Angewandte
Chemie
(Table 1, entries 12–15). Clearly, none of the natural bases
make stable pairs with PurP·Ni2+. Indeed, the DTm values of
the mismatched pairs relative to the PurP·Ni2+·PurP base pair
(not the D values listed in Table 1 which are relative to the
C·G pair) range from À17 to À19.58C. By contrast, T·G and
C·A mismatches of the parent natural duplex under the same
conditions show DTm values of À7.4 and À18.58C under the
same conditions.[7] Thus, all four PurP·Ni2+ mismatches with
natural bases are much less stable than the PurP·Ni2+·PurP
match. A further point to note is that the instabilities seen for
all four PurP·Ni2+ mismatches with natural bases rival the
most severe natural nucleobase mismatches such as C·A.
Within the double helix, three possible geometries could
be envisioned for divalent metal ion complexation by PurP2 :
square planar, tetrahedral, and Dd2 (a geometry intermediate
between square planar and tetrahedral). In the absence of a
geometric preference by the metal ion, the most productive
geometry for a metallo base pair in forming the double helix is
expected to be square planar because this will maximize
favorable nearest-neighbor stacking interactions. Low-energy
square-planar geometries should be accessible for Ni2+, Co2+,
Cu2+, Ag+, and Pd2+ ions. The first two of these five ions
appreciably stabilize the PurP2-bearing helix, whereas the
latter three do not. As a result, it may be concluded that
geometry alone is an insufficient predictor of metal-ion
affinity for PurP. A circular dichroism spectrum of duplex 4/5
in the presence of Ni2+ is consistent with a B-DNA structure.
To assess the viability of a square-planar geometry for
PurP·Ni2+·PurP, an ab initio geometry optimization was per-
formed on the complex by using Gaussian98[8] at the B3LYP/
6-31G*(CHN)/SDD(Ni) level of theory. Figure 3 (left panel)
shows the square-planar geometry found to be a (local)
minimum on the energy surface. Interestingly, this structure
bears an N9–N9’ (purine numbering) PurP–PurP, distance of
9.54 ꢀ, which nearly replicates the N9–N1 purine–pyrimidine
distance of 9.05 ꢀ that occurs in natural B-DNA helices for
both G·C and A·T base pairs. This suggests PurP·Ni2+·PurP is a
good dimensional mimic of natural base pairs despite the fact
that the metallo base pair incorporates two purine-like
bases towards the major groove, with a corresponding short-
ening of the distance between interstrand N9 atoms.
The PurP·Ni2+·PurP structure in Figure 3 results from
head-to-head dimerization (N1,N1’-PurP·Ni2+·N1,N1’-PurP).
An alternative head-to-tail dimerization mode of PurP
(N1,N1’-PurP·Ni2+·N7,N1’-PurP) was also investigated compu-
tationally. The geometry of this latter complex was found to
be highly nonplanar due to ligand encroachment resulting
from the 1,5-relationship of the nitrogen atoms (N7,N1’)
presented by the “tail”-oriented PurP. (In contrast, the
opposing “head”-oriented PurP bears the optimal 1,4-rela-
tionship of nitrogen atoms, as found in bipyridine.) Therefore,
the head-to-tail dimer is predicted to be less compatible with a
helix than the head-to-head dimer.
Metallo base pairs could become functional elements of
oligonucleotides that activate or suppress enzymatic activity
(for example, transcription or translation) in the presence or
absence of a metal ion. For a proof of principle, we have
incorporated three consecutive PurP residues into a helix to
attain “on” and “off” states (in the presence and absence of
Ni2+, respectively) that are sufficiently insulated from one
another to be effectively binary (0 or 1). The following
tetradecamer DNA strands were prepared: 5’-d-
CTTTCTPurpPurpPurpTCCCT (12) and 5’-d-AGGGAPurp-
PurpPurPAGAAAG (13). Gratifyingly, the Tm values for the
12/13 duplex under the conditions reported in Table 1 were
64.38C in the presence of 10.0 mm NiC12 (1.3 equiv per Purp
residue) and 20.68C in the absence of Ni2+. Thus, the Tm
values between the “on” (Ni2+ present) and “off” (Ni2+
absent) states of this system are separated by 43.78C, a
difference sufficient to produce binary behavior at 378C (that
is, at this temperature, in the presence of Ni2+ the helix is
present and in the absence of Ni2+ the helix is absent).
In summary, PurP leads to a metallo base pair with Ni2+
selectivity that is more stable than natural G·C and A·T base
pairs. Additionally, PurP·Ni2+·PurP is orthogonal in its pairing
properties relative to the four genomic nucleobases: all
mismatches are highly destabilizing to the helix in comparison
to the parent metallo base pair. Finally, PurP·Ni2+·PurP
appears to resemble natural base pairs dimensionally and
has the potential to serve as the functional component of an
ion-activated switch. Given the resemblance between natural
purines and PurP it is possible that enzymes, including those
components.
Superposition
of
ab initio
optimized
PurP·Ni2+·PurP and A·T base-pair structures (Figure 3, right
panel) further supports this idea and shows that PurP
coordination of Ni2+ is attended by rotation of the PurP
Figure 3. Left: Stereoview of the structure of PurP·Ni2+·PurP with optimized geometry obtained with Gaussian98.[8] Right: Superposition of opti-
mized PurP·Ni2+·PurP and A·T structures. The superposition was guided by PurP N9/A N9, PurP N9/T N1, and the hydrogen atoms attached to
these nitrogen atoms.
Angew. Chem. Int. Ed. 2005, 44, 1529 –1532
ꢀ 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
1531