Kinetics of Transient End-to-End Contact of Single-Stranded DNAs

Nanosecond chain dynamics of single-stranded nucleic acids

The conformational dynamics of single-stranded nucleic acids are fundamental for nucleic acid folding and function. However, their elementary chain dynamics have been difficult to resolve experimentally. Here we employ a combination of single-molecule Förster resonance energy transfer, nanosecond fluorescence correlation spectroscopy, and nanophotonic enhancement to determine the conformational ensembles and rapid chain dynamics of short single-stranded nucleic acids in solution. To interpret the experimental results in terms of end-to-end distance dynamics, we utilize the hierarchical chain growth approach, simple polymer models, and refinement with Bayesian inference to generate structural ensembles that closely align with the experimental data. The resulting chain reconfiguration times are exceedingly rapid, in the 10-ns range. Solvent viscosity-dependent measurements indicate that these dynamics of single-stranded nucleic acids exhibit negligible internal friction and are thus dominated by solvent friction. Our results provide a detailed view of the conformational distributions and rapid dynamics of single-stranded nucleic acids.

Mechanochemical Preparation of Edge-Selectively justify Hydroxylated Graphene Nanosheets Using Persulfate via a Sulfate Radical-Mediated Process

The production of water-dispersed graphene with low defects remains a challenge. The dry ball milling of graphite with additives produces edge-selectively functionalized graphene. However, the "inert" additives require a long milling time and cause inevitable in-plane defects. Here, the mechanochemical reaction of graphite with persulfate solved the above drawback and produced edge-selectively hydroxylated graphene (EHG) nanosheets through a 2 h ball-milling and a subsequent 0.5 h sonication. The mechanochemical cleavage of persulfate yielded SO₄ ⋅^- to spontaneously oxidize graphite to form the carbon radical cations selectively at edges, followed by hydroxylation with water of moisture. Because the O-O bond dissociation energy of persulfate is 20 % of the graphitic C-C bond, the rather low milling energy allowed the hydroxylation of graphite at edges with nearly no in-plane defects. The obtained EHG showed high water-dispersibility and excellent photothermal and electrochemical properties, thereby opening up a new door to fabricate graphene-based composites.

Formation of the Charge-Localized Dimer Radical Cation of 2-Ethyl-9,10-dimethoxyanthracene in Solution Phase

Although dimer radical ions of aromatic molecules in the liquid-solution phase have been intensely studied, the understanding of charge-localized dimers, in which the extra charge is localized in a single monomer unit instead of being shared between two monomer units, is still elusive. In this study, the formation of a charge-localized dimer radical cation of 2-ethyl-9,10-dimethoxyanthracene (DMA), (DMA)₂ ^.+ is investigated by transient absorption (TA) and time-resolved resonance Raman (TR³ ) spectroscopic methods combined with a pulse radiolysis technique. Visible- and near-IR TA signals in highly concentrated DMA solutions supported the formation of non-covalent (DMA)₂ ^.+ by association of DMA and DMA^.+ . TR³ spectra obtained from 30 ns to 300 μs time delays showed that the major bands are quite similar to those of DMA except for small transient bands, even at 30 ns time delay, suggesting that the positive charge of non-covalent (DMA)₂ ^.+ is localized in a single monomer unit. From DFT calculations for (DMA)₂ ^.+ , our TR³ spectra showed the best agreement with the calculated Raman spectrum of charge-localized edge-to-face T-shaped (DMA)₂ ^.+ , termed DT^.+ , although the charge-delocalized asymmetric π-stacked face-to-face (DMA)₂ ^.+ , termed DF3^.+ , is the most stable structure of (DMA)₂ ^.+ according to the energetics from DFT calculations. The calculated potential energy curves for the association between DMA^.+ and DMA showed that DT^.+ is likely to be efficiently formed and contribute significantly to the TR³ spectra as a result of the permanent charge-induced Coulombic interactions and a dynamic equilibrium between charge localized and delocalized structures.

