Electron Transfer In DNA Research Articles

Programmed Control of Fluorescence Blinking Patterns based on Electron Transfer in DNA.

Fluorescence imaging uses changes in the fluorescence intensity and emission wavelength to analyze multiple targets simultaneously. To increase the number of targets that can be identified simultaneously, fluorescence blinking can be used as an additional parameter. To understand and eventually control blinking, we used DNA as a platform to elucidate the processes of electron transfer (ET) leading to blinking, down to the rate constants. With a fixed ET distance, various blinking patterns were observed depending on the DNA sequence between the donor and acceptor units of the DNA platform. The blinking pattern was successfully described with a combination of ET rate constants. Therefore, molecules with various blinking patterns can be developed by tuning ET. It is expected that the number of targets that can be analyzed simultaneously will increase by the power of the number of blinking patterns.

Tunneling or Hopping? A Direct Electrochemical Observation of Electron Transfer in DNA

We developed an axis-mode donor-DNA-acceptor electrochemical system to distinguish whether electron transfer in DNA occurs by tunneling or hopping. In the axis-mode, rigid stem-loop DNA was designed with the redox probe Ag+ embedded at the axis of the strand through a C-Ag+-C mismatch, which was immobilized onto the electrode surface in a saturated manner. Thus, the rotation, swing, and bending of the DNA strand were restricted and then the number of Ag+, the distance L between Ag+ and the electrode, and the chemical environment could be precisely controlled. In addition, fast scan cyclic voltammetry was applied to realize the in situ redox reaction of Ag+, without diffusion away from the electrode and the ensuing deconstruction of the stem-loop DNA. In this case, as a direct indicator of rate, the peak Faradaic current ip was extracted and used to fit the tunneling mechanism i ∝ exp (-βL) and the hopping mechanism i ∝ L-η. The value of β was determined to be 0.100 Å-1, which is consistent with the range of 0.1∼1.5 Å-1 reported previously, while η was determined to be 0.677, which is completely beyond the correct range of 1 ≤ η ≤ 2, demonstrating that electron transfer in DNA occurs by tunneling instead of hopping or that tunneling dominates. Additionally, current additivity and the irrelevance of the base sequence illustrate this point again. Thus, the possibility of independent parallel tunneling currents in DNA strands is revealed, which is helpful for recognizing the feasibility of DNA-based wires and devices.

Comment on “Spin-orbit interaction and spin selectivity for tunneling electron transfer in DNA”

The observation of chiral-induced spin selectivity (CISS) in biological molecules still awaits a full theoretical explanation. In a recent Rapid Communication, Varela et al. [Phys. Rev. B 101, 241410(R) (2020)] presented a model for electron transport in biological molecules by tunneling in the presence of spin-orbit interactions. They then claimed that their model produces a strong spin asymmetry due to the intrinsic atomic spin-orbit strength. As their Hamiltonian is time-reversal symmetric, this result contradicts a theorem by Bardarson [J. Phys. A: Math. Theor. 41, 405203 (2008)], which states that such a Hamiltonian cannot generate a spin asymmetry for tunneling between two terminals (in which there are only a spin-up and a spin-down channels). Here we solve the model proposed by Varela et al. and show that it does not yield any spin asymmetry, and therefore cannot explain the observed CISS effect.

Coherence preservation and electron-phonon interaction in electron transfer in DNA.

We analyze the influence of electron-phonon (e-ph) interaction in a model for electron transfer (ET) processes in DNA in terms of the envelope function approach for spinless electrons. We are specifically concerned with the effect of e-ph interaction on the coherence of the ET process and how to model the interaction of DNA with phonon reservoirs of biological relevance. We assume that the electron bearing orbitals are half filled and derive the physics of e-ph coupling in the vicinity in reciprocal space. We find that at half filling, the acoustical modes are decoupled to ET at first order, while optical modes are predominant. The latter are associated with inter-strand vibrational modes in consistency with previous studies involving polaron models of ET. Coupling to acoustic modes depends on electron doping of DNA, while optical modes are always coupled within our model. Our results yield e-ph coupling consistent with estimates in the literature, and we conclude that large polarons are the main result of such e-ph interactions. This scenario will have strong consequences on decoherence of ET under physiological conditions due to relative isolation from thermal equilibration of the ET mechanism.

