Comparative radiation tolerance based on the induction of DNA double-strand breaks in tobacco BY-2 cells and CHO-K1 cells irradiated with gamma rays

Higher plants are generally more tolerant to ionizing radiation than mammals. To explore the radiation tolerance of higher plants, the induction of DNA double-strand breaks (DSBs) by gamma rays was investigated in tobacco BY-2 cells and compared with that in Chinese hamster ovary (CHO)-K1 cells as a reference. This is the first examination of radiation-induced DSBs in a higher plant cell. The resulting DNA fragments were separated by pulsed-field gel electrophoresis and stained with SYBR Green I. The initial yield of DSBs was then quantified from the fraction of DNA fragments shorter than 1.6 Mbp based on the assumption of random distribution of DSBs. The DSB yield in tobacco BY-2 cells (2.0 +/- 0.1 DSBs Gbp(-1) Gy(-1)) was only one-third of that in CHO-K1 cells. Furthermore, the calculated number of DSBs per diploid cell irradiated with gamma rays at the mean lethal dose was five times greater in BY-2 cells (263 +/- 13) than in CHO-K1 cells. These results suggest that the radiation tolerance of BY-2 cells appears to be due not only to a lower induction of DNA damage but also to a more efficient repair of the induced DNA damage.     

Spatial distribution of radiation-induced double-strand breaks in plasmid DNA as resolved by atomic force microscopy

Atomic force microscopy (AFM) has been used to directly visualize, size and compare the DNA fragments resulting from exposure to low- and high-LET radiation. Double-stranded pUC-19 plasmid ("naked") DNA samples were irradiated by electron-beam or reactor neutron fluxes with doses ranging from 0.9 to 10 kGy. AFM scanning in the tapping mode was used to image and measure the DNA fragment lengths (ranging from a few bp up to 2864 bp long). Double-strand break (DSB) distributions resulting from high-LET neutron and lower-LET electron irradiation revealed a distinct difference between the effects of these two types of radiation: Low-LET radiation-induced DSBs are distributed more uniformly along the DNA, whereas a much larger proportion of neutron-induced DSBs are distributed locally and densely. Furthermore, comparisons with predictions of a random DSB model of radiation damage show that neutron-induced DSBs deviate more from the model than do electron-induced DSBs. In summary, our high-resolution AFM measurements of radiation-induced DNA fragment-length distributions reveal an increased number of very short fragments and hence clustering of DSBs induced by the high-LET neutron radiation compared with low-LET electron radiation and a random DSB model prediction.     

Chromatin structure in double strand break repair

Cells are under constant assault by endogenous and environmental DNA damaging agents. DNA double strand breaks (DSBs) sever entire chromosomes and pose a major threat to genome integrity as a result of chromosomal fragment loss or chromosomal rearrangements. Exogenous factors such as ionizing radiation, crosslinking agents, and topoisomerase poisons, contribute to break formation. DSBs are associated with oxidative metabolism, form during the normal S phase, when replication forks collapse and are generated during physiological processes such as V(D)J recombination, yeast mating type switching and meiosis. It is estimated that in mammalian cells ∼10 DSBs per cell are formed daily. If left unrepaired DSBs can lead to cell death or deregulated growth, and cancer development. Cellular response to DSB damage includes mechanisms to halt the progression of the cell cycle and to restore the structure of the broken chromosome. Changes in chromatin adjacent to DNA break sites are instrumental to the DNA damage response (DDR) with two apparent ends: to control compaction and to bind repair and signaling molecules to the lesion. Here, we review the key findings related to each of these functions and examine their cross-talk.     

Locations of radiation-produced DNA double strand breaks along chromosomes: a stochastic cluster process formalism.

