Cell inactivation and DNA single- and double-strand breaks in cultured mammalian cells irradiated by a thermal neutron beam

The effects on the cellular viability and induction and repair kinetics of DNA strand breaks in HeLa cells were examined after exposure to a thermal neutron beam and compared with those after gamma-irradiation. The thermal neutron survival curve had no initial shoulder. The relative biological effectiveness (r.b.e.) value of the neutron beam was determined to be 2.2 for cell killing (ratio of D0 values), 1.8 and 0.89 for single strand breakage (ssb) by alkaline sedimentation and alkaline elution respectively, and for double strand breakage (dsb) 2.6 by neutral elution. No difference was observed between thermal neutrons and gamma-rays in the repair kinetics of ssb and dsb. It is suggested that the effect induced by the intracellular nuclear reaction, 14N(n,p)14C is mainly responsible for the high r.b.e. values observed.     

Mutation induction and relative biological effectiveness of neutrons in mammalian cells. Experimental observations

The induction of mutation by graded doses of monoenergetic neutrons was examined using the human-hamster hybrid cell system. The AL cells, formed by fusion of human fibroblasts with the gly- A mutant of the Chinese hamster ovary cells, contain the standard set of hamster chromosomes plus a single human chromosome, number 11. These cells contain specific human cell surface antigens that render them sensitive to killing by specific antisera in the presence of complement. Mutant AL cells that have lost the surface markers, however, would survive and give rise to scorable colonies. The cells were irradiated with neutrons produced at the Radiological Research Accelerator Facility of Columbia University. Doses corresponding to low, moderate, and high cytotoxicities and in energies ranging from 0.33 to 14 MeV were used. Neutrons induced a dose-dependent cytotoxicity and mutation frequency in the AL cells. Over the range of doses examined, it was found that the mutagenesis induced by neutrons was energy-dependent and the frequencies were a curvilinear function of dose for both the a1 and a2 antigenic loci examined. In comparison to gamma rays, the relative biological effectiveness (RBE) for cell lethality at the 10% survival level ranged from 5.2 for 0.33 MeV to 1.8 for 14 MeV neutrons. The RBE for mutation induction at the a1 locus, however, ranged from 30 for 0.33 MeV to 4.2 for 14 MeV neutrons at or around the lowest levels of effect examined. Results of the present study demonstrated that neutrons, when measured under conditions which permit detection of a spectrum of gene and chromosomal mutations, in fact, are more efficient mutagens than previously thought.     

Molecular structural analysis of HPRT mutations induced by thermal and epithermal neutrons in Chinese hamster ovary cells

Chinese hamster ovary (CHO) cells were exposed to thermal and epithermal neutrons, and the occurrence of mutations at the HPRT locus was investigated. The Kyoto University Research Reactor (KUR), which has been improved for use in neutron capture therapy, was the neutron source. Neutron energy spectra ranging from nearly pure thermal to epithermal can be chosen using the spectrum shifters and thermal neutron filters. To determine mutant frequency and cell survival, cells were irradiated with thermal and epithermal neutrons under three conditions: thermal neutron mode, mixed mode with thermal and epithermal neutrons, and epithermal neutron mode. The mutagenicity was different among the three irradiation modes, with the epithermal neutrons showing a mutation frequency about 5-fold that of the thermal neutrons and about 1.5-fold that of the mixed mode. In the thermal neutron and mixed mode, boron did not significantly increase the frequency of the mutants at the same dose. Therefore, the effect of boron as used in boron neutron capture therapy (BNCT) is quantitatively minimal in terms of mutation induction. Over 300 independent neutron-induced mutant clones were isolated from 12 experiments. The molecular structure of HPRT mutations was determined by analysis of all nine exons by multiplex polymerase chain reaction. In the thermal neutron and mixed modes, total and partial deletions were dominant and the fraction of total deletions was increased in the presence of boron. In the epithermal neutron mode, more than half of the mutations observed were total deletions. Our results suggest that there are clear differences between thermal and epithermal neutron beams in their mutagenicity and in the structural pattern of the mutants that they induce. Mapping of deletion breakpoints of 173 partial-deletion mutants showed that regions of introns 3-4, 7/8-9 and 9-0 are sensitive to the induction of mutants by neutron irradiation.     

