Nanoswitches based on DNA base pairs: why adenine-thymine is less suitable than guanine-cytosine.

Substituted Watson–Crick guanine–cytosine (GC) base pairs were recently shown to yield robust three‐state nanoswitches. Here, we address the question: Can such supramolecular switches also be based on Watson–Crick adenine‐thymine (AT) base pairs? We have theoretically analyzed AT pairs in which purine‐C8 and/or pyrimidine‐C6 positions carry a substituent X=NH^?, NH₂, NH₃⁺ (N series), O^?, OH or OH₂⁺ (O series), using the generalized gradient approximation (GGA) of density functional theory at the BP86/TZ2P level. Thus, we explore the trend in geometrical shape and hydrogen bond strengths in AT pairs along a series of stepwise protonations of the substituents. Introducing a charge on the substituents leads to substantial and characteristic changes in the individual hydrogen bond lengths when compared to the neutral AT pair. However, the trends along the series of negative, neutral, and positive substituents are less systematic and less pronounced than for GC. In certain instances, internal proton transfer from thymine to adenine occurs. Our results suggest that AT is a less suitable candidate than GC in the quest for chemically controlled nanoswitches.     

A Pyrimidopyrimidine Janus‐AT Nucleoside with Improved Base‐Pairing Properties to both A and T within a DNA Duplex: The Stabilizing Effect of a Second Endocyclic Ring Nitrogen

Janus bases are heterocyclic nucleic acid base analogs that present two different faces able to simultaneously hydrogen bond to nucleosides that form Watson–Crick base pairs. The synthesis of a Janus‐AT nucleotide analogue, ^N J_AT , that has an additional endocyclic ring nitrogen and is thus more capable of efficiently discriminating T/A over G/C bases when base‐pairing in a standard duplex‐DNA context is described. Conversion to a phosphoramidite ultimately afforded incorporation into an oligonucleotide. In contrast to the first generation of carbocyclic Janus heterocycles, it remains in its unprotonated state at physiological pH and, therefore, forms very stable Watson–Crick base pairs with either A or T bases. Biophysical and computational methods indicate that ^N J_AT is an improved candidate for sequence‐specific genome targeting.     

Quantum chemical study of the hydrogen‐bonded patterns in A · T base pair of DNA: Origins of tautomeric mispairs,base flipping,and Watson–Crick ⇒ Hoogsteen conversion

The current work aims to thoroughly investigate a variety of facets of the hydrogen‐bond pattern of the Watson–Crick A · T base pair of DNA. It offers a novel mechanism of the origin of the hydrogen‐bonded mispairing in the A · T base pair based on the analysis of the lower‐energy portion of the total potential energy surface of all possible rearrangements of the hydrogen‐bond patterns in this pair, performed at the Hartree–Fock (HF), second‐order Moller–Plesset (MP2)//HF, and B3LYP computational levels in conjunction with 6‐31+G(d) basis set. The specific novelty of this mechanism is that the primary step consists of a single proton transfer along the N₃(T)–H … N₁ (A) hydrogen bond, thus leading to a transition state that is not directly related to the proton transfer. Rather, it governs the interbase shift within the A · T pair switching the hydrogen‐bonded pattern and then separating the normal A · T pair from the mispairing valley on its potential energy surface. The latter comprises three mismatched base pairs, easily converted to each other because of lower barriers (≈1 kcal/mol) of the corresponding proton transfers. It is demonstrated that, in terms of the Gibbs free energy taken at room T = 298.15 K, the most stable mispair in such valley is predicted to be less stable by 9.7 ± 2 kcal/mol than the Watson–Crick pair, thus implying that the spontaneous point mutations of this type occur as infrequently as to be characterized by an equilibrium constant of 10^?6 to 10^?9. This estimate falls into the well‐known experimental range of mutation frequency per base pair. The structure of a so‐called “base flipping” of the A · T base pair, originated from a breaking of its N₃(T)‐H … N₁ (A) hydrogen bond, is also found and reported in the current work for the first time. The transition state A · T ${}_{\text{ts}}^{\text{WC?H}}$ , which governs the conversion of the Watson–Crick pair of adenine · thymine into the Hoogsteen one and is related to a breaking of the N₆(A)–H … O₄(T), is also obtained and its energetical and geometrical features are discussed. © 2003 Wiley Periodicals, Inc. Int J Quantum Chem, 2003     

Pyrrolo‐dC Metal‐Mediated Base Pairs in the Reverse Watson–Crick Double Helix: Enhanced Stability of Parallel DNA and Impact of 6‐Pyridinyl Residues on Fluorescence and Silver‐Ion Binding

