DNA damage by the direct effect of ionizing radiation: products produced by two sequential one-electron oxidations.

It has long been assumed that the population of radicals trapped in irradiated DNA (that is, the radicals escaping recombination) would quantitatively account for the lesions observed in DNA. Recent results indicate that this is not the case. The yield of DNA lesions exceed the yield of trappable radicals. To account for a portion of this shortfall, it is thought that some of the initially formed 2'-deoxyribose radicals undergo a second oxidation by nearby base cation radicals to form 2'-carbocations. The carbocations react to give strand breaks and free base release. Schemes are presented to account for the major oxidation products observed including 8-oxoGua, 8-oxoAde, 5-OHMeUra, and free base release. Theoretical calculations were performed to ascertain the likelihood of the second oxidation step in these reaction pathways actually occurring, and to account for base sequence dependence and various levels of hydration.

An unexpected copper catalyzed 'reduction' of an arylazide to amine through the formation of a nitrene intermediate.

Azido nitrobenzoxadiazole (NBD) was observed to undergo a 'reduction' reaction in the absence of an obvious reducing agent, leading to amine formation. In the presence of an excess amount of DMSO, a sulfoxide conjugate was also formed. The ratio of these two products was both temperature- and solvent-dependent, with the addition of water significantly enhancing the ratio of the 'reduction' product. Two intermediates of the azido-NBD reaction in DMSO were trapped and characterized by low-temperature EPR spectroscopy. One was an organic free radical (S=1/2) and another was a triplet nitrene (S=1) species. A mechanism was proposed based on the characterized free radical and triplet intermediates.

Role of calcium in metalloenzymes: effects of calcium removal on the axial ligation geometry and magnetic properties of the catalytic diheme center in MauG.

MauG is a diheme enzyme possessing a five-coordinate high-spin heme with an axial His ligand and a six-coordinate low-spin heme with His-Tyr axial ligation. A Ca(2+) ion is linked to the two hemes via hydrogen bond networks, and the enzyme activity depends on its presence. Removal of Ca(2+) altered the electron paramagnetic resonance (EPR) signals of each ferric heme such that the intensity of the high-spin heme was decreased and the low-spin heme was significantly broadened. Addition of Ca(2+) back to the sample restored the original EPR signals and enzyme activity. The molecular basis for this Ca(2+)-dependent behavior was studied by magnetic resonance and Mössbauer spectroscopy. The results show that in the Ca(2+)-depleted MauG the high-spin heme was converted to a low-spin heme and the original low-spin heme exhibited a change in the relative orientations of its two axial ligands. The properties of these two hemes are each different than those of the heme in native MauG and are now similar to each other. The EPR spectrum of Ca(2+)-free MauG appears to describe one set of low-spin ferric heme signals with a large g(max) and g anisotropy and a greatly altered spin relaxation property. Both EPR and Mössbauer spectroscopic results show that the two hemes are present as unusual highly rhombic low-spin hemes in Ca(2+)-depleted MauG, with a smaller orientation angle between the two axial ligand planes. These findings provide insight into the correlation of enzyme activity with the orientation of axial heme ligands and describe a role for the calcium ion in maintaining this structural orientation that is required for activity.

EPR, ENDOR, and DFT study of free radicals in L-lysine·HCl·2H2O single crystals X-irradiated at 298 K.

