Int. J. Radiat. Biol., Vol. 81, No. 2, February 2005, pp. 125 – 138 ORIGINAL ARTICLE Dose – response for radiation-induced apoptosis, residual 53BP1 foci and DNA-loop relaxation in human lymphocytes J. TORUDD1, M. PROTOPOPOVA2, R. SARIMOV1,3, J. NYGREN4,5, S. ERIKSSON5, E. MARKOVÁ1,6, M. CHOVANEC1,6, G. SELIVANOVA2 and I. Y. BELYAEV1,3 1 Department of Genetics, Microbiology and Toxicology, Stockholm University, Stockholm, Sweden 2Cancer Centrum Karolinska, Karolinska Institutet, Stockholm, Sweden 3Laboratory of Radiobiology, General Physics Institute, Russian Academy of Science, Moscow, Russia 4Laboratory of Molecular and Cellular Toxicology, Department of Industrial Hygiene and Toxicology, Finnish Institute of Occupational Health, Helsinki, Finland 5Former Department of Molecular Genome Research, Stockholm University, Stockholm, Sweden 6Laboratory of Molecular Genetics, Cancer Research Institute, Bratislava, Slovak Republic (Received 4 November 2003; accepted 20 January 2005) Abstract The purpose was to compare the radiation-induced apoptosis in human lymphocytes with DNA-loop relaxation and DNA damage as a function of radiation dose and time after exposure. Morphological changes were analysed by staining with fluorescent dyes and apoptotic fragmentation of DNA with conventional agarose gel electrophoresis, pulsed-field gel electrophoresis (PFGE) and alkaline comet assay. Viability was estimated by trypan blue assay. The levels of protein p53 (TP53) were determined with Western blot. Relaxation of DNA-loops was analysed by the method of anomalous viscosity time dependence (AVTD) and neutral comet assay. Induction and repair of double-strand breaks (DSB) was studied by PFGE and by immunostaining of the TP53 binding protein 1 (53BP1). At various time points of apoptosis, there was a linear dose dependence for all apoptotic end-points up to 1 – 2 Gy followed by a plateau at higher doses. Immediately after irradiation, relaxation of DNA-loops due to strand breaks was observed. This relaxation had a similar dose – response with saturation at 2 – 3 Gy. This dose induced approximately one single-strand break (SSB) per 2 Mb of DNA, a value close to the average size of DNA-loops in resting lymphocytes. Similar saturations in dose – responses for apoptosis and DNA-loop relaxation were also observed if cells were treated by camptothecin (CPT) or etoposide VP-16, drugs that relax DNA-loops by induction of SSB and DSB, respectively. The PFGE data showed that the vast majority of DSB were repaired within few hours after irradiation. However, approximately 1.4 foci/Gy/cell, that corresponded to around 3.5% of initial DSB, remained in cells even 24 h after irradiation as measured with immunostaining. The probability to produce one or more than one residual foci per cell was calculated. Radiation at 2 – 3 Gy induced at least one residual 53BP1 focus per cell. The dose – responses for DNA-loop relaxation, induction of at least one residual 53BP1 foci per cell and apoptosis saturated at 2 – 3 Gy. The correlation between dose – responses obtained suggested that the DSB in residual foci and relaxation of DNA-loops may be linked to induction of radiation-induced apoptosis in lymphocytes. Keywords: Apoptosis, chromatin, human lymphocytes, radiation, repair, DNA-loops. Introduction Apoptosis has become recognized as a genetically controlled mechanism for the regulation of biological processes such as development, differentiation, embryogenesis, tissue homeostasis and cell maturation (Raff 1992). It also appears to be of a great importance as a part of the defence mechanism for the elimination of deleterious or damaged cells such as self-reactive lymphocytes, virus-infected or neoplastic cells. Acquisition of resistance to apoptosis may confer a selective advantage of clonal expansion upon pre-neoplastic and neoplastic cells. On the other hand, abnormally increased rates of cell death may result in degenerative diseases and blood cell disorders such as Alzheimer’s disease and myelodis- Correspondence: I. Belyaev, Department of