Reverse Watson–Crick DNA with parallel‐strand orientation (ps DNA) has been constructed. Pyrrolo‐dC (PyrdC) nucleosides with phenyl and pyridinyl residues linked to the 6 position of the pyrrolo[2,3‐d]pyrimidine base have been incorporated in 12‐ and 25‐mer oligonucleotide duplexes and utilized as silver‐ion binding sites. Thermal‐stability studies on the parallel DNA strands demonstrated extremely strong silver‐ion binding and strongly enhanced duplex stability. Stoichiometric UV and fluorescence titration experiments verified that a single ^2pyPyrdC–^2pyPyrdC pair captures two silver ions in ps DNA. A structure for the PyrdC silver‐ion base pair that aligns 7‐deazapurine bases head‐to‐tail instead of head‐to‐head, as suggested for canonical DNA, is proposed. The silver DNA double helix represents the first example of a ps DNA structure built up of bidentate and tridentate reverse Watson–Crick base pairs stabilized by a dinuclear silver‐mediated PyrdC pair.     

Comparative studies between hydrated hydrogen bonded and stacked DNA base pair

Influence of hydration on the Watson–Crick guanine–cytosine hydrogen bonded (h-bonded) base pair (GC) and stacked pair (G/C) was investigated in their first hydration shell. An electrostatic based approach has been used to identify the potential binding sites for water molecules around GC and G/C pairs. Several geometries of the complexes, GC…(H₂O)_n and G/C…(H₂O)_n (n=1–6) were investigated using HF/6-31G** and HF/6-31G++** methods. Further minimization calculations were performed at both B3P86/6-31G** and MP2/6-31G** levels to assess the role of electron correlation contribution in the hydration process. It can be concluded from the present findings that the stacked base-pair hydrate better than the corresponding h-bonded base pair, and DNA base pairs can accommodate up to 4–5 water molecules whereas stacked pair do accommodate 5–6 water molecules.     

High‐Resolution Crystal Structure of a Silver(I)–RNA Hybrid Duplex Containing Watson–Crick‐like C?Silver(I)?C Metallo‐Base Pairs

Metallo‐base pairs have been extensively studied for applications in nucleic acid‐based nanodevices and genetic code expansion. Metallo‐base pairs composed of natural nucleobases are attractive because nanodevices containing natural metallo‐base pairs can be easily prepared from commercially available sources. Previously, we have reported a crystal structure of a DNA duplex containing T Hg^II T base pairs. Herein, we have determined a high‐resolution crystal structure of the second natural metallo‐base pair between pyrimidine bases C Ag^I C formed in an RNA duplex. One Ag^I occupies the center between two cytosines and forms a C Ag^I C base pair through N3 Ag^I N3 linear coordination. The C Ag^I C base pair formation does not disturb the standard A‐form conformation of RNA. Since the C Ag^I C base pair is structurally similar to the canonical Watson–Crick base pairs, it can be a useful building block for structure‐based design and fabrication of nucleic acid‐based nanodevices.     

High‐Resolution Crystal Structure of a Silver(I)–RNA Hybrid Duplex Containing Watson–Crick‐like CSilver(I)C Metallo‐Base Pairs

Metallo‐base pairs have been extensively studied for applications in nucleic acid‐based nanodevices and genetic code expansion. Metallo‐base pairs composed of natural nucleobases are attractive because nanodevices containing natural metallo‐base pairs can be easily prepared from commercially available sources. Previously, we have reported a crystal structure of a DNA duplex containing T? Hg^II? T base pairs. Herein, we have determined a high‐resolution crystal structure of the second natural metallo‐base pair between pyrimidine bases C? Ag^I? C formed in an RNA duplex. One Ag^I occupies the center between two cytosines and forms a C? Ag^I? C base pair through N3? Ag^I? N3 linear coordination. The C? Ag^I? C base pair formation does not disturb the standard A‐form conformation of RNA. Since the C? Ag^I? C base pair is structurally similar to the canonical Watson–Crick base pairs, it can be a useful building block for structure‐based design and fabrication of nucleic acid‐based nanodevices.     