With K-band EPR (Electron Paramagnetic Resonance), ENDOR (Electron-Nuclear DOuble Resonance), and EIE (ENDOR-induced EPR) techniques, three free radicals (RI-RIII) in L-lysine hydrochloride dihydrate single crystals X-irradiated at 298 K were detected at 298 K, and six radicals (R1, R1', R2-R5) were detected if the temperature was lowered to 66 K from 298 K. R1 and RI dominated the central portion of the EPR at 66 and 298 K, respectively, and were identified as main chain deamination radicals, (-)OOCCH(CH(2))(4)(NH(3))(+). R1' was identified as a main chain deamination radical with the different configuration from R1 at 66 K, and it probably formed during cooling the temperature from 298 to 66 K. The configurations of R1, R1', and RI were analyzed with their coupling tensors. R2 and R3 each contain one α- and four ß-proton couplings and have very similar EIEs at three crystallographic axes. The two-layer ONIOM calculations (at B3LYP/6-31G(d,p):PM3) support that R2 and R3 are from different radicals: dehydrogenation at C4, (-)OOCCH(NH(3))(+)CH(2)CH(CH(2))(2)(NH(3))(+), and dehydrogenation at C5, (-)OOCCH(NH(3))(+)(CH(2))(2)CHCH(2)(NH(3))(+), respectively. The comparisons of the coupling tensors indicated that R2 (66 K) is the same radical as RII (298 K), and R3 is the same as RIII. Thus, RII and RIII also are the radicals of C4 and C5 dehydrogenation. R4 and R5 are minority radicals and were observed only when temperature was lowered to 66 K. R4 and R5 were only tentatively assigned as the side chain deamination radical, (-)OOCCH (NH(3))(+)(CH(2))(3)CH(2), and the radical dehydrogenation at C3, (-)OOCCH(NH(3))(+)CH(CH(2))(3)(NH(3))(+), respectively, although the evidence was indirect. From simulation of the EPR (B//a, 66 K), the concentrations of R1, R1', and R2-R5 were estimated as: R1, 50%; R1', 11%; R2, 14%; R3, 16%; R4, 6%; R5, 3%.

Primary oxidation products of 5-methylcytosine: methyl dynamics and environmental influences.

The primary oxidation product in X-irradiated single crystals of 5-methylcytosine hemihydrate and 5-methylcytosine hydrochloride has been studied at 10 K, using electron paramagnetic resonance (EPR), electron-nuclear double resonance (ENDOR), and ENDOR-induced EPR (EIE) spectroscopies. The radical is characterized by large couplings to the methyl protons and appears to be deprotonated at N1 in both crystal systems. In the hydrochloride crystal the methyl group is completely frozen at 10 K, whereas in the hemihydrate crystal it undergoes tunneling rotation. For the hemihydrate crystal, four ENDOR lines associated with transitions within the A and E rotational states were followed in three planes of rotation. Large ENDOR shifts as measured by saturation of the high- and low-field parts of the EPR spectrum indicate that the rotation is rather slow. Sidebands due to mixing of A and E rotational states are expected for slow rotation and were observed in both the EPR and the EIE spectra. The ENDOR shifts and the sideband frequencies indicate a tunneling splitting between 40 and 60 MHz. Estimates of the barrier to rotation in both crystalline systems were calculated using cluster and single-molecule density functional theory methods, and the results are consistent with those obtained by analysis of the experimental results.

Guanine radical reaction processes: a computational description of proton transfer in X-irradiated 9-ethylguanine single crystals.

Computational methods based on DFT procedures have been used to investigate proton-transfer processes in irradiated 9-ethylguanine crystals. Previous experimental results from X-irradiation and study of this system at 10 K found significant concentrations of two main products, R1, formed by N7-hydrogenation of the purine ring, and R2, the primary one-electron oxidation product (Jayatilaka, N.; Nelson, W. H. J. Phys. Chem. B 2007, 111, 7887). The objective of this work is to describe the processes leading to these products using computational methods that take into account molecular packing and bulk dielectric properties. The basic concept is that a proton will transfer following ionization if the net electronic energy of the system, consisting of the donor plus the acceptor plus any intervening molecules, becomes lower. Three approaches were used to investigate this concept, two based on energies computed for single molecules and one based on energies computed for two-molecule clusters arranged as in the crystals. The results are that the methods successfully predict the observed behavior, that it is energetically favorable on one-electron reduction for proton H1 to transfer from a neutral molecule to N7 of the neighbor, forming the N7-hydrogenated product, and that there is virtually no energy advantage for a proton to transfer upon one-electron oxidation. The results also support the proposal that the C8 H-addition radical, found only upon irradiation at 300 K, was the product of intramolecular transfer of the H7 proton to C8 in a process apparently requiring sufficient thermal energy for activation. Finally, the computations predict hyperfine couplings and tensors in very good agreement with those from experiment, thereby providing additional evidence for the success of the computations in describing the experimental observations.