Ionizing radiation produces DNA double strand breaks (DSBs) in chromosomes. For densely ionizing radiation, the DSBs are not spaced randomly along a chromosome: recent data for size distributions of DNA fragments indicate break clustering on kbp-Mbp scales. Different DSB clusters on a chromosome are typically made by different, statistically independent, stochastically structured radiation tracks, and the average number of tracks involved can be small. We therefore model DSB positions along a chromosome as a stationary Poisson cluster process, i.e. a stochastic process consisting of secondary point processes whose locations are determined by a primary point process that is Poisson. Each secondary process represents a break cluster, typically consisting of 1-10 DSBs in a comparatively localized stochastic pattern determined by chromatin geometry and radiation track structure. Using this Poisson cluster process model, which we call the randomly located clusters (RLC) formalism, theorems are derived for how the DNA fragment-size distribution depends on radiation dose. The RLC dose-response relations become non-linear when the dose becomes so high that DSB clusters from different tracks overlap or adjoin closely. The RLC formalism generalizes previous models, fits current data adequately and facilitates mechanistically based extrapolations from high-dose experiments to the much lower doses of interest for most applications.     

DNA double-strand break misrejoining after exposure of primary human fibroblasts to CK characteristic X rays, 29 kVp X rays and 60Co gamma rays

The efficiency of ionizing photon radiation for inducing mutations, chromosome aberrations, neoplastic cell transformation, and cell killing depends on the photon energy. We investigated the induction and rejoining of DNA double-strand breaks (DSBs) as possible contributors for the varying efficiencies of different photon energies. A specialized pulsed-field gel electrophoresis assay based on Southern hybridization of single Mbp genomic restriction fragments was employed to assess DSB induction and rejoining by quantifying the restriction fragment band. Unrejoined and misrejoined DSBs were determined in dose fractionation protocols using doses per fraction of 2.2 and 4.4 Gy for CK characteristic X rays, 4 and 8 Gy for 29 kVp X rays, and 5, 10 and 20 Gy for 60Co gamma rays. DSB induction by CK characteristic X rays was about twofold higher than for 60Co gamma rays, whereas 29 kVp X rays showed only marginally elevated levels of induced DSBs compared with 60Co gamma rays (a factor of 1.15). Compared with these modest variations in DSB induction, the variations in the levels of unrejoined and misrejoined DSBs were more significant. Our results suggest that differences in the fidelity of DSB rejoining together with the different efficiencies for induction of DSBs can explain the varying biological effectiveness of different photon energies.     

Influence of chromatin structure on induction of double-strand breaks in mammalian cells irradiated with DNA-incorporated 125I

In this study the induction of double-strand breaks (DSBs) was investigated in Chinese hamster V79-379A cells irradiated with the Auger-electron emitter (125)I incorporated into DNA. The role of chromatin organization was studied by pulse-labeling synchronized cells with (125)IdU before decay accumulation in early or late S phase. Pulsed-field gel electrophoresis and fragment-size analysis were used to quantify the distribution of DNA fragments in irradiated intact cells and naked DNA as well as in DNA from asynchronously labeled cultures in a different scavenging environment. The results show that in intact cells, after accumulation of decays at -70 degrees C in the presence of 10% DMSO, almost four times more DSBs were induced in late S phase compared with early S phase and the fragment distribution was clearly non-random with an excess of fragments <0.2 Mbp. The DSB yield was 0.6 DSB/cell and decay for cells irradiated in early S phase and 2.3 DSBs/cell and decay for cells irradiated in late S phase. When similar experiments were performed on naked genomic DNA or intact cells irradiated with gamma rays, the difference in yield was not as prominent. These data imply a role of chromatin organization in the induction of DSBs by DNA-incorporated (125)I. In summary, the results presented here suggest that the yield of DSBs as well as the fragment distribution induced by (125)IdU decay may vary significantly depending on the chromatin organization during S phase and the labeling procedure used.     