A Novel DNA Helical Wire Containing HgII‐Mediated T:T and T:G Pairs

Numerous applications of metal‐mediated base pairs (metallo‐base‐pairs) to nucleic acid based nanodevices and genetic code expansion have been extensively studied. Many of these metallo‐base‐pairs are formed in DNA and RNA duplexes containing Watson–Crick base pairs. Recently, a crystal structure of a metal–DNA nanowire with an uninterrupted one‐dimensional silver array was reported. We now report the crystal structure of a novel DNA helical wire containing Hg^II‐mediated T:T and T:G base pairs and water‐mediated C:C base pairs. The Hg‐DNA wire does not contain any Watson–Crick base pairs. Crystals of the Hg‐DNA wire, which is the first DNA wire structure driven by Hg^II ions, were obtained by mixing the short oligonucleotide d(TTTGC) and Hg^II ions. This study demonstrates the potential of metallo‐DNA to form various structural components that can be used for functional nanodevices.     

Computational investigation of thermochemical properties of non-natural C-nucloebases: different hydrogen-bonding preferences for non-natural Watson–Crick base pairs

In the present density functional theory study, we have compared intrinsic properties of non-natural nucleobases (acA, acG, acC, and acT nucleobases) such as proton affinities, gas phase acidities, tautomerization, and hydrogen-bonding properties with those in normal Watson–Crick nucleobases (A, G, C, T nucleobases). The hydrogen-bonding interactions in non-natural and Watson–Crick base pairs were studied at B3LYP/6-311++G (d,p) level regarding their geometries, energies, and topological features of the electron density. The quantum theory of atoms-in-molecule (QTAIM) and natural bond orbital (NBO) analyses were employed to elucidate the interaction characteristics in base pairs. The electron density ρ(r) as well as its Laplacian $ \nabla^{2} $ ρ(r) at the hydrogen bond critical point predicted by QTAIM is strongly correlated with hydrogen bond structural parameter and the second-order perturbation energies in NBO scheme. Our results show that most of hydrogen bonds in normal Watson–Crick and non-natural base pairs must be considered as electrostatic interactions. Results of calculations revealed that energetic values of hydrogen bonds in T–A base pair are more than those in ac T–ac A base pair, while values of hydrogen bonds in C–G base pair and ac C–ac G base pair are almost the same. These results confirmed stability order of stabilization energies of these base pairs.     

Atomistic understanding of the C·T mismatched DNA base pair tautomerization via the DPT: QM and QTAIM computational approaches

It was established that the cytosine·thymine (C·T) mismatched DNA base pair with cis‐oriented N1H glycosidic bonds has propeller‐like structure (|N3C4C4N3| = 38.4°), which is stabilized by three specific intermolecular interactions–two antiparallel N4H…O4 (5.19 kcal mol^?1) and N3H…N3 (6.33 kcal mol^?1) H‐bonds and a van der Waals (vdW) contact O2…O2 (0.32 kcal mol^?1). The C·T base mispair is thermodynamically stable structure (ΔG_int = ?1.54 kcal mol^?1) and even slightly more stable than the A·T Watson–Crick DNA base pair (ΔG_int = ?1.43 kcal mol^?1) at the room temperature. It was shown that the C·T ? C*·T* tautomerization via the double proton transfer (DPT) is assisted by the O2…O2 vdW contact along the entire range of the intrinsic reaction coordinate (IRC). The positive value of the Grunenberg's compliance constants (31.186, 30.265, and 22.166 Å/mdyn for the C·T, C*·T*, and TS_{C·T ? C*·T*}, respectively) proves that the O2…O2 vdW contact is a stabilizing interaction. Based on the sweeps of the H‐bond energies, it was found that the N4H…O4/O4H…N4, and N3H…N3 H‐bonds in the C·T and C*·T* base pairs are anticooperative and weaken each other, whereas the middle N3H…N3 H‐bond and the O2…O2 vdW contact are cooperative and mutually reinforce each other. It was found that the tautomerization of the C·T base mispair through the DPT is concerted and asynchronous reaction that proceeds via the TS_{C·T ? C*·T*} stabilized by the loosened N4? H? O4 covalent bridge, N3H…N3 H‐bond (9.67 kcal mol^?1) and O2…O2 vdW contact (0.41 kcal mol^?1). The nine key points, describing the evolution of the C·T ? C*·T* tautomerization via the DPT, were detected and completely investigated along the IRC. The C*·T* mispair was revealed to be the dynamically unstable structure with a lifetime 2.13·× 10^?13 s. In this case, as for the A·T Watson–Crick DNA base pair, activates the mechanism of the quantum protection of the C·T DNA base mispair from its spontaneous mutagenic tautomerization through the DPT. © 2013 Wiley Periodicals, Inc.     

