Schonland ambiguity in the electron nuclear double resonance analysis of hyperfine interactions: principles and practice.

For the analysis of the angular dependence of electron paramagnetic resonance (EPR) spectra of low-symmetry centres with S=1/2 in three independent planes, it is well-established-but often overlooked-that an ambiguity may arise in the best-fit g<--> tensor result. We investigate here whether a corresponding ambiguity also arises when determining the hyperfine coupling (HFC) A<--> tensor for nuclei with I=1/2 from angular dependent electron nuclear double resonance (ENDOR) measurements. It is shown via a perturbation treatment that for each set of M(S) ENDOR branches two best-fit A<--> tensors can be derived, but in general only one unique solution simultaneously fits both. The ambiguity thus only arises when experimental data of only one M(S) multiplet are used in analysis or in certain limiting cases. It is important to realise that the ambiguity occurs in the ENDOR frequencies and therefore the other best-fit result for an ENDOR determined A<--> tensor depends on various details of the ENDOR experiment: the M(S) state of the fitted transitions, the microwave frequency (or static magnetic field) in the ENDOR measurements and the rotation planes in which data have been collected. The results are of particular importance in the identification of radicals based on comparison of theoretical predictions of HFCs with published literature data. A procedure for obtaining the other best-fit result for an ENDOR determined A<--> tensor is outlined.

Identification and conformational study of stable radiation-induced defects in sucrose single crystals using density functional theory calculations of electron magnetic resonance parameters.

One of the major stable radiation-induced radicals in sucrose single crystals (radical T2) has been identified by means of density functional theory (DFT) calculations of electron magnetic resonance parameters. The radical is formed by a net glycosidic bond cleavage, giving rise to a glucose-centered radical with the major part of the spin density residing at the C 1 carbon atom. A concerted formation of a carbonyl group at the C 2 carbon accounts for the relatively small spin density at C 1 and the enhanced g factor anisotropy of the radical, both well-known properties of this radical from several previous experimental investigations. The experimentally determined and DFT calculated proton hyperfine coupling tensors agree very well on all accounts. The influence of the exact geometrical configuration of the radical and its environment on the tensors is explored in an attempt to explain the occurrence and characteristics of radical T3, another major species that is most likely another conformation of T2. No definitive conclusions with regard to the actual structure of T3 could be arrived at from this study. However, the results indicate that, most likely, T3 is identical in chemical structure to T2 and that changes in the orientation of neighboring hydroxy groups or changes in the configuration of the neighboring fructose ring can probably not account for the type and size of the discrepancies between T2 and T3.

Radiation-induced defects in sucrose single crystals, revisited: a combined electron magnetic resonance and density functional theory study.

The results are presented of an electron magnetic resonance analysis at 110 K of radiation-induced defects in sucrose single crystals X-irradiated at room temperature, yielding a total of nine (1)H hyperfine coupling tensors assigned to three different radical species. Comparisons are made with results previously reported in the literature. By means of electron paramagnetic resonance and electron nuclear double resonance temperature variation scans, most of the discrepancies between the present 110 K study and a previous 295 K study by Sagstuen and co-workers are shown to originate from the temperature dependence of proton relaxation times and hyperfine coupling constants. Finally, radical models previously suggested in the literature are convincingly refuted by means of quantum chemical density functional theory calculations.

Formates and dithionates: sensitive EPR-dosimeter materials for radiation therapy.

Polycrystalline formates and dithionates are promising materials for EPR dosimetry, as large yields of radiation induced stable radicals are formed with a linear dose response. Rapid spin relaxation rates were detected in many of the substances, indicating that a high microwave power can be applied during EPR acquisition in order to improve sensitivity. Different techniques used to further improve the sensitivity, such as the replacement of 7Li with 6Li or exchange of protons with deuterons in the corresponding crystalline matrices and metal ion doping are discussed. It is concluded that formates and dithionates may be up to 10 times as sensitive as L-alpha-alanine.

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.

EPR study of light illumination effects on radicals in gamma-irradiated L-alanine.

