
ð2Þ
where k2 is the orientation factor, n is the refractive index of
the medium, FD is the quantum yield of the donor in the ab-
sence of acceptor J(l) is the overlap integral of the fluores-
cence emission spectrum of the donor and the absorption
spectrum of the acceptor. Using the values of k2 =2/3, n=
1.33, FD =0.51, and the obtained overlap integral, J(l)=1.03
1017, the Fçrster radius (R0) was obtained as 48.7 . Moreover,
the designed system showed that upon conformational
change from single strand to G-quadruplex structure leads to
the stacking interaction between the fluorophore and external
G-quartet. However, stacking interaction onto the external G-
quartet tends to slip, and thus the orientation of the FRET
pairs was not fully controlled during energy transfer in G-quad-
ruplex structure. Thus, the observed FRET of this designed
system might be due to both distant-dependent as well as ori-
entation-dependent phenomena.
In order to further gain insight in the FRET pair positions
and the interactions with the external G-quartet units upon
conformational change to a tetraplex/G-quadruplex structure,
MacroModel minimization was carried using AMBER* force
field.[35] Solution structure of the human telomeric G-quadru-
plex, PDB ID: 143D (5’-A GGG TTA GGG TTA GGG TTA GGG-3’)
was used for this calculation where A7 and A13 bases were re-
placed by PyA and PerA, respectively. The energy minimized
conformation of ODN 2 is shown in Figure 5. Thus, the Macro-
Model study showed that PyA placed the pyrene chromophore
parallel to the external G-quartet plane and stabilized through
hydrophobic stacking interaction with the G-quartet unit. In
contrast, due to the large size of the perylene unit, it resides
slightly outside from the G-quartet. However, PerA also placed
the perylene chromophore almost parallel to the G-quartet
plane.
Figure 4. Fluorescence emission spectra (lex =385 nm) of the donor/accept-
or tethered ODN 1, 2, and 3 in absence of KCl solution (single strand) and in
presence of KCl solution (G-quadruplex). All samples, [DNA]=1.5 mm,
[KCl]=400 mm, were prepared in 10 mm Tris- HCl buffer (pH 7.2) at 258C.
emission behavior was observed while adding KCl solution
into the ODNs. Decrease of emission intensity of the band at
450 nm and increase of emission intensity of the band at
520 nm were observed due to FRET for the ODN 1, 2, and 3
upon conformational change from a single strand to an anti-
parallel G-quadruplex. However, the decrease and increase of
emission intensities from the single strand to corresponding G-
quadruplex are not same for all the ODNs. ODN 1 contains two
G-quartet units; thus, smaller distance between FRET pair and
showed maximum decrease of emission intensity at 450 nm
and increase of emission intensity at 520 nm over ODN 2 and
3.
In conclusion, G-tetraplex-induced fluorescence resonance
energy transfer within telomeric repeat sequences was studied
using a nucleoside-tethered FRET pair embedded in the
human telomeric G-quadruplex forming sequence (5’-A GGG
TTPyA GGG TTPerA GGG TTA GGG-3’). Conformational change
from a single strand to an anti-parallel G-quadruplex upon
Chem. Asian J. 2016, 11, 198 – 201
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