Radiation-induced free radicals in solid 5-halouracil derivatives: single crystals of 5-iododeoxyuridine

X-irradiation of single crystals of 5-iododeoxyuridine (IUdR) in the temperature range 8-300 K produces mainly four different radicals which have been studied by electron spin resonance (e.s.r.) and electron nuclear double resonance (ENDOR)-spectroscopy. At low temperatures, a pi-anion is formed which shows predominantly an interaction of the unpaired electron with a proton at carbon C6 of the base (-11.8 G, -23.9 G, -4.6 G). Above 10-20 K, the anion protonates at C6 to yield a RC-I(CH2)-R' radical comprising alpha-iodo and beta-methylene proton hyperfine interactions. The primary oxidation product is an O5'-situated alkoxy radical RCH2O which shows inequivalent beta-proton couplings of about 100 G and 35 G together with a highly anisotropic g-tensor. Upon warming to 265 K, a C2'-located radical on the deoxyribose is formed which is stable at room temperature. A detailed account of its spectral features as obtained by ENDOR exhibits three different alpha-type couplings, two small beta-protons and a dipolar interaction. Other radicals, not reproducibly observed, involve a C5'-hydroxyalkyl radical and a species related to the base cation at low temperatures.     

EPR and ENDOR study of crystalline cytosine x HCl doped with 5-methylcytosine. Radiation-induced radical formation and hole transfer

Radical formation and hole transfer were investigated in crystals of cytosine.HCl (C.HCl) doped with 0-1.1 mol-% 5-methylcytosine x HCl (5MC x HCl). The doping level was determined by NMR spectroscopy. Crystals and polycrystalline samples were X-irradiated at 295 K, 77 K and 12 K and studied with EPR, ENDOR and FSE spectroscopy at these temperatures. At 295 K the dominant radicals were the so-called 3alphaH radical, formed in 5MC by a net H-abstraction from the methyl group, and the cytosine C6 H-addition (5-yl) radical. At 12 K five radicals were identified. These were the 3alphaH radical, cytosine reduction and oxidation products, and the cytosine C6 and C5 H-addition (5-yl and 6-yl, respectively) radicals. The spectroscopic parameters for the 3alphaH radical are very similar to those of a radical observed previously in the crystalline cytosine derivatives cytidine (CR), 2'deoxycytidine hydrochloride (CdR x HCl), 5'dCMP and 3'CMP as well as in the uracil derivative 2-thiouracil (2-TU). It was shown that amounts of the order of tenths of a percent 5MC x HCl doped into crystals of C.HCl give rise to a considerable yield of 3alphaH radicals after exposure to ionizing radiation both at room temperature and at lower temperatures. This supports a previous suggestion that naturally occurring 5-methylated cytosine impurities may be responsible for the formation of 3alphaH radicals in the crystalline cytosine derivatives CR, CdR.HCl, 5'dCMP and 3'CMP and suggests that the 3alphaH radical in these systems is a 5-methylated base-centered radical. The total radical yield in doped C x HCl crystals increased considerably with the doping level, both at low temperatures and at room temperature, implying that the 3alphaH radical is more stable than the primary cytosine radicals. The relative amounts of the 3alphaH radical were obtained by using simulated benchmark spectra to reconstruct experimental EPR spectra of doped polycrystalline samples. Evidence is presented suggesting that the enhanced yield of the 3alphaH radical in doped samples is due to holes originally formed at cytosine bases and transferred to 5-methylcytosine bases in addition to the 3alphaH radical being less exposed to recombination than other cytosine radicals.     

Free radical formation in X-irradiated anhydrous crystals of inosine studied by EPR and ENDOR spectroscopy.