Structure of radicals from X-irradiated guanine derivatives. 2. An experimental and computational study of 9-ethylguanine single crystals.

An EPR (electron paramagnetic resonance) and ENDOR (electron-nuclear double resonance) study of 9-ethylguanine crystals X-irradiated at 10 K detected evidence for three radical forms. Radical R1, characterized by three proton and two nitrogen hyperfine interactions, was identified as the product of net hydrogenation at N7 of the guanine unit. R1, which evidently formed by protonation of the primary electron addition product, exhibited an unusually distorted structure leading to net positive isotropic components of the alpha-coupling to the hydrogen attached to C8 of the guanine unit. Radical R2, characterized by two nitrogen and three proton hyperfine couplings, was identified as the primary electron loss product, *G+. Distinguishing between *G+ and its N1-deprotonated product is difficult because their couplings are so similar, and density functional theory (DFT) calculations were indispensable for doing so. The results for R2 provide the most complete ENDOR characterization of *G+ presented so far. Radical R3 exhibited a narrow EPR pattern but could not be identified. The identification of radicals R1 and R2 was supported by DFT calculations using the B3LYP/6-311+G(2df,p)//6-31+G(d,p) approach. Radical R4, detected after irradiation of the crystals at room temperature, was identified as the well-known product of net hydrogenation at C8 of the guanine component. Spectra from the room temperature irradiation contained evidence for R5, an additional radical that could not be identified. Radical concentrations from the low temperature irradiation were estimated as follows: R1, 20%; R2, 65%; R3, 15%.

Structure of radicals from X-irradiated guanine derivatives: an experimental and computational study of sodium guanosine dihydrate single crystals.

In sodium guanosine dihydrate single crystals, the guanine moiety is deprotonated at N1 due to growth from high-pH (>12) solutions. Electron paramagnetic resonance (EPR) and electron-nuclear double resonance (ENDOR) studies of crystals X-irradiated at 10 K detected evidence for three radical forms. Radical R1, characterized by two proton and two nitrogen hyperfine interactions, was identified as the product of net hydrogenation at N7 of the N1-deprotonated guanine unit. R1 exhibited an unusually distorted structure leading to net positive isotropic components of the hydrogen alpha-couplings. Radical R2, characterized by one proton and one nitrogen hyperfine coupling, was identified as the primary electron-loss product. This product is equivalent to that of deprotonation at N1 by the guanine cation and represents the first ENDOR characterization of that product. Radical R3, characterized by a single hydrogen hyperfine coupling, was identified as the product of net dehydrogenation at C1' of the ribose moiety. The identification of radicals R1-R3 was supported by density functional theory (DFT) calculations on several possible structures using the B3LYP/6-311G(2df,p)//6-31G(d,p) approach. Radical R4, detected after warming the crystals to room temperature, was identified as the well-known product of net hydrogenation of C8 of the (N1-deprotonated) guanine component. Radical R1, evidently formed by protonation of the primary electron addition product, was present as roughly 60% of the total radicals detected at 10 K. Radical R2 was present as roughly 27% of the total yield, and the concentration of R3 contributed the remaining 13%. R3 is evidently the product of one-electron oxidation followed by deprotonation; thus, the balance of oxidation and reduction products is approximately equal within experimental uncertainty.

Dose-response relationships for radicals trapped in irradiated solids.

This work develops a modified description of the dose-response relationships for radical production by ionizing radiation. The main new feature is incorporation of the concept of the target and the possibility that the population of targets can undergo depletion at increased doses. The resulting mathematical relationships are capable of describing the decrease in product yield at increasing doses as is sometime observed. In addition, the description preserves the general properties of the widely used relationships. Finally, the expressions provide the possibility for estimating the average mass of the target.