Evidence to support the existence of efficient DNA double-strand break rejoining in a radiosensitive mutant of V79-4 following irradiation with 250 kVp X-rays or neutrons

The repair of ionising-radiation-induced DNA double-strand break type damage was measured by Kohn neutral elution in an X-ray-sensitive mutant of V79-4, irs1. This was done in order to investigate further the likelihood that irs1 carries a defect which leads to error-prone repair of DNA damage, and not simply a reduced ability to rejoin DNA double-strand breaks. The mutant displayed an equal increase in sensitivity to the lethal effects of neutrons, as compared to X-rays. Both irs1 and V79-4 showed an increased sensitivity to the killing effects of neutrons of around 2 at 10% survival. irs1 also showed an exponential survival after either X-rays or neutrons. The induction of DNA double-strand breaks was measured in both cell lines over a dose range of 10-40 Gy using Kohn neutral filter elution. Induction of breaks by X-rays in irs1 seemed to increase slightly with dose, relative to induction in V79-4, so that at 40 Gy 1.5 times more DNA double-strand breaks were measured in irs1 cells than in V79-4. Neutron irradiation resulted in a more similar level of induction in either strain after 10-40 Gy. This difference in induction of damage may be due to a different cell-cycle composition in either cell line. The rejoining of X-ray induced double-strand breaks showed a very similar pattern (on a percentage rejoined basis) in both cell lines, although from the induction data at 40 Gy, the dose at which rejoining was measured, fewer breaks were rejoined in V79-4 but also fewer breaks remained unsealed. Neutron-induced breaks, however, were rejoined more efficiently in irs1 again on a percentage basis, but also in absolute terms since similar induction was seen after 40 Gy. This data, together with the differences seen in the rejoining of X-ray compared to neutron induced breaks, may indirectly support the proposal that irs1 is a misrepair mutant.     

LET and ion-species dependence for cell killing and mutation induction in normal human fibroblasts.

We have been studying LET and ion species dependence of RBE values in cell killing and mutation induction. Normal human skin fibroblasts were irradiated with heavy-ion beams such as carbon (290 Mev/u and 135 Mev/u), neon (230 Mev/u and 400 Mev/u), silicon (490 Mev/u) and iron (500 Mev/u) ion beams, generated by Heavy Ion Medical Accelerator in Chiba (HIMAC) at National Institute of Radiological Sciences (NIRS). Cell killing effect was detected as reproductive cell death using a colony formation assay. Mutation induction in hprt locus was detected to measure 6-thioguanine resistant colonies. The RBE-LET curves of cell killing and mutation induction were different each ion beam. So, we plotted RBE for cell killing and mutation induction as function of Z*2/beta2 instead of LET. RBE-Z*2/beta2 curves of cell killing indicated that the discrepancy of RBE-LET curves was reconciled each ion species. But RBE-Z*2/beta2 curves of mutation induction didn't corresponded between carbon- and silicon-ion beams. These results suggested that different biological endpoints may be suitable for different physical parameter, which represent the track structure of energy deposition of ion beams.     

Lethal and mutagenic effects of 252Cf radiation in cultured human cells

HeLa MR cells were exposed to radiation emitted from a man-made spontaneously fissioning isotope, californium-252. The neutron to gamma-ray ratio in the radiation dose was measured to be 2.0. The extrapolation number of the dose-survival curve was 1.3 and the Do was 200 cGy. A dose-dependent increase in mutation to 6-TGr (6-thioguanine resistant) was observed. The relative biological effectiveness (r.b.e.) for cell killing of the neutrons from 252Cf, calculated relative to high-dose-rate X-rays, was 2.6 at 50 per cent survival. The r.b.e. for mutation induction was 2.7 at a mutation frequency of 5 X 10(-5) per surviving cell.     

The response of spermatogonia and spermatocytes of the Northern vole Microtus oeconomus to the induction of sex-chromosome nondisjunction, diploidy and chromosome breakage by X-rays and fast fission neutrons