Single crystals of anhydrous inosine were studied subsequent to exposure to high and low doses of X radiation at 10 K using K-band, EPR, ENDOR, and field-swept-ENDOR (FSE) techniques. Immediately following high radiation doses at 10 K at least eight different radicals, RI-RVIII, were observed. All radicals, except for RVIII, were also observed at low doses, but the relative yields varied with the radiation doses. RI, which decayed with no observable successor at about 65 K, has magnetic characteristics similar to those expected for the hypoxanthine base cation. RII, the dominating radical at low radiation doses, exhibits only one hyperfine coupling amenable for ENDOR analysis. From the nature of this coupling and the EPR and FSE characteristics of the resonance, it is suggested that RII is formed by addition of a neighbor sugar fragment to the C2 position of a hypoxanthine base, forming a C2-O5'-C5' ester bond. RII is unstable and decayed at about 60 K without any detectable successor. RIII and RIV are the C2 and C8 H-addition radicals, respectively. These species are formed in minor amounts after irradiation at low temperatures, and they are the only observable radicals left at room temperature. Two sugar-centered radicals, RV and RVI, are formed by net H-abstraction from the C4' and C5' positions, respectively. These radicals dominate the EPR spectra after high radiation doses at low temperatures. A transformation from RV into RIII, the C2 H-adduct, started at about 80 K. Similarly, a transformation of RVI into RIV started at about 210 K. Several minor species were analyzed. RVII is characterized by an alpha-coupling due to 26% spin density at C8, and RVIII is characterized by 12% pi-spin density at N1. Possible structures for these radicals are discussed.     

Free radical formation in single crystals of 2'-deoxyguanosine 5'-monophosphate tetrahydrate disodium salt: an EPR/ENDOR study.

Single crystals of 2'-deoxyguanosine 5'-monophosphate were X-irradiated at 10 K and at 65 K, receiving doses between 4.5 and 200 kGy, and studied using K-band EPR, ENDOR, and field-swept ENDOR (FSE) spectroscopy. Evidence for five base-centered and more than nine sugar-centered radicals was found at 10 K following high radiation doses. The base-centered radicals were the charged anion, the N10-deprotonated cation, the C8 H-addition radical, a C5 H-addition radical, and finally a stable radical so far unidentified but with parameters similar to those expected for the charged cation. The sugar-centered radicals were the H-abstraction radicals centered at C1', C2', C3', and C5', an alkoxy radical centered at O3', a C5'-centered radical in which the C5'-O5' phosphoester bond appears to be ruptured, a radical tentatively assigned to a C4'-centered radical involving a sugar-ring opening, as well as several additional unidentified sugar radicals. Most radicals were formed regardless of radiation doses. All radicals formed following low doses (4.5-9 kGy) were also observed subsequent to high doses (100-200 kGy). The relative amount of some of the radicals was dose dependent, with base radicals dominating at low doses, and a larger relative yield of sugar radicals at high doses. Above 200 K a transformation from a sugar radical into a base radical occurred. Few other radical transformations were observed. In the discussion of primary radicals fromed in DNA, the presence of sugar-centered radicals has been dismissed since they are not apparent in the EPR spectra. The present data illustrate how radicals barely traceable in the EPR spectra may be identified due to strong ENDOR resonances. Also, the observation of a stable radical with parameters similar to those expected for the charge guanine cation is interesting with regard to the nature of the primary radicals stabilized in X-irradiated DNA.     

ESR/ENDOR study of guanosine 5'-monophosphate (free acid) single crystals X-irradiated at 10 K

Single crystals of the free base of guanosine 5'-monophosphate were X-irradiated at 10 and at 65 K and investigated between these temperatures and room temperature using K-band ESR and ENDOR spectroscopy. Three free radicals were detected in this temperature range. Two of these were identified as the O6-protonated anion radical and the C8 H-addition radical. Both of these species were present immediately after irradiation at 10 K. The anion radical was formed in two slightly different conformations, of which one decayed at about 150 K and the second at about 250 K. No successor radicals could be detected following the decay of the anion radical. The C8 H-adduct was stable at all temperatures used. The use of partially deuterated crystals confirmed the assignments made and showed that the main pathway for the formation of the C8 H-adduct consisted of addition of a proton from an easily exchangeable site. It is suggested that the C8 H-adduct is formed subsequent to a primary oxidation event localized either at the guanine base or at a nearby water of crystallization. Possible mechanisms for the formation of this product are discussed.     

Free radical formation in crystals of guanine hydrochloride dihydrate: an ESR and ENDOR study

Radiation-induced free radical formation in single crystals of guanine hydrochloride dihydrate has been studied at temperatures between 20 and 300 K using ESR and ENDOR spectroscopy. At low temperatures three radical species are trapped. Two of these are the C8 H-addition radical R1 previously analysed by Alexander and Gordy (1967) and the O6-protonated anion radical R2. The third species (R4) remains unidentified. Upon annealing at 280 K for an extended period the protonated anion R2 transforms into a new radical R3 which exhibit a well-defined hyperfine pattern but still could not be identified unambiguously. Also radical R4 probably transforms into a new radical (R5) upon such treatment. One proton coupling due to R5 was detected. A scheme of radical reactions incorporating these five radicals is proposed. This scheme also suggests that differences in radical formation between the monohydrate and dihydrate crystals of guanine hydrochloride depends upon differences in the hydrogen bonding network.     

