Communications
Table 2: Fluorescence properties of binaphthyl-modified oligonucleoti-
des.[a]
[b]
[b]
Single strands
I/IB
Double strands
I/IB
binaphthyl
1Bn
2Bn
3Bn
4Bn
1
–
–
0.055
0.531
0.091
0.474
0.078
0.664
1.350
0.052
0.365
-
1Bn·1’A
2Bn·2’A
3Bn·3’A
4Bn·4’A
5Bn·5’
5Bn·5’Bn
5Bn·5’Bn2
5Bn2·5’Bn
5Bn2·5’Bn2
5Bn3·5’Bn2
0.099
0.217
0.050
0.075
0.160
0.327
0.744
1.092
2.419
3.227
5Bn
5Bn2
5Bn3
5’Bn
5’Bn2
–
[a] c=1 mm in 10 mm NaH2PO4, 0.1m NaCl, pH 7.0, 208C. [b] Relative
fluorescence based on the fluorescence intensity of 1,1’-binaphthyl at
l(emission)=380 nm and l(excition)=305 nm.
Figure 3. The influence of additional nucleotides X and Y on the
stabilities of duplexes 5Xn·5’Ym (X=Bn, T, or A; Y=Bn, T, or A; n=0–
3; m=0–2). Data obtained for biphenyl-modified duplexes (dashed
line)[9] is added for comparison.
of fluorescence upon multiple introduction of planar fluo-
rophores such as pyrene and perylenes.[3h,14] We speculate that
the first binaphthyl base serves as an insulator that protects
the second and third binaphthyl fluorophore from quenching
interactions with the pyrimidines.[15] This implies that the
binaphthyl chromophore experiences only little self-quench-
ing in this system.[16] Indeed, the experiments that involved
two or more interacting binaphthyl units revealed enhance-
ments of binaphthyl fluorescence upon hybridization
(Table 2, see also Figure S8B in the Supporting Information).
Duplexes 5Bnn·5’Bnm fluoresced with 50–150% higher inten-
sity than expected based on the sum of the fluorescence of the
corresponding single strands.
The purpose of this investigation was to explore torsion-
ally flexible, nonplanar base surrogates in DNA. At first
glance, the observed stabilization of a DNA duplex upon
successive introduction of multiple binaphthyl units may seem
surprising. However, the ground-state potential energy curve
of 1,1’-binaphthyl is flat in the region corresponding to a
dihedral angle between 608 and 1208.[10b] Thus, the binaphthyl
system may be well suited to adjust the two, flexibly linked
aromatic units for stacking interactions which may involve
both intrahelical and extrahelical partners. Of note, these
interactions do not lead to the self-quenching of fluorescence
as is frequently observed when planar aromatic base surro-
gates such as pyrenes are in contact.[3h,14] This behavior may
be of interest for the design of oligonucleotide assemblies
with light-harvesting properties.[17]
At present it remains unclear whether the DNA helix
induces axial chirality of binaphthyl stacks. Preliminary
modeling studies (Figure S5 in the Supporting Information)
suggest that both the R and the S forms can be accommo-
dated. Circular dichroism studies may be a useful means to
probe the chirality of the binaphthyl systems. However, this
would require modifications of the binaphthyl fluorophore in
order to avoid overlap with the absorption of the nucleobases.
The introduction of stable axial chirality through the incor-
poration of substituents in the 2- and 2’-positions would also
provide interesting opportunities. The resulting three-dimen-
sional chiral nucleobases could be useful tools in the
fluorescence-based diagnosis of the handedness of nucleic
perturbation of nucleobase–nucleobase stacking.[8a] By con-
trast, it is difficult to imagine planarization of the binaphthyl
residue investigated in this study. It is, thus, unlikely that the
distal naphthyl rings in 5Bn·5’Bn are in face-to-face contact.
This explains why the binaphthyl–binaphthyl pair destabilized
the duplex more efficiently (DTM = À5.28C) than a biphenyl–
biphenyl pair (DTM = À2.58C).[9] However, additional
binaphthyl units may result in intrastrand interactions
between the distal naphthyl rings within the major groove
(Figure 2B; Figure S5B in the Supporting Information).[13,3j]
These interactions involve larger surfaces than the stacked
phenyl rings in biphenyl base pairs, which may explain why
the TM increase upon introduction of one additional
binaphthyl pair (DTM = 7.88C) is higher than that upon
introduction of one additional biphenyl pair (DTM =
4.48C).[9] It is also feasible that the distal naphthyl units of
two binaphthyl bases interact in an edge-to-face fashion
(Figure S5C in the Supporting Information). Regardless of
the exact mechanism involved, we assume that the torsional
flexibility of the binaphthyl hinge facilitates stacking inter-
actions which can occur at both the interior and the exterior
of the DNA duplex.
The fluorescence properties also support the notion of
binaphthyl–binaphthyl interactions in DNA. The oligonu-
cleotides were excited at a wavelength of 305 nm. The
fluorescence properties were characterized by means of the
relative fluorescence I/IB (I, IB: fluorescence emission of
binaphthyl-modified oligonucleotides and free 1,1’-
binaphthyl, respectively). The investigation of oligonucleo-
tides 1Bn–4Bn revealed thymine and cytosine to be efficient
quenchers of binaphthyl fluorescence (90–95% quenching,
Table 2; see also Figure S8A in the Supporting Information).
By comparison guanine and adenine were inefficient (ca.
50%) quenchers. Interestingly, the incorporation of a second
or a third fluorophore in 5Bn2, 5Bn3, or 5’Bn2 led to a strong
enhancement of the fluorescence. For example, the oligonu-
cleotide 5Bn3 (I/IB = 1.350) was found to fluoresce with a 17-
fold higher intensity than oligonucleotide 5Bn (I/IB = 0.078).
This behavior is in contrast to the recently observed decreases
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Angew. Chem. Int. Ed. 2009, 48, 8250 –8253