Exposure of gamma-irradiated L-alanine samples to sunlight and to light from a regular, fluorescent lamp resulted in significant changes in their EPR resonance patterns, both to spectral shapes and intensities. The experimental EPR spectra were numerically decomposed into three components reflecting contributions of three different radicals (R1-R3) generated by ionizing radiation in alanine. The light exposure caused a decay of the measured EPR signal intensity. For similar light intensities and exposure times the decay was much more pronounced in samples illuminated by sunlight than in samples illuminated by the fluorescent lamp. In both cases light-induced decay of R1 radicals was observed. Sunlight illumination resulted in a moderate decay of R2 radicals and in a doubling of the R3 radical population. On the other hand, fluorescent light caused a significant increase of R2 radicals and did not change the amount of R3 radicals. A quantitative analysis of the variations of the three radical contributions to the total EPR spectra upon fluorescent light exposure suggests a net R1-->R2 free radical transformation. These effects of light on the alanine dosimetric signal should be taken into account in dosimetry protocols, assuring protection of alanine dosimeters from extended exposure to light.

The effects of aliphatic (n-nonane), naphtenic (1,2, 4-trimethylcyclohexane), and aromatic (1,2,4-trimethylbenzene) hydrocarbons on respiratory burst in human neutrophil granulocytes.

This study investigates the effects of aliphatic (n-heptane, n-nonane), naphtenic (methylcyclohexane, 1,2,4-trimethylcyclohexane (TMCH)), and aromatic (methylbenzene, 1,2,4-trimethylbenzene (TMB)) hydrocarbons on respiratory burst in human granulocytes. The free radical formation was measured as 2,7-dichlorofluorescein diacetate-amplified (DCF) fluorescence, by electron paramagnetic resonance (EPR) spectroscopy and by hydroxylation of 4-hydroxybenzoate. The chemotactic peptide N-formyl-met-leu-phe (fMLP) and phorbol 12-myristate 13-acetate (PMA), a diacylglycerol analogue, were included as positive controls. DCF fluorescence was elevated in a concentration-dependent manner by C9 hydrocarbons. The C7 hydrocarbons did not stimulate respiratory burst in the concentration range examined. The naphtenic hydrocarbon TMCH showed the strongest effect on respiratory burst and was therefore selected for mechanistic studies of this free radical formation. In the absence of extracellular Ca(2+), fluorescence in response to TMCH and fMLP was reduced by 77 and 90%, respectively. Preincubation of the granulocytes with the protein kinase C inhibitor bisindolylmaleimide reduced the DCF fluorescence stimulated with TMCH, fMLP, and PMA by 82, 56, and 90%, respectively. The phospholipase C inhibitor U73122 lowered the TMCH- and fMLP-activated DCF fluorescence by 87 and 76%. In addition, the TMCH- and fMLP-induced DCF fluorescence, after the preincubation with the phospholipase D modulator n-butanol, was lowered by 83 and 52%, respectively. The importance of protein kinase C, phospholipase C, and phospholipase D for elevation of respiratory burst was also demonstrated by the EPR experiments using the spin trap 5-diethoxyphosphoryl-5-methyl-1-pyrroline-N-oxide (DEPMPO). Preincubation with the NADPH oxidase inhibitor diphenyleneiodonium and diethyldithiocarbamate, which inhibits superoxide dismutase, led to an almost complete reduction of DCF fluorescence in response to TMCH, fMLP, and PMA. Preincubation with diethyldithiocarbamate led to the elevation of superoxide adducts of DEPMPO. The hydrocarbons stimulated formation of mainly the superoxide (O(*-)(2)) adduct of DEPMPO (DEPMPO-OOH) but also small amounts of the hydroxyl adduct ((*)OH) (DEPMPO-OH). Using 4-hydroxybenzoate as a hydroxyl radical trap confirmed formation of (*)OH after stimulation with the hydrocarbons. In conclusion, our findings indicate that TMCH-activated respiratory burst is dependent on the Ca(2+)-dependent phospholipase C, phospholipase D, and protein kinase C prior to activation of the NADPH oxidase.

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.

Radiation-induced radical formation in beta-glycerophosphate single crystals studied by electron paramagnetic resonance and electron nuclear double resonance spectroscopy: formation of an allylic-type radical.