Microtus males were exposed to different doses of 250 kV X-rays or fast fission neutrons of 1 MeV mean energy. Early (= round) spermatids were analyzed for the presence of extra sex chromosomes, diploidy and micronuclei at different time intervals corresponding with treated differentiating spermatogonia and spermatocytes. Induction of nondisjunction of sex chromosomes could not be detected. In contrast, induction of diploids by both types of radiation was statistically significant at all sampling times. Dose-effect relationships for most of the sampling times were linear and sometimes linear-quadratic concave upward or downward. There were pronounced stage-specific differences in sensitivity as reflected by differences in doubling doses that ranged from 4 to 22 cGy for X-rays and from 0.4 to 4 cGy for neutrons. Spermatocytes at pachytene were the most sensitive cells and proliferating spermatogonia the least sensitive ones. The relative biological effectiveness (RBE) of neutrons depended on the cell stage treated and fluctuated between 1.4 and 9.2. Evidence for radiation-induced chromosomal breakage events was obtained via detection of micronuclei. Induction of micronuclei by X-rays or neutrons was statistically significant at all spermatocyte stages tested. There was no effect in spermatogonia. With a few exceptions dose-effect relationships were linear. Differences in stage sensitivity were clearly present as evidenced by doubling dose which ranged from 5 to 29 cGy for X-rays and from 1 to 3 cGy for neutrons. RBE values varied from 5.2 to 12.7. Maximum sensitivity was detected in spermatocytes at diakinesis, MI and MII. Resting primary spermatocytes (G1 and S phase) were somewhat less sensitive and actively proliferating spermatogonia were the least sensitive cells. The pattern of stage sensitivity for induction of diploids was distinctly different from that for induction of chromosomal breakage.     

Distinct superinfection interference properties yet similar receptor utilization by cytopathic and noncytopathic feline leukemia viruses.

Cell killing by cytopathic retroviruses is often associated with a delay or failure in the establishment of superinfection interference. Superinfection has been observed during T-cell killing and fatal immunodeficiency disease induction by the feline leukemia virus (FeLV) chimera FeLV-FAIDS-EECC, containing the surface envelope glycoprotein (SU) of FeLV-FAIDS clone 61C. We demonstrate here that 61C SU has a defect that results in a nearly complete failure to establish superinfection interference against homologous virus challenge. This failure was evident only in feline T (FeT) cell clones expressing envelope protein, not in the rare cells that have survived cytopathic infection to become chronically infected. The regions of SU responsible for this defect were the same as those previously identified as responsible for T-cell killing. The superinfection interference properties of a noncytophatic molecular clone, FeLV-FAIDS-61E, were different in that 61E established interference to homologous virus challenge, both in SU-expressing cell clones and in chronically infected cells. Neither 61E nor EECC established interference against heterologous virus challenge. Viruses expressing chimeric SU proteins displayed varied and intermediate interference properties. Purified 61E and 61C SU competed for binding sites on FeT cell surfaces, and purified 61E SU blocked infection of virus bearing 61E or 61C SU. In addition, purified 61E and 61C SU each coprecipitated 70-kDa FeT cell surface proteins. Our data are consistent with the hypothesis that there are multiple cellular components necessary for 61E and 61C attachment to and penetration of FeT cells, a primary receptor that is utilized by both 61E and 61C, and secondary receptors that are likely to be virus specific.     

Fast neutron r.b.e. for lethality and genotoxicity in a wild-type and a repair-deficient strain of yeast

The relative biological effectiveness (r.b.e.) of cyclotron-produced fast neutrons (11 MeV) in relation to 60Co gamma-rays, was studied in a wild-type and a DNA repair-deficient yeast strain for cell killing and genotoxicity. In the wild-type (D7) strain the r.b.e. varied from 2.7 to 4.1 for lethality, 2.8 to 7.1 for reverse mutation and 3.5 to 7.8 for mitotic gene conversion. At different survival levels, the repair deficient strain (D7 rad 52/rad 52) generally showed a lower r.b.e. for both cell killing and genotoxicity (25.2 to 37.2 per cent reduction for the cell death and 24.8 to 70.6 per cent for mutation and gene conversion) compared to the wild type. Except at very low dose levels, the r.b.e. values for cell killing and genotoxicity were similar within a given strain. At similar survival levels, neutrons were no more genotoxic than gamma-rays.     