Inhibition of homologous recombination by hyperthermia shunts early double strand break repair to non-homologous end-joining

In S and G2 phase mammalian cells DNA double strand breaks (DSBs) can potentially be repaired by homologous recombination (HR) or non-homologous end-joining (NHEJ). Results of several studies suggest that these two mechanistically distinct repair pathways can compete for DNA ends. Because HR and NHEJ differ with respect to error susceptibility, generation of chromosome rearrangements, which are potentially carcinogenic products of DSB repair, may depend on the pathway choice. To investigate this hypothesis, the influence of HR and NHEJ inhibition on the frequencies of chromosome aberrations in G2 phase cells was investigated. SW-1573 and RKO cells were treated with mild (41 °C) hyperthermia in order to disable HR and/or NU7441/cisplatin to inactivate NHEJ and frequencies of chromosomal fragments (resulting from unrepaired DSBs) and translocations (products of erroneous DSB rejoining) were studied using premature chromosome condensation (PCC) combined with fluorescence in situ hybridization (FISH).It is shown here that temporary inhibition of HR by hyperthermia results in increased frequency of ionizing-radiation (IR)-induced chromosomal translocations and that this effect is abrogated by NU7441- or cisplatin-mediated inhibition of NHEJ. The results suggest that in the absence of HR, DSB repair is shifted to the error-prone NHEJ pathway resulting in increased frequencies of chromosomal rearrangements. These results might be of consequence for clinical cancer treatment approaches that aim at inhibition of one or more DSB repair pathways.     

DNA double-strand break and chromosomal rejoining defects with misrejoining in Nijmegen breakage syndrome cells

NBS1-deficient cells exhibit pronounced radiosensitivity and defects in chromosome integrity after ionizing radiation (IR) exposure, yet show only a minor defect in DNA double-strand break (DSB) rejoining, leaving an as yet unresolved enigma as to the nature of the radiosensitivity of these cells. To further investigate the relationship between radiosensitivity, DSB repair, and chromosome stability, we have compared cytological and molecular assays of DSB misrejoining and repair in NBS1-defective, wild type, and NBS1-complemented cells after IR damage. Our findings suggest a subtle defect in overall DSB rejoining in NBS1-defective cells and uniquely also reveal reduced ability of NBS1-defective cells to rejoin correct ends of DSBs. In agreement with published results, one of two different NBS1-defective cell lines showed a slight defect in overall rejoining of DSBs compared to its complemented counterpart, whereas another NBS line did not show any difference from wild type cells. Significant defects in the correct rejoining of DSBs compared to their respective controls were observed for both NBS1-defective lines. The defect in DSB rejoining and the increased misrejoining detected at the molecular level were also reflected in higher levels of fragments and translocations, respectively, at the chromosomal level. This work provides both molecular and cytological evidence that NBS1-deficient cells have defects in DSB processing and reveals that these molecular events can be manifest cytologically.     

A non-radioactive, PFGE-based assay for low levels of DNA double-strand breaks in mammalian cells

A PFGE method was adapted to measure DNA double-strand breaks (DSBs) in mammalian cells after low (0-25 Gy) doses of ionising radiation. Instead of radionuclide incorporation, DNA staining in the gel by SYBR-Gold was used, which lowered the background of DNA damage and could be applied to non-cycling cells. DSB level was defined as a product of a fraction of DNA released to the gel (FR) and a number of DNA fragments in the gel (DNA(fragm)) and expressed as a percentage above control value. The slope of the dose-response curve was two-fold higher compared to that with FR alone as DSB level indicator (31.4 versus 15.6% per Gy). Two alternative ways were proposed to determine the total amount of DNA, used for FR calculation: measurement of DNA content in a plug not subjected to electrophoresis, with the use of Pico-Green, or estimation of DNA released to the gel from a plug irradiated with 600 Gy of gamma-rays. The limit of DSB detection was 0.25 Gy for human G1-lymphocytes and 0.5-1 Gy for asynchronous cultures of human glioma M059 K and J or mouse lymphoma L5178Y-R and -S cells. Specificity of our PFGE assay to DSB was confirmed by the fact that no damage was detected after treatment of the cells with H(2)O(2), an inducer of single-strand DNA breaks (SSBs). On the contrary, the H(2)O(2) inflicted damage was detected by neutral comet assay, attaining 160% above control (equivalent to 2.5 Gy of X-radiation). DSB rejoining, measured in cells after X-irradiation with a dose of 10 Gy, generally proceeded faster than that measured previously after higher (30-50 Gy) doses of ionising radiation. Clearly seen were defects in DSB rejoining in radiosensitive M059 J and L5178Y-S cells compared to their radioresistant counterparts, M059 K and L5178Y-R. In some cell lines, a secondary post-irradiation increase in DSB levels was observed. The possibility is considered that these additional DSBs may accumulate during processing of non-DSB clustered DNA damage or/and represent early apoptotic events.     

