DNA lesions that signal the induction of radioresistance and DNA repair in yeast

DNA recombinational repair, and an increase in its capacity induced by DNA damage, is believed to be the major mechanism that confers resistance to killing by ionizing radiation in yeast. We have examined the nature of the DNA lesions generated by ionizing radiation that induce this mechanism, using two different end points: resistance to cell killing and ability of the error-free recombinational repair system to compete for other DNA lesions and thereby suppress chemical mutation. Under the various conditions examined in this study, the "maximum" inducible radiation resistance was increased approximately 1.5- to 3-fold and suppression of mutation about 10-fold. DNA lesions produced by low-LET gamma rays at doses greater than about 20 Gy given in oxygen were shown to be more efficient, per unit dose, at inducing radioresistance to killing than were lesions produced by neutrons (high-LET radiation). This suggests that DNA single-strand breaks are more important lesions in the induction of radioresistance than DNA double-strand breaks. Oxygen-modified lesions produced by gamma rays (low-LET radiation) were particularly efficient as induction signals. DNA damage due to hydroxyl radicals (OH.) derived from the radiolytic decomposition of H2O produced lesions that strongly induced this DNA repair mechanism. Similarly, OH. derived from aqueous electrons (e-aq) in the presence of N2O also efficiently induced the response. Cells induced to radioresistance to killing with high-LET radiation did not suppress N-methyl-N'-nitro-N-nitrosoguanidine (MNNG)-generated mutations as well as cells induced with low-LET radiation, supporting the conclusion that the type of DNA damage produced by low-LET radiation is a better inducer of recombinational repair. Surprisingly, however, cells induced with gamma radiation in the presence of N2O that became radioresistant to killing were unable to suppress MNNG mutations. This result indicates that OH. generated via e-aq (in N2O) may produce unusual DNA lesions which retard normal repair and render the system unavailable to compete for MNNG-generated lesions. We suggest that the repairability of these unique lesions is restricted by either their chemical nature or topological accessibility. Attempted repair of these lesions has lethal consequences and accounts for N2O radiosensitization of repair-competent but not incompetent cells. We conclude that induction of radioresistance in yeast by ionizing radiation responds variably to different DNA lesions, and these affect the availability of the induced recombinational repair system to deal with subsequent damage.     

Induction of minisatellite mutations in the mouse germline by low-dose chronic exposure to gamma-radiation and fission neutrons

Germline mutation induction at mouse minisatellite loci by paternal low-dose (0.125-1 Gy) exposure to chronic (1.66 x 10(-4) Gy min(-1)) low-linear energy transfer (low-LET) gamma-irradiation and high-LET fission neutrons (0.003 Gy min(-1)) was studied at pre-meiotic stages of spermatogenesis. Both types of radiation produced linear dose-response curves for mutation of the paternal allele. In contrast to previous results using higher doses, the pattern of induction of minisatellite mutation after chronic gamma-irradiation was similar to acute (0.5 Gy min(-1)) exposure to X-rays, indicating that the elevated mutation rate was independent of the ability of the cell to repair damage induced immediately or over a period of up to 100 h. Chronic exposure to fission neutrons was more effective than acute or chronic low-LET exposure (relative biological effectiveness, RBE=3.36). The data also provide strong support for the previous conclusion that increases in minisatellite mutation rate are not caused by radiation-induced DNA damage at minisatellite loci themselves, but rather from damage induced by ionising radiation elsewhere in the genome/cell.     

The saturated repair kinetics of Chinese hamster V79 cells suggests a damage accumulation--interaction model of cell killing