Pairing of Isolated Nucleobases: Double Resonance Laser Spectroscopy of Adenine–Thymine

The vibronic spectrum of the adenine–thymine (A–T) base pair was obtained by one‐color resonant two‐photon ionization (R2PI) spectroscopy in a free jet of thermally evaporated A and T under conditions favorable for formation of small clusters. The onset of the spectrum at 35 064 cm^?1 exhibits a large red shift relative to the π–π* origin of 9H‐adenine at 36 105 cm^?1. The IR–UV spectrum was assigned to cluster structures with HNH???O?C/N???HN hydrogen bonding by comparison with the IR spectra of A and T monomers and with ab initio calculated vibrational spectra of the most stable A–T isomers. The Watson–Crick A–T base pair is not the most stable base‐pair structure at different levels of ab initio theory, and its vibrational spectrum is not in agreement with the observed experimental spectrum. Experiments with methylated A and T were performed to further support the structural assignment.     

Mismatch base pairing of the mutagen 8‐oxoguanine and its derivatives with adenine: A theoretical search for possible antimutagenic agents

Molecular geometries of 8‐oxoguanine (8OG), those of its substituted derivatives with the substitutions CH₂, CF₂, CO, CNH, O, and S in place of the N7H7 group, adenine (A), and the base pairs of 8OG and its substituted derivatives with adenine were optimized using the RHF/6‐31+G* and B3LYP/6‐31+G* methods in gas phase. All the molecules and their hydrogen‐bonded complexes were solvated in aqueous media employing the polarized continuum model (PCM) of the self‐consistent reaction field (SCRF) theory using the RHF/6‐31+G* and B3LYP/6‐31+G* methods. The optimized geometrical parameters of the 8OG‐A base pair at the RHF/6‐31+G* and B3LYP/6‐31+G* levels of theory agree satisfactorily with those of an oligonucleotide containing the base pair found from X‐ray crystallography. The pattern of hydrogen bonding in the CF₂‐ and O‐substituted 8OG‐A base pair is of Watson–Crick type and that in the unsubstituted and CH₂‐, CNH‐, and S‐substituted base pairs is of Hoogsteen type. In the CO‐substituted base pair, the hydrogen bonding pattern is of neither Watson–Crick nor Hoogsteen type. The CF₂‐substitution appears to introduce steric hindrance for stacking of DNA bases. On the basis of these results, it appears that among all the substituted 8OG molecules considered here, the O‐substituted derivative may be useful as an antimutagenic drug. It is, however, subject to experimental verification. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2005     

A Highly Stabilizing Silver(I)‐Mediated Base Pair in Parallel‐Stranded DNA

The first parallel‐stranded DNA duplex with Hoogsteen base pairing that readily incorporates an Ag⁺ ion into an internal mispair to form a metal‐mediated base pair has been created. Towards this end, the highly stabilizing 6 FP ‐Ag⁺‐ 6 FP base pair comprising the artificial nucleobase 6‐furylpurine ( 6 FP ) was devised. A combination of temperature‐dependent UV spectroscopy, CD spectroscopy, and DFT calculations was used to confirm the formation of this base pair. The nucleobase 6 FP is capable of forming metal‐mediated base pairs both by the Watson–Crick edge (i.e. in regular antiparallel‐stranded DNA) and by the Hoogsteen edge (i.e. in parallel‐stranded DNA), depending on the oligonucleotide sequence and the experimental conditions. The 6 FP ‐Ag⁺‐ 6 FP base pair within parallel‐stranded DNA is the most strongly stabilizing Ag⁺‐mediated base pair reported to date for any type of nucleic acid, with an increase in melting temperature of almost 15 °C upon the binding of one Ag⁺ ion.     

Analysis of stacking overlap in nucleic acid structures: algorithm and application

RNA contains different secondary structural motifs like pseudo-helices, hairpin loops, internal loops, etc. in addition to anti-parallel double helices and random coils. The secondary structures are mainly stabilized by base-pairing and stacking interactions between the planar aromatic bases. The hydrogen bonding strength and geometries of base pairs are characterized by six intra-base pair parameters. Similarly, stacking can be represented by six local doublet parameters. These dinucleotide step parameters can describe the quality of stacking between Watson–Crick base pairs very effectively. However, it is quite difficult to understand the stacking pattern for dinucleotides consisting of non canonical base pairs from these parameters. Stacking interaction is a manifestation of the interaction between two aromatic bases or base pairs and thus can be estimated best by the overlap area between the planar aromatic moieties. We have calculated base pair overlap between two consecutive base pairs as the buried van der Waals surface between them. In general, overlap values show normal distribution for the Watson–Crick base pairs in most double helices within a range from 45 to 50 Å² irrespective of base sequence. The dinucleotide steps with non-canonical base pairs also are seen to have high overlap value, although their twist and few other parameters are rather unusual. We have analyzed hairpin loops of different length, bulges within double helical structures and pseudo-continuous helices using our algorithm. The overlap area analyses indicate good stacking between few looped out bases especially in GNRA tetraloop, which was difficult to quantitatively characterise from analysis of the base pair or dinucleotide step parameters. This parameter is also seen to be capable to distinguish pseudo-continuous helices from kinked helix junctions.     