Genetics, Microbiology and Toxicology, Stockholm University, SE-106 91 Stockholm, Sweden. Tel: 46-8-16-41-08. Fax: 46-8-16-43-15. Email: Igor.Belyaev@gmt.su.se ISSN 0955-3002 print/ISSN 1362-3095 online # 2005 Taylor & Francis Group Ltd DOI: 10.1080/09553000500077211 126 J. Torudd et al. plastic syndrome, respectively. Many of the genes involved in the induction (cell growth associated genes such as p53 and c-myc) and mediation (the interleukin-1-converting enzyme (ICE) family of proteases, the bcl-2 gene family involving B-cell leukaemia 2 (BCL-2) and B cell associated protein x (BAX)) of apoptosis have been identified (Wyllie 1995, Shen and White 2001). Ionizing radiation and many anticancer drugs induce apoptosis by a TP53-dependent pathway that is triggered by DNA damage. TP53 functions for the apoptotic process and for the sensitivity of tumour cells to radiation have been reviewed (Brown and Wouters 1999). About 50% of all tumours have mutations in TP53. Relationships between TP53 status and radiation-induced radioresistance have been analysed (Russell et al. 1995, Li et al. 2001). The radioresistant phenotype is often, but not always, correlated with a decreased rate of apoptosis (Brown and Wouters 1999). There are also TP53independent processes that are involved in radiationinduced apoptosis (Hara et al. 2004). It is widely accepted that DNA strand breaks are responsible for radiation-induced apoptosis. DSB are assumed to be the most important lesion to induce apoptosis (Story et al. 1994). The role of SSB in apoptosis has also been addressed (Tounekti et al. 2001). Although hydrogen peroxide (H2O2) induces mostly SSB, apoptosis is induced in human lymphocytes upon treatment with H2O2 as analysed by nuclear morphology and high molecular weight DNA fragmentation (Marini et al. 1996). We and others have previously shown that g-rayinduced apoptosis in human lymphocytes saturates at doses of 1 – 3 Gy (Vral et al. 1998, Belyaev et al. 2001). In previous studies (Vral et al. 1998, Kern et al. 1999, Belyaev et al. 2001), doses below 5 Gy were used and apoptosis might hypothetically be increased at higher doses, especially at the earliest time points after irradiation. The time points earlier than 24 and later than 72 h have not previously been investigated. In the present study, cells were irradiated in the dose range up to 15 Gy and apoptosis was analysed at 4 h and up to several days following irradiation. We also present new data suggesting that apoptosis correlates with relaxation of DNA-loops caused by SSB or DSB in response to treatment with the anticancer drugs camptothecin (CPT) or the etoposide VP-16, respectively. These drugs are specific inhibitors for topoisomerases I and II. CPT produces SSB by stabilizing the topoisomerase I – DNA cleavable complexes. Similarly, VP-16 produces DSB by stabilizing the topoisomerase II – DNA cleavable complexes (Kingma and Osheroff 1998). Radiation-induced strand breaks are repaired within a few hours following irradiation. However, specific slowly repaired or unrepaired DSB may be responsible for induction of apoptosis. Using PFGE, it has recently been found that the cellular radiosensitivity measured after delayed plating of 12 human fibroblast lines, derived from the breast cancer patients, did not correlate with the initial number of DSB or their repair kinetics, but rather with the number of residual DSB (Dikomey and Brammer 2000). In another study (Eastham et al. 2001), only a correlation of borderline significance was seen between clonogenic survival and residual DSB in nine human cervix carcinoma cell lines. However, in these studies DSB and radiosensitivity were measured at fairly different doses. Cellular radiosensitivity was usually determined for doses of up to 8 Gy, while the yield of DSB has been measured for a dose range of 50 – 200 Gy. For the PFGE assay, these high doses had to be used in order to detect residual DSB. Several proteins involved in DNA repair and DNA damage signalling such as the tumour suppressor 53BP1, phosphorylated histone H2AX (g-H2AX) and