Radiation-induced hydroxyl addition to purine molecules: EPR and ENDOR study of hypoxanthine hydrochloride monohydrate single crystals.

Three radical species were detected in an EPR/ENDOR study of X-irradiated hypoxanthine.HCl.H2O single crystals at room temperature: RI was identified as the product of net H addition to C8, RII was identified as the product of net H addition to C2, and RIII was identified as the product of OH addition to C8. The observed set of radicals was the same for room-temperature irradiation as for irradiation at 10 K followed by warming the crystals to room temperature; however, the C2 H-addition and C8 OH-addition radicals were not detectable after storage of the crystals for about 2 months at room temperature. Use of selectively deuterated crystals permitted unique assignment of the observed hyperfine couplings, and results of density functional theory calculations on each of the radical structures were consistent with the experimental results. Comparison of these experimental results with others from previous crystal-based systems and model system computations provides insight into the mechanisms by which the biologically important purine C8 hydroxyl addition products are formed. The evidence from solid systems supports the mechanism of net water addition to one-electron oxidized purine bases and demonstrates the importance of a facial approach between the reactants.

Electronic g-factor measurement from ENDOR-induced EPR patterns: malonic acid and guanine hydrochloride dihydrate.

Measurement of electronic g-factors (g) from radicals in irradiated organic crystals is generally difficult because the overall EPR pattern is usually the composite of several components, e.g., from multiple radicals and from multiple magnetic sites. However, when an ENDOR line is fully resolved, the method of ENDOR-induced EPR (EI-EPR, or EIE) in principle permits identification of the EPR pattern from the individual component yielding the line. To examine this method as an approach useful for measuring g, we used it to measure those of known radicals in two different crystal systems. First, to verify correspondence of the EIE and EPR sufficient for using EIE patterns to extract g, we used both EIE and EPR to measure g of (*CH(COOH)(2) from irradiated crystals of malonic acid. Then, to illustrate the procedure applied to a system giving a more complex EPR pattern, we used EIE to measure g of the O6-protonated anion radical of guanine in irradiated guanine.HCl.2H(2)O crystals. EPR results from the malonic acid radical are g(max)=2.00374(2), g(mid)=2.00331(2), and g(min)=2.00234(3); EIE results from the same radical are g(max)=2.00375(2), g(mid)=2.00334(2), and g(min)=2.00238(2), where numbers in parentheses indicate statistical uncertainties in the respective least significant digits. In addition, eigenvectors from the two sets of measurements agree to approximately 1 degrees. Results from the guanine radical are g(max)=2.00490(2), g(mid)=2.00318(4), and g(min)=2.00218(4). (The uncertainties should reliably indicate relative accuracy, while absolute accuracy is within +/-0.0002 as indicated by simultaneous measurement of Cr(3+) in MgO.)

Lithium formate for EPR dosimetry: radiation-induced radical trapping at low temperatures.

Radiation-induced primary radicals in lithium formate. A material used in EPR dosimetry have been studied using electron paramagnetic resonance (EPR), electron nuclear double resonance (ENDOR) and ENDOR-Induced EPR (EIE) techniques. In this study, single crystals were X irradiated at 6-8 K and radical formation at these and higher temperatures were investigated. Periodic density functional theory calculations were used to assist in assigning the radical structures. Mainly two radicals are present at 6 K, the well-known CO2(•-) radical and a protonated electron-gain product. Hyperfine coupling tensors for proton and lithium interactions were obtained for these two radicals and show that the latter radical exists in four conformations with various degrees of bending at the radical center. Pairs of CO2(•-) radicals were also observed and the tensor for the electron-electron dipolar coupling was determined for the strongest coupled pair, which exhibited the largest spectral intensity. Upon warming, both the radical pairs and the reduction product decay, the latter apparently by a transient species. Above 200 K the EPR spectrum was mainly due to the CO2(•-) (mono) radicals, which were previously characterized as the dominant species present at room temperature and which account for the dosimetric EPR signal.

Free radicals in L-arginine x HCl x H2O single crystals X-irradiated at 66K- EPR, ENDOR, EIE and DFT studies.