Mechanisms of DNA double strand break repair and chromosome aberration formation

It is widely accepted that unrepaired or misrepaired DNA double strand breaks (DSBs) lead to the formation of chromosome aberrations. DSBs induced in the DNA of higher eukaryotes by endogenous processes or exogenous agents can in principle be repaired either by non-homologous endjoining (NHEJ), or homology directed repair (HDR). The basis on which the selection of the DSB repair pathway is made remains unknown but may depend on the inducing agent, or process. Evaluation of the relative contribution of NHEJ and HDR specifically to the repair of ionizing radiation (IR) induced DSBs is important for our understanding of the mechanisms leading to chromosome aberration formation. Here, we review recent work from our laboratories contributing to this line of inquiry. Analysis of DSB rejoining in irradiated cells using pulsed-field gel electrophoresis reveals a fast component operating with half times of 10-30 min. This component of DSB rejoining is severely compromised in cells with mutations in DNA-PKcs, Ku, DNA ligase IV, or XRCC4, as well as after chemical inhibition of DNA-PK, indicating that it reflects classical NHEJ; we termed this form of DSB rejoining D-NHEJ to signify its dependence on DNA-PK. Although chemical inhibition, or mutation, in any of these factors delays processing, cells ultimately remove the majority of DSBs using an alternative pathway operating with slower kinetics (half time 2-10 h). This alternative, slow pathway of DSB rejoining remains unaffected in mutants deficient in several genes of the RAD52 epistasis group, suggesting that it may not reflect HDR. We proposed that it reflects an alternative form of NHEJ that operates as a backup (B-NHEJ) to the DNA-PK-dependent (D-NHEJ) pathway. Biochemical studies confirm the presence in cell extracts of DNA end joining activities operating in the absence of DNA-PK and indicate the dominant role for D-NHEJ, when active. These observations in aggregate suggest that NHEJ, operating via two complementary pathways, B-NHEJ and D-NHEJ, is the main mechanism through which IR-induced DSBs are removed from the DNA of higher eukaryotes. HDR is considered to either act on a small fraction of IR induced DSBs, or to engage in the repair process at a step after the initial end joining. We propose that high speed D-NHEJ is an evolutionary development in higher eukaryotes orchestrated around the newly evolved DNA-PKcs and pre-existing factors. It achieves within a few minutes restoration of chromosome integrity through an optimized synapsis mechanism operating by a sequence of protein-protein interactions in the context of chromatin and the nuclear matrix. As a consequence D-NHEJ mostly joins the correct DNA ends and suppresses the formation of chromosome aberrations, albeit, without ensuring restoration of DNA sequence around the break. B-NHEJ is likely to be an evolutionarily older pathway with less optimized synapsis mechanisms that rejoins DNA ends with kinetics of several hours. The slow kinetics and suboptimal synapsis mechanisms of B-NHEJ allow more time for exchanges through the joining of incorrect ends and cause the formation of chromosome aberrations in wild type and D-NHEJ mutant cells.     