The structure of the guanine cation: ESR/ENDOR of cyclic guanosine monophosphate single crystals after X irradiation at 10 K.

Following X irradiation of 3',5'-cyclic guanosine monophosphate single crystals at 10 K, several free radicals were trapped and detected by ESR/ENDOR/FSE spectroscopy. The two dominant species both have unpaired spin located on the guanine base. One is the product of net hydrogen atom loss from the exocyclic amino group. The spectroscopic characteristics of this resonance leave this assignment unambiguous. The experimental conditions make it likely that this species was formed by deprotonation of the guanine base cation. The nature of the other species is more uncertain. However, the evidence is consistent with the assignment that it is a net OH adduct to the C4 position of the base. Several species in which the unpaired spin was located on the sugar-phosphate region of the molecule were also observed. The mechanisms for the decay of the primary radicals, also leading to the well-known C8 hydrogen addition radical of the guanine base, are described and discussed.     

ENDOR-assisted study of the stable EPR spectrum of X-irradiated alpha-L-sorbose single crystals: MLCFA and simulation decomposition analyses

After X irradiation of single crystals of alpha-L-sorbose at 295 K, previous electron paramagnetic resonance (EPR), electron nuclear double resonance (ENDOR), and ENDOR-induced EPR (EI-EPR) results have indicated the formation of at least 10 different free radicals, and also that conceivably each carbon in the pyranose ring is a possible radical center. The radicals appear to be formed mostly by net H-abstraction reactions followed by standard elimination (e.g. beta-OH elimination) reactions or proton shifts, in turn leading to ring opening and fragmentation. In the present work, EPR spectra were recorded at room temperature with the external magnetic field along each of the three crystallographic axes subsequent to careful annealing at different temperatures using a high-temperature cavity. Each of the three sets of spectra was subjected to a maximum likelihood common factor analysis (MLCFA) that contributed to a better understanding of the spectral decays. Furthermore, the most stable spectra were simulated by optimization of previous ENDOR and EI-EPR results. The optimized EPR parameters resulted in excellent simulations of the experimental stable sorbose spectra and hence provided an improved insight of their spectral compositions.     

Radical formation in X-irradiated single crystals of guanine hydrochloride monohydrate. II. ESR and ENDOR in the range 10-77 K

In a study of guanine.HCl.H2O (Gm) single crystals X-irradiated at temperatures between 10 and 77 K, three radical species were found and characterized by ESR and ENDOR spectroscopy. All three are primary products in that they were present immediately following irradiation at T less than 10 K. Radical I, which apparently can exist in two slightly different conformations, was identified as the product of electron gain by the parent molecule and subsequent protonation at O6. Radical I decayed only after warming the crystals beyond 250 K. Radical II was the guanine cation previously reported (D. M. Close, E. Sagstuen, and W. H. Nelson, J. Chem. Phys. 82, 4386 (1985)); however, ENDOR data are reported here which confirm the previous results. The guanine cation in Gm resulted from electron loss from the parent and subsequent deprotonation at N7. It is proposed that Radical III results from OH attack at C8 of the parent molecule, followed by rupture of the C8-N9 bond and ring opening. The OH radicals thought to produce Radical III result from electron loss by the cocrystallized water molecules. The reaction leading to Radical III, unusual in solid-state radiation chemistry, is thought to be mediated by the specific hydrogen bonding network in this crystal.     

Free radicals from X-irradiated single crystals of uridine-5'-phosphate disodium salt

X-irradiation of single crystals of uridine-5'-phosphate (disodium salt) between 10 and 300 K as well as storage of irradiated crystals at 300 K produces at least seven different radical species. Between 10 and 77 K, the uracil base anion and a secondary alkoxy radical at the ribose-O3'-site are formed. The latter transforms into a C5'-centred alkylphosphate species between 110 and 130 K which in turn decays between 180 and 220 K under formation of a base 5-yl hydrogen addition radical. Irradiation at 300 K additionally produces the base-located 6-yl radical together with a radical tentatively assigned to the doubly protonated base anion. Storage of crystals for several months results in decay of most of these species leaving a radical possibly located at c5' of the ribose. The spectral parameters of these radicals are given and discussed.     