The cytogenetic effect of thermal neutrons inLens esculenta (Moench)

The first information concerning the cytogenetic efficiency of thermal neutrons in lentil are presented in this paper. The range of cytologically effective dosages of thermal neutrons in lentil was determined. This determination enables us to compare the efficiency with the mutagenic effect of thermal neutrons and with their effect on the growth and development of plants of M₁ generation. These effects were already evaluated in previous communications. Thermal neutron irradiation significantly affected all the characters studied. A linear dependence of the effect on the dose of the neutron radiation was found for most of the analyzed characters. From a sample of scored cells, whose nuclei were in the anaphase or early telophase, 9.0 to 72.0% of them had chromosomal bridges and fragments after irradiation with dosages from 3.3×10¹¹ n cm^?2 to 4.5×10¹² n cm^?2. The highest number of rearrangements per one cell reached 2.16 after irradiation with 4.25×10¹² n cm^?2 while the lowest dosage used, 3.3×10¹¹ n cm^?2, induced 0.17 of chromosomal rearrangements per one cell. Irradiation with thermal neutrons is capable of inducing a large number of very complicated chromosome rearragements.     

Bystander killing during avian leukosis virus subgroup B infection requires TVB(S3) signaling

Cell killing by avian leukosis virus subgroup B (ALV-B) in cultures has been extensively studied, but the molecular basis of this process has not been established. Here we show that superinfection, which has been linked to cell killing by ALV-B, plays no crucial role in cell death induction. Instead, we show that signaling by the ALV-B receptor, TVB(S3), a member of the tumor necrosis factor receptor family, is essential for ALV-B-mediated cell death. TVB(S3) activated caspase-dependent apoptosis during ALV-B infection. Strikingly, apoptosis induction occurred predominantly in uninfected cells, while ALV-B-infected cells were protected against cell death. This bystander killing phenomenon was reproduced in a virus-free system by cocultivating ALV-B Env-expressing cells with TVB(S3)-expressing cells. Taken together, our results indicated that ALV-B-mediated apoptosis is triggered by ALV-B Env-TVB(S3) interactions.     

Effect of inhibitors of poly(ADP-ribose) polymerase on the heat response of HeLa S3 cells

The purpose of this study was to investigate a possible involvement of poly(ADP-ribosyl)ation reactions in hyperthermic cell killing and hyperthermic DNA strand-break induction and repair in HeLa S3 cells. The inhibitors of poly(ADP-ribose) polymerase, 3-aminobenzamide (3AB) and 4-aminobenzamide (4AB), were used as tools in this study. Both inhibitors could sensitize the cells for hyperthermic cell killing equally well, although 3AB is known to be a more effective enzyme inhibitor. The heat sensitization at the level of cell killing could be reversed when the compounds were still present during a 4-h postincubation at 37 degrees C. More heat-induced DNA strand breaks were formed in the presence of 3AB and 4AB. Repair of strand breaks was inhibited during the postincubation at 37 degrees C. Thus the effect of 3AB and 4AB on DNA strand-break repair was different from the cited effect on cell survival. It is concluded that the sensitizing effect of 3AB and 4AB on hyperthermic cell killing is not caused by inhibition of poly(ADP-ribose) polymerase and is also not related to repair of DNA strand breaks.     

Ultraviolet radiation induction of endogenous murine type C virus

Induction of endogenous type C RNA virus occurred following exposure of mouse cells to ultraviolet radiation. Irradiation of A1-2 cells, derived from the BALB/c mouse, induced endogenous xenotropic type C virus as determined by infectious center focus-forming assay on normal rat-kidney (NRK) cells. Viral induction by UV radiation was compared to that for the halogenated pyrimidines, 5-iodo-2-deoxyuridine (IdU) and 5-bromo-2-deoxyuridine (BrdU). Although the fraction of A1-2 cells induced to release virus by UV radiation (0.17%) was less than that observed for IdU (3.0%) and BrdU (0.46%), use of the sensitive infectious center assay demonstrated reproducible UV induction. Dose-response studies showed that the level of viral induction by UV was dependent upon cellular UV exposure. Study of A1-2 cell survival following irradiation showed that optimum viral induction occurred at a UV exposure corresponding to the edge of the shoulder of the survival curve, suggesting that UV sensitivity of the host cell may be a factor limiting the level of induction. Since less radiation was required for viral induction than for inactivation of colony-forming ability, viral induction may be a more sensitive dosimeter of in vitro UV bioeffects than cell survival for this system.     

Highly inducible cell lines derived from mice genetically transmitting the Moloney murine leukemia virus genome.