X-irradiation of L-arginine hydrochloride monohydrate crystals at 66 K led to at least five radicals detectable with K-band Electron Paramagnetic Resonance (EPR), Electron-Nuclear DOuble Resonance (ENDOR) and ENDOR-induced EPR (EIE) techniques. Radicals R1a and R1b were identified as carboxyl-centered radicals from one-electron reduction, (H(2)OOC*)CH (NH(3))(+)(CH(2))(3)NHC(NH(2))(2)(+) in two different conformations arising from the two geometrically distinct molecules of the asymmetric unit in the crystal. Density-Functional Theory (DFT) calculations on cluster models constructed separately for each molecule of the asymmetric unit support the assignments. Radical R2 was identified as the decarboxylation radical, *CH(NH(3))(+)(CH(2))(3)NHC (NH(2))(2)(+). Radical R3, with two proton couplings and one nitrogen coupling, was identified as a radical with the unpaired electron localized on the guanidyl group, (-)(OOC)CH(NH(3))(+)(CH(2))(3)NHC*(NH(2))(2)(+). R3 is a product of one-electron reduction different from radicals R1a and R1b. DFT calculations on a cluster model reproduced the experimental values very well and thus supported the assignment of R3. Geometry optimization indicated that the guanidyl group transformed from planar to pyramidal upon trapping the electron. Radical R4 was identified as a side chain dehydrogenation radical, (-)(OOC)CH(NH(3))(+)(CH(2))(2)*CH NHC(NH(2))(2)(+). It was not possible to collect sufficient data to identify radical R5, although it clearly exhibited hyperfine coupling to one nonexchangeable beta-proton.

Radicals in 5-methylcytosine induced by ionizing radiation. Electron magnetic resonance for structural and mechanistic analyses.

Single crystals of 5-methylcytosine hemihydrate and 5-methylcytosine hydrochloride were X-irradiated and studied at 10 K and at higher temperatures using X- and K-band EPR, ENDOR and EIE spectroscopy. In the hemihydrate crystals, four radicals were identified at 10 K, one of them being the recently reported N1-deprotonated one-electron oxidation product (Krivokapic et al., J. Phys. Chem. A 113, 9633-9640, 2009). The other radicals were the 3alphaH radical and the C6 and C5 H-addition radicals (the 5-yl and 6-yl radicals, respectively). After irradiation at 295 K, only the 3alphaH and the 5-yl radicals were observed. In the hydrochloride crystals, at least seven different radicals were present after irradiation at 10 K. These were the N1-deprotonated one-electron oxidation product, the 3alphaH radical, three different one-electron reduction products, and the 5- and 6-yl radicals. DFT calculations were used to assist in assigning the observed couplings. The 3alphaH and 5-yl radicals were dominant after thermal annealing to room temperature. In neither crystal system did the N1-deprotonated oxidation product transform into the 3alphaH radical upon warming. The radical yield was significantly greater after irradiation at 300 K compared to that after irradiation at 10 K followed by warming to 300 K and was also considerably greater in the hydrochloride crystals than in the hemihydrate crystals.

EPR and ENDOR study of radiation-induced radical formation in purines: sodium inosine crystals X-irradiated at 10 K.