Free radicals in pyrimidines:single crystals of dihydro-6-methyl uracil irradiated and observed at 77 K.

Electron-spin-resonance measurements have been made on single crystals of dihydro-6-methyl uracil, which were irradiated by 4-0 MeV electrons at 77 K. At low temperature, four radicals have been identified. Two, the C5 and C6 hydrogen abstraction radicals, were also studied in a previous work. On exposure of U.V., the C6 abstraction radical was found to convert into the C5 abstraction radical. Annealing at room temperature reversed the process. The other radicals identified are that formed after H-atom addition to O4, and that formed after H-atom abstractions from N1, C5, and C6. The latter was not present in deuterated crystals. Both radicals were found to be unstable at intermediate temperatures. Thermoluminescence glow-curves were found to correlate to the formation and the decay of these radicals. Semi-empirical INDO MO-calculations have been performed for identification purposes.     

E.S.R. of spin-trapped radicals in gamma-irradiated polycrystalline nucleic acid constituents and their halogenated derivatives

Free radicals in gamma-irradiated polycrystalline nucleic acid constituents and their 5-halogenated derivatives have been studied by e.s.r. and spin-trapping. After gamma-irradiation at room temperature, the polycrystalline samples were dissolved in aqueous solutions of t-nitrosobutane (tNB) in the absence or presence of oxygen. For many of the nucleic acid constituents, two types of radicals, -C(5)RH-C(6)H- and -C(5)R-C(6)H2-, formed by H-addition to the double bond [-C(5)R=C(6)H-] of the base, were observed, where R is -CH3 or -H. In addition, radicals formed on the sugar moiety were found for some nucleosides. When oxygen was present in the tNB solution, the relative stability of trapped radicals was changed, and thus the presence of more than one radical species could be established. For halogenated bases, the radical produced by H-abstraction from N(1) was observed, and an additional radical species formed by H-addition to the C(6) position was found for 5-fluorouracil. For halogenated nucleosides, the same spectrum was observed in all compounds except the 5-fluoroderivatives, and was assigned to the radicals produced on the sugar moiety. For 5-fluorodeoxyuridine and 5-fluorouridine, the radical formed by H-addition to the C(6) position of the base was observed. In general, the present results are in good agreement with those of previous single crystal studies, but in the case of halogenated compounds other than the 5-fluoroderivatives, it was not possible to spin-trap the alpha-halo radicals which were the most prominent radicals formed from gamma-irradiation of single crystals at room temperature.     

Radical formation in salts of pyrimidines III. Cytosine . H2O cyrstals.

The radicals produced by X-irradiation at 77 K and at 300 K in cytosine monohydrate crystals have been analysed by electron-spin-resonance (e.s.r.) spectroscopy. Three radicals have been identified at 77 K: the anion radical and the cation radical of the cytosine molecule, together with the radical resutling from H-abstraction from the nitrogen N1. Irradiation at 300 K produces radicals resulting from H-adition at three different positions of the cytosine molecule. These are the C5-addition radical, the C6-addition radical, and the O2-addition radical. The results are compared with those found previously by other authors.     

Ionization of adenine derivatives: EPR and ENDOR studies of X-irradiated adenine.HCl.1/2H2O and adenosine.HCl.

Following X irradiation of adenine.HCl.H2O at 10 K, evidence for five distinct radical products was present in the EPR/ENDOR. (In both adenine.HCl.1/2H2O and adenosine.HCl, the adenine base is present in a cationic form as it is protonated at N1). From ENDOR data, radical R1, stable at temperatures up to 250 K, was identified as the product of net hydrogen loss from N1. This product, evidently formed by electron loss followed by proton loss, is equivalent to the radical cation of the neutral adenine base. Radical R2, unstable at temperatures above 60 K, was identified as the product of net hydrogen addition to N3, and evidently formed by electron addition followed by proton addition. Radicals R3-R5 could not be identified with certainty. Similar treatment of adenosine.HCl provided evidence for six identifiable radical products. Radical R6, stable to ca. 150 K, was identified as the result of net hydrogen loss from the amino group, and evidently was the product of electron loss followed by proton loss. Radical R7 was tentatively identified as the product of net hydrogen addition to C4 of the adenine base. Radical R8 was found to be the product of net hydrogen addition to C2 of the adenine base, and R9 was the product of net hydrogen addition to C8. Radical R10 was identified as the product of net hydrogen abstraction from C1' of the ribose, and R11 was an alkoxy radical formed from the ribose. With the exception of R11, all products were also found following irradiation at 65 K. Only radical R8 and R9 were stable at room temperature. Most notable is the different deprotonation behavior of the primary electron-loss products (radical R1 vs. R6) and the different protonation behavior of the primary electron-gain products (radical R2 vs. no similar product in adenosine.HCl). The major structural difference in the two crystals is the electrostatic environment of the adenine base. Therefore, this study provides further evidence that environmental influences are important in determining proton transfer processes.     