Sequence and temperature dependence of the end-to-end collision dynamics of single-stranded DNA

Intramolecular collision dynamics play an essential role in biomolecular folding and function and, increasingly, in the performance of biomimetic technologies. To date, however, the quantitative studies of dynamics of single-stranded nucleic acids have been limited. Thus motivated, here we investigate the sequence composition, chain-length, viscosity, and temperature dependencies of the end-to-end collision dynamics of single-stranded DNAs. We find that both the absolute collision rate and the temperature dependencies of these dynamics are base-composition dependent, suggesting that base stacking interactions are a significant contributor. For example, whereas the end-to-end collision dynamics of poly-thymine exhibit simple, linear Arrhenius behavior, the behavior of longer poly-adenine constructs is more complicated. Specifically, 20- and 25-adenine constructs exhibit biphasic temperature dependencies, with their temperature dependences becoming effectively indistinguishable from that of poly-thymine above 335 K for 20-adenines and 328 K for 25-adenines. The differing Arrhenius behaviors of poly-thymine and poly-adenine and the chain-length dependence of the temperature at which poly-adenine crosses over to behave like poly-thymine can be explained by a barrier friction mechanism in which, at low temperatures, the energy barrier for the local rearrangement of poly-adenine becomes the dominant contributor to its end-to-end collision dynamics.

Kinetics and dynamics of DNA hybridization

DNA hybridization, wherein strands of DNA form duplex or larger hybrids through noncovalent, sequence-specific interactions, is one of the most fundamental processes in biology. Developing a better understanding of the kinetic and dynamic properties of DNA hybridization will thus help in the elucidation of molecular mechanisms involved in numerous biochemical processes. Moreover, because DNA hybridization has been widely adapted in biotechnology, its study is invaluable to the development of a range of commercially important processes. In this Account, we examine recent studies of the kinetics and dynamics of DNA hybridization, including (i) intramolecular collision of random coil, single-stranded DNA (ssDNA), (ii) nucleic acid hairpin folding, and (iii) considerations of DNA hybridization from both a global view and a detailed base-by-base view. We also examine the spontaneous single-base-pair flipping in duplex DNA because of its importance to both DNA hybridization and repair. Intramolecular collision of random coil ssDNA, with chemical relaxation times ranging from hundreds of nanoseconds to a few microseconds, is investigated both theoretically and experimentally. The first passage time theory of Szabo, Schulten, and Schulten, which determines the average reaction time of the intrachain collision, was tested. Although it was found to provide an acceptable approximation, a more sophisticated theoretical treatment is desirable. Nucleic acid hairpin folding has been extensively investigated as an important model system of DNA hybridization. The relaxation time of hairpin folding and unfolding strongly depends on the stem length, and it may range from hundreds of microseconds to hundreds of milliseconds. The traditional two-state model has been revised to a multistate model as a result of new experimental observations and theoretical study, and partially folded intermediate states have been introduced to the folding energy landscape. On the other hand, new techniques are needed to provide more accurate and detailed information on the dynamics of DNA hairpin folding in the time domain of sub-milliseconds to tens of milliseconds. From a global view, the hybridization of unstructured ssDNA goes through an entropy-controlled nucleation step, whereas the hybridization of ssDNA with a hairpin structure must overcome an extra, enthalpy-controlled energy barrier to eliminate the hairpin. From a detailed base-by-base view, however, there exist many intermediate states. The average single-base-pair hybridization and dehybridization rates in a duplex DNA formation have been determined to be on the order of a millisecond. Meanwhile, accurate information on the early stages of hybridization, such as the dynamics of nucleation, is still lacking. The investigation of spontaneous flipping of a single base in a mismatched base pair in a duplex DNA, although very important, has only recently been initiated because of the earlier lack of suitable probing tools. In sum, the study of DNA hybridization offers a rich range of research opportunities; recent progress is highlighting areas that are ripe for more detailed investigation.