The aim of this study is to determine whether the repair process in log-phase Chinese hamster V79 cells exposed to X rays is unsaturated, saturable, or saturated. The kinetics of recovery from damage induced by 2 to 14 Gy of 250 kVp X rays was studied by treating cells with 0.5 M hypertonic saline for 20 min at different postirradiation repair intervals. From the kinetic data, the repair half-time (t1/2), the repair time (time needed to attain maximal survival), and the recovery ratio were calculated. The results show that the t1/2 (1.42 min/Gy) and the repair time (6.04 min/Gy) increase linearly with dose, the logarithm of the recovery ratio increases linear-quadratically with dose, and the D0 increases linearly with repair interval at a rate of 2.4 cGy/min. From these results we suggest a model: the repair of damage (undefined lesions) necessary for cell survival is effected by a repair process (t 1/2 of 1.42 min/Gy) which is saturated at doses as low as 2.4 cGy; repair saturation leads to a dose-dependent accumulation of repairable lesions; and interaction among accumulated repairable lesions results in the induction of irreparable (lethal) lesions. We call this the accumulation-interaction model of cell killing by low-LET radiation.     

Delayed cell cycle progression in human lymphoblastoid cells after exposure to high-LET radiation correlates with extremely localized DNA damage

To compare the genotoxic effects of high-LET ionizing radiation to those of low-LET radiation, we investigated the responses of human lymphoblastoid cells to DNA damage TK6 after treatment with either low-LET X rays or high-LET iron ions (1000 keV/microm). A highly localized distribution of gammaH2AX/RAD51 foci was observed in the nuclei of cells irradiated with iron ions, in sharp contrast to cells exposed to X rays, where the distribution of foci was much more uniform. This implied the occurrence of a relatively high frequency of closely spaced double-strand breaks, i.e. clustered DNA damage, after iron-ion exposure. Despite the well-established notion that clustered DNA damage is refractory to repair compared to isolated DNA lesions, there were no significant differences in the levels of clonogenic survival and apoptosis between cells treated with iron ions or X rays. Strikingly, however, cells accumulated in G(2)/M phase to a much lesser extent after iron-ion exposure than after X-ray exposure. This differential accumulation could be attributed to a much slower evacuation of the S-phase compartment in the case of cells irradiated with iron ions. Taken together, our results indicate that, relative to the situation for low-LET X rays, exposure to high-LET iron ions results in a substantially greater inhibition of S-phase progression as a result of a higher frequency of DNA replication-blocking clustered DNA damage.     

Relative biological effectiveness of accumulated 125IdU and 125I-estrogen decays in estrogen receptor-expressing MCF-7 human breast cancer cells

The therapeutic potential for delivering a cytotoxic dose of radiation (using the decay of Auger-electron emitters) to the cell nucleus of cancer cells that express estrogen receptors (ERs) by radiolabeled estrogen was investigated in the ER-expressing human breast cancer cell line, MCF-7. The radiolabeled estrogen/ER complex irradiates the cell nucleus by binding specific DNA sequences called estrogen response elements (EREs). Cell clonogenicity and induction of DNA double-strand breaks (DSBs) by gamma radiation or accumulation of (125)I-iododeoxyuridine ((125)IdU) or E-17alpha[(125)I]iodovinyl-11betamethoxyestradiol ((125)IVME2) decays were determined. MCF-7 cells were efficiently killed by accumulation of (125)IdU (D(0) = 30 decays per cell) and (125)IVME2 decays (D(0) = 28 decays per cell). DNA DSBs were induced by the accumulation of (125)IdU (approximately 3750 decays per cell required to reduce the mean value of the elution profile to 50%) or (125)IVME2 decays (approximately 465 decays per cell required to reduce the mean value to 50%). For survival of MCF-7 cells after gamma irradiation, the D(0) was 1 Gy, and approximately 65 Gy was required to reduce the mean value to 50% for induction of DSBs. The RBE values for cell killing and induction of DSBs by (125)IVME2 relative to gamma radiation were 4.8 and 18.8, respectively. The RBE values for cell killing and induction of DSBs by (125)IdU relative to gamma radiation were 4.5 and 2.3, respectively. Cell killing in a manner similar to that induced by high-LET radiation and the high RBE for induction of DSBs by (125)IVME2 in the ER-expressing MCF-7 cells provide a biological rationale for the use of Auger electron-emitting radionuclides covalently bound to estrogen to deliver a cytotoxic dose of radiation to ER-positive cancers.     