Watson–Crick versus imidazopyridopyrimidine base pairs: theoretical study on differences in stability and hydrogen bonding strength

Matsuda and coworkers demonstrated that imidazopyridopyrimidine nucelobases (N ^N , O ^O , N ^O , tO ^O , and O ^N ) can mimic Watson–Crick nucleobase in forming H-bonds in DNA double helix. In the present study, we address the question about the strengths of the H-bonds in imidazopyridopyrimidine base pairs compared to those in Watson–Crick ones by focusing particularly on the nature of these interactions. Optimized structures of imidazopyridopyrimidine, imidazopyridopyrimidine–Watson–Crick, and Watson–Crick base pairs are obtained at the DFTB3LYP/6-311++G (d,p). The nature and strength of the intramolecular H-bonds in these base pairs have been investigated based on natural bond orbital (NBO method) to consider the effect of charge transfer, “atoms-in-molecules” (AIM) topological parameters, and decomposition of the interaction energies using the energy decomposition analysis (EDA). These investigations imply that N ^N –O ^O and N ^O –O ^N can form base pairs with four H-bonds (most stable than those of Watson–Crick base pairs) when they incorporated into DNA double helix. Furthermore, it can be deduced that O ^N and N ^N nucleobases form energetically more favorable pairs with adenine and guanine than the normal Watson–Crick counter parts. These results can be helpful for the stabilization and regulation of a variety of new base-pairing motif of DNA structures.     

Replication Experiments with Nucleotide Base Analogues

The principles governing the replication fidelity of genomes are not fully understood yet. Watson and Crick's base-pairing principle for matched deoxyribonucleotide (DNA) bases can explain why the guanine–cytosine and adenine-thymine base pairs are approximately one hundred times more stable thermodynamically than mismatched combinations. In vitro, DNA polymerases reduce the number of mismatched base pairs to about 10^?6 per Watson–Crick base pair. Replication fidelity can further be enhanced to a mutation probability of 10^?10or less in vivo if optimal conditions for DNA synthesis are provided by polymerase–assisting proteins and DNA-repairing enzymes. The precise reasons for the formation of mismatched base pairs (mispairs), which are responsible for a substantial part of DNA mutations, are still in debate. Although it is agreed that a template-directed “reading” of the hydrogen-substitution pattern in the heterocyclic bases is crucial for proper base pairing during DNA synthesis, it is not clear which type of “misreading” leads to mispairs. Misreading may be due to a non-Watson–Crick base pairing as well as to a change in the hydrogen-substitution pattern, leading to Watson-Crick-like mispairs. The surprising discovery of the selective and quantitative DNA-polymerase-catalyzed formation of a pyridine-pyrimidine base pair (involving a nucleotide base analogue) indicated that rare tautomeric forms in template DNA strands can lead to Watson-Crick-like mispairings that are hardly recognized by the polymerase's proofreading activity. This reveals new pathways for substitution mutations (replication-dependent DNA point mutations) and suggests a new type of mutagen in vivo.     

