On the apparently anomalous distance dependence of charge-transfer rates in 9-amino-6-chloro-2-methoxyacridine-modified DNA

From previous thermal and photoinduced charge-transfer reactions in duplex DNA there is accumulative evidence for an attenuation parameter beta of the distance dependence in the range 0.6-0.8 A(-1), with the exception of one specific system exhibiting beta = 1.5 A(-1) which is reinvestigated in this paper. Femtosecond to nanosecond time-resolved pump-probe spectroscopy has been used to follow photoinduced charge-shift dynamics in DNA duplexes containing a covalently appended, protonated 9-alkylamino-6-chloro-2-methoxyacridine chromophore. This acridine derivative (X+) resides in the DNA duplex at a specific abasic site, which is highly defined as reflected in the monoexponentiality of the kinetics. In the presence of only neighboring A:T base pairs, no charge transfer occurs within the excited-state lifetime (18 ns) of the chromophore. However, the presence of a guanine nucleobase as either a nearest neighbor or with one interspersed A:T base pair does result in fluorescence quenching. In the case of nearest neighbors, the intermediate radical state X* is formed within 4 ps and decays on the 30 ps time scale. Placing one A:T base pair between the X+ and guanine slows down the forward transfer rate by 3 orders of magnitude, corresponding to an apparent beta value of >2.0 A(-1). This dramatic decrease in the rate is due to a change in charge-transfer mechanism from a (nearly) activationless to a thermally activated regime in which the forward transfer is slower than the back transfer and the X* state is no longer observed. These observations indicate that the distance dependence of charge injection in the X+-labeled DNA duplex is not solely caused by a decrease in electronic couplings but also by a concomitant increase of the activation energy with increasing distance. This increase in activation energy may result from the loss of driving force due to excited-state relaxation competing with charge transfer, or reflect distance-dependent changes in the energetics, predominantly of the low-frequency reorganization energy in this charge-shift reaction, on purely electrostatic grounds. To test the hypothesis of distance-dependent activation energy, guanine has been replaced by 7-deazaguanine, its easier-to-oxidize purine analogue. In these duplexes, a similar change of charge-transfer mechanism is found. However, consistent with an a priori larger driving force this change occurs at a larger donor-acceptor separation than in the X+-guanine systems. Independent of the detailed contributions to the distance-dependent activation energy, this phenomenon illustrates the complex nature of experimental beta values.     

Molecular dynamics studies of ion distributions for DNA duplexes and DNA clusters: salt effects and connection to DNA melting

We present extensive molecular dynamics simulations of the ion distributions for DNA duplexes and DNA clusters using the Amber force field with implicit water. The distribution of ions and the electrostatic energy of ions around an isolated DNA duplex and clusters of DNA duplexes in different salt (NaCl) concentrations over the range 0.2-1.0 mol/L are determined on the basis of the simulation results. Using the electrostatic energy profile, we determine a local net charge fraction phi, which is found to increase with increasing of salt concentration. For DNA clusters containing two DNA duplexes (DNA pair) or four DNA duplexes, phi increases as the distance between the duplexes decreases. Combining this result with experimental results for the dependence of the DNA melting temperature on bulk salt concentration, we conclude that for a pair of DNA duplexes the melting temperature increases by 5-10 K for interaxis separations of 25-40 A. For a cluster of four DNA duplexes, an even larger melting temperature increase should occur. We argue that this melting temperature increase in dense DNA clusters is responsible for the cooperative melting mechanism in DNA-linked nanoparticle aggregates and DNA-linked polymer aggregates.     

