Room temperature Q-band electron magnetic resonance study of radicals in X-ray-irradiated l-threonine single crystals

In the past, decennia radiation-induced radicals were successfully identified by electron magnetic resonance (EMR) in several solid-state amino acids and sugars. The authors present a room temperature (RT) EMR study of the stable radicals produced by X-ray-irradiation in the amino acid l-threonine (CH₃CH(OH)CH(NH₃ (+))COO(-)). Its chemical structure is similar to that of the well-known dosimetric material l-alanine (CH₃CH(NH₃(+))COO(-)), and radiation defects in l-threonine may straightforwardly be compared with the extensively studied l-alanine radicals. The hyperfine coupling tensors of three different radicals were determined at RT using electron nuclear double resonance. These results indicate that the two most abundant radicals share the same basic structure CH₃(•)C(OH)CH(NH₃(+))COO(-), obtained by H-abstraction, but are stabilised in slightly different conformations. The third radical is most probably obtained by deamination (CH₃CH(OH)(•)CHCOO(-)), similar in structure to the stable alanine radical.

Excess electron trapping in duplex DNA: long range transfer via stacked adenines

An understanding of charge transfer (CT) in DNA lies at the root of assessing the risks and benefits of exposure to ionizing radiation. Energy deposition by high-energy photons and fast-charged particles creates holes and excess electrons (EEs) in DNA, and the subsequent reactions determine the complexity of DNA damage and ultimately the risk of disease. Further interest in CT comes from the possibility that hole transfer, excess electron transfer (EET), or both in DNA might be used to develop nanoscale circuits. To study EET in DNA, EPR spectroscopy was used to determine the distribution of EE trapping by oligodeoxynucleotides irradiated and observed at 4 K. Our results indicate that stretches of consecutive adenine bases on the same strand serve as an ideal conduit for intrastrand EET in duplex DNA at 4 K. Specifically, we show that A is an efficient trap for EE at 4 K if, and only if, the A strand of the duplex does not contain one of the other three bases. If there is a T, C, or G on the A strand, then trapping occurs at T or C instead of A. This holds true for stretches up to 32 A's. Whereas T competes effectively against A for the EE, it does not compete effectively against C. Long stretches of T pass the majority of EE to C. Our results show that AT stretches channel EE to cytosine, an end point with significance to both radiation damage and the photochemical repair of pyrimidine dimers.

Sugar radical formation by a proton coupled hole transfer in 2'-deoxyguanosine radical cation (2'-dG*+): a theoretical treatment

Previous experimental and theoretical work has established that electronic excitation of a guanine cation radical in nucleosides or in DNA itself leads to sugar radical formation by deprotonation from the dexoxyribose sugar. In this work, we investigate a ground electronic state pathway for such sugar radical formation in a hydrated one electron oxidized 2'-deoxyguanosine (dG(*+) + 7H(2)O), using density functional theory (DFT) with the B3LYP functional and the 6-31G* basis set. We follow the stretching of the C(5')-H bond in dG(*+) to gain an understanding of the energy requirements to transfer the hole from the base to sugar ring and then to deprotonate to proton acceptor sites in solution and on the guanine ring. The geometries of reactant (dG(*+) + 7H(2)O), transition state (TS) for deprotonation of the C(5') site, and product (dG((*)C(5'), N(7)-H(+)) + 7H(2)O) were fully optimized. The zero point energy (ZPE) corrected activation energy (TS) for the proton transfer (PT) from C(5') is calculated to be 9.0 kcal/mol and is achieved by stretching the C(5')-H bond by 0.13 A from its equilibrium bond distance (1.099 A). Remarkably, this small bond stretch is sufficient to transfer the "hole" (positive charge and spin) from guanine to the C(5') site on the deoxyribose group. Beyond the TS, the proton (H(+)) spontaneously adds to water to form a hydronium ion (H(3)O(+)) as an intermediate. The proton subsequently transfers to the N(7) site of the guanine (product). The 9 kcal/mol barrier suggests slow thermal conversion of the cation radical to the sugar radical but also suggests that localized vibrational excitations would be sufficient to induce rapid sugar radical formation in DNA base cation radicals.

Influence of hydration on proton transfer in the guanine-cytosine radical cation (G*+-C) base pair: a density functional theory study

Upon one-electron oxidation, all molecules including DNA bases become more acidic in nature. For the GC base pair, experiments suggest that a facile proton transfer takes place in the G(*+)-C base pair from N(1) of G(*+) to N(3) of cytosine. This intrabase pair proton-transfer reaction has been extensively considered using theoretical methods for the gas phase, and it is predicted that the proton transfer is slightly unfavorable, in disagreement with experiment. In the present study, we consider the effect of the first hydration layer on the proton-transfer reaction in G(*+)-C by the use of density functional theory (DFT) using B3LYP/6-31+G** calculations of the G(*+)-C base pair in the presence of 6 and 11 water molecules. Under the influence of hydration of 11 waters, a facile proton transfer from N(1) of G(*+) to N(3) of C is predicted. The zero-point energy (ZPE)-corrected forward and backward energy barriers, for the proton transfer from N(1) of G(*+) to N(3) of C, was found to be 1.4 and 2.6 kcal/mol, respectively. The proton-transferred G(*)-(H(+))C + 11H(2)O was found to be 1.2 kcal/mol more stable than G(*+)-C + 11H(2)O, in agreement with experiment. The present calculation demonstrates that the inclusion of the first hydration shell around the G(*+)-C base pair has an important effect on the internal proton-transfer energetics.

