The difference in LET and ion species dependence for induction of initially measured and non-rejoined chromatin breaks in normal human fibroblasts

We studied the LET and ion species dependence of the induction of chromatin breaks measured immediately after irradiation as initially measured breaks and after 24 h postirradiation incubation (37 degrees C) as non-rejoined breaks in normal human fibroblasts with different heavy ions, such as carbon, neon, silicon and iron, generated by the Heavy Ion Medical Accelerator in Chiba (HIMAC) at the National Institute of Radiological Science (NIRS). Chromatin breaks were measured as an excess number of fragments of prematurely condensed chromosomes using premature chromosome condensation (PCC). The results showed that the number of excess fragments per cell per Gy for initially measured chromatin breaks was dependent on LET in the range from 13.3 to 113.1 keV/mum but was not dependent on ion species. On the other hand, the number of non-rejoined chromatin breaks detected after 24 h postirradiation incubation was clearly dependent on both LET and ion species. No significant difference was observed in the cross section for initially measured breaks, but a statistically significant difference was observed in the cross section for non-rejoined breaks among carbon, neon, silicon and iron ions. This suggests that the LET-dependent structure in the biological effects is reflected in biological consequences of repair processes.     

Truly incomplete and complex exchanges in prematurely condensed chromosomes of human fibroblasts exposed in vitro to energetic heavy ions

Confluent human fibroblast cells (AG1522) were irradiated with gamma rays, 490 MeV/nucleon silicon ions, or iron ions at either 200 or 500 MeV/nucleon. The cells were allowed to repair at 37 degrees C for 24 h after exposure, and a chemically induced premature chromosome condensation (PCC) technique was used to condense chromosomes in the G2 phase of the cell cycle. Incomplete and complex exchanges were analyzed in the irradiated samples. To verify that chromosomal breaks were truly unrejoined, chromosome aberrations were analyzed using a combination of whole-chromosome specific probes and probes specific for the telomere region of the chromosome. Results showed that the frequency of unrejoined chromosome breaks was higher after irradiation with the heavy ions of high LET, and consequently the ratio of incomplete to complete exchanges increased steadily with LET up to 440 keV/microm, the highest LET included in the present study. For samples exposed to 200 MeV/nucleon iron ions, chromosome aberrations were analyzed using the multicolor FISH (mFISH) technique, which allows identification of both complex and truly incomplete exchanges. Results of the mFISH study showed that 0.7 and 3 Gy iron ions produced similar ratios of complex to simple exchanges and incomplete to complete exchanges; these ratios were higher than those obtained after exposure to 6 Gy gamma rays. After 0.7 Gy of iron ions, most complex aberrations were found to involve three or four chromosomes, which is a likely indication of the maximum number of chromosome domains traversed by a single iron-ion track.     

High yields of isochromatid breaks and successive formation of chromosome exchanges may lead to reproductive cell death following high-LET irradiation

To clarify the relationship between cell death and chromosomal aberrations following exposure to heavy-charged ion particles beams, exponentially growing Human Salivary Gland Tumor cells (HSG cells) were irradiated with various kinds of high energy heavy ions; 13 keV/μm carbon ions as a low-LET charged particle radiation source, 120 keV/μm carbon ions and 440 keV/μm iron ions as high-LET charged particle radiation sources. X-rays (200 kVp) were used as a reference. Reproductive cell death was evaluated by clonogenic assays, and the chromatid aberrations in G2/M phase and their repairing kinetics were analyzed by the calyculin A induced premature chromosome condensation (PCC) method. High-LET heavy-ion beams introduced much more severe and un-repairable chromatid breaks and isochromatid breaks in HSG cells than low-LET irradiation. In addition, the continuous increase of exchange aberrations after irradiation occurred in the high-LET irradiated cells. The cell death, initial production of isochromatid breaks and subsequent formation of chromosome exchange seemed to be depend similarly on LET with a maximum RBE peak around 100–200 keV/μm of LET value. Conversely, un-rejoined isochromatid breaks or chromatid breaks/gaps seemed to be less effective in reproductive cell death. These results suggest that the continuous yield of chromosome exchange aberrations induced by high-LET ionizing particles is a possible reason for the high RBE for cell death following high-LET irradiation, alongside other chromosomal aberrations additively or synergistically.     