Coordination-driven inversion of handedness in ligand-modified PNA

Peptide nucleic acid (PNA) is a synthetic analogue of DNA, which has the same nucleobases as DNA but typically has a backbone based on aminoethyl glycine (Aeg). PNA forms duplexes by Watson Crick hybridization. The Aeg-based PNA duplexes adopt a chiral helical structure but do not have a preferred handedness because they do not contain a chiral center. An L-lysine situated at the C-end of one or both strands of a PNA duplex causes the duplex to preferably adopt a left-handed structure. We have introduced into the PNA duplexes both a C-terminal L-lysine and one or two PNA monomers that have a γ-(S)-methyl-aminoethyl glycine backbone, which is known to induce a preference for a right-handed structure. Indeed, we found that in these duplexes the γ-methyl monomer exerts the dominant chiral induction effect causing the duplexes to adopt a right-handed structure. The chiral PNA monomer had a 2,2':6',2'-terpyridine (Tpy) ligand instead of a nucleobase and PNA duplexes that contained one or two Tpys formed [Cu(Tpy)(2)](2+) complexes in the presence of Cu(2+). The CD spectroscopy studies showed that these metal-coordinated duplexes were right-handed due to the chiral induction effect exerted by the S-Tpy PNA monomer(s) except for the cases when the [Cu(Tpy)(2)](2+) complex was formed with Tpy ligands from two different PNA duplexes. In the latter case, the metal complex bridged the two PNA duplexes and the duplexes were left-handed. The results of this study show that the preferred handedness of a ligand-modified PNA can be switched as a consequence of metal coordination to the ligand. This finding could be used as a tool in the design of functional nucleic-acid based nanostructures.     

Oligonucleotides with 1,4-dioxane-based nucleotide monomers

An epimeric mixture of H-phosphonates 5R and 5S has been synthesized in three steps from known secouridine 1. Separation of the epimers has been accomplished by RP-HPLC, allowing full characterization and incorporation of monomers X and Y into 9-mer oligonucleotides using H-phosphonates building blocks 5R and 5S, respectively. A single incorporation of either monomer X or monomer Y in the central position of a DNA 9-mer results in decreased thermal affinity toward both DNA and RNA complements (ΔT(m) = -3.5 °C/-3.5 °C for monomer X and ΔT(m) = -11.0 °C/-6.5 °C for monomer Y). CD measurements do not reveal major rearrangements of the duplexes formed, but molecular modeling suggests that local rearrangement of the sugar phosphate backbone and decreased base interactions with neighboring bases might be the origin of the decreased stability of duplexes.     

Charge transport in DNA via thermally induced hopping.

In this contribution we advance and explore the thermally induced hopping (TIH) mechanism for long-range charge transport (CT) in DNA and in large-scale chemical systems. TIH occurs in donor-bridge-acceptor systems, which are characterized by off-resonance donor-bridge interactions (energy gap DeltaE > 0), involving thermally activated donor-bridge charge injection followed by intrabridge charge hopping. We observe a "transition" from superexchange to TIH with increasing the bridge length (i.e., the number N of the bridge constituents), which is manifested by crossing from the exponential N-dependent donor-acceptor CT rate at low N (< N(X)) to a weakly (algebraic) N-dependent CT rate at high N (>N(X)). The "critical" bridge size N(X) is determined by the energy gap, the nearest-neighbor electronic couplings, and the temperature. Experimental evidence for the TIH mechanism was inferred from our analysis of the chemical yields for the distal/proximal guanine (G) triplets in the (GGG)(+)TTXTT(GGG) duplex (X = G, azadine (zA), and adenine (A)) studied by Nakatani, Dohno and Saito [J. Am. Chem. Soc. 2000, 122, 5893]. The TIH sequential model, which involves hole hopping between (GGG) and X, is analyzed in terms of a sequential process in conjunction with parallel reactions of (GGG)(+) with water, and provides a scale of (free) energy gaps (relative to (GGG)(+)) of Delta = 0.21-0.24 eV for X = A, Delta = 0.10-0.14 eV for X = zA, and Delta = 0.05-0.10 eV for X = G. We further investigated the chemical yields for long-range TIH in (G)l(+)Xn(G)l (l = 1-3) duplexes, establishing the energetic constraints (i.e., the donor - bridge base (X) energy gap Delta), the bridge structural constraints (i.e., the intrabridge X-X hopping rates k(m)), and the kinetic constraints (i.e., the rate k(d) for the reaction of with water). Effective TIH is expected to prevail for Delta less than or approximately equal to 0.20 eV with a "fast" water reaction (k(d)/k(m) approximately 10(-3)) and for Delta < 0.30 eV with a "slow" water reaction (k(d)/k(m) approximately 10(-5)). We conclude that (T)n bridges (for which Delta approximately equals 0.6 eV) cannot act in TIH of holes. From an analysis based on the energetics of the electronic coupling matrix elements in G(+)(T-A)n(GGG) duplexes we conclude that the superexchange mechanism is expected to dominate for n = 1-4. For long (A)n bridges (n > or approximately equal to 4) the TIH prevails, provided that the water side reaction is slow, raising the issue of chemical control of TIH through long (A)n bridges in DNA attained by changing the solution composition.     