Single crystals of disodium beta-glycerophosphate pentahemihydrate (betaGP), Na2x(HO)CH2CH(PO(4)2-)CH2(OH)x5 1/2H2O, were X-irradiated at 77 and 280 K. EPR, ENDOR and FSE techniques were used to study the formation of free radicals in these irradiated crystals to characterize possible reaction mechanisms leading to dephosphorylation. Irradiation at 77 K reveals the presence of four different radicals: two alkoxy radical conformations, AR1 and AR2, (HO)CH2CH(PO(4)2-)CH2O. and two carbon-centered hydroxyalkyl radicals, LTR1, (HO)CH2CH(PO(4)2-) C.HOH, and LTR2, with a tentative structure (HO)CH2C.H(PO(4)2-)CH2OH. AR1 and AR2 were determined to be formed on each of the two independent molecules A and B of the asymmetrical unit of betaGP, each on the 3-end of the molecule. Irradiation at 280 K reveals the presence of three hydroxyalkyl allyl radicals, R1, R2 and R3, with the common chemical structure (HO)C.H-H=CH(OH). Radicals R1 and R2 are determined to form on molecules B and A of the asymmetrical unit, respectively. The site of radical formation for R3 could not be ascertained absolutely from the available data, and there is also evidence that suggests the possibility that R3 has a hydroxyphospho-allyl radical structure. Possible reaction mechanisms for the formation of both the 77 K radicals and the 280 K radicals are suggested and discussed. The formation of an allyl-type radical in such a small-molecule single-crystal model system is an interesting and surprising result which may be relevant to the formation of the so-called 3alphaH radical species commonly observed in irradiated solid cytosine nucleosides and nucleotides. The result is also important because of the formation of the hydroxyalkyl allyl radical in solid beta-glycerophosphate is at variance with mechanisms and products shown to dominate for this and similar systems in solution radiolysis.

Electron paramagnetic resonance and electron nuclear double resonance studies of X-irradiated crystals of cytosine hydrochloride. Part I: free radical formation at 10 K after high radiation doses.

Anhydrous single crystals of cytosine hydrochloride (protonated at N3) have been X-irradiated at 10 K and studied using K-band EPR, ENDOR and FSE spectroscopy. At least seven radicals were present at 10 K after X irradiation with a dose of about 150 kGy. Two different protonation states of the one-electron reduced cytosine cation were observed: an amino-protonated species (R1) and the pristine one-electron reduced species (R2) with zero net charge. Apparently three deprotonated versions of the one-electron oxidized cytosine cation were formed: the amino-deprotonated cation (R3), an N3-deprotonated cation (R4) and an N1-deprotonated cation (R5). Finally, two products formed by net hydrogen addition to the cytosine base were observed: a C5 hydrogen-addition radical (R6) and a C6 hydrogen-addition radical (R7). The crystalline lattice of cytosine hydrochloride is characterized in part by a cytosine base initially protonated at the N3-position, thus forming a cytosine base cation, and in part by an extended network of hydrogen bonding involving the chlorine anions. Proton transfer properties of pristine one-electron oxidation and reduction base products in this lattice are discussed and are suggested as explanations of the unusual multitude of positions for deprotonation of the one-electron oxidized species as well as for the two protonation states of the reduction product observed. The magnetic parameters for the amino-protonated species R1 agree well with those extracted from previous studies of cytosine derivatives in frozen solutions and in various glasses.

Radiation damage to DNA base pairs. II. Paramagnetic resonance studies of 1-methyluracil x 9-ethyladenine complex crystals X-irradiated at 10 K.

Single crystals of the co-crystalline complex of 1-methyluracil and 9-ethyladenine were X-irradiated and studied using EPR, ENDOR and FSE spectroscopic techniques at 10 K. All together seven radicals were identified, and experimental evidence for at least one more species, as well as for a very low population of radical pairs, is available. Oxidation and reduction products appear to be stabilized at both base constituents of the pair. Of the 1-methyluracil moiety, the product formed by net hydrogen abstraction from the methyl group was observed, together with the 1-methyluracil anion and the 1-methyluracil-5-yl radical. From the 9-ethyladenine moiety, the N3-protonated 9-ethyladenine anion is stabilized. In addition, the 9-ethyladenine cation as well as traces of the amino-deprotonated cation were observed, together with the C8-H hydrogen adduct. The presence of oxidation and reduction products in each of the two bases may indicate that negligible energy transfer takes place between them. This behavior is different from that observed in the similar pair of 1-methylthymine-9-methyladenine. There also seems to be minor proton exchange between the two stacks of molecules: Interbase protonation-deprotonation channeled through the hydrogen-bonding scheme seems to be almost completely suppressed.