Repair of DNA damage induced by accelerated heavy ions in mammalian cells proficient and deficient in the non-homologous end-joining pathway

Human and rodent cells proficient and deficient in non-homologous end joining (NHEJ) were irradiated with X rays, 70 keV/microm carbon ions, and 200 keV/microm iron ions, and the biological effects on these cells were compared. For wild-type CHO and normal human fibroblast (HFL III) cells, exposure to iron ions yielded the lowest cell survival, followed by carbon ions and then X rays. NHEJ-deficient xrs6 (a Ku80 mutant of CHO) and 180BR human fibroblast (DNA ligase IV mutant) cells showed similar cell survival for X and carbon-ion irradiation (RBE = approximately 1.0). This phenotype is likely to result from a defective NHEJ protein because xrs6-hamKu80 cells (xrs6 cells corrected with the wild-type KU80 gene) exhibited the wild-type response. At doses higher than 1 Gy, NHEJ-defective cells showed a lower level of survival with iron ions than with carbon ions or X rays, possibly due to inactivation of a radioresistant subpopulation. The G(1) premature chromosome condensation (PCC) assay with HFL III cells revealed LET-dependent impairment of repair of chromosome breaks. Additionally, iron-ion radiation induced non-repairable chromosome breaks not observed with carbon ions or X rays. PCC studies with 180BR cells indicated that the repair kinetics after exposure to carbon and iron ions behaved similarly for the first 6 h, but after 24 h the curve for carbon ions approached that for X rays, while the curve for iron ions remained high. These chromosome data reflect the existence of a slow NHEJ repair phase and severe biological damage induced by iron ions. The auto-phosphorylation of DNA-dependent protein kinase catalytic subunits (DNA-PKcs), an essential NHEJ step, was delayed significantly by high-LET carbon- and iron-ion radiation compared to X rays. This delay was further emphasized in NHEJ-defective 180BR cells. Our results indicate that high-LET radiation induces complex DNA damage that is not easily repaired or is not repaired by NHEJ even at low radiation doses such as 2 Gy.     

Effect of linear energy transfer (LET) on the complexity of alpha-particle-induced chromosome aberrations in human CD34+ cells

The aim of this study was to assess the relative influence of the linear energy transfer (LET) of alpha particles on the complexity of chromosome aberrations in the absence of significant other differences in track structure. To do this, we irradiated human hemopoietic stem cells (CD34+) with alpha particles of various incident LETs (110-152 keV/microm, with mean LETs through the cell of 119-182 keV/microm) at an equi-fluence of approximately one particle/cell and assayed for chromosome aberrations by mFISH. Based on a single harvest time to collect early-division mitotic cells, complex aberrations were observed at comparable frequencies irrespective of incident LET; however, when expressed as a proportion of the total exchanges detected, their occurrence was seen to increase with increasing LET. Cycle analysis to predict theoretical DNA double-strand break rejoining cycles was also carried out on all complex chromosome aberrations detected. By doing this we found that the majority of complex aberrations are formed in single non-reducible cycles that involve just two or three different chromosomes and three or four different breaks. Each non-reducible cycle is suggested to represent "an area" of finite size within the nucleus where double-strand break repair occurs. We suggest that the local density of damage induced and the proximity of independent repair areas within the interphase nucleus determine the complexity of aberrations resolved in metaphase. Overall, the most likely outcome of a single nuclear traversal of a single alpha particle in CD34+ cells is a single chromosome aberration per damaged cell. As the incident LET of the alpha particle increases, the likelihood of this aberration being classed as complex is greater.     