Synthesis of [Ru(phen)(2)dppz](2+)-tethered oligo-DNA and studies on the metallointercalation mode into the DNA duplex

To explore the binding properties of [Ru(phen)(2)dppz](2+) complex (phen = 1,10-phenanthroline, dppz = dipyrido[3,2-a:2',3'-c]phenazine) in a sequence-specific manner in DNA duplex, it was tethered through the dppz ligand to a central position as well as both at the 3'- and 5'-ends of oligodeoxyribonucleotide (ODN). The middle [Ru(phen)(2)dppz](2+)-ODN tethered was resolved and isolated as four pure diastereomers, while the 3'- or 5'-[Ru(phen)(2)dppz](2+)-ODNs were inseparable on RP-HPLC. Thermal stability of the (Ru(2+)-ODN).DNA duplexes is found to increase considerably (DeltaT(m) = 12.8-23.4 degrees C), depending upon the site of the covalent attachment of the tethered [Ru(phen)(2)dppz](2+) complex, or the chirality of the [Ru(phen)(2)dppz](2+)-linker tethered at the middle of the ODN, compared to the unlabeled counterpart. Gross differences in CD between the [Ru(phen)(2)dppz](2+)-tethered and the native DNA duplexes showed that the global duplex conformation of the former has considerably altered from the B-type, but is still recognized by DNase I. The thermal melting studies, CD measurements, as well as DNase I digestion data, are interpreted as a result of intercalation of the dppz moiety, which is realized by threading of the Ru(phen)(2) complex part through the DNA duplex core. DNase I footprinting with four diastereomerically pure middle ([Ru(phen)(2)dppz](2+)-ODN).DNA duplexes furthermore showed that the tethered [Ru(phen)(2)dppz](2+)-linker chirality dictates the stereochemical accessibility of various phosphodiester moieties (around the intercalation site) toward the cleavage reaction by the enzyme. The diastereomerically pure ruthenium-modified duplexes, with the well-defined pi-stack, will be useful to explore stereochemistry-dependent energy- and electron-transfer chemistry to understand oxidative damage to the DNA double helix as well as the long-range energy- and electron-transfer processes with DNA as a reactant.     

Activation energies for dissociation of double strand oligonucleotide anions: evidence for watson-crick base pairing in vacuo

The dissociation kinetics of a series of complementary and noncomplementary DNA duplexes, (TGCA)(2) (3-), (CCGG)(2) (3-), (AATTAAT)(2) (3-), (CCGGCCG)(2) (3-), A(7).T(7) (3-), A(7).A(7) (3-), T(7).T(7) (3-), and A(7).C(7) (3-) were investigated using blackbody infrared radiative dissociation in a Fourier transform mass spectrometer. From the temperature dependence of the unimolecular dissociation rate constants, Arrhenius activation parameters in the zero-pressure limit are obtained. Activation energies range from 1.2 to 1.7 eV, and preexponential factors range from 10(13) to 10(19) s(-1). Dissociation of the duplexes results in cleavage of the noncovalent bonds and/or cleavage of covalent bonds leading to loss of a neutral nucleobase followed by backbone cleavage producing sequence-specific (a - base) and w ions. Four pieces of evidence are presented which indicate that Watson-Crick (WC) base pairing is preserved in complementary DNA duplexes in the gas phase: i. the activation energy for dissociation of the complementary dimer, A(7).T(7) (3-), to the single strands is significantly higher than that for the related noncomplementary A(7).A(7) (3-) and T(7).T(7) (3-) dimers, indicating a stronger interaction between strands with a specific base sequence, ii. extensive loss of neutral adenine occurs for A(7).A(7) (3-) and A(7).C(7) (3-) but not for A(7).T(7) (3-) consistent with this process being shut down by WC hydrogen bonding, iii. a correlation is observed between the measured activation energy for dissociation to single strands and the dimerization enthalpy (-DeltaH(d)) in solution, and iv. molecular dynamics carried out at 300 and 400 K indicate that WC base pairing is preserved for A(7).T(7) (3-) duplex, although the helical structure is essentially lost. In combination, these results provide strong evidence that WC base pairing can exist in the complete absence of solvent.     