histone deacetylase 4 (HDAC4) have been shown to produce discrete foci colocalizing to DSB (Rogakou et al. 1999, Schultz et al. 2000, Rappold et al. 2001, Fernandez-Capetillo et al. 2002, Sedelnikova et al. 2002, Kao et al. 2003). The g-H2AX foci are formed in megabase size domains, presumably representing condensed globules of DNA-loops (Rogakou et al. 1999). The 53BP1 protein shares sequence homology with the checkpoint protein Rad9 in S. cerevisiae and functions in the same checkpoint pathway as ATM (ataxia telangiectasia mutated) (DiTullio et al. 2002). The 53BP1 has a Myb domain responsible for binding to DNA, kinetochore-binding domain (KBD) and the Tudor domain that is able to bind to chromatin (Iwabuchi et al. 2003). The g-H2AX and 53BP1 proteins are phosphorylated in response to DNA damage providing a scaffold structure for DSB repair (DiTullio et al. 2002). According to the current model, this scaffold functions by recruiting proteins involved in the repair of DSB (Fernandez-Capetillo et al. 2002, Iwabuchi et al. 2003, Kao et al. 2003). The scaffold is organized within a megabase-size chromatin domain at a site of an actual DNA double-strand break regardless of the type of repair that is further involved in processing DSB (Paull et al. 2000). We studied radiation-induced 53BP1 foci in human cells of different types: G0 lymphocytes, normal fibroblasts VH-10 and HeLa cells. We have found that residual foci remained in these cells for a long time after irradiation, 12 – 24 h, depending on cell type (Belyaev et al. 2002, Markova et al. 2003). Recent studies indicated correlation between radiosensitivity of cells and residual foci (Belyaev et al. 2002, Iwabuchi et al. 2003, Markova et al. 2003, Rothkamm and Lobrich 2003). Dose – response in human lymphocytes Dose dependence for residual 53BP1 foci in lymphocytes 24 h after irradiation is presented here. The results obtained suggested that DSB in residual 53BP1 foci and relaxation of DNA-loops might be linked with induction and execution of radiationinduced apoptosis in lymphocytes. 127 changes characteristic for apoptosis, such as chromatin condensation, fragmentation of nuclei and nuclei shrinkage, were scored by using fluorescence microscope, three times, 100 counted cells each time, as previously described (Belyaev et al. 2001). Anomalous viscosity time dependence (AVTD) measurements Materials and methods Peripheral blood from healthy donors was obtained from Blodcentralen, Karolinska Hospital, Stockholm. Experiments were performed with lymphocytes from different individuals. Lymphocytes were isolated by density gradient centrifugation in Ficoll-Paque (Pharmacia LKB Biotechnology, Uppsala, Sweden) according to the manufacturer’s instructions. The cells were transferred to basal medium (BM); Roswell Park Memorial Institute (RPMI) 1640 medium supplemented with 10% foetal calf serum, 2 mM L-glutamine, 50 IU ml – 1 penicillin, 50 mg ml – 1 streptomycin (ICN Pharmaceuticals, Inc., Costa Mesa, CA, USA). Adherent monocytes were removed by overnight incubation of the cell suspension in 170-cm2 Falcon culture flasks (Becton Dickinson & Co., Franklin Lakes, NJ, USA) at the cell density of 3 6 106 cells ml – 1. After the preincubation, the cells in suspension were collected by centrifugation. The cell density was adjusted to 2 – 3 6 106 cells ml – 1 in fresh Basal Medium (BM) and the lymphocytes were maintained at 5% CO2 and 378C in a humidified incubator (Nunc, Roskilde, Denmark). The viability of cells was above 95% as measured with the trypan blue exclusion assay. DNA-loop relaxation was studied by the AVTD method. Cell lysis was performed as previously described with some modifications (Belyaev et al. 1999). Before lysis, the samples were taken from the cell suspension and diluted with fresh media to a concentration of 8 6 105 cells ml – 1. Lymphocytes were lysed in 14-mm polyallomer centrifuge tubes (Beckman Coulter, Inc., Fullerton, CA, USA) by addition of 3 ml lysis solution (0.25 M disodium salt of ethylenediaminetetraacetic acid (Na2EDTA), 2% w/v sarcosyl, 