Facilitated detection of chromosome break and repair at low levels of ionizing radiation by addition of wortmannin to G1-type PCC fusion incubation

We have measured rejoining kinetics of chromosome breaks using a modified cell fusion-based premature chromosome condensation (PCC) technique in confluent cultures of normal human fibroblasts irradiated at low doses of X-rays. In order to enhance the sensitivity of the fusion-based PCC assay, we added a DNA double strand break (DSB) repair inhibitor wortmannin during the incubation period for PCC/fusion process resulting in a significantly higher yield of G1-type chromosome breaks. The initial number of chromosome breaks (without repair) gave a linear dose response with about 10 breaks per cell per Gy which is about two times higher than the value with the conventional G1-type PCC method. The chromosome rejoining kinetics at 0.5 and 2.0 Gy X-rays reveal a bi-phasic curve with both a fast and a slow component. The fast component (0-30 min) is nearly identical for both doses, but the slow component for 2 Gy kinetics is much slower than that for 0.5 Gy, indicating that the process occurring during this period may be crucial for the ultimate fate of irradiated cells. The chromosome rejoining kinetics obtained here is similar to that of other methods of detecting DNA DSB repair such as the gammaH2AX assay. Our chromosome repair assay is useful for evaluating the accuracy of other assays measuring DNA DSB repair at doses equal or less than 0.5 Gy of ionizing radiation.     

Induction and rejoining of DNA double-strand breaks in normal human skin fibroblasts after exposure to radiation of different linear energy transfer: possible roles of track structure and chromatin organization

DNA double-strand breaks are nonrandomly induced by high-LET radiation. Differences in the induction and rejoining of DSBs after irradiation with ions having different LET were detected by fragment analysis. The data obtained indicate that the track structure of the traversing particle and its interaction with the different chromatin structures of the cellular DNA influence the yield as well as the distribution of the induced damage. The induction and rejoining of clustered DSBs induced by the same nitrogen ion fluence at LETs of 80-225 keV/microm were investigated by a detailed analysis of the DNA fragmentation patterns in normal human fibroblasts. The DSBs in the cells were allowed to rejoin during incubations for 0-20 h. Two separate pulsed-field gel electrophoresis protocols were used, optimized for separation of fragments in the size ranges 1-6 Mbp and 5 kbp-1.5 Mbp. A strong influence of LET on the level of DSB induction was evident. The DSB yield increased from 4.5 +/- 0.2 to 10.0 +/- 0.3 DSBs per particle traversal through the cell nucleus when LET increased from 80 to 225 keV/microm. Further, the size distribution of the DNA fragments showed a significant dependence on radiation quality, with an excess of fragments at 50-200 kbp and around 1 Mbp. Differences in repair kinetics were also evident, with slower rejoining for increasing LET, and the initial nonrandom fragment distributions were still present after 1 h of repair.     

LET and ion species dependence for cell killing in normal human skin fibroblasts

We studied the LET and ion species dependence of the RBE for cell killing to clarify the differences in the biological effects caused by the differences in the track structure that result from the different energy depositions for different ions. Normal human skin fibroblasts were irradiated with heavy-ion beams such as carbon, neon, silicon and iron ions that were generated by the Heavy Ion Medical Accelerator in Chiba (HIMAC) at the National Institute of Radiological Science (NIRS) in Japan. Cell killing was measured as reproductive cell death using a colony formation assay. The RBE-LET curves were different for carbon ions and for the other ions. The curve for carbon ions increased steeply up to around 98 keV/microm. The RBE of carbon ions at 98 keV/microm was 4.07. In contrast, the curves for neon, silicon and iron ions had maximum peaks around 180 keV/microm, and the RBEs at the peak position ranged from 3.03 to 3.39. When the RBEs were plotted as a function of Z*2/beta2 (where Z* is the effective charge and beta is the relative velocity of the ion) instead of LET, the discrepancies between the RBE-LET curves for the different ion beams were reduced, but branching of the RBE-Z*2/beta2 curves still remained. When the inactivation cross section was plotted as a function of either LET or Z*2/beta2, it increased with increasing LET. However, the inactivation cross section was always smaller than the geometrical cross section. These results suggest that the differences in the energy deposition track structures of the different ion sources have an effect on cell killing.     