Structures and energetics of base flipping of the thymine dimer depend on DNA sequence

The cis,syn-cyclobutane pyrimidine dimer (CPD) is a photoinduced DNA lesion leading to a significant distortion of the DNA structure. Its repair by DNA photolyase requires a flip of the damaged base into an extrahelical position. This base flip is expected to be sequence-dependent, but the structures and energetics as a function of the bases 3' and 5' to the CPD lesion are unknown. Eight-nanosecond MD simulations of four different hexadecamer duplexes with the CPD were performed for the flipped-in and flipped-out structures. Analysis of these results indicates clear sequence-dependent differences. Significant disruptions of the base pairs to the 3' side of the CPD are observed for the flipped-out structures with adjacent A-T pairs, whereas those with G-C pairs adjacent show no such distortions. The conformational spaces occupied by these two duplexes are significantly different. The structural differences correlate well with the free energy differences for base flipping calculated using the previously established 2D potential of mean force (PMF) method. The energy differences for base flipping in duplexes containing A, T, G, and C pairs adjacent to the CPD were found to be 6.25-6.5, 5.25-5.5, 7.25-7.5, and 6.5-6.75 kcal/mol, respectively. These energy differences of up to 2 kcal/mol should be large enough to be detected experimentally using sensitive probes.     

Multilabeled pyrene-functionalized 2'-amino-LNA probes for nucleic acid detection in homogeneous fluorescence assays

Homogeneous fluorescence assays for detection of nucleic acids are widely used in biological sciences. Typically, probes such as molecular beacons that rely on distance-dependent fluorescence quenching are used for such assays. Less attention has been devoted to tethering a single kind of fluorophores to oligonucleotides and exploiting hybridization-induced modulation of fluorescence intensity for nucleic acid detection. Herein, thermal denaturation experiments and fluorescence properties of oligodeoxyribonucleotides containing one or more 2'-N-(pyren-1-yl)carbonyl-2'-amino-LNA monomer(s) X are described. These pyrene-functionalized 2'-amino-LNAs display large increases in thermal stability against DNA/RNA complements with excellent Watson-Crick mismatch discrimination. Upon duplex formation of appropriately designed 2'-N-(pyren-1-yl)carbonyl-2'-amino-LNA probes and complementary DNA/RNA, intensive fluorescence emission with quantum yields between 0.28 and 0.99 are observed. Quantum yields of such magnitudes are unprecedented among pyrene-labeled oligonucleotides. Molecular modeling studies suggest that the dioxabicyclo[2.2.1]heptane skeleton and amide linkage of monomer X fix the orientation of the pyrene moiety in the minor groove of a nucleic acid duplex. Interactions between pyrene and nucleobases, which typically lead to quenching of fluorescence, are thereby reduced. Duplexes between multiple modified probes and DNA/RNA complements exhibit additive increases in fluorescence intensity, while the fluorescence of single stranded probes becomes increasingly quenched. Up to 69-fold increase in fluorescence intensity (measured at lambda(em) = 383 nm) is observed upon hybridization to DNA/RNA. The emission from duplexes of multiple modified probes and DNA/RNA at concentrations down to less than 500 nM can easily be seen by the naked eye using standard illumination intensities.     

Highly sensitive, selective, and rapid fluorescence Hg2+ sensor based on DNA duplexes of poly(dT) and graphene oxide

Coupling T base with Hg(2+) to form stable T-Hg(2+)-T complexes represents a new direction in detection of Hg(2+). Here a graphene oxide (GO)-based fluorescence Hg(2+) analysis using DNA duplexes of poly(dT) that allows rapid, sensitive, and selective detection is first reported. The Hg(2+)-induced T(15)-(Hg(2+))(n)-T(15) duplexes make T(15) unable to hybridize with its complementary A(15) labelled with 6'-carboxyfluorescein (FAM-A(15)), which has low fluorescence in the presence of GO. On the contrary, when T(15) hybridizes with FAM-A(15) to form double-stranded DNA because of the absence of Hg(2+), the fluorescence largely remains in the presence of GO. A linear range from 10 nM to 2.0 μM (R(2) = 0.9963) and a detection limit of 0.5 nM for Hg(2+) were obtained under optimal experimental conditions. Other metal ions, such as Al(3+), Ag(+), Ca(2+), Ba(2+), Mg(2+), Zn(2+), Mn(2+), Co(2+), Pb(2+), Ni(2+), Cu(2+), Cd(2+), Cr(3+), Fe(2+), and Fe(3+), had no significant effect on Hg(2+) detection. Moreover, the sensing system was used for the determination of Hg(2+) in river water samples with satisfactory results.     