Electron spin resonance and electron nuclear double resonance study of X-irradiated deoxyadenosine: proton transfer behavior of primary ionic radicals.

A study of deoxyadenosine crystals (anhydrous form) after irradiation at 10 K found four base-centered radicals and one sugar-centered radical. Radical R1, thermally stable to about 100 K and photobleachable easily with white light, was the product of deprotonation at the amino group by the primary radical cation. Radical R2, also thermally stable to about 100 K, was the product of protonation at N3 of the primary radical anion. Radical R3, stable to about 170 K, was centered in the deoxyribose moiety and evidently was the result of net hydrogen abstraction from C4'. Radicals R4 and R5 were the C2 and C8 H-addition products with couplings typical of those species. Both R4 and R5 were formed at 10 K and were stable at room temperature. The behavior of R1 in several systems provides additional evidence for significant involvement of the hydrogen-bonding environment in controlling the stabilization (or formation) of radicals resulting directly from ionization, as described previously (Radiat. Res. 131, 272-284, 1992). From comparison of amino-group hydrogen-bonding environments in which radicals with the structure of R1 were stabilized, we conclude that oxygen atoms as proton acceptors are important in permitting the charge and spin separation necessary for radical stabilization. In particular, oxygens of ROH structures seem most efficient by readily permitting a multi-proton shuffle through a mechanism amounting to proton exchange. The collective results show that stabilization of these products is unlikely unless the charge and spin can be separated by at least one intervening molecule.

Radiation damage to DNA base pairs. I. Electron paramagnetic resonance and electron nuclear double resonance study of single crystals of the complex 1-methylthymine.9-methyladenine X-irradiated at 10K.

Single crystals of the complex 1-methylthymine.9-methyl-adenine were X -irradiated at 10 and at 65 K and studied in the temperature range 10 to 290 K using K-band EPR, ENDOR and field-swept ENDOR (FSE) techniques. The EPR and ENDOR spectra are dominated by two major and four minor resonances. The two major resonances are: MTMA1, the well-known radical formed by net hydrogen abstraction fr om the CS methyl group of the thymine moiety, and MTMA2, the radical formed by net hydrogen abstraction from the N1 methyl group of the thymine moiety. The latter product has not been observed previously in any 1-methylthymine derivative. The four minor resonances are: MTMA3, the anion of 1-methylthymine, possibly protonated at the O4 position; MTMA4, the well-known species formed by net hydrogen addition to C6 of the thymine moiety; MTMA5, the species formed by net hydrogen addition to C2 of the adenine moiety; and MTMA6, the species formed by net hydrogen addition to C8 of the adenine moiety. Radical MTMA3, the O4-protonated thymine anion, was clearly detected at 10 K, but upon thermal annealing at 40 K the lines began to disappear. In crystals irradiated at 65 K MTMA3 was only weakly present. Radical MTMA2 decayed at about 250 K with no detectable successor, and radical MTMA5 disappeared at about 180 K. It was not possible to learn from the d ata if MTMA5 transformed into MTMA6. The radical distribution in the 1-methylthymine.9-methyladenine crystal system is different from that in crystals of the individual components. Reasons for this behavior are discussed in light of the hydrogen bonding schemes and molecular stacking interactions in each of the crystals. An important feature is the concept of excited-state transfer from the adenine to the thymine moiety, followed by dehydrogenation at the thymine Nl-methyl group, the mechanism resulting in radical MTMA2.

Free radical formation in single crystals of 9-methyladenine X-irradiated at 10 K. An electron paramagnetic resonance and electron nuclear double resonance study.

Single crystals of 9-methyladenine were X-irradiated at 10 K and at 65 K and were studied using K-band EPR, ENDOR and field-swept ENDOR (FSE) techniques in the temperature range 10 K to 290 K. Three major radicals are stabilized in 9-methyladenine at 10 K. These are: MA1, the adenine anion, probably protonated at N3; MA2, the species formed by net hydrogen abstraction from the 9-methyl group; and MA3, the radical formed by net hydrogen addition to C8 of the adenine moiety. Radical MA1 decayed at about 80 K, possibly into the C2 H adduct (MA4). The other two species (MA2, MA3) were stable at room temperature. A fifth radical species was clearly present in the EPR spectra at 10 K but was not detectable by ENDOR. This species, which decayed above 200 K (possibly into MA3), remains unidentified. The radical population at room temperature is as described by previous authors. The mechanisms for radical formation in 9-methyladenine are discussed in light of the hydrogen bonding scheme and molecular stacking interactions.