Biological effectiveness of accelerated particles for the induction of chromosome damage measured in metaphase and interphase human lymphocytes

Chromosome aberrations were investigated in human lymphocytes after in vitro exposure to 1H-, 3He-, 12C-, 40Ar-, 28Si-, 56Fe-, or 197Au-ion beams, with LET ranging from approximately 0.4-1393 keV/microm in the dose range of 0.075-3 Gy. Dose-response curves for chromosome exchanges, measured at the first mitosis postirradiation using fluorescence in situ hybridization (FISH) with whole-chromosome probes, were fitted with linear or linear-quadratic functions. The relative biological effectiveness (RBE) was estimated from the initial slope of the dose-response curve for chromosomal damage with respect to low- or high-dose-rate gamma rays. Estimates of RBEmax values for mitotic spreads, which ranged from near 0.7 to 11.1 for total exchanges, increased with LET, reaching a maximum at about 150 keV/microm, and decreased with further increase in LET. RBEs for complex aberrations are undefined due to the lack of an initial slope for gamma rays. Additionally, the effect of mitotic delay on RBE values was investigated by measuring chromosome aberrations in interphase after chemically induced premature chromosome condensation (PCC), and values were up to threefold higher than for metaphase analysis.     

Heavy ion effects on cellular DNA: strand break induction and repair in cultured diploid lens epithelial cells

The relative biological effectiveness (RBE) for the induction of DNA strand breaks and the efficiency of repair of these breaks in cultured diploid bovine lens epithelial cells was measured, using accelerated heavy ions in the linear energy transfer (LET)-range up to 16,200 keV/micron. At LET values above 800 keV/micron, the number of DNA strand breaks induced per particle increases both with the atomic number of the projectile and with its kinetic energy. About 90 per cent or more of the strand breaks induced by ions with an LET of less than 10,000 keV/micron are repaired within 24 h. Repair kinetics show a dependence on the particle fluence (irradiation dose). At higher particle fluences a higher proportion of non-rejoined breaks is found, even after prolonged periods of incubation. At any LET value, repair is much slower after heavy-ion exposure than after X-irradiation. This is especially true for low energetic particles with a very high local density of energy deposition within the particle track. At the highest LET value (16,200 keV/micron), no significant repair is observed.     

Investigation of switch from ATM to ATR signaling at the sites of DNA damage induced by low and high LET radiation

Upon induction of DNA damage by ionizing radiation (IR), members of the phosphatidylinositol 3-kinase-like kinase family of proteins namely ataxia-telangiectasia mutated (ATM), DNA-PKcs, and ATM- and Rad3-related (ATR) maintain genomic integrity by mounting DNA damage response (DDR). Recent reports suggest that activation of ATM and ATR are oppositely regulated by the length of single stranded overhangs generated during end processing by nucleases at the break sites. These stretches of single stranded overhangs hold the clue for the transition from ATM to ATR signaling at broken DNA ends. We investigated whether differential processing of breaks induced by low and high LET radiation augments the phenomenon of switching from ATM to ATR kinase and hence a concomitant NHEJ to HR transition at the sites of DNA damage. 82-6 human fibroblasts were irradiated with 1 or 2 Gy of γ-rays and particle radiation of increasing LET in order to increase the complexity and variability of DNA double strand breaks (DSB) structures. The activation kinetics of ATM and ATR kinases along with their downstream substrates were determined utilizing Western blotting and immunofluorescence techniques. Our data provide evidence of a potential switch from ATM to ATR kinase signaling in cells treated with γ-rays at approximately 2 h post irradiation, with induction and completion of resection denoted by Rad51 foci resolution kinetics and observed with a significant decline of phosphorylated ATR kinase 8 h after IR. On the other hand, irradiation with high LET 600 MeV/u ⁵⁶Fe (180 keV/μm) and 170 MeV/u ²⁸Si (99 keV/μm) particles show a similar Rad51 foci decay kinetics, however, exhibiting prolonged resection, evident by the persistent phosphorylated ATM and ATR kinase until 24 h post irradiation. This residual effect, however, was significantly reduced for 250 MeV/u ¹⁶O particles of moderate LET (25 keV/μm) and absent for γ-rays. Hence, our results support the hypothesis that the transition from ATM to ATR signaling at DNA break sites is extended for longer periods of time, indicated by sustained resection due to the complex type of damage induced, a hallmark of high LET radiation, which may contribute to its increased biological effectiveness.     