Relative biological effectiveness of the alpha-particle emitter (211)At for double-strand break induction in human fibroblasts

The purpose of this study was to quantify and to determine the distribution of DNA double-strand breaks (DSBs) in human cells irradiated in vitro and to evaluate the relative biological effectiveness (RBE) of the alpha-particle emitter (211)At for DSB induction. The influence of the irradiation temperature on the induction of DSBs was also investigated. Human fibroblasts were irradiated as intact cells with alpha particles from (211)At, (60)Co gamma rays and X rays. The numbers and distributions of DSBs were determined by pulsed-field gel electrophoresis with fragment analysis for separation of DNA fragments in sizes 10 kbp-5.7 Mbp. A non-random distribution was found for DSB induction after irradiation with alpha particles from (211)At, while irradiation with low-LET radiation led to more random distributions. The RBEs for DSB induction were 2.1 and 3.1 for (60)Co gamma rays and X rays as the reference radiation, respectively. In the experiments studying temperature effects, nuclear monolayers were irradiated with (211)At alpha particles or (60)Co gamma rays at 2 degrees C or 37 degrees C and intact cells were irradiated with (211)At alpha particles at the same temperatures. The dose-modifying factor (DMF(temp)) for irradiation of nuclear monolayers at 37 degrees C compared with 2 degrees C was 1.7 for (211)At alpha particles and 1.6 for (60)Co gamma rays. No temperature effect was observed for intact cells irradiated with (211)At. In conclusion, irradiation with alpha particles from (211)At induced two to three times more DSB than gamma rays and X rays.     

Clusters of DNA double-strand breaks induced by different doses of nitrogen ions for various LETs: experimental measurements and theoretical analyses

The yields and clustering of DNA double-strand breaks (DSBs) were investigated in normal human skin fibroblasts exposed to gamma rays or to a wide range of doses of nitrogen ions with various linear energy transfers (LETs). Data obtained by pulsed-field gel electrophoresis on the dose and LET dependence of DNA fragmentation were analyzed with the randomly located clusters (RLC) formalism. The formalism considers stochastic clustering of DSBs along a chromosome due to chromatin structure, particle track structure, and multitrack action. The relative biological effectiveness (RBE) for the total DSB yield did not depend strongly on LET, but particles with higher LET produced higher fractions of small DNA fragments, corresponding in the formalism to an increase in the average number of DSBs per DSB cluster. The results are consistent with the idea that DSB clustering along chromosomes is what leads to large RBEs of high-LET radiations for major biological end points. At a given dose, large fragments are less affected by the variability in LET than small fragments, suggesting that the two free ends in large fragments are often produced by two different tracks. The formalism successfully described an extra increase in small DNA fragments as dose increases and a related decrease in large fragments, mainly due to interlacing of DSB clusters produced along a chromosome by different tracks, since interlacing cuts larger DNA fragments into smaller ones.     

Two-lesion kinetic model of double-strand break rejoining and cell killing

Radiobiological models, such as the lethal and potentially lethal (LPL) model and the repair-misrepair (RMR) model, have been reasonably successful at explaining the cell killing effects of radiation. However, the models have been less successful at relating cell killing to the formation, repair and misrepair of double-strand breaks (DSBs), which are widely accepted as the main type of DNA damage responsible for radiation-induced cell killing. A fully satisfactory model should be capable of predicting cell killing for a wide range of exposure conditions using a single set of model parameters. Moreover, these same parameters should give realistic estimates for the initial DSB yield, the DSB rejoining rate, and the residual number of unrepaired DSBs after all repair is complete. To better link biochemical processing of the DSB to cell killing, a two-lesion kinetic (TLK) model is proposed. In the TLK model, the family of all possible DSBs is subdivided into simple and complex DSBs, and each kind of DSB may have its own repair characteristics. A unique aspect of the TLK model is that break ends associated with both kinds of DSBs are allowed to interact in pairwise fashion to form irreversible lethal and nonlethal damages. To test the performance of the TLK model, nonlinear optimization methods are used to calibrate the model based on data for the survival of CHO cells for an extensive set of single-dose and split-dose exposure conditions. Then some of the postulated mechanisms of action are tested by comparing measured and predicted estimates of the initial DSB yield and the rate of DSB rejoining. The predictions of the TLK model for CHO cell survival and the initial DSB yield and rejoining rate are all shown to be in good agreement with the measured data. Studies suggest a yield of about 25 DSBs Gy(-1) cell(-1). About 20 DSBs Gy(-1) cell(-1) are rejoined quickly (15-min repair half-time), and 4 to 6 DSBs Gy(-1) cell(-1) are rejoined very slowly (10- to 15-h repair half-time). Both the slowly and fast-rejoining DSBs make substantial contributions to the killing of CHO cells by radiation. Although the TLK model provides a much more satisfactory formalism to relate biochemical processing of DSBs to cell killing than did the earlier kinetic models, some small differences among the measured and predicted CHO cell survival and DSB rejoining data suggest that additional factors and processes not considered in the present work may affect biochemical processing of DSBs and hence cell killing.     