Paradoxical effects of iodine-125 decays in parent and daughter DNA: a new target model for radiation damage

Chinese hamster ovary cells were synchronized at the G(1)/S-phase boundary of the cell cycle and were pulse-labeled with (125)I-iododeoxyuridine 30 min after they entered the S phase. Cell samples were harvested and frozen for accumulation of (125)I decays during the first and second G(2) phase after labeling. Cell aliquots that had accumulated the desired number of decays were thawed and plated for evaluation micronucleus formation and cell death. Cells subjected to (125)I decays during the first G(2) phase after labeling exhibited single-hit kinetics of cell killing (n = 1, D(0) 41 decays/cell). In contrast, decays accumulated during the second G(2) phase killed cells with dual-hit kinetics (n = 1.9, D(0) 81 decays/cell). A similar divergence in the action of (125)I was noted for micronucleus formation. These findings indicate that the effects of (125)I varied depending on whether the decays occurred in daughter DNA (first G(2) phase) or parent DNA (second G(2) phase). Control studies with external X rays showed no such divergence of the action of radiation. To account for this paradox, a model is proposed that invokes higher-order chromatin structures as radiation targets. This model implies differential spatial arrangements for parent and daughter DNA in the genome, with DNA strands organized such that a single (125)I decay originating in daughter DNA damages two targets during the first G(2) phase, but identical decays occurring during the second G(2) phase damage only one of the targets.     

Targets for radiation-induced cell death: when DNA damage doesn't kill

Chinese hamster ovary (CHO) K1 and radiosensitive CHO irs-20 cells were synchronized in S phase and labeled for 10 min with 5-[(125)I]-iodo-2'-deoxyuridine ((125)IdU). The cells were washed, incubated in fresh medium for 1 h for incorporation of the intracellular radionucleotides into DNA, and then frozen (-80 degrees C) for accumulation of (125)I decays. At intervals after freezing, when the cells had accumulated the desired number of decays, aliquots of the frozen cells were thawed and plated to determine survival. The survival curves for K1 and irs-20 cells were similar from 100% to 30% survival. At higher (125)I doses (more decays/cell), the survival of K1 cells continued to decline exponentially, but the survival of X-ray-sensitive irs-20 cells remained at approximately 30% even after the cells had accumulated 1265 decays/cell. The results contradict the notion that increased DNA damage inevitably causes increased cell death. To account for these findings, we propose a model that postulates the existence of a second radiation target. According to this model, radiation damage to DNA may be necessary to induce cell death, but DNA damage alone is not sufficient to kill cells. We infer from the survival response of irs-20 cells that damage to a second (non-DNA) structure is involved in cell death, and that this structure directly affects the repair of DNA and cell survival.     

Sequential exposures of mammalian cells to low- and high-LET radiations. II. As a function of cell-cycle stages

The synergistic effects of low- and high-LET radiations were further studied with partially synchronized Chinese hamster V79 cells. Principally, nearly monoenergetic 425 MeV/u neon ions and 570 MeV/u argon ions produced near the Bragg peak were employed as the high-LET radiations and 225 kVp X rays as the low-LET counterpart. It was found that the killing effect due to damage interaction after sequential irradiations with the particle beam and X rays varies throughout the cell cycle. The greatest effect was observed in late-S phase which was most resistant to either of the radiations. The effect was quantitatively less in the G1/S border and in G2. Effects on pure mitotic cells have not been investigated in this study. For all cell stages studied, a dose of high-LET particles modified the shape of the X-ray survival curve in a way similar to the modification predicted by an appropriately selected X-ray dose. This finding suggests that the mechanism for the synergistic effects is similar to that operating for sequential treatments with X rays alone. Experiments with an S population, either incubated at 37 degrees C or room temperature between fractionation of high- and low-LET radiation treatments further verified that the damage involved is a repairable type. At a certain fractionation interval (6 to 8 h) following a dose of high-LET treatment, initially asynchronous cells were found to be very sensitive to X-irradiation. It is noteworthy that the net killing measured at this "radiosensitive window" was as effective as the killing observed by "immediately" sequential treatments with the same doses of high- and low-LET radiations. Such a time window also existed when the order of the treatment sequence was reversed except that the time of occurrence was earlier and the window was broader. This sensitization effect may be explained by radiation-induced G2 arrest together with an increase of radiosensitivity as the previously irradiated cells progress into S phase. Radiotherapy strategies using combined high-LET and low-LET radiations for rapidly proliferative tumors are presented.     

Sensitivity of SP cell line of melanoma B16 to low- and high-ionizing radiation

Cancer stem cells (CSC) found in multiple tumor types and cancer cell lines were shown to be more resistant to low-LET radiation in comparison to other cancer cells. Therefore, CSC are supposed to determine the long-term effect of cancer therapy. Research into the CSC sensitivity to high-LET radiation is of great interest because of the advances in hadron therapy. The aim of this investigation is to compare CSC and other cancer cell sensitivity to the low- (60Co gamma-rays) and high-LET (neutron) radiation. To identify CSC, we used the low cytometry-based side population (SP) technique based on the CSC capacity to produce the efflux of the vital dye Hoechst 33342. SP and non SP cells were sorted and exposed to gamma and neutron radiation at doses of 1-10 Gy and 0.1-4.7 Gy, correspondingly. We applied the colony-formation test to examine the SP and non SP survival rate after irradiation. It was shown that the sensitivity of SP to gamma-irradiation was lower than that of other cells: D0 average values (+/- SE) made up 2.3 +/- 0.3 Gy and 1.4 +/- 0.2 Gy, correspondingly (p = 0.047). The survival rate of SP and non SP did not differ after neutron irradiation. The values of relative biological effectiveness of neutron radiation relative to gamma-radiation at the D10 level were 2.6 for SP and 2.1 for other cells. The obtained results justify for the first time a high efficiency of application of neutrons in radiotherapy from the point of view of CSC elimination.     

p53-independent downregulation of histone gene expression in human cell lines by high- and low-let radiation

Using microarrays to analyze differential gene expression as a function of p53 status and radiation quality, we observed downregulation of a large set of histone genes in p53 wild-type TK6 cells 24 h after exposure to equitoxic doses of high-LET (1.67 Gy 1 GeV/amu (56)Fe ions) or low-LET (2.5 Gy γ rays) radiation. Quantitative real-time PCR of specific subtypes of core (H2A, H2B, H3 and H4) and linker (H1) histones confirmed this result. DNA synthesis and histone gene expression are tightly coordinated during the S phase of the cell cycle, and both processes are regulated by cell cycle checkpoints in response to DNA damage caused by ionizing radiation. However, we observed similar repression of histone gene expression in both TK6 cells and their p53-null derivative NH32 after radiation exposure, although the histone gene expression was not decreased to the same extent in NH32 cells as it was in TK6 cells. We also found decreased histone gene expression that was dose- and time-dependent in the colon cancer cell line HCT116 and its p53-null derivative. These results show that both high- and low-LET radiation exposure negatively regulate histone gene expression in human lymphoblastoid and colon cancer cell lines independent of p53 status.     

Survivin expressions in human hepatoma HepG2 cells exposed to ionizing radiation of different LET

Survivin is a member of the inhibitors of apoptosis (IAP) protein family that interferes with post-mitochondrial events including activation of caspases. To examine the regulation of survivin expression in response to irradiation with different linear energy transfer (LET), human hepatoma HepG2 cells were irradiated in vitro with X-rays and carbon ions. Cellular sensitivities to low- and high-LET radiation were determined by colony formation. Survivin expression at mRNA and protein level were measured with RT-PCR and Western blot analyses, respectively. Radiation-induced cell cycle arrest and apoptosis were investigated with flow cytometry. We found that low-LET X-rays induced dose-dependent increases in survivin expression. After exposure to high-LET carbon ions, survivin expression gradually increased from 0 to 4 Gy, and then declined at 6 Gy. More pronounced survivin expression, stronger G(2)/M phase arrest was observed after exposure to carbon ions in comparison with X-rays at doses from 0 to 4 Gy. These observations indicate that there is a differential survivin expression in response to different LET radiations and the cycle arrest mechanism may be associated with it. In addition, our data on induction of apoptosis are compatible with the assumption that survivin expression induced by low-LET X-rays radiation may play a critical role in inhibiting apoptosis. However, after irradiation with ions, an anti-apoptotic function of survivin is not evident, possibly because of the serious damage produced by densely ionizing radiation.     

Dose-rate effect on the induction of HPRT mutants in human G0 lymphocytes exposed in vitro to gamma radiation

The influence of dose rate on expression time, cell survival and mutant frequency at the hypoxanthine-guanine phosphoribosyltransferase (HPRT) locus was evaluated in human G(0) peripheral blood lymphocytes exposed in vitro to gamma rays at low (0.0014 Gy/min) and high (0.85 Gy/min) dose rates. A cloning assay performed on different days of postirradiation incubation indicated an 8-day maximum expression period for the induction of HPRT mutants at both high and low dose rates. Cell survival increased markedly with decreasing dose rate, yielding D(0) values of 3.04 Gy and 1.3 Gy at low and high dose rates, respectively. The D(0) of 3.04 Gy obtained at low dose rate could be attributed to the repair of sublethal DNA damage taking place during prolonged exposure to low-LET radiation. Regression analysis of the mutant frequency yielded slopes of 12.35 x 10(-6) and 3.66 x 10(-6) mutants per gray at high and low dose rate, respectively. A dose and dose-rate effectiveness factor of 3.4 indicated a marked dose-rate effect on the induced HPRT mutant frequency. The results indicate that information obtained from in vitro measurements of dose-rate effects in human G(0) lymphocytes may be a useful parameter for risk estimation in radiation protection.     

In vitro evaluation of combined temozolomide and radiotherapy using X rays and high-linear energy transfer radiation for glioblastoma

High-linear energy transfer radiation offers superior biophysical properties over conventional radiotherapy and may have a great potential for treating radioresistant tumors, such as glioblastoma. However, very little pre-clinical data exists on the effects of high-LET radiation on glioblastoma cell lines and on the concomitant application of chemotherapy. This study investigates the in vitro effects of temozolomide in combination with low-energy protons and α particles. Cell survival, DNA damage and repair, and cell growth were examined in four human glioblastoma cell lines (LN18, T98G, U87 and U373) after treatment with either X rays, protons (LET 12.91 keV/μm), or α particles (LET 99.26 keV/μm) with or without concurrent temozolomide at clinically-relevant doses of 25 and 50 μM. The relative biological effectiveness at 10% survival (RBE(10)) increased as LET increased: 1.17 and 1.06 for protons, and 1.84 and 1.68 for α particles in the LN18 and U87 cell lines, respectively. Temozolomide administration increased cell killing in the O(6)-methylguanine DNA methyltransferase-methylated U87 and U373 cell lines. In contrast, temozolomide provided no therapeutic enhancement in the methylguanine DNA methyltransferase-unmethylated LN18 and T98G cell lines. In addition, the residual number of γ-H2AX foci at 24 h after treatment with radiation and concomitant temozolomide was found to be lower than or equal to that expected by DNA damage with either of the individual treatments. Kinetics of foci disappearance after X-ray and proton irradiation followed similar time courses; whereas, loss of γ-H2AX foci after α particle irradiation occurred at a slower rate than that by low-LET radiation (half-life 12.51-16.87 h). The combination of temozolomide with different radiation types causes additive rather than synergistic cytotoxicity. Nevertheless, particle therapy combined with chemotherapy may offer a promising alternative with the additional benefit of superior biophysical properties. It is also possible that new fractionation schedules could be designed to exploit the change in DNA repair kinetics when MGMT-methylated cells respond to high-LET radiation.     