Chromosomal radiosensitivity of human breast carcinoma cells and blood lymphocytes following photon and proton exposures

Breast carcinomas (BC) are among the most frequent cancers in women. Studies on radiosensitivity and ionizing radiation response of BC cells are scarce and mainly focused on intrinsic molecular mechanisms but do not include clinically relevant features as chromosomal rearrangements important for radiotherapy. The main purpose of this study was to compare the ionizing radiation response and efficiency of repair mechanisms of human breast carcinoma cells (Cal 51) and peripheral blood lymphocytes (PBL) for different doses and radiation qualities (⁶⁰Co γ-rays, 150 MeV and spread-out Bragg peak (SOBP) proton beams). The radiation response functions obtained using the conventional metaphase assay and premature chromosome condensation (PCC) technique enabled us to determine the number of chromosomal breaks at different time after irradiation. Both cytogenetic assays used confirmed the higher biological radiosensitivity for proton beams in tumor cells compared to PBL, corresponding to higher values of the linear LQ parameter α. additionally, the ratio of the LQ parameters β/α describing efficiency of the repair mechanisms, obtained for chromosome aberrations, showed higher numbers for PBL than for Cal 51 for all exposures. Similar results were observed for the ratio of PCC breaks determined directly after irradiation to that obtained 12 h later. This parameter (t0/t12) showed faster decrease of the repair efficiency with increasing LET value for Cal 51 cells. This finding supports the use of the proton therapy for breast cancer patients.

     

Long-term consequences of radiation-induced bystander effects depend on radiation quality and dose and correlate with oxidative stress

Widespread evidence indicates that exposure of cell populations to ionizing radiation results in significant biological changes in both the irradiated and nonirradiated bystander cells in the population. We investigated the role of radiation quality, or linear energy transfer (LET), and radiation dose in the propagation of stressful effects in the progeny of bystander cells. Confluent normal human cell cultures were exposed to low or high doses of 1GeV/u iron ions (LET ～ 151 keV/μm), 600 MeV/u silicon ions (LET ～ 51 keV/μm), or 1 GeV protons (LET ～ 0.2 keV/μm). Within minutes after irradiation, the cells were trypsinized and co-cultured with nonirradiated cells for 5 h. During this time, irradiated and nonirradiated cells were grown on either side of an insert with 3-μm pores. Nonirradiated cells were then harvested and allowed to grow for 20 generations. Relative to controls, the progeny of bystander cells that were co-cultured with cells irradiated with iron or silicon ions, but not protons, exhibited reduced cloning efficiency and harbored higher levels of chromosomal damage, protein oxidation and lipid peroxidation. This correlated with decreased activity of antioxidant enzymes, inactivation of the redox-sensitive metabolic enzyme aconitase, and altered translation of proteins encoded by mitochondrial DNA. Together, the results demonstrate that the long-term consequences of the induced nontargeted effects greatly depend on the quality and dose of the radiation and involve persistent oxidative stress due to induced perturbations in oxidative metabolism. They are relevant to estimates of health risks from exposures to space radiation and the emergence of second malignancies after radiotherapy.     