Spin-orbit interaction and spin selectivity for tunneling electron transfer in DNA

Electron transfer (ET) in biological molecules such as peptides and proteins consists of electrons moving between well defined localized states (donors to acceptors) through a tunneling process. Here we present an analytical model for ET by tunneling in DNA, in the presence of Spin-Orbit (SO) interaction, to produce a strong spin asymmetry with the intrinsic atomic SO strength in meV range. We obtain a Hamiltonian consistent with charge transport through $\pi$ orbitals on the DNA bases and derive the behavior of ET as a function of the injection state momentum, the spin-orbit coupling and barrier length and strength. A highly consistent scenario arises where two concomitant mechanisms for spin selection arises; spin interference and differential spin amplitude decay. High spin filtering can take place at the cost of reduced amplitude transmission assuming realistic values for the spin-orbit coupling. The spin filtering scenario is completed by addressing the spin dependent torque under the barrier, with a consistent conserved definition for the spin current.

The effect of spermidine on guanine decomposition via photoinduced electron transfer in DNA.

Spermidine, a trivalent organic cation, induced DNA structural changes and suppressed guanine photooxidative decomposition via electron transfer through pyrene-modified DNA. On the other hand, adding higher concentrations of spermidine resulted in DNA condensation. The efficiency of guanine decomposition in condensed pyrene-modified DNA was promoted remarkably.

Electron Transfer in DNA at Electrified Interfaces.

The ability of the DNA double helix to transport electrons underlies many life-centered biological processes and bio-electronic applications. However, there is little consensus on how efficiently the base pair π-stacks of DNA mediate electron transport. This minireview scrutinizes the current state-of-the-art knowledge on electron transfer (ET) properties of DNA and its long-range ability to transfer (mediate) electrical signals at electrified interfaces, without being oxidized or reduced. Complex changes an electric field induces in the DNA structure and its electronic properties govern the efficiency of DNA-mediated ET at electrodes and allow addressing the existing phenomenological riddles, while recently discovered rectifying properties of DNA contribute both to our understanding of DNA's ET in living systems and to advances in molecular bioelectronics.

Electron injection from mitochondrial transcription factor A to DNA associated with thymine dimer photo repair.

Electron transfer through π-stacked arrays of double-stranded DNA contributes to the redox chemistry of bases, including guanine oxidation and thymine-thymine dimer repair by photolyase. 5-Bromouracil is an attractive photoreactive thymine analogue that can be used to investigate electron transfer in DNA, and is a useful probe for protein-DNA interaction analysis. In the present study using BrU we found that UV irradiation facilitated electron injection from mitochondrial transcription factor A into DNA. We also observed that this electron injection could lead to repair of a thymine-thymine dimer.

Photoactivated proton coupled electron transfer in DNA: insights from quantum mechanical calculations.

The energetics of the two main proton coupled electron transfer processes that could occur in DNA are determined by means of time dependent-DFT calculations, using the M052X functional and the polarizable continuum model to include solvent effect. This approach has been applied to fragments of GC and AT alternated duplexes containing up to 4 base pairs. In GC DNA, intra-strand G → C charge transfer (CT) can trigger inter-strand Proton Transfer (PT) involving the C anion, since the reaction is exothermic and the related energy barrier is <0.3 eV. In AT DNA, the minimum resulting from intra-strand A → T CT is not predicted to undergo inter-strand PT. These conclusions are in full agreement with the indication of time-resolved IR spectra. In both systems, inter-strand CT can be coupled to inter-strand PT, and the resulting minimum, reached after overcoming a moderate energy barrier (<0.4 eV), is close to a crossing region with the ground electronic state, providing a relatively fast non-radiative deactivation route.