Contiguous metal-mediated base pairs comprising two Ag(I) ions

The incorporation of transition‐metal ions into nucleic acids by using metal‐mediated base pairs has proved to be a promising strategy for the site‐specific functionalization of these biomolecules. We report herein the formation of Ag⁺‐mediated Hoogsteen‐type base pairs comprising 1,3‐dideaza‐2′‐deoxyadenosine and thymidine. By defunctionalizing the Watson–Crick edge of adenine, the formation of regular base pairs is prohibited. The additional substitution of the N3 nitrogen atom of adenine by a methine moiety increases the basicity of the exocyclic amino group. Hence, 1,3‐dideazaadenine and thymine are able to incorporate two Ag⁺ ions into their Hoogsteen‐type base pair (as compared with one Ag⁺ ion in base pairs with 1‐deazaadenine and thymine). We show by using a combination of experimental techniques (UV and circular dichroism (CD) spectroscopies, dynamic light scattering, and mass spectrometry) that this type of base pair is compatible with different sequence contexts and can be used contiguously in DNA double helices. The most stable duplexes were observed when using a sequence containing alternating purine and pyrimidine nucleosides. Dispersion‐corrected density functional theory calculations have been performed to provide insight into the structure, formation and stabilization of the twofold metalated base pair. They revealed that the metal ions within a base pair are separated by an Ag???Ag distance of about 2.88 Å. The Ag–Ag interaction contributes some 16 kcal mol^?1 to the overall stability of the doubly metal‐mediated base pair, with the dominant contribution to the Ag–Ag bonding resulting from a donor–acceptor interaction between silver 4d‐type and 4s orbitals. These Hoogsteen‐type base pairs enable a higher functionalization of nucleic acids with metal ions than previously reported metal‐mediated base pairs, thereby increasing the potential of DNA‐based nanotechnology.     

5-Aza-7-deazaguanine–Isoguanine and Guanine–Isoguanine Base Pairs in Watson–Crick DNA: The Impact of Purine Tracts,Clickable Dendritic Side Chains,and Pyrene Adducts

The Watson–Crick coding system depends on the molecular recognition of complementary purine and pyrimidine bases. Now, the construction of hybrid DNAs with Watson–Crick and purine–purine base pairs decorated with dendritic side chains was performed. Oligonucleotides with single and multiple incorporations of 5-aza-7-deaza-2′-deoxyguanosine, its tripropargylamine derivative, and 2′-deoxyisoguanosine were synthesized. Duplex stability decreased if single modified purine–purine base pairs were inserted, but increased if pyrene residues were introduced by click chemistry. A growing number of consecutive 5-aza-7-deazaguanine–isoguanine base pairs led to strong stepwise duplex stabilization, a phenomenon not observed for the guanine–isoguanine base pair. Spacious residues are well accommodated in the large groove of purine–purine DNA tracts. Changes to the global helical structure monitored by circular dichroism spectroscopy show the impact of functionalization to the global double-helix structure. This study explores new areas of molecular recognition realized by purine base pairs that are complementary in hydrogen bonding, but not in size, relative to canonical pairs.     

Ultraviolet Absorption Induces Hydrogen‐Atom Transfer in G⋅C Watson–Crick DNA Base Pairs in Solution

Ultrafast deactivation pathways bestow photostability on nucleobases and hence preserve the structural integrity of DNA following absorption of ultraviolet (UV) radiation. One controversial recovery mechanism proposed to account for this photostability involves electron‐driven proton transfer (EDPT) in Watson–Crick base pairs. The first direct observation is reported of the EDPT process after UV excitation of individual guanine–cytosine (G?C) Watson–Crick base pairs by ultrafast time‐resolved UV/visible and mid‐infrared spectroscopy. The formation of an intermediate biradical species (G[?H]?C[+H]) with a lifetime of 2.9 ps was tracked. The majority of these biradicals return to the original G?C Watson–Crick pairs, but up to 10 % of the initially excited molecules instead form a stable photoproduct G*?C* that has undergone double hydrogen‐atom transfer. The observation of these sequential EDPT mechanisms across intermolecular hydrogen bonds confirms an important and long debated pathway for the deactivation of photoexcited base pairs, with possible implications for the UV photochemistry of DNA.     

Highly Stable Double‐Stranded DNA Containing Sequential Silver(I)‐Mediated 7‐Deazaadenine/Thymine Watson–Crick Base Pairs

The oligonucleotide d(TX)₉, which consists of an octadecamer sequence with alternating non‐canonical 7‐deazaadenine (X) and canonical thymine (T) as the nucleobases, was synthesized and shown to hybridize into double‐stranded DNA through the formation of hydrogen‐bonded Watson–Crick base pairs. dsDNA with metal‐mediated base pairs was then obtained by selectively replacing W‐C hydrogen bonds by coordination bonds to central silver(I) ions. The oligonucleotide I adopts a duplex structure in the absence of Ag⁺ ions, and its stability is significantly enhanced in the presence of Ag⁺ ions while its double‐helix structure is retained. Temperature‐dependent UV spectroscopy, circular dichroism spectroscopy, and ESI mass spectrometry were used to confirm the selective formation of the silver(I)‐mediated base pairs. This strategy could become useful for preparing stable metallo‐DNA‐based nanostructures.