Direct measurement of the rates and barriers on forward and reverse diffusions of intramolecular collision in overhang oligonucleotides

The dynamics of end-to-interior (Type I) and end-to-end (Type II) collisions in a dangling overhang anchored on a double-stranded DNA (dsDNA) was studied by monitoring the fluorescence quenching of tetramethylrhodamine (TMR) by guanosine residues through combining photoinduced electron transfer (PET) with fluorescence correlation spectroscopy (FCS) at different temperatures. TMR and guanosine residues are separated by a double helix with dangling bases ranging from 2 to 16. By analyzing the FCS data, we obtained the forward and reverse intrachain diffusion rate constants and respective barriers. For both Type I and Type II collisions, the intrachain diffusion rates followed the scaling law of the Gaussian chain model. Especially, the reverse intrachain diffusion rate was insensitive to the base length of separation. Both the activation enthalpy and activation entropy of the forward and reverse diffusions were length independent. The comparison between Type I and Type II collisions shows that the collision rate of end-to-interior is slower than that of end-to-end. The phenomenon is further checked in detail by a series of dangling DNA with the same separation length but different tail lengths (Type III).

End-to-surface reaction dynamics of a single surface-attached DNA or polypeptide

The dynamics of surface-attached polymers play a key role in the operation of a number of biological sensors, yet its current understanding is rather limited. Here we use computer simulations to study the dynamics of a reaction between the free end of a polymer chain and a surface, to which its other end has been attached. We consider two limiting cases, the diffusion-controlled limit, where the reaction is accomplished whenever the free chain end diffuses to within a specified distance from the surface, and the reaction-controlled limit, where slow, intrinsic reaction kinetics rather than diffusion of the chain is rate limiting. In the diffusion-controlled limit, we find that the overall rate scales as N(-b), where N is the number of monomers in the chain and b approximately = 2.2 for excluded volume chains. This value of the scaling exponent b is close to that derived from a simple approximate theory treating the dynamics of the chain end relative to the surface as one-dimensional diffusion in an effective potential. In the reaction-controlled limit, the value of the scaling exponent b is close to 1. We compare our findings with those for the related (and better studied) problem of end-to-end reactions within an unconstrained polymer chain and discuss their implications for electrochemical DNA sensors.

The rate of intramolecular loop formation in DNA and polypeptides: the absence of the diffusion-controlled limit and fractional power-law viscosity dependence

The problem of determining the rate of end-to-end collisions for polymer chains has attracted the attention of theorists and experimentalists for more than three decades. The typical theoretical approach to this problem has focused on the case where a collision is defined as any instantaneous fluctuation that brings the chain ends to within a specific capture distance. In this paper, we study the more experimentally relevant case, where the end-to-end collision dynamics are probed by measuring the excited state lifetime of a fluorophore (or other lumiphore) attached to one chain end and quenched by a quencher group attached to the other end. Under this regime, a "contact" is defined not by the chain ends approach to within some sharp cutoff but, instead, typically by an exponentially distance-dependent process. Previous theoretical models predict that, if quenching is sufficiently rapid, a diffusion-controlled limit is attained, where such measurements report on the probe-independent, intrinsic end-to-end collision rate. In contrast, our theoretical considerations, simulations, and an analysis of experimental measurements of loop closure rates in single-stranded DNA molecules all indicate that no such limit exists, and that the measured effective collision rate has a nontrivial, fractional power-law dependence on both the intrinsic quenching rate of the fluorophore and the solvent viscosity. We propose a simple scaling formula describing the effective loop closure rate and its dependence on the viscosity, chain length, and properties of the probes. Previous theoretical results are limiting cases of this more general formula.

The length and viscosity dependence of end-to-end collision rates in single-stranded DNA

Intramolecular dynamics play an essential role in the folding and function of biomolecules and, increasingly, in the operation of many biomimetic technologies. Thus motivated we have employed both experiment and simulation to characterize the end-to-end collision dynamics of unstructured, single-stranded DNAs ranging from 6 to 26 bases. We find that, because of the size and flexibility of the optical reporters employed experimentally, end-to-end collision dynamics exhibit little length dependence at length scales <11 bases. For longer constructs, however, the end-to-end collision rate exhibits a power-law relationship to polymer length with an exponent of -3.49 +/- 0.13. This represents a significantly stronger length dependence than observed experimentally for unstructured polypeptides or predicted by polymer scaling arguments. Simulations indicate, however, that the larger exponent stems from electrostatic effects that become important over the rather short length scale of these highly charged polymers. Finally, we have found that the end-to-end collision rate also depends linearly on solvent viscosity, with an experimentally significant, nonzero intercept (the extrapolated rate at zero viscosity) that is independent of chain length--n observation that sheds new light on the origins of the "internal friction" observed in the dynamics of many polymer systems.

Charge separation in acridine- and phenothiazine-modified DNA

The formation of the long-lived, charge-separated state in DNA upon visible light irradiation is of particular interest in molecular-scale optoelectronics, sensor design, and other areas of nanotechnology. However, the efficient generation of the charge-separated state is hampered by fast charge recombination within a contact ion pair, which limits the application of DNA for photoelectrochemical sensors and devices. In this study, a series of protonated 9-alkylamino-6-chloro-2-methoxyacridine (Acr+)- and phenothiazine (Ptz)-modified DNAs were synthesized for the further understanding of the mechanism of charge separation in DNA to generate a long-lived, charge-separated state with a high quantum yield (Phi). The Acr+ serves as a photosensitizer to produce a hole on guanine (G), and the G-C base pairs were used as a hole-transporting pathway to separate a hole from Acr* (the one-electron-reduced form of Acr+) to be trapped at Ptz. Since Acr+ oxides only G upon photoexcitation, the A-T base pair can be used as a spacer between Acr+ and the G-C base pair to avoid the formation of a contact ion pair. The charge injection dynamics was investigated by steady-state fluorescence spectra and fluorescence lifetime measurements, and the Phi and the lifetime of the charge-separated state produced upon photoirradiation were assessed by nanosecond laser flash photolysis of the Acr+- and Ptz-modified DNA. A long-lived, charge-separated state was successfully formed upon visible-light irradiation, and the Phi was the highest for the DNA having a single intervening A-T base pair between Acr+ and the G-C base pair. These results clearly demonstrated that the charge separation process in DNA can be refined by putting a redox-inactive intervening base pair as a spacer between a photosensitizer and the nucleobase to be oxidized to slow down the charge recombination rate.

1-Phenylethynylpyrene (1-PEPy) as Refined Excimer Forming Alternative to Pyrene: Case of DNA Major Groove Excimer

1-Phenylethynylpyrene fluorochrome was studied as meta- and para-derivatives of arabino-uridine-2'-carbamates in ss and dsDNA. 1-PEPy showed red-shifted emission and increased fluorescence quantum yield compared to pyrene. Although 1-PEPy has very short excited lifetime (<2.5 ns), it is able to form inter- and intrastrand excimers on DNA, probably resulting from spatial preorganization of two dye molecules.

Insertion of two pyrene moieties into oligodeoxyribonucleotides for the efficient detection of deletion polymorphisms

For the detection of deletion polymorphisms, two pyrene moieties are tethered to an oligodeoxyribonucleotide (ODN) on both sides of the intervening base; one- and two-base deletions can be selectively detected by the strength of the excimer emission.

Hole Transfer Rates in A-Form DNA/2′-OMeRNA Hybrid

The hole transfer rates in the DNA/DNA B-form duplex and DNA/2'-OMeRNA A-form duplex were measured which occurred in the time range of approximately 100 micros. The hole transfer rates in the A-form duplexes were slower and more strongly dependent on the temperature compared to those in the B-form duplexes, suggesting that the A-form is more rigid than the B-form duplex in this time scale.