Chromosome segregation and double-strand break repair - a complex connection

Genome stability requires correct chromosome segregation and DNA repair. Failure of these processes leads to cell death or accumulation of chromosomal aberrations, as often observed in tumor cells. An increasing number of observations indicate that segregation and DNA double-strand break (DSB) repair are functionally connected by the Cohesin and Smc5/6 protein complexes. Through their interaction with the duplicated genome, these complexes play essential roles in both chromosome segregation and repair by sister chromatid recombination. Both are also recruited to DSBs, and their chromosomal association is similarly regulated. Interestingly, recent studies of Cohesin suggest that DSB formation could promote proper mitotic chromosome segregation. This is reminiscent of segregation in meiotic cells, which is facilitated by break-induced chromosomal tethering.     

In situ visualization of DSBs to assess the extranuclear/extracellular effects induced by low-dose alpha-particle irradiation

Extranuclear/extracellular effects may have a significant effect on low-dose radiation risk assessment as well as on the shape of the dose-response relationship. Numerous studies using different end points such as sister chromatid exchanges, micronuclei and mutation have shown that this phenomenon exists in many cell types. However, these end points mostly reflect the late events after radiation damage, and little is known about the early response in this phenomenon. DNA double-strand breaks (DSBs) induced by ionizing radiation or carcinogenic chemicals can be visualized in situ using gamma-H2AX immunofluorescence staining, and there is evidence that the number of gamma-H2AX foci can be closely correlated with DSBs induced. Here we used gamma-H2AX as a biomarker to assess the extranuclear/extracellular effects induced by low-dose alpha particles in situ. The results show that a greater fraction of positive cells with DSBs (48.6%) was observed than the number of cells whose nuclei were actually traversed by the 1-cGy dose of alpha particles (9.2%). The fraction of DSB-positive cells was greatly reduced after treatment with either lindane or DMSO. These results suggest that in situ visualization of DSBs can be used to assess radiation-induced extranuclear/extracellular effects soon after irradiation. Moreover, the in situ DSB assay may provide a means to evaluate the spatial effect on unirradiated cells that are located in the neighboring region of cells irradiated by alpha particles.     

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.     

Accumulation of DNA damage and cell death after fractionated irradiation

The purpose of this work was to determine how fractionated radiation used in the treatment of tumors affects the ability of cancer as well as normal cells to repair induced DNA double-strand breaks (DSBs) and how cells that have lost this ability die. Lymphocytic leukemia cells (MOLT4) were used as an experimental model, and the results were compared to those for normal cell types. The results show that cancer and normal cells were mostly unable to repair all DSBs before the next radiation dose induced new DNA damage. Accumulation of DSBs was observed in normal human fibroblasts and healthy lymphocytes irradiated in vitro after the second radiation dose. The lymphocytic leukemia cells irradiated with 4 × 1 Gy and a single dose of 4 Gy had very similar survival; however, there was a big difference between human fibroblasts irradiated with 4 × 1.5 Gy and a single dose of 6 Gy. These results suggest that exponentially growing lymphocytic leukemia cells, similar to rapidly proliferating tumors, are not very sensitive to fraction size, in contrast to the more slowly growing fibroblasts and most late-responding (radiation therapy dose-limiting) normal tissues, which have a low proliferation index.     