10 mM Tris-base, pH 7.4) to 0.3 ml cell suspension. The lysates were kept at 268C for 4 h in darkness before AVTD measurements. The AVTD in lysates were measured as described previously (Belyaev et al. 1999) using an AVTD analyser (Archer-Aquarius Ltd, Moscow, Russia). The AVTD were measured at the shear rate of 5.6 s – 1 and shear stress of 0.007 N m – 2. For each experimental condition, AVTD was measured in three replicates. AVTD parameters were described in detail previously (Belyaev et al. 1999). Briefly, the AVTD is characterized by three main parameters: (1) maximum viscosity, measured as normalized maximum relative viscosity (NRV); (2) area under AVTD, measured as relative area; and (3) time for maximum viscosity, measured as relative time. All these parameters depend on conformation, rigidity and molecular weight of nucleoids (Belyaev et al. 1999). Normalized maximum relative viscosity is the most sensitive parameter and usually used to determine the effects of irradiation. Irradiation Western blot Chemicals When not otherwise stated, reagent grade chemicals were obtained from Sigma (St Louis, MO, USA) and Merck KgaA (Darmstadt, Germany). Cells 137 The cells were irradiated with Cs g-rays using Gammacell 1000 (Atomic Energy of Canada Limited, Ottawa, Canada) source. The dose rate was 10.6 Gy min – 1. After irradiation, the cells were incubated in a CO2 incubator at 378C. Fluorescence microscopy At different time points after exposure, samples from both irradiated and control cell suspensions were taken for the assessment of morphological changes. After staining with fluorescent dyes (acridine orange and propidium iodide), the cells with morphological The cells were lysed and proteins were separated by 12% sodium dodecyl sulphate polyacrylamide gel electrophoresis (SDS-PAGE) using Mini-PROTEAN II Electrophoresis Cell according to the manufacturer’s instruction manual (BioRad, Richmond, CA, USA). Transfer of the proteins onto the membrane was performed using Mini Trans-Blot Electrophoretic Transfer Cell (BioRad). Western blot analysis was performed using the RPN 2108 ECL system according to the manufacturer (Amersham Life Science, Amersham, UK) with some modifications. Membranes were incubated with the primary and secondary antibodies, 0.1 mg ml – 1 128 J. Torudd et al. mouse monoclonal anti-TP53 (Ab-6) or 0.2 mg ml – 1 mouse monoclonal anti-TP53 (DO-1), 1 mg ml – 1 mouse monoclonal anti-BCL-2 and 5 mg ml – 1 mouse monoclonal anti-actin antibodies from Calbiochem (Cambridge, MA, USA), Santa Cruz Biotechnology, Inc. (Santa Cruz, CA, USA), DAKO (Glostrup, Denmark) and Boehringer Mannheim (Scandinavia AB, Bromma, Sweden), respectively. Secondary anti-mouse Ig antibody NA 931 (Amersham) was used at the concentration of 1 mg ml – 1. Detection of the labelled antibodies was performed according to the manufacturer manual for ECL Western blotting detection (Amersham). The membranes were exposed to ECL Hyperfilms (Amersham) or charge-coupled device (CCD) camera (FUJIFILM Luminescent Image Analyser LAS1000plus). Measurements of integrated optical density (IOD) and area were performed on the films using Quantiscan (Biosoft, Cambridge, UK) software. Both methods of measurements provided approximately the same results. Comet assay The neutral comet assay as described by Ostling and Johanson (1984) is sensitive to the loss of supercoiling produced by single- and double-strand breaks. The comet assay was performed as previously described with some modifications (Klaude et al. 1996). For each slide, 5000 – 10 000 cells were mixed with 150 ml 0.75% lowmelting agarose type VII (Sigma) in phosphatebuffered saline (PBS) held at 378C. The agarose was spread on ordinary clear-glass slides (Menzel Superfrost, Braunschweig, Germany) that had been pretreated with a small amount of agarose and airdried. After solidifying on a chilled plate, the slides were transferred to the same lysis buffer as for the AVTD assay and incubated at room temperature for 4 h in darkness. All subsequent steps were carried out at room temperature. The