Influence of radiation quality on the yield of DNA strand breaks in SV40 DNA irradiated in solution.

Using highly energetic particles to irradiate plasmid DNA in aerobic aqueous solution, we have compiled an extensive database on how yields of DNA single- and double-strand breaks (SSBs and DSBs) vary with radiation quality. This study was performed in a low-scavenging buffer system and covers a wide range of ion species (helium to uranium) and LETs (5 to 16,000 keV/microm). For LETs up to around 40 keV/microm for SSBs and 400 keV/microm for DSBs, the total energy deposition determines cross section. At higher LET, cross sections level off and individual plateaus for particles of different atomic numbers are observed. For each ion species this is more pronounced and occurs at lower LET for SSBs than for DSBs, leading to an increase in the DSB:SSB ratio from 1:70 for X rays to 1:6 at 500 keV/microm. At this LET, the influence of track structure becomes evident, with high local concentrations of ionization events favoring the formation of DSBs and also intratrack recombination reactions. For lower-energy ions, a saturation in production of measurable DSBs is apparent, due to correlated lesion induction within densely ionizing particle tracks. For very heavy low-energy ions, both SSB and DSB cross sections decrease with particle velocity at nearly constant LET, forming individual hooked curves when plotted as a function of LET.     

Simulation of DNA damage after proton irradiation

The biophysical radiation track simulation model PARTRAC was improved by implementing new interaction cross sections for protons in water. Computer-simulated tracks of energy deposition events from protons and their secondary electrons were superimposed on a higher-order DNA target model describing the spatial coordinates of the whole genome inside a human cell. Induction of DNA double-strand breaks was simulated for proton irradiation with LET values between 1.6 and 70 keV/microm and various reference radiation qualities. The yield of DSBs after proton irradiation was found to rise continuously with increasing LET up to about 20 DSBs per Gbp and Gy, corresponding to an RBE up to 2.2. About half of this increase resulted from a higher yield of DSB clusters associated with small fragments below 10 kbp. Exclusion of experimentally unresolved multiple DSBs reduced the maximum DSB yield by 30% and shifted it to an LET of about 40 keV/microm. Simulated fragment size distributions deviated significantly from random breakage distributions over the whole size range after irradiation with protons with an LET above 10 keV/microm. Determination of DSB yields using equations derived for random breakage resulted in an underestimation by up to 20%. The inclusion of background fragments had only a minor influence on the distribution of the DNA fragments induced by radiation. Despite limited numerical agreement, the simulations reproduced the trends in proton-induced DNA DSBs and fragment induction found in recent experiments.     

Cytogenetic effects of densely ionising radiation in human lymphocytes: impact of cell cycle delays

The classical cytogenetic assay to estimate the dose to which an individual has been exposed relies on the measurement of chromosome aberrations in lymphocytes at the first post-irradiation mitosis 48 h after in vitro stimulation. However, evidence is accumulating that this protocol results in an underestimation of the cytogenetic effects of high LET radiation due to a selective delay of damaged cells. To address this issue, human lymphocytes were irradiated with C-ions (25-mm extended Bragg peak, LET: 60-85 keV/ micro m) and aberrations were measured in cells reaching the first mitosis after 48, 60, 72 and 84 h and in G2-phase cells collected after 48 h by calyculin A induced premature chromosome condensation (PCC). The results were compared with recently published data on the effects of X-rays and 200 MeV/u Fe-ions (LET: 440 keV/ micro m) on lymphocytes of the same donor (Ritter et al., 2002a). The experiments show clearly that the aberration yield rises in first-generation metaphase (M1) with culture time and that this effect increases with LET. Obviously, severely damaged cells suffer a prolonged arrest in G2. The mitotic delay has a profound effect on the RBE: RBE values estimated from the PCC data were about two times higher than those obtained by conventional metaphase analysis at 48 h. Altogether, these observations argue against the use of single sampling times to quantify high LET induced chromosomal damage in metaphase cells.     