Phosphorylation Within DNA Duplexes. Synthesis of Modified Oligodeoxyribonucleotide

Abstract

An effective method was suggested for the activation of phos-phomonoester groups in nicks of a double-strand DNA (1,2). This approach allows to incorporate various sugar phosphate backbone modifications at a particular site when DNA duplexes are being assembled. A modifying group is first introduced at the 5′- or 3′-termini of oligonucleotides, then a duplex is formed and oligomers are coupled on the complementary template using water-soluble l-ethyl-3-(3-dimethyl-aminopropyl)carbodiimide or cyanogen bromide as the condensing agents. Various DNA duplexes containing not only natural phosphodiester but also phosphoramidate and pyrophospha-te internucleotide bonds, as well as phosphodiester bonds between nucleotide residues with modified sugar analogs (ribo-, arabino- and xylo-derivatives) were assembled by this method.     

Incorporation of porphyrin acetylides into duplexes of the simplified nucleic acid GNA

A porphyrin-acetylide-modified GNA (glycol nucleic acid) phosphoramidite building block was synthesized in an economical fashion starting from (S)-glycidyl-4,4'- dimethoxytrityl ether in just 4 steps with an overall yield of 48%. The porphyrin acetylide nucleotide was incorporated into GNA duplexes opposite ethylene glycol abasic sites and the duplexes were analyzed by UV-melting, UV-vis, fluorescence spectroscopy, and circular dichroism. The modified GNA duplexes display lower thermal stabilities, however, the stabilities of the duplexes can be modulated by the incorporation of Zn(2+) (further destabilization) or Ni(2+) (stabilization relative to the uncomplexed porphyrin). Uncomplexed as well as Ni(2+)-coordinated porphyrins intercalate into the GNA duplex whereas Zn(2+)-coordinated porphyrins are most likely located outside the base stack. Adjacent porphyrins in opposite strands of GNA duplexes show an electronic interaction with each other which might be exploited in the future for the design of photoelectrical devices.     

Site-selective RNA cleavage by DNA bearing a base pair-mimic nucleoside

We have synthesized the deoxyadenosine derivative tethering a phenyl group (X), which mimics the Watson-Crick A/T base pair. The RNA/DNA hybrid duplexes containing X in the middle of the DNA sequence showed a similar thermal stability regardless of the ribonucleotide species (A, G, C, or U) opposite to X, probably because of the phenyl group stacking inside of the duplex accompanied by the opposite ribonucleotide base flipped in an extrahelical position. The RNA strand hybridized with the DNA strand bearing X was cleaved on the 3'-side of the ribonucleotide opposite to X in the presence of MgCl2, and the RNA sequence to be cleaved was not restricted. The site-specific RNA hydrolysis suggests that the DNA strand bearing X has the advantage of the site-selective base flipping in the target sequence and the development of a "universal deoxyribozyme" to exclusively cleave a target RNA sequence.     

Label-free emission assay of mercuric ions using DNA duplexes of poly(dT)

In this study, an assay to quantify the presence of mercuric ions and methyl mercury by double-stranded DNA containing a poly(dT) sequence was developed using a light switch compound, Ru(phen)(2)(dppz)(2+) (1), which is known to intercalate into double-stranded DNA. Upon treatment with mercuric ions, the metal-to-ligand charge transfer (MLCT) emission derived from the intercalation of 1 was reduced due to the formation of DNA duplexes containing T-Hg(2+)-T base pairs by the dehybridization of poly(dT)-poly(dA) duplexes at room temperature. As the concentration of Hg(2+) was increased, the emission of 1 gradually decreased. This label-free method had a detection limit of 5 nM. Other metal ions, such as K(+), Ag(+), Ca(2+), Mg(2+), Zn(2+), Mn(2+), Co(2+), Ni(2+), Cu(2+), Cd(2+), Cr(3+), Fe(3+), had no significant effect on reducing emission. This emission method can differentiate matched and mismatched poly(dT) sequences based on the dehybridization rate of dsDNA and the rate decreased in the order of T(10)C·A(11)～ T(10)A·A(11) > T(10)G·A(11) > T(11)·A(11).     

Contributions of the distance-dependent reorganization energy and proton-transfer to the hole-transfer process in DNA

A kinetic study of the single-step hole transfer in DNA was performed by measuring time-resolved transient absorption. DNA molecules with various sequences were designed and conjugated with naphthalimide (NI) and phenothiazine (PTZ) to investigate the sequence and distance dependence of the single-step hole transfer between guanines (Gs). Hole injection into DNA was accomplished by excitation of the NI site with a 355 nm laser pulse, and the kinetics of the hole-transfer process were investigated by monitoring the transient absorption of the PTZ radical cation (PTZ.+). Kinetic analysis of the time profile of PTZ.+ based on the kinetic model showed that the distance dependence of the hole-transfer process was significantly influenced by the DNA sequence. Results of temperature- and isotope-effect experiments demonstrated that the activation energy increased as the number of bridge bases separating the Gs increased. This is because of the distance-dependent reorganization energy and contribution of the proton-transfer process to the hole transfer in DNA.     

The Contribution of the Activation Entropy to the Gas-Phase Stability of Modified Nucleic Acid Duplexes

Tricyclo-DNA (tcDNA) is a sugar-modified analogue of DNA currently tested for the treatment of Duchenne muscular dystrophy in an antisense approach. Tandem mass spectrometry plays a key role in modern medical diagnostics and has become a widespread technique for the structure elucidation and quantification of antisense oligonucleotides. Herein, mechanistic aspects of the fragmentation of tcDNA are discussed, which lay the basis for reliable sequencing and quantification of the antisense oligonucleotide. Excellent selectivity of tcDNA for complementary RNA is demonstrated in direct competition experiments. Moreover, the kinetic stability and fragmentation pattern of matched and mismatched tcDNA heteroduplexes were investigated and compared with non-modified DNA and RNA duplexes. Although the separation of the constituting strands is the entropy-favored fragmentation pathway of all nucleic acid duplexes, it was found to be only a minor pathway of tcDNA duplexes. The modified hybrid duplexes preferentially undergo neutral base loss and backbone cleavage. This difference is due to the low activation entropy for the strand dissociation of modified duplexes that arises from the conformational constraint of the tc-sugar-moiety. The low activation entropy results in a relatively high free activation enthalpy for the dissociation comparable to the free activation enthalpy of the alternative reaction pathway, the release of a nucleobase. The gas-phase behavior of tcDNA duplexes illustrates the impact of the activation entropy on the fragmentation kinetics and suggests that tandem mass spectrometric experiments are not suited to determine the relative stability of different types of nucleic acid duplexes.

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Fluorescent silver nanoclusters in hybridized DNA duplexes for the turn-on detection of Hg2+ ions

Using the Hg(2+)-mediated T-T formation to strengthen the DNA duplexes and influence the configuration of fluorescent Ag NCs-forming sequences, a turn-on fluorescence detection method for Hg(2+) has been established.     

Consecutive GC base pairs determine the energy barrier of DNA duplex formation under molecularly crowded conditions

The kinetics of DNA duplex formation was affected by the addition of PEGs with different masses (MW = 200-8000) to an aqueous solution; for each condition, two duplexes (5'-TAGGTTATAA-3'/5'-TTATAACCTA-3' and 5'-CAGGTCACAG-3'/5'-CTGTGACCTG-3') with different stabilities were formed after overcoming the same association activation energy barrier, suggesting that the formation of consecutive GC base pairs in the helices rather than the helix terminus is the initiation nucleus for DNA duplex formation not only in the absence, but also in the presence of PEGs.     

Reductive Charge Transfer through an RNA Aptamer

The transfer of charges through double helical DNA is a very well investigated bioelectric phenomenon. RNA, on the contrary, has been less studied in this regard. The few available data report on charge transfer through RNA duplex structures mainly composed of homonucleotide sequences. In the light of the RNA world scenarios, it is an interesting question, if charge transfer can be coupled with RNA function. Functional RNAs however, contain versatile structural motifs. Therefore, electron transport also through non-Watson–Crick base-paired regions might be required. We here demonstrate distance-dependent reductive charge transfer through RNA duplexes and through the non-Watson–Crick base-paired region of an RNA aptamer.