Characteristics of DNA-binding proteins determine the biological sensitivity to high-linear energy transfer radiation

Non-homologous end-joining (NHEJ) and homologous recombination repair (HRR), contribute to repair ionizing radiation (IR)-induced DNA double-strand breaks (DSBs). Mre11 binding to DNA is the first step for activating HRR and Ku binding to DNA is the first step for initiating NHEJ. High-linear energy transfer (LET) IR (such as high energy charged particles) killing more cells at the same dose as compared with low-LET IR (such as X or γ rays) is due to inefficient NHEJ. However, these phenomena have not been demonstrated at the animal level and the mechanism by which high-LET IR does not affect the efficiency of HRR remains unclear. In this study, we showed that although wild-type and HRR-deficient mice or DT40 cells are more sensitive to high-LET IR than to low-LET IR, NHEJ deficient mice or DT40 cells are equally sensitive to high- and low-LET IR. We also showed that Mre11 and Ku respond differently to shorter DNA fragments in vitro and to the DNA from high-LET irradiated cells in vivo. These findings provide strong evidence that the different DNA DSB binding properties of Mre11 and Ku determine the different efficiencies of HRR and NHEJ to repair high-LET radiation induced DSBs.     

Induction of preneoplastic alterations by X rays and neutrons in exposed rat tracheas and isolated tracheal epithelial cells

The relative potential of high- and low-LET radiation to induce preneoplastic alterations in rat tracheal epithelial cells was evaluated using a combined in vivo-cell culture model. The capacity of X rays and high- and low-dose-rate neutrons to induce preneoplastic changes in isolated rat tracheal epithelial cells and in the intact tissue was compared. The presence of altered populations was determined in culture in terms of the frequency of tracheal epithelial cell populations which exhibit enhanced growth capacity in culture and in terms of the induction of persistent morphological alterations in exposed transplanted tracheas. Prior to assaying for altered cells, tracheal epithelial cells were irradiated as part of the intact tissue or as single cells. Low- and high-LET radiation induced similar maximum frequencies of altered cells when cultures were exposed as single cells, although high-LET radiation was more radiobiologically effective (RBE = 20) than low-LET radiation. The most marked difference between high- and low-LET radiation was observed after irradiation of the intact tissue. Damage induced by low-LET radiation, giving rise to altered populations, was modified in the intact tissue, whereas similar damage induced by high-LET radiation was apparently not.     

Depression of p53-independent Akt survival signals in human oral cancer cells bearing mutated p53 gene after exposure to high-LET radiation

Although mutations and deletions in the p53 tumor suppressor gene lead to resistance to low linear energy transfer (LET) radiation, high-LET radiation efficiently induces cell lethality and apoptosis regardless of the p53 gene status in cancer cells. Recently, it has been suggested that the induction of p53-independent apoptosis takes place through the activation of Caspase-9 which results in the cleavage of Caspase-3 and poly (ADP-ribose) polymerase (PARP). This study was designed to examine if high-LET radiation depresses serine/threonine protein kinase B (PKB, also known as Akt) and Akt-related proteins. Human gingival cancer cells (Ca9-22 cells) harboring a mutated p53 (mp53) gene were irradiated with 2 Gy of X-rays or Fe-ion beams. The cellular contents of Akt-related proteins participating in cell survival signaling were analyzed with Western Blotting 1, 2, 3 and 6h after irradiation. Cell cycle distributions after irradiation were assayed with flow cytometric analysis. Akt-related protein levels decreased when cells were irradiated with high-LET radiation. High-LET radiation increased G(2)/M phase arrests and suppressed the progression of the cell cycle much more efficiently when compared to low-LET radiation. These results suggest that high-LET radiation enhances apoptosis through the activation of Caspase-3 and Caspase-9, and suppresses cell growth by suppressing Akt-related signaling, even in mp53 bearing cancer cells.     