Permanent, non-virus-producing cell lines have been established from a mouse embryo carrying an endogenous, genetically transmitted Moloney murine leukemia virus (M-MuLV) genome. These cells carry the M-MuLV genome, as demonstrated by hybridization of cellular DNA to M-MuLV complementary DNA, but do not express it at the levels of virus production, accumulation of intracellular viral p30, or M-MuLV-specific RNA. Treatment with bromodeoxyuridine (50 microgram/ml for 24 h) resulted in induction of XC-positive NB-tropic virus, although only a small fraction of the cells released virus (less than 0.1% after 48 h). Immunofluorescent staining and flow microfluorometry indicated that a wave of p30 accumulation occurs in the induced cells, with a maximum at 24 to 48 h after the addition of bromodeoxyuridine. Furthermore, most, if not all, cells were induced to produce p30 protein. Similar kinetics were found for the accumulation of M-MuLV-specific RNA in the cytoplasm of induced cells. This rapid induction of virus expression in a majority of cells was dependent on the presence of the M-MuLV genome and probably represents primarily the expression of this endogenous virus since induction was not observed in cells similarly derived from a sibling embryo lacking the M-MuLV genome.     

Late effects of radiation on the central nervous system: role of vascular endothelial damage and glial stem cell survival

Selective irradiation of the vasculature of the rat spinal cord was used in this study, which was designed specifically to address the question as to whether it is the endothelial cell or the glial progenitor cell that is the target responsible for late white matter necrosis in the CNS. Selective irradiation of the vascular endothelium was achieved by the intraperitoneal (ip) administration of a boron compound known as BSH (Na(2)B(12)H(11)SH), followed by local irradiation with thermal neutrons. The blood-brain barrier is known to exclude BSH from the CNS parenchyma. Thirty minutes after the ip injection of BSH, the boron concentration in blood was 100 microg (10)B/ g, while that in the CNS parenchyma was below the detection limit of the boron analysis system, <1 microg (10)B/g. An ex vivo clonogenic assay of the O2A (oligodendrocyte-type 2 astrocyte) glial progenitor cell survival was performed 1 week after irradiation and at various times during the latent period before white matter necrosis in the spinal cord resulted in myelopathy. One week after 4.5 Gy of thermal neutron irradiation alone (approximately one-third of the dose required to produce a 50% incidence of radiation myelopathy), the average glial progenitor cell surviving fraction was 0.03. The surviving fraction of glial progenitor cells after a thermal neutron irradiation with BSH for a comparable effect was 0.46. The high level of glial progenitor cell survival after irradiation in the presence of BSH clearly reflects the lower dose delivered to the parenchyma due to the complete exclusion of BSH by the blood-brain barrier. The intermediate response of glial progenitor cells after irradiation with thermal neutrons in the presence of a boron compound known as BPA (p-dihydroxyboryl-phenylalanine), again for a dose that represents one-third the ED(50) for radiation-induced myelopathy, reflects the differential partition of boron-10 between blood and CNS parenchyma for this compound, which crosses the blood-brain barrier, at the time of irradiation. The large differences in glial progenitor survival seen 1 week after irradiation were also maintained during the 4-5-month latent period before the development of radiation myelopathy, due to selective white matter necrosis, after irradiation with doses that would produce a high incidence of radiation myelopathy. Glial progenitor survival was similar to control values at 100 days after irradiation with a dose of thermal neutrons in the presence of BSH, significantly greater than the ED(100), shortly before the normal time of onset of myelopathy. In contrast, glial progenitor survival was less than 1% of control levels after irradiation with 15 Gy of thermal neutrons alone. This dose of thermal neutrons represents the approximate ED(90-100) for myelopathy. The response to irradiation with an equivalent dose of X rays (ED(90): 23 Gy) was intermediate between these extremes as it was to thermal neutrons in the presence of BPA at a slightly lower dose equivalent to the approximate ED(60) for radiation myelopathy. The conclusions from these studies, performed at dose levels approximately iso-effective for radiation-induced myelopathy as a consequence of white matter necrosis, were that the large differences observed in glial progenitor survival were directly related to the dose distribution in the parenchyma. These observations clearly indicate the relative importance of the dose to the vascular endothelium as the primary event leading to white matter necrosis.     