Independent Generation and Reactivity of Thymidine Radical Cations.

Thymidine radical cation (1) is produced by ionizing radiation and has been invoked as an intermediate in electron transfer in DNA. Previous studies on its structure and reactivity have utilized thymidine as a precursor, which limits quantitative product analysis because thymidine is readily reformed from 1. In this investigation, radical cation 1 is independently generated via β-heterolysis of a pyrimidine radical generated photochemically from an aryl sulfide. Thymidine is the major product (33%) from 1 at pH 7.2. Diastereomeric mixtures of thymidine glycol and the corresponding 5-hydroxperoxides resulting from water trapping of 1 are formed. Significantly lower yields of products such as 5-formyl-2'-deoxyuridine that are ascribable to deprotonation from the C5-methyl group of 1 are observed. Independent generation of the N3-methyl analogue of 1 (NMe-1) produces considerably higher yields of products derived from water trapping, and these products are formed in much higher yields than those attributable to the C5-methyl group deprotonation in NMe-1. N3-Methyl-thymidine is, however, the major product and is produced in as high as 70% yield when the radical cation is produced in the presence of excess thiol. The effects of exogenous reagents on product distributions are consistent with the formation of diffusively free radical cations (1, NMe-1). This method should be compatible with producing radical cations at defined positions within DNA.

Microsecond Simulation of Electron Transfer in DNA: Bottom-Up Parametrization of an Efficient Electron Transfer Model Based on Atomistic Details.

The transfer of electrons over long distances in complex molecular systems is a phenomenon of significance in both biochemistry and technology. In recent years, we have been developing efficient models to study ET in complex systems, including DNA as a prominent example. Ab initio and model approaches have been combined in an "on-the-fly" calculation of ET parameters, which can be used to propagate nuclear and electronic degrees of freedom simultaneously. These previous efforts have aimed at deriving an efficient nonadiabatic quantum mechanical-molecular mechanical (QM/MM) simulation scheme for ET, making nanosecond simulations of ET in realistic systems possible. This, however, is still insufficient for the treatment of large donor-bridge-acceptor systems, like the ET in DNA, overcoming long adenine bridges. Therefore, we have constructed a theoretical model in a bottom-up manner. All quantum-chemical as well as force-field calculations are substituted by theoretical models of the involved phenomena on a molecular level, including polarization and relaxation of the molecular environment, which are often omitted in other recently developed theoretical models of ET. A nonadiabatic simulation scheme is employed, and no assumptions regarding the ET mechanism are needed. Thus, the predictive power of the simulations is preserved, while pushing the limits of the accessible time scales beyond microseconds. This model-based simulation scheme is applied to ET in various DNA species. Good agreement with the "full" atomistic nonadiabatic QM/MM scheme is observed for the archetypal DNA ET systems, the polyA sequence, as well as the sequences GTnGGG, containing adenines as bridge sites. Furthermore, ET in larger, more complex DNA sequences is simulated, and the results are discussed.

Acceleration of Long-Range Photoinduced Electron Transfer through DNA by Hydroxyquinolines as Artificial Base Pairs.

The C-nucleoside based on the hydroxyquinoline ligand (Hq) is complementary to itself and forms stable Hq-Hq pairs in double-stranded DNA. These artificial Hq-Hq pairs may serve as artificial electron carriers for long-range photoinduced electron transfer in DNA, as elucidated by a combination of gel electrophoretic analysis of irradiated samples and time-resolved transient absorption spectroscopy. For this study, the Hq-Hq pair was combined with a DNA-based donor-acceptor system consisting of 6-N,N-dimethylaminopyrene conjugated to 2'-deoxyuridine as photoinducible electron donor, and methyl viologen attached to the 2'-position of uridine as electron acceptor. The Hq radical anion was identified in the time-resolved measurements and strand cleavage products support its role as an intermediate charge carrier. Hence, the Hq-Hq pair significantly enhances the electron hopping capability of DNA compared to natural DNA bases over long distances while keeping the self-assembly properties as the most attractive feature of DNA as a supramolecular architecture.