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.     

Free radical formation in X-irradiated crystals of 2'-deoxycytidine hydrochloride. Electron magnetic resonance studies at 10 K

Single crystals of deoxycytidine hydrochloride (CdR.HCl) have been X-irradiated at 10 K with doses up to about 150 kGy and studied using 24 GHz (K-band) EPR, ENDOR and FSE spectroscopy. In this system, the cytosine base is protonated at the N3 position. Nine different radicals were characterized and identified. Three of these are ascribed to three versions of the one-electron reduced species, probably differing in their protonation state. Radicals formed by net hydrogen addition to the cytosine C5 and C6 positions were observed at 10 K. The hydrogen-abstraction radical at the deoxyribose C1' position most probably results from initial oxidation of the base. The remaining radical species are all localized to the sugar moiety, representing products formed by net hydrogen abstraction from three of the five available carbons of the deoxyribose sugar. The lack of base-centered oxidation products as well as the structures of the one-electron reduced species is rationalized by considering the specific proton donor-acceptor properties of this crystalline lattice in comparison with similar systems.     

ESR and ENDOR study of adenosine single crystals X-irradiated at 10 K

Single crystals of adenosine were X-irradiated at 10 K and investigated between 10 and 300 K using K-band ESR and ENDOR spectroscopy. Two free radicals were analyzed. Radical I exhibits small hyperfine couplings to the C8-H, C2-H, and a N3-H protons, and was identified as the N3 protonated base anion radical. Radical II exhibits small hyperfine couplings to a C8-H and an exocyclic -N10-H proton. It is suggested that this is therefore the N10 deprotonated base cation radical. Enough data were not available to analyze a third primary radical believed to be located on the ribose moiety. Upon warming Radical I decays at ca. 40 K with no apparent successor. Likewise, no successor was identified for Radical II, which decays at ca. 100 K. At ca. 200 K there is ESR evidence for the C2 and C8 H-addition radicals. Their precursors have not been identified.     

Studies of electrons trapped in X-irradiated rhamnose crystals

The electrons trapped in single crystals of rhamnose X-irradiated at low temperature were studied by ENDOR spectroscopy. Hyperfine couplings of protons in the environs of the electron have been determined from ENDOR measurements, including those of some of the more remote carbon-bound hydrogen atoms. The likely site of electron trapping in the crystal structure of rhamnose was inferred from calculations of the electric potential generated by the dipoles of hydroxy groups about preexisting void spaces. Electron-proton distances for nonexchangeable hydrogen atoms from points within the void were calculated from the crystal structure and compared with distances obtained from hyperfine couplings. Good agreement was obtained between experimental and calculated values.     

Radical formation in single crystals of hypoxanthine.HCl.H2O, inosine, and the disodium salt of 5'-inosine-monophosphate.

Radical formation in single crystals of hypoxanthine.HCl.H2O, inosine and Na2-5'-IMP.(7.5 H2O) by X-irradiation has been studied using electron-spin-resonance spectroscopy at 9.5 and 35 GHz. In all crystals both H-addition radicals at position C2 and C8 of the purine ring are found. The coupling constants of these two radicals are different and depend strongly on the protonation state of the base. INDO-calculations indicate that the C8-radical is protonated at O6. In Na2-5'-IMP OH-addition radicals at position C2 of the purine ring are formed. Electron adduct radicals are found in the neutral and the N7-protonated base after X-irradiation at 77 K. In Na2-5'-IMP no electron adduct is formed but a radical which probably is the cation. In hypoxanthine.HCl.H2O a radical could be observed after X-irradiation at 77 K, which results from addition of a Cl- to the nitrogen N1.