Induction and subsequent repair of DNA damage by fast neutrons in cultured mammalian cells

The induction and repair of DNA damage were studied by a DNA unwinding method in mouse L5178Y cells exposed to fast neutrons. DNA lesions induced by fast neutrons were classified into three types from their repair profiles: fast-reparable breaks (T1/2 = 3-5 min), slow-reparable breaks (T1/2 = 70 min), and nonreparable breaks. The repair rates of both fast-reparable and slow-reparable breaks were almost the same as those of corresponding damage induced by low-LET radiation. Neutrons induced a smaller amount of fast-reparable damage, an almost equal amount of slow-reparable damage, and a larger amount of nonreparable damage than those induced by equal doses of gamma rays or X rays. RBEs for fast- and slow-reparable damage were 0.3 and 0.9, respectively. The RBE for nonreparable damage was dose dependent and was 1.4 at the level of 100 breaks/10(12) Da DNA. Among the three types of lesions, only the nonreparable damage levels correlated with the linear-quadratic shape of the survival curves and with the enhanced killing effectiveness of neutrons (RBE = 1.7 at D0).     

Differential modulation of specific gene expression following high- and low-LET radiations

Experiments were designed to examine the effects of radiation quality on specific gene expression within the first 3 h following radiation exposure in Syrian hamster embryo (SHE) cells. Preliminary work demonstrated the induction of c-fos and alpha-interferon genes following exposure to low-linear-energy-transfer (low-LET) radiations (X rays or gamma rays). More detailed experiments revealed induction of c-fos mRNA within the first 3 h following exposure to either X rays (75 cGy) or gamma rays (90 cGy). We could not detect induction of c-fos following exposure of SHE cells to fission-spectrum neutrons (high-LET) from the JANUS reactor administered at either high (12 cGy/min) or low (0.5 cGy/min) dose rates. Expression of alpha-interferon mRNA was similarly induced by low-LET radiations but only modestly by JANUS neutrons. The induction by gamma rays was dose-dependent, while induction by neutrons was specific for low doses and low dose rates. These experiments demonstrate the differential gene inductive response of cells following exposure to high- and low-LET radiations. These experiments suggest that these different qualities of ionizing radiation may have different mechanisms for inducing many of the cellular consequences of radiation exposure, such as cell survival and cell transformation.     

Cytogenetic effects induced by neutrons in human peripheral blood lymphocytes in vitro. I. Dose-effect relationship for different types of chromosome aberrations when exposed to neutrons with different energies]

Human lymphocytes were irradiated in vitro during G0 stage by graded doses of thermal neutrons and of neutrons with mean energy of 0.04; 0.09; 0.35; 0.85 and 14.7 MeV as well as by 60Co gamma-rays. The data were fitted to the linear and linear-quadratic relations. The neutrons of low and intermediate energies showed the linear dependence on the dose, 14.7 MeV neutrons and gamma-rays--a linear-quadratic one, whereas the data obtained with 0.85 MeV neutrons fitted well the both models. Terminal and interstitial deletions produced by both gamma-rays and neutrons showed different dependencies upon the dose. Some qualitative pecularities of aberration spectra were found in the experiments with neutrons as compared with the data on gamma-irradiation: the ratio of exchanges to fragments was greater, and aberrations of chromatid type were produced. The specially designed experiments and calculations showed that the last effect was not connected with induced radioactivity.     

The influence of oxygen on the induction of radiation damage in DNA in mammalian cells after sensitization by intracellular glutathione depletion

Treatment of mammalian cells with buthionine sulphoximine (BSO) or diethyl maleate (DEM) results in a decrease in the intracellular GSH (glutathione) and non-protein-bound SH (NPSH) levels. The effect of depletion of GSH and NPSH on radiosensitivity was studied in relation to the concentration of oxygen during irradiation. Single- and double-strand breaks (ssb and dsb) and cell killing were used as criteria for radiation damage. Under aerobic conditions, BSO and DEM treatment gave a small sensitization of 10-20 per cent for the three types of radiation damage. Also under severely hypoxic conditions (0.01 microM oxygen in the medium) the sensitizing effect of both compounds on the induction of ssb and dsb and on cell killing was small (0-30 per cent). At somewhat higher concentrations of oxygen (0.5-10 microM) however, the sensitization amounted to about 90 per cent for the induction of ssb and dsb and about 50 per cent for cell killing. These results strengthen the widely accepted idea that intracellular SH-compounds compete with oxygen and other electron-affinic radiosensitizers with respect to reaction with radiation-induced damage, thus preventing the fixation of DNA damages by oxygen. These results imply that the extent to which SH-compounds affect the radiosensitivity of cells in vivo depends strongly on the local concentration of oxygen.