X-irradiated single crystals of sodium inosine (Na(+)*Inosine(-)*2.5H(2)O), in which the hypoxanthine base is present as the N1-deprotonated anion, were investigated using K-band (24 GHz) electron paramagnetic resonance (EPR), electron-nuclear double resonance (ENDOR), and ENDOR induced EPR (EIE) techniques at 10 K. At least five different radicals were present immediately after irradiation at 10 K. R1, which decayed upon warming the crystals to 50 K, was identified as the electron-loss product of the parent N1-deprotonated hypoxanthine base. Hyperfine couplings to HC8 and HC2 were fully characterized with ENDOR spectroscopy, and the identification was supported by DFT calculations. R2, which also decayed on warming to 50 K, exhibited nearly equal couplings to HC2 and HC8. Taken in combination with an extensive set of DFT calculations, the experimental results indicate that R2 is the (doubly negative) product of electron-gain by the initially anionic N1-deprotonated hypoxanthine parent. R3, which exhibited hyperfine coupling only to HC8 could not be identified. R4, which persisted on annealing to 260 K, exhibited one large alpha-proton hyperfine coupling which was fully characterized by ENDOR. Based on DFT calculations and the experimental data, R4 was identified as the product of net H-abstraction from C5'. The remaining HC5' was the source of the measured alpha-proton coupling. R5, present at low temperature and the only observable radical after warming the crystals to room temperature, was identified as the C8-H addition radical. The alpha-coupling to HC2 and beta-couplings to the pair of C8 methlyene protons were fully characterized by ENDOR.

Electron transfer in amino acid.nucleic acid base complexes: EPR, ENDOR, and DFT study of X-irradiated N-formylglycine.cytosine complex crystals.

Single crystals of the 1:1 complex of the nucleic acid base cytosine and the dipeptide N-formylglycine (C.NFG) have been irradiated at 10 and 273 K to doses of about 70 kGy and studied at temperatures between 10 and 293 K using 24 GHz (K-band) and 9.5 GHz (X-band) electron paramagnetic resonance (EPR), electron nuclear double resonance (ENDOR), and ENDOR-induced EPR (EIE) spectroscopy. In this complex, the cytosine base is hydrogen bonded at positions N3 and N4 to the carboxylic group of the dipeptide, and the N3 position of cytosine has become protonated by the carboxylic group. At 10 K, two major radicals were characterized and identified. One of these (R1) is ascribed to the decarboxylated N-formylglycine one-electron oxidized species. The other (R2) is the N3-protonated cytosine one-electron reduced species. A third minority species (R3) appears to be a different conformation or protonation state of the one-electron reduced cytosine radical. Upon warming, the R2 and R3 radicals decay at about 100 K, and at 295 K, the only cytosine-centered radicals present are the C5 and C6 H-addition radicals (R5, R6). The R1 radical decays at about 150 K, and a glycine backbone radical (R4) grows in slowly. Thus, in the complex, a complete separation of initial oxidation and reduction events occurs, with oxidation localized at the dipeptide moiety, whereas reduction occurs at the nucleic acid base moiety. DFT calculations indicate that this separation is driven by large differences in electron affinities and ionization potentials between the two constituents of the complex. Once the initial oxidation and reduction products are trapped, no further electron transfer between the two constituents of the complex takes place.

EPR and ENDOR study of radiation-induced radical formation in purines: hypoxanthine hydrochloride monohydrate crystals X-irradiated at 10 K.

Electron paramagnetic resonance (EPR) and electron-nuclear double resonance (ENDOR) study of hypoxanthine.HCl.H(2)O crystals irradiated at low temperatures (10 K) identified three radical species. In these crystals, the parent molecules exist in a cationic form with a proton at N7. R1 was the product of net hydrogen addition to N3 and exhibited alpha-proton hyperfine couplings to HC2, HN1, HC8, and HN3. The coupling to HC2 has an isotropic component smaller than usual, evidently an indication that the bonds to C2 are nonplanar. R2 was the product of net hydrogen loss from N7, equivalent to the one-electron oxidation product of neutral hypoxanthine, and exhibited alpha-proton hyperfine couplings to HC2 and HC8. Both couplings are characteristic of planar bonding arrangements at the centers of spin. R3 was provisionally identified as the product of net hydrogen addition to O6 and exhibited hyperfine alpha-proton couplings to HC8 and NH1. To identify the set of radicals, the experiments employed four crystal types: normal, deuterated only at NH positions, deuterated at HC8 and NH positions, and deuterated at HC8 only. The low-temperature data also showed clear evidence for H/D isotope effects in formation and/or stabilization of all radicals. To aid and support the identifications, the experimental results were compared to DFT calculations performed on a variety of radical structures plausible for the parent molecule and molecular packing within the crystal.