Photoinduced Electron Transfer in DNA: Charge Shift Dynamics Between 8-Oxo-Guanine Anion and Adenine.

Femtosecond time-resolved IR spectroscopy is used to investigate the excited-state dynamics of a dinucleotide containing an 8-oxoguanine anion at the 5'-end and neutral adenine at the 3'-end. UV excitation of the dinucleotide transfers an electron from deprotonated 8-oxoguanine to its π-stacked neighbor adenine in less than 1 ps, generating a neutral 8-oxoguanine radical and an adenine radical anion. These species are identified by the excellent agreement between the experimental and calculated IR difference spectra. The quantum efficiency of this ultrafast charge shift reaction approaches unity. Back electron transfer from the adenine radical anion to the 8-oxguanine neutral radical occurs in 9 ps, or approximately 6 times faster than between the adenine radical anion and the 8-oxoguanine radical cation (Zhang, Y. et al. Proc. Natl. Acad. Sci. U.S.A. 2014, 111, 11612-11617). The large asymmetry in forward and back electron transfer rates is fully rationalized by semiclassical nonadiabatic electron transfer theory. Forward electron transfer is ultrafast because the driving force is nearly equal to the reorganization energy, which is estimated to lie between 1 and 2 eV. Back electron transfer is highly exergonic and takes place much more slowly in the Marcus inverted region.

Cobalt(III)hexaammine-dependent photocrosslinks in the hairpin ribozyme

We have utilized the hairpin ribozyme, an RNA enzyme whose structure has been solved by high-resolution methods, to develop a new tool for mapping nucleobase–stacking interactions and potential metal-binding sites in RNA molecules. This tool involves the photoactivation of a specifically bound cobalt(III)hexaammine molecule at wavelengths corresponding to excitation of the metal ion complex only; no base excitation is involved. The photoexcitation initiates a process which strongly promotes the formation of a novel covalent bond or crosslink between one base (termed the “first base”), which is close in space to the excited cobalt(III)hexaammine complex, and another base upon which the first base is closely stacked. These crosslinked species can be isolated and sequenced; their activities can be analyzed to ensure that the crosslinked structures represent an active conformation of the molecule. We have shown that, as in electron transfer in DNA, several criteria must be met to result in the successful formation of these crosslinks. These include the appropriate oxidation potential of the first donor base, the stacking and close interaction of the two donor bases involved in the crosslink, and the binding of a specific cobalt(III)hexaammine molecule to the first donor base. Additionally, we have determined that this crosslinking is pH-sensitive, although the cause of this sensitivity remains unknown. This tool has proven useful in the past for the analysis of the hairpin ribozyme folded structure, and has been applied to identify potential metal-binding sites on the hairpin and extended hammerhead ribozymes.

Development of a Metal‐Ion‐Mediated Base Pair for Electron Transfer in DNA

A new C-nucleoside structurally based on the hydroxyquinoline ligand was synthesized that is able to form stable pairs in DNA in both the absence and the presence of metal ions. The interactions between the metal centers in adjacent Cu(II)-mediated base pairs in DNA were probed by electron paramagnetic resonance (EPR) spectroscopy. The metal-metal distance falls into the range of previously reported values. Fluorescence studies with a donor-DNA-acceptor system indicate that photoinduced charge-transfer processes across these metal-ion-mediated base pairs in DNA occur more efficiently than over natural base pairs.

Sequence-specific electron injection into DNA from an intermolecular electron donor.

Electron transfer in DNA has been intensively studied to elucidate its biological roles and for applications in bottom-up DNA nanotechnology. Recently, mechanisms of electron transfer to DNA have been investigated; however, most of the systems designed are intramolecular. Here, we synthesized pyrene-conjugated pyrrole-imidazole polyamides (PPIs) to achieve sequence-specific electron injection into DNA in an intermolecular fashion. Electron injection from PPIs into DNA was detected using 5-bromouracil as an electron acceptor. Twelve different 5-bromouracil-containing oligomers were synthesized to examine the electron-injection ability of PPI. Product analysis demonstrated that the electron transfer from PPIs was localized in a range of 8 bp from the binding site of the PPIs. These results demonstrate that PPIs can be a useful tool for sequence-specific electron injection.

A Theory of Hole Transfer in DNA

A theory, which was previously applied to electron transfer in DNA, is applied to hole transfer between a dye molecule and an electrode coupled through a DNA bridge, because the applicability to such hole transfer has not yet been studied. The results calculated using the theory are compared with the experimental results for the same system. The theory reproduces the dependence of the current between the dye molecule and the electrode on the length of DNA. However, the agreement with experimental results requires that the reorganization energy in the ground state of a dye molecule be larger than that employed in previous studies of electron transfer.

Unmediated by DNA Electron Transfer in Redox-Labeled DNA Duplexes End-Tethered to Gold Electrodes

Electron transfer (ET) between gold electrodes and redox-labeled DNA duplexes, immobilized onto the electrodes through the alkanethiol linker at the 3'-end and having internal either methylene blue (MB) or anthraquinone (AQ) redox labels, was shown to depend on the redox label charge and the way the redox label is linked to DNA. For loosely packed DNA monolayers, the conjugation of the positively charged MB to DNA through the long and flexible alkane linker provided ET whose kinetics was formally governed by the diffusion of the redox label to the negatively charged electrode surface. For the uncharged AQ label no ET signal was detected. The conjugation of AQ to DNA through the short and more conductive acetylene linker did not provide the anticipated DNA-mediated ET to the AQ-moiety: ET appeared to be low-efficient if any in the studied system, for which no intercalation of AQ within the DNA duplex occurred. The ET communication between the electrode and AQ, built in DNA through the acetylene linker, was achieved only when Ru(NH(3))(6)(3+) molecules were electrostatically attached to the DNA duplex, thus forming the electronic wire. These results are of particular importance both for the fundamental understanding of the interfacial behavior of the redox labeled DNA on electrodes and for the design of biosensors exploiting a variation of ET properties of DNA in the course of hybridization.

Electron transfer in DNA

AbstractDuring the last two decades, electron transfer (ET) through DNA and its artificial analogues has been an area of extensive experimental and theoretical studies. This process plays an important role in biology (damage and repair of DNA in living cells) and is of potential interest in material sciences. Because structural dynamics of the π stack and its environment affect essentially the electron transport, some significant details of excess charge migration cannot be derived from experiments. Computer simulations of the ET process provide microscopic insights into mechanisms of this process. In the paper, we consider computational methods used to describe the propagation of excess charges through π stacks of DNA and related systems. © 2012 John Wiley &amp; Sons, Ltd.This article is categorized under: Molecular and Statistical Mechanics &gt; Molecular Dynamics and Monte-Carlo Methods

DFT performance for the hole transfer parameters in DNA π stacks

Recently, we showed that unoccupied Kohn-Sham (KS) orbitals stemming from DFT calculations of a neutral system can be used to derive accurate estimates of the free energy and electronic couplings for excess electron transfer in DNA (Felix and Voityuk, J Phys Chem A 2008, 112, 9043). In this article, we consider the propagation of radical cation states (hole transfer) through DNA π-stacks and compare the performance of different exchange-correlation functionals to estimate the hole transfer (HT) parameters. Two different approaches are used: (1) calculations that use occupied KS orbitals of neutral π stacks of nucleobases, and (2) the time-dependent DFT method which is applied to the radical cation states of these stacks. Comparison of the calculated parameters with the reference data suggests that the best results are provided by the KS scheme with hybrid functionals (B3LYP, PBE0, and BHH in contrast, the spin-unrestricted DFT method considerably overestimates the hole delocalization in the radical cations. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2011