Monte carlo simulation of base and nucleotide excision repair of clustered DNA damage sites. II. Comparisons of model predictions to measured data

Clustered damage sites other than double-strand breaks (DSBs) have the potential to contribute to deleterious effects of ionizing radiation, such as cell killing and mutagenesis. In the companion article (Semenenko et al., Radiat. Res. 164, 180-193, 2005), a general Monte Carlo framework to simulate key steps in the base and nucleotide excision repair of DNA damage other than DSBs is proposed. In this article, model predictions are compared to measured data for selected low-and high-LET radiations. The Monte Carlo model reproduces experimental observations for the formation of enzymatic DSBs in Escherichia coli and cells of two Chinese hamster cell lines (V79 and xrs5). Comparisons of model predictions with experimental values for low-LET radiation suggest that an inhibition of DNA backbone incision at the sites of base damage by opposing strand breaks is active over longer distances between the damaged base and the strand break in hamster cells (8 bp) compared to E. coli (3 bp). Model estimates for the induction of point mutations in the human hypoxanthine guanine phosphoribosyl transferase (HPRT) gene by ionizing radiation are of the same order of magnitude as the measured mutation frequencies. Trends in the mutation frequency for low- and high-LET radiation are predicted correctly by the model. The agreement between selected experimental data sets and simulation results provides some confidence in postulated mechanisms for excision repair of DNA damage other than DSBs and suggests that the proposed Monte Carlo scheme is useful for predicting repair outcomes.     

Nanoscale analysis of clustered DNA damage after high-LET irradiation by quantitative electron microscopy – The heavy burden to repair

Low- and high-linear energy transfer (LET) ionising radiation are effective cancer therapies, but produce structurally different forms of DNA damage. Isolated DNA damage is repaired efficiently; however, clustered lesions may be more difficult to repair, and are considered as significant biological endpoints. We investigated the formation and repair of DNA double-strand breaks (DSBs) and clustered lesions in human fibroblasts after exposure to sparsely (low-LET; delivered by photons) and densely (high-LET; delivered by carbon ions) ionising radiation. DNA repair factors (pKu70, 53BP1, γH2AX, and pXRCC1) were detected using immunogold-labelling and electron microscopy, and spatiotemporal DNA damage patterns were analysed within the nuclear ultrastructure at the nanoscale level. By labelling activated Ku-heterodimers (pKu70) the number of DSBs was determined in electron-lucent euchromatin and electron-dense heterochromatin. Directly after low-LET exposure (5 min post-irradiation), single pKu70 dimers, which reflect isolated DSBs, were randomly distributed throughout the entire nucleus with a linear dose correlation up to 30 Gy. Most euchromatic DSBs were sensed and repaired within 40 min, whereas heterochromatic DSBs were processed with slower kinetics. Essentially all DNA lesions induced by low-LET irradiation were efficiently rejoined within 24 h post-irradiation. High-LET irradiation caused localised energy deposition within the particle tracks, and generated highly clustered DNA lesions with multiple DSBs in close proximity. The dimensions of these clustered lesions along the particle trajectories depended on the chromatin packing density, with huge DSB clusters predominantly localised in condensed heterochromatin. High-LET irradiation-induced clearly higher DSB yields than low-LET irradiation, with up to ∼500 DSBs per μm³ track volume, and large fractions of these heterochromatic DSBs remained unrepaired. Hence, the spacing and quantity of DSBs in clustered lesions influence DNA repair efficiency, and may determine the radiobiological outcome.     

Quantitative modelling of DNA damage using Monte Carlo track structure method

This paper presents data on modelling of DNA damage induced by electrons, protons and alpha-particles to provide an insight into factors which determine the biological effectiveness of radiations of high and low linear energy transfer (LET). These data include the yield of single- and double-strand breaks (ssb, dsb) and base damage in a cellular environment. We obtain a ratio of 4–15 for ssb:dsb for solid and cellular DNA and a preliminary ratio of about 2 for base damage to strand breakage. Data are also given on specific characteristics of damage at the DNA level in the form of clustered damage of varying complexity, that challenge the repair processes and if not processed adequately could lead to the observed biological effects. It is shown that nearly 30% of dsb are of complex form for low-LET radiation, solely by virtue of additional breaks, rising to about 70% for high-LET radiation. Inclusion of base damage increases the complex proportion to about 60% and 90% for low- and high-LET radiation, respectively. The data show a twofold increase in frequencies of complex dsb from low-LET radiation when base damage is taken into account. It is shown that most ssb induced by high-LET radiation have associated base damages, and also a substantial proportion is induced by low-energy electrons. Received: 20 September 1998 / Accepted in revised form: 15 December 1998