Electron paramagnetic resonance of X-irradiated sodium and potassium salts of glucose-1-phosphate. Identification of PO3(2-) radicals at room temperature.

Single crystals of the disodium and dipotassium salt of glucose-1-phosphate, X-irradiated at 80 K or at 280 K, show the presence of PO3(2-) radicals at 295 K, formed by scission of the phosphate-ester bond at the phosphate side. The 31P hyperfine coupling constants were measured using X- and Q-band EPR spectroscopy. Typical values for these coupling constants are a magnitude of = 68 mT and a perpendicular = 53 mT. The g values were almost isotropic, slightly smaller than that of the free electron spin (g = 2.0023). There is no substantial reorientation of the phosphate group in the crystalline lattice upon radical formation. Directly after irradiation at 77 K the PO3(2-) radicals are not present, but their characteristic resonance grows in upon thermal annealing of the crystals. The radicals are probably formed from a carbon-centered radical precursor by secondary reactions resulting in the loss of the phosphate group, leaving a (diamagnetic) modified carbohydrate molecule behind. The alternative process of reductive cleavage of the phosphate-ester bond by electrons released from traps in the crystal upon thermal annealing is considered less likely. A second phosphate-centered species, with a magnitude of about 21 mT and a perpendicular about 15 mT, was detected in the dipotassium salt of glucose-1-phosphate only. Possible structures for this species are discussed.

ESR and ENDOR study of single crystals of deoxyadenosine monohydrate X-irradiated at 10 K.

Five free radicals have been detected by detailed ESR/ENDOR experiments on single crystals of deoxyadenosine monohydrate (AdRm), X-irradiated and observed at 10 K. In a previous study of adenosine (Radiat. Res. 117, 367-378, 1989), only the anion (protonated at N3) and the cation (deprotonated at the exocyclic NH2) were detected at 10 K. In AdRm, Radical R1 is the N3-protonated anion, similar to that observed previously in adenosine. Radical R3 is a C5' hydroxyalkyl radical formed by net H-abstraction from C5'. A second sugar radical is formed by net C1' H-abstraction. Two other base radicals observed in AdRm at 10 K are the C2 and C8 H-addition radicals. The C2 H-addition radical (Radical R5) exhibits inequivalent methylene hydrogen couplings of 5.43 and 3.29 mT, while in the C8 H-addition radical (Radical R6) the couplings are somewhat more equivalent (3.63 and 4.17 mT). No link between RAdical R1 and the H-addition radicals has been observed. The reduced base appears to protonate rapidly even at 10 K, while at the same time both H-addition radicals are clearly present. On warming, Radical R1 appears to decay at about 80 K with no apparent successor. Although no base cation was stabilized in AdRm at 10 K, it is interesting to note that Radicals R3 and R4 could both be formed as the result of deprotonation of primary oxidation products.

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.

On the proton transfer behavior of the primary oxidation product in irradiated DNA.

Results are surveyed from investigations of six adenine and six guanine crystal systems X-irradiated and studied at temperatures near that of liquid helium (T less than 10 K). Basic conclusions from the overall results are that the primary oxidation products deprotonate rapidly, and that the specific site of deprotonation is environment-dependent. The following systematic behaviors were identified: (1) in no case was there deprotonation at a site hydrogen-bonded to a halide ion (three examples with guanine and two with adenine); (2) likewise, in no case was there deprotonation at a site hydrogen-bonded to a phosphate group (three examples, all with guanine); (3) in no case was there deprotonation at a site involving an greater than N-H . . . N less than hydrogen bond; (4) in all cases except one, the site of net deprotonation involved greater than N-H . . . O hydrogen bonds. In the remaining case, the leaving proton was uninvolved in hydrogen bonding. A review of results obtained previously from DNA leads to the conclusion that the actual protonation states of DNA oxidation products are unknown at the present time. The results presented here predict with high probability that such DNA products also will deprotonate, but the environment dependence makes it difficult to predict the specific sites. Thus the importance of obtaining this information from direct experimental evidence is increased.

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.