Accumulation of the cell cycle regulators TP53 and CDKN1A (p21) in human fibroblasts after exposure to low- and high-LET radiation

The accumulation of the cell cycle regulators TP53 and CDKN1A (p21/CIP1/WAF1) was investigated after exposure to X rays and carbon ions (170 keV microm(-1)) and xenon, bismuth and uranium ions (8900-15,000 keV microm(-1)) in normal human fibroblasts. The influence of the overall dose and the LET of these radiation types was studied systematically and the kinetics of the cell response was followed up to 24 h after exposure. The accumulation of TP53 protein was dependent on the dose and the LET, and TP53 levels declined to lower levels for all radiation types within 24 h after exposure. CDKN1A levels increased and peaked at 3 to 6 h after exposure. The persisting level of this protein at 24 h was strongly dependent on the dose and the LET for X rays and carbon ions. The exposure to very high-LET ions (8900-15,000 keV microm(-1)) did not lead to a further increase in CDKN1A, suggesting a saturation effect for the induction of this protein. The cellular effects of elevated CDKN1A after particle irradiation are discussed.     

Microdosimetric measurements and estimation of human cell survival for heavy-ion beams

The microdosimetric spectra for high-energy beams of photons and proton, helium, carbon, neon, silicon and iron ions (LET = 0.5-880 keV/microm) were measured with a spherical-walled tissue-equivalent proportional counter at various depths in a plastic phantom. Survival curves for human tumor cells were also obtained under the same conditions. Then the survival curves were compared with those estimated by a microdosimetric model based on the spectra and the biological parameters for each cell line. The estimated alpha terms of the liner-quadratic model with a fixed beta value reproduced the experimental results for cell irradiation for ion beams with LETs of less than 450 keV/microm, except in the region near the distal peak.     

Spectrum of complex DNA damages depends on the incident radiation

Ionizing radiation induces bistranded clustered damages--two or more abasic sites, oxidized bases and strand breaks on opposite DNA strands within a few helical turns. Since clusters are refractory to repair and are potential sources of double-strand breaks (DSBs), they are potentially lethal and mutagenic. Although induction of single-strand breaks (SSBs) and isolated lesions has been studied extensively, little is known about the factors affecting induction of clusters other than DSBs. To determine whether the type of incident radiation could affect the yields or spectra of specific clusters, we irradiated genomic T7 DNA, a simple 40-kbp linear, blunt-ended molecule, with ion beams [iron (970 MeV/nucleon), carbon (293 MeV/nucleon), titanium (980 MeV/nucleon), silicon (586 MeV/nucleon), protons (1 GeV/nucleon)] or 100 kVp X rays and then quantified DSBs, Fpg-oxypurine clusters and Nfo-abasic clusters using gel electrophoresis, electronic imaging and number average length analysis. The yields (damages/Mbp Gy(-1)) of all damages decreased with increasing linear energy transfer (LET) of the radiation. The relative frequencies of DSBs compared to abasic and oxybase clusters were higher for the charged particles-including the high-energy, low-LET protons-than for the ionizing photons.     

The effects of low-dose, high-LET radiation exposure on three models of behavior in C57BL/6 mice

To investigate the behavioral consequences of exposure to whole-body irradiation such as might occur for astronauts during space flight, female C57BL/6 mice were exposed to 0, 0.1, 0.5 or 2 Gy accelerated iron ions (56Fe, Z = 26, beta = 0.9, LET = 148.2 keV/microm) of 1 GeV per nucleon using the Alternating Gradient Synchrotron at the Brookhaven National Laboratory. Animal testing began 2 weeks after exposure and continued for 8 weeks. Under these conditions, there were few significant effects of radiation on open-field, rotorod or acoustic startle activities at any of the times examined. The lack of radiation effects in these behavioral models appears to offer reassurance to NASA mission designers. These results suggest that there may be negligible effects of HZE radiation on many behaviors during a 2-8-week period immediately after radiation.