Hole transfer in DNA and photosensitized DNA damage: importance of adenine oxidation

Photosensitized DNA damage reactions were investigated for two well-known DNA-damaging photosensitizers (Sens), naphthalimide (NI) and napthaldiimide (NDI), which have similar photophysical properties but differ in their redox properties. NI and NDI derivatives (NIN, NDIN), which have cationic side chains and electrostatically binding to DNA due to favorable electrostatic interactions between the negatively charged phosphate groups of DNA and cationic groups, and NIP and NDIP, which possess phosphate groups and do not bind to DNA, were synthesized. NIN and NDIN can oxidize A and G via their singlet excited state, and NDIP oxidizes A and G via its triplet excited state, whereas NIP oxidizes only G. A combination of laser flash photolysis kinetic studies and quantitative HPLC analyses of photosensitized DNA damage was performed for several DNA sequences in the presence of Sens. NIN, NDIN, and NDIP, which oxidizes A, caused significant DNA damage upon photoirradiation, and DNA damage yield increased with the length of the consecutive A stretch. In contrast, NIP, which oxidizes only G, caused only moderate damage to DNA and showed no preference for the consecutive A sequences. These results clearly demonstrate the importance of A-oxidation, especially in consecutive A sequences, which triggers the rapid hole transfer between A's.

Luminescent metal-ligand complexes as probes of macromolecular interactions and biopolymer dynamics

The knowledge of microsecond dynamics is important for an understanding of the mechanism and function of biological systems. Fluorescent techniques are well established in biophysical studies, but their applicability to probe microsecond timescale processes is limited. Luminescent metal-ligand complexes (MLCs) have created interest mainly due to their unique luminescent properties, such as the exceptionally long decay times and large fundamental anisotropy values, allowing examination of microsecond dynamics by fluorescence methods. MLC properties also greatly simplify instrumentation requirements and enable the use of light emitting diode excitation for time-resolved measurements. Recent literature illustrates how MLC labels take full advantage of well developed fluorescence techniques and how those methods can be extended to timescales not easily accessible with nanosecond probes. MLCs are now commercially available as reactive labels which give researchers access to methods that previously required more complex approaches. The present paper gives an overview of the applications of MLC probes to studies of molecular dynamics and interactions of proteins, membranes and nucleic acids.

Photodissociation of Naphthalene Dimer Radical Cation during the Two-Color Two-Laser Flash Photolysis and Pulse Radiolysis−Laser Flash Photolysis

Photodissociation of naphthalene (Np) dimer radical cation (Np2*+) to give naphthalene radical cation (Np*+) and Np and the subsequent regeneration of Np2*+ by the dimerization of Np*+ and Np were directly observed during the two-color two-laser flash photolysis in solution at room temperature. When Np2*+ was excited at the charge-resonance (CR) band with the 1064-nm laser, the bleaching and recovery of the transient absorption at 570 and 1000 nm, assigned to the local excitation (LE) and CR bands of Np2*+, respectively, were observed together with the growth and decay of the transient absorption at 685 nm, assigned to Np*+. The dissociation of Np2*+ proceeds via a one-photon process within the 5-ns laser flash to give Np*+ and Np in the quantum yield of 3.2 x 10(-3) and in the chemical yield of 100%. The recovery time profiles of Np2*+ at 570 and 1000 nm were equivalent to the decay time profile of Np*+ at 685 nm, suggesting that the dimerization of Np*+ and Np occurs to regenerate Np2*+ in 100% yield. Similar experimental results of the photodissociation and regeneration of Np2*+ were observed during the pulse radiolysis-laser flash photolysis of Np in 1,2-dichloroethane. The photodissociation mechanism can be explained based on the crossing between two potential surfaces of the excited-state Np2*+ and ground-state Np*+.

Electron transfer processes in DNA: mechanisms, biological relevance and applications in DNA analytics

In principle, DNA-mediated charge transfer processes can be categorized as oxidative hole transfer and reductive electron transfer. With respect to the routes of DNA damage most of the past research has been focused on the investigation of oxidative hole transfer or transport. On the other hand, the transport or transfer of excess electrons has a large potential for biomedical applications, mainly for DNA chip technology.