Particularities of blood lymphocyte response to irradiation in vitro in breast cancer patients

DNA breaks and their repair efficiency were analyzed in irradiated in vitro lymphocytes (at doses 1 Gy, gamma-radiation of 60Co, dose rate 1 Gy/min) isolated from peripheral blood of 41 untreated patients with breast cancer and 25 healthy donors using the DNA comet assay under non-denaturing conditions (mainly double-strand DNA breaks (DSB), as well as apoptotic cell death using the DNA halo assay. To estimate the expression of bystander effect, the cells were incubated in a culture medium obtained from lymphocytes irradiated in vitro at doses 1 Gy. The average DSB level in blood lymphocytes of breast cancer patients was shown to be significantly higher (p < 0.05) compared with that in control donors. In general, the following effects were observed in irradiated in vitro lymphocytes of cancer patients: (1) increased sensitivity to y-radiation-induced DNA DSBs compared with lymphocytes from healthy donors, (2) reduced repair efficiency of these damages. Incubation of irradiated blood lymphocytes in a medium from irradiated cells led to an increased relative number of DNA DSBs and an elevated fraction of cells dying through apoptotic pathway both in blood lymphocytes from cancer patients and control donors. However, these non-targeted effects were more expressed for the blood lymphocytes of breast cancer patients.     

Functions and regulation of human artemis in double strand break repair

Cells, which lacked the activity of the nuclease Artemis, retained approximately 10% of unrepaired double strand breaks (DSBs) at later timepoints after ionizing radiation. Ionizing radiation induced hyperphosphorylation of Artemis mainly by ATM and in ATM deficient cells to a minor extent by DNA PK. After induction of DSBs with modified ends by a high dose of calicheamicin gamma1, Artemis was phosphorylated by DNA PK. The type of calicheamicin gamma1-induced DSBs is likely to represent a subclass of DSBs induced by ionizing radiation. DNA PK-dependent phosphorylation of Artemis after treatment with DSB inducing agents increased the cellular retention of Artemis, maintained its interaction with DNA ends and activated its endonucleolytic activity. The following model is suggested: ATM-dependent phosphorylation of Artemis after ionizing radiation could prevent DNA PK-dependent phosphorylation and activation of undesired endonucleolytic activity at DSBs, which do not require endonucleolytic processing by Artemis. The Artemis:DNA PK complex could be involved in the repair of DSBs, which carry modified ends and are refractory to repair by otherwise lesion specific enzymes because of the presence of an inhibitory lesion in the opposite strand.     

Rejoining of DNA double-strand breaks in Ku80-deficient mouse fibroblasts

The role of Ku80 in the repair of DNA double-strand breaks (DSBs) was examined in fibroblasts derived from a Ku80 knockout mouse model described by Nussenzweig et al. (Nature 382, 551-555, 1996). Primary fibroblasts from Ku80+/+ and Ku80-/- mice were immortalized by transfection with plasmids containing either the human MYC proto-oncogene or the Simian virus 40 (SV40) T antigen and were used to measure induction and rejoining of DSBs after exposure to ionizing radiation. The number of DSBs in the cells was quantified by either asymmetric field-inversion gel electrophoresis (AFIGE) or clamped homogeneous electrical-field gel electrophoresis (CHEF). The latter method was introduced for a more reliable quantification of repair even when DNA degradation occurs in a fraction of the irradiated cell population during the postirradiation incubation time. The results confirm that Ku80-deficient mouse fibroblasts are sensitive to ionizing radiation and demonstrate that the increased radiosensitivity may result from a deficiency in DSB rejoining. The results further indicate that unless techniques are employed that allow for distinction between DNA degradation and DNA repair, erroneous conclusions may be drawn regarding the potential of cells to repair DSBs.