Role of excited states in low-energy electron (LEE) induced strand breaks in DNA model systems: influence of aqueous environment

Low-energy electrons (LEEs) interact with a DNA model system to create a variety of excited states. In the gas phase, dissociative (sigma*) states are accessible by LEEs with energy <4 eV (see picture) and cause facile strand breaks through a dissociative electron attachment mechanism. However, under solvation these dissociative (sigma*) states are blue-shifted and are less accessible to LEEs.

On the chemical yield of base lesions, strand breaks, and clustered damage generated in plasmid DNA by the direct effect of X rays

The purpose of this study was to determine the yield of DNA base damages, deoxyribose damage, and clustered lesions due to the direct effects of ionizing radiation and to compare these with the yield of DNA trapped radicals measured previously in the same pUC18 plasmid. The plasmids were prepared as films hydrated in the range 2.5 < Gamma < 22.5 mol water/mol nucleotide. Single-strand breaks (SSBs) and double-strand breaks (DSBs) were detected by agarose gel electrophoresis. Specific types of base lesions were converted into SSBs and DSBs using the base-excision repair enzymes endonuclease III (Nth) and formamidopyrimidine-DNA glycosylase (Fpg). The yield of base damage detected by this method displayed a strikingly different dependence on the level of hydration (Gamma) compared with that for the yield of DNA trapped radicals; the former decreased by 3.2 times as Gamma was varied from 2.5 to 22.5 and the later increased by 2.4 times over the same range. To explain this divergence, we propose that SSB yields produced in plasmid DNA by the direct effect cannot be analyzed properly with a Poisson process that assumes an average of one strand break per plasmid and neglects the possibility of a single track producing multiple SSBs within a plasmid. The yields of DSBs, on the other hand, are consistent with changes in free radical trapping as a function of hydration. Consequently, the composition of these clusters could be quantified. Deoxyribose damage on each of the two opposing strands occurs with a yield of 3.5 +/- 0.5 nmol/J for fully hydrated pUC18, comparable to the yield of 4.1 +/- 0.9 nmol/J for DSBs derived from opposed damages in which at least one of the sites is a damaged base.

Q-band EPR and ENDOR of low temperature X-irradiated beta-D-fructose single crystals

Beta-D-fructose single crystals were in situ X-irradiated at 80 K and measured using electron paramagnetic resonance (EPR), electron nuclear double resonance (ENDOR) and ENDOR-induced EPR (EIE) techniques at Q-band (34 GHz) microwave frequencies. The measurements revealed the presence of at least four carbon-centered radicals stable at 80 K. By means of ENDOR angular variations in the three principal crystallographic planes, six proton hyperfine coupling tensors could be determined and were assigned to four different radicals by the aid of EIE. Two of the radicals exhibit only beta-proton hyperfine couplings and reveal almost identical EIE spectra. For the other two radicals, the major hyperfine splitting originates from a single alpha-proton hyperfine coupling and their EIE spectra were also quite similar. The similarity of the EIE spectra and hyperfine tensors led to the assumption that there are only two essentially different radical structures. The radical exhibiting only beta-proton hyperfine couplings was assigned to a C3 centered radical arising from H3 abstraction and the other radical suggested to be an open-ring species with a disrupted C2-C3 bond and a double C2-O2 bond. A possible formation mechanism for the latter open-ring radical is presented. By means of cluster density functional theory (DFT) calculations, the structures of the two radicals were determined and a fairly good agreement between the calculated and experimental hyperfine tensors was found.

Photo-induced hole transfer from base to sugar in DNA: relationship to primary radiation damage

This work presents the hypothesis that photo-excitation of G.+ in DNA and model systems results in the same electronic states expected from direct ionization of the sugar phosphate backbone and that these states lead to specific sugar radicals on the DNA sugar phosphate backbone. As evidence we show that visible photo-excitation of guanine cation radicals (G.+) in the dinucleoside phosphate TpdG results in high yields (about 85%) of deoxyribose sugar radicals at the C1' and C3' sites. Further, we have calculated transition energies of hole transfer from G.+ in TpdG using time-dependent density functional theory (TD-DFT) at the B3LYP/6-31G(d) level in gas phase as well as in a solvated environment. These calculations clearly predict that visible excitation of G.+ in TpdG causes transitions from only inner-shell filled molecular orbitals (MOs) to the singly occupied molecular orbital (SOMO) that effectively result in hole transfer from guanine either to the sugar phosphate backbone or to the adjacent base, thymine. The hole transfer is followed by rapid deprotonation from the sugar to form C1' and C3' radicals. These experimental and theoretical results are in agreement with our previously published experimental and theoretical results that photo-excitation of G.+ results in high yields of deoxyribose sugar radicals in DNA, guanine deoxyribonucleosides and deoxyribonucleotides. Photo-excitation of G.+ therefore provides a convenient method to produce and study sugar radicals that are expected to be formed in gamma-irradiated DNA systems unencumbered by the many other pathways involved in direct ionization.