slides were then processed according to either neutral or alkaline methods as described below: . Neutral method: slides were incubated in Trisacetate/EDTA buffer (TAE), pH 8.3 for 1 h and electrophoresis was run at 2 V cm – 1 for 15 min in TAE buffer. . Alkaline method: after a 1-h incubation in TAE, the slides were denatured in 0.03 M NaOH, 1 M NaCl, 2 mM EDTA and 0.5% sarcosyl for 1 h. Afterwards, they were rinsed in 0.03 M NaOH, 2 mM EDTA for 1 h and electrophoresed at 0.8 V cm – 1 for 15 min in the same solution. The slides were then neutralized in 0.4 M Tris-HCl (pH 7.5), rinsed in distilled water and air dried. When dry, they were fixed in methanol, stained . 5 min with 1 mg ml – 1 ethidium bromide and rinsed 5 min with TAE buffer. Analysis of tail moments was done with an Olympus fluorescence microscope, aided by the Perceptive Instruments Comet Assay V1.03 image analysis system. We also stained with 4’,6-diamidino-2-phenylindole (DAPI) and both techniques of staining provided similar results. Analysis of apoptotic cells with extensive fragmentation of DNA was performed using the comet assay as previously described (Czene et al. 2002). The cells with highly damaged DNA releasing low molecular weight fragments of DNA (the visible bright rest of the head is accompanied with a diffuse but still distinct tail that is well separated from the head and wider than the head’s diameter) were counted in blind to treatment condition. Pulsed-field gel electrophoresis (PFGE) PFGE grade agarose, S. cerevisiae, S. pombe, l ladder and l digest pulse markers and low melting agarose were purchased from BioRad. A 1 Kb Plus DNA Ladder was from Gibco BRL, Life Technologies (Gaithersburg, MD, USA). Proteinase K was purchased from Boehringer Mannheim (Scandinavia AB, Bromma, Sweden). The cells were washed twice with and resuspended in PBS at a density of 0.5 – 1.0 6 107 cell ml – 1. The suspensions were mixed 1:1 with 1% low melting point agarose (Sigma). Agarose blocks were prepared using 100 ml plug moulds. The cells were lysed by incubation of agarose blocks in NDS (1% lauryl sarcosyl, 0.5 M EDTA, 10 mM Tris, pH 8.0 adjusted by NaOH) with 0.5 mg ml – 1 proteinase K at 378C for 24 h (Protocol A) or 48 h (Protocols B, C). After being washed three times with TE buffer (10 mM Tris, 1 mM EDTA, pH 8.0), blocks were loaded into the wells in duplicate or triplicate. PFGE was run either by Protocols A and B for apoptotic DNA fragmentation or by Protocol C for DSB measurements (Belyaev and Harms-Ringdahl 2002). All runs were at 148C in 0.5 6 Tris-borate-EDTA (TBE) buffer (Maniatis et al. 1982) using a CHEFDR II apparatus (Bio-Rad). Protocol A: 1% agarose gel, 180 V, run time 22 h and ramped pulse from 10 to 90 s. Protocol B: 1.5% agarose gel, 190 V, run time was 7 h and pulse time was ramping from 1 to 30 s. In this protocol, apoptotic DNA fragments are compressed into one compression zone with the same position on the gels as compressed l digest markers (Belyaev and Harms-Ringdahl 2002). To quantify apoptotic fragmentation, different concentrations of the l digest marker of similar size distribution, 8.3 – 48.5 kb, were embedded in plugs and run along with apoptotic samples. Calibration Dose – response in human lymphocytes curves were obtained based on image analysis and assuming that each cell has 6 pg DNA. Protocol C employed the following steps in 0.9% agarose gel: (1) 48 h, at 35 V; (2) 48 h, at 50 V; a 96 h, pulse ramp overlapped these two steps with pulses decreasing from 90 to 45 min; and (3) 48 h, at 60 V with pulse ramp from 45 min to 2 s. On completion, the gels were stained with 0.5 mg ml – 1 ethidium bromide, destained and images were acquired at appropriate saturation using a CCD-camera (Molecular Dynamics). The images were analysed using Quantiscan (Biosoft) software. Agarose gel electrophoresis DNA was extracted with standard phenol-chloroform technique (Maniatis et al. 1982). Conventional gel electrophoresis was run at 50 V in 1.5% molecular biology grade agarose (Saveen, Kungsangen, Sweden) with 0.5 mg ml – 1 ethidