Bifunctional photobinding of psoralen to single stranded nucleic acids.

Noncanonical G-C+ and A-T Hoogsteen base pairs can form in duplex DNA and play roles in recognition, damage repair, and replication. Identifying Hoogsteen base pairs in DNA duplexes remains challenging due to difficulties in resolving syn versus antipurine bases with X-ray crystallography; and size limitations and line broadening can make them difficult to characterize by NMR spectroscopy. Here, we show how infrared (IR) spectroscopy can identify G-C+ and A-T Hoogsteen base pairs in duplex DNA across a range of different structural contexts. The utility of IR-based detection of Hoogsteen base pairs is demonstrated by characterizing the first example of adjacent A-T and G-C+ Hoogsteen base pairs in a DNA duplex where severe broadening complicates detection with NMR.

Since life began on Earth, the four types of bases (A, G, C, and T(U)) that form two sets of base pairs have remained unchanged as the components of nucleic acids that replicate and transfer genetic information. Throughout evolution, except for the U to T modification, the four base structures have not changed. This constancy within the genetic code raises the question of how these complicated nucleotides were generated from the molecules in a primordial soup on the early Earth. At some prebiotic stage, the complementarity of base pairs might have accelerated the generation and accumulation of nucleotides or oligonucleotides. We have no clues whether one pair of nucleobases initially appeared on the early Earth during this process or a set of two base pairs appeared simultaneously. Recently, researchers have developed new artificial pairs of nucleobases (unnatural base pairs) that function alongside the natural base pairs. Some unnatural base pairs in duplex DNA can be efficiently and faithfully amplified in a polymerase chain reaction (PCR) using thermostable DNA polymerases. The addition of unnatural base pair systems could expand the genetic alphabet of DNA, thus providing a new mechanism for the generation novel biopolymers by the site-specific incorporation of functional components into nucleic acids and proteins. Furthermore, the process of unnatural base pair development might provide clues to the origin of the natural base pairs in a primordial soup on the early Earth. In this Account, we describe the development of three representative types of unnatural base pairs that function as a third pair of nucleobases in PCR and reconsider the origin of the natural nucleic acids. As researchers developing unnatural base pairs, they use repeated "proof of concept" experiments. As researchers design new base pairs, they improve the structures that function in PCR and eliminate those that do not. We expect that this process is similar to the one functioning in the chemical evolution and selection of the natural nucleobases. Interestingly, the initial structures designed by each research group were quite similar to those of the latest successful unnatural base pairs. In this regard, it is tempting to form a hypothesis that the base pairs on the primordial Earth, in which the natural purine bases, A and G, and pyrimidine bases, C and T(U), originated from structurally similar compounds, such as hypoxanthine for a purine base predecessor. Subsequently, the initial base pair evolved to the present two sets of base pairs via a keto-enol tautomerization of the initial compounds.

Solar simulation photodegradation of polystyrene: Phthalocyanine pigments as inhibitor of the photodegradation process

Processing and characterizations: Effect of PPG molecular weight on properties of phosphate based polyurethanes

The effect of low-temperature plasma on sterility, molecular, mechanical, and crystalline properties of poly (L-lactide), poly (L/D-lactide) and poly (L/DL-lactide) was investigated. Polymers were treated for 15 and 30 min at 100 W with nitrogen, argon, oxygen, and carbon dioxide plasma. All polymers treated with oxygen or carbon dioxide plasma were rendered sterile after 15 min of treatment. Only 70% of the samples treated under similar conditions with nitrogen or argon plasma were sterile. Extension of the exposure time to 30 min and increasing power to 200 W did not improve sterilization efficiency. Plasma sterilization, under the conditions used, caused no significant decrease or increase in overall molecular weight or polydispersity of the polylactides used. In most instances the effect of plasma sterilization was to slightly increase the overall molecular weight of the polymers studied. Treatment with argon plasma led to a more consistent increase in molecular weight than did treatment with nitrogen, oxygen, or carbon dioxide. Analysis of the surface (skin) of a poly(L-lactide) injection-molded rod following plasma sterilization indicated an increase in molecular weight as related to the interior (core) of the rod. Comparison of Mark-Houwink plots for the surface and interior of poly(L-lactide) injection-molded rods following plasma sterilization indicated an increase in chain branching for the surface relative to the interior of the rod. Generally the highly crystalline poly(L-lactide) was less susceptible to change upon plasma treatment than was the less crystalline poly(L/D-lactide) and poly(L/DL-lactide). The mechanical properties (shear strength, bending strength, and moduli) of the polylactides were not affected by plasma treatment. The overall melting temperature and the heat of melting of polylactides studied were not affected by plasma treatment. The melting temperature of the skin of the samples was about 1 degree C higher than the melting temperature of the core due to the chain orientation upon injection-molding. Plasma treatment of the polylactides reduced the melting temperature of the skin by 3 degrees C to 5 degrees C due to the crosslinking or branching at the surface layer.

Proton exchange and nuclear magnetic resonance spectroscopy are being used to characterize the kinetics and energetics of base-pair opening in two nucleic acid double helices. One is the RNA duplex 5'-r(GCGAUAAAAAGGCC)-3'/5'-r(GGCCUUUUUAUCGC)-3', which contains a central tract of five AU base pairs. The other is the homologous DNA duplex with a central tract of five AT base pairs. The rates and the equilibrium constants of the opening reaction of each base pair are measured from the dependence of the exchange rates of imino protons on ammonia concentration, at 10 °C. The results reveal that the tract of AU base pairs in the RNA duplex differs from the homologous tract of AT base pairs in DNA in several ways. The rates of opening of AU base pairs in RNA are high and increase progressively along the tract, reaching their largest values at the 3'-end of the tract. In contrast, the opening rates of AT base pairs in DNA are much lower than those of AU base pairs. Within the tract, the largest opening rate is observed for the AT base pair at the 5'-end of the tract. These differences in opening kinetics are paralleled by differences in the stabilities of individual base pairs. All AU base pairs in the RNA are less stable than the AT base pairs in the DNA. The presence of the tract enhances these differences by increasing the stability of AT base pairs in DNA while decreasing the stability of AU base pairs in RNA. Due to these divergent trends, along the tracts, the AU base pairs become progressively less stable than AT base pairs. These findings demonstrate that tracts of AU base pairs in RNA have specific dynamic and energetic signatures that distinguish them from similar tracts of AT base pairs in DNA.

Effects of solvent power on dynamic moduli of polydimethylsiloxane-treated fumed silica suspension gels

The conformation of poly(methyl methacrylate) adsorbed from dilute solution on nonporous silica was investigated by ESR method using three-component spectrum analysis. The fraction of the polymer segments in train, short loop, and long loop or tail, as well as the rotational correlation time for the segments were examined with regard to molecular weight (M=103–3×106), the degree of adsorption, and the particle size of silica. In CCl4, the saturation adsorption, As, increased from 6 to 16×10−8 g cm−2, the fraction of polymer segments in train, p, decreased from 0.9 to 0.4, and the segment mobility reduced with the increase in molecular weight, respectively. Remarkable changes in As and p were found in a range of molecular weight of 5×104. In benzene, the values of As and p were less dependent on molecular weight than the cases of adsorption in CCl4. Marked effects of intrachain interactions on the conformation were revealed for the adsorption of coiled polymers with high molecular weight from CCl4 solution at low degrees of adsorption, where the loop formation was observed for polymers of M>104. The intrachain force was attributed to overlapping among the segments. The difference in the adsorption behavior between the cases in CCl4 and benzene was interpreted by the difference in the degree of deformation of polymer molecules upon adsorption.

Attempts were made to apply atomic force microscopy (AFM) imaging to the detection and mapping of the sites of base substitutions in DNA molecules. In essence, DNA fragments to be examined for possible base substitutions were mixed with an equal amount of a corresponding DNA standard and subjected to heat denaturation and subsequent annealing. The reassociated DNA was incubated with MutS protein, a protein that recognizes and binds to mismatched base pairs in duplex DNA. Bound MutS protein molecules were then detected by AFM and their positions along the DNA molecules were determined by calculating the distance from one of the DNA termini, which had been tagged with a biotin-avidin complex. Base substitutions present in DNA molecules >1 kb were effectively detected by this procedure, and the positions determined were in good agreement with the actual mutation sites. This method is quite simple, has virtually no limitations on the size of DNA fragments to be examined and requires only a very small amount of DNA sample.

Nuclear magnetic resonance spectroscopy has been used to characterize opening reactions and stabilities of individual base pairs in two related DNA structures. The first is the triplex structure formed by the DNA 31-mer 5'-AGAGAGAACCCCTTCTCTCTTTTTCTCTCTT-3'. The structure belongs to the YRY (or parallel) family of triple helices. The second structure is the hairpin double helix formed by the DNA 20-mer 5'-AGAGAGAACCCCTTCTCTCT-3' and corresponds to the duplex part of the YRY triplex. The rates of exchange of imino protons with solvent in the two structures have been measured by magnetization transfer from water and by real-time exchange at 10 degrees C in 100 mM NaCl and 5 mM MgCl2 at pH 5.5 and in the presence of two exchange catalysts. The results indicate that the exchange of imino protons in protonated cytosines is most likely limited by the opening of Hoogsteen C+G base pairs. The base pair opening parameters estimated from imino proton exchange rates suggest that the stability of individual Hoogsteen base pairs in the DNA triplex is comparable to that of Watson-Crick base pairs in double-helical DNA. In the triplex structure, the exchange rates of imino protons in Watson-Crick base pairs are up to 5000-fold lower than those in double-helical DNA. This result suggests that formation of the triplex structure enhances the stability of Watson-Crick base pairs by up to 5 kcal/mol. This stabilization depends on the specific location of each triad in the triplex structure.

The structural dynamics of mismatched base pairs in duplex DNA have been studied by time-resolved fluorescence anisotropy decay measurements on a series of duplex oligodeoxynucleotides of the general type d[CGG(AP)GGC].d[GCCXCCG], where AP is the fluorescent adenine analogue 2-aminopurine and X = T, A, G, or C. The anisotropy decay is caused by internal rotations of AP within the duplex, which occur on the picosecond time scale, and by overall rotational diffusion of the duplex. The correlation time and angular range of internal rotation of AP vary among the series of AP.X mismatches, showing that the native DNA bases differ in their ability to influence the motion of AP. These differences are correlated with the strength of base-pairing interactions in the various AP.X mismatches. The interactions are strongest with X = T or C. The ability to discern differences in the strength of base-pairing interactions at a specific site in DNA by observing their effect on the dynamics of base motion is a novel aspect of the present study. The extent of AP stacking within the duplex is also determined in this study since it influences the excited-state quenching of AP. AP is thus shown to be extrahelical in the AP.G mismatch. The association state of the AP-containing oligodeoxynucleotide strand is determined from the temperature-dependent tumbling correlation time. An oligodeoxynucleotide triplex is formed with a particular base sequence in a pH-dependent manner.

1,3-Diaza-2-oxophenoxazine (X) has been introduced as a ligand in silver(I)-mediated base pairing in a parallel DNA duplex. This fluorescent cytosine analog is capable of forming stabilizing X-Ag(I)-X and X-Ag(I)-C base pairs in DNA duplexes, as confirmed by temperature-dependent UV spectroscopy and luminescence spectroscopy. DFT calculations of the silver(I)-mediated base pairs suggest the presence of a synergistic hydrogen bond. Molecular dynamics (MD) simulations of entire DNA duplexes nicely underline the geometrical flexibility of these base pairs, with the synergistic hydrogen bond facing either the major or the minor groove. Upon silver(I) binding to the X:X or X:C base pairs, the luminescence emission maximum experiences a red shift from 448 to 460nm upon excitation at 370nm. Importantly, the luminescence of the 1,3-diaza-2-oxophenoxazine ligand is not quenched significantly upon binding a silver(I) ion. In fact, the luminescence intensity even increases upon formation of a X-Ag(I)-C base pair, which is expected to be beneficial for the development of biosensors. As a consequence, the silver(I)-mediated phenoxazinone base pairs represent the first strongly fluorescent metal-mediated base pairs.

The ability of a triplex-forming oligonucleotide to recognize T-A and C-G base pairs in a DNA duplex is enhanced by incorporating N-acetyl-2,7-diaminoquinoline

In contrast to Watson-Crick (WC) base pairing, Hoogsteen (HG) base pairing involves flipping a purine base 180° between its anti and syn conformation. Recent studies have shown that HG pairs coexist in dynamical equilibrium, and several biological functions depend on them. This significance has stirred computational research on this base-pairing transition. However, a methodical reproduction of sequence variations has continued to be out of reach. It is becoming increasingly clear that Hoogsteen base pairs play a crucial role in DNA replication, recognition, damage repair, and incorrect sequence repair. The Protein Data Bank contains a variety of Hoogsteen base pairing modes that include the preference for A–T versus G–C bps, TA versus GG steps, and a preference for 5'-purines at terminal ends. RNA A-form duplexes are strongly disfavored by Hoogsteen base pairs, in stark contrast to B-form DNA. Therefore, N1-methyl adenosine and N1-methyl guanosine, which transpire in DNA as alkylation impairment and in RNA as posttranscriptional adjustments, have great differences in effects. They create G–C+ and A–U Hoogsteen base pairs in duplex DNA that preserve the structural integrity of the double helix, but obstruct base pairing altogether and induce local duplex melting in RNA, providing a mechanism for potently disrupting RNA structure through posttranscriptional modifications. In duplex DNA, they maintain the structural integrity of the double helix by creating G–C+ and A–U Hoogsteen base pairs, but block base pairing altogether and cause local duplex melting in RNA, thus providing a potent means for disrupting RNA structure post transcriptionally. As a result of the markedly different inclinations for B-DNA and A-RNA to form Hoogsteen base pairs, they may be able to balance the opposing demands of maintaining genome stability and dynamically modulating the epitranscriptome. This review examines the occurrence of Hoogsteen base pairs in DNA and RNA duplexes.

Hoogsteen Base Pairing in DNA vs RNA: Thermodynamics and Kinetics from Enhanced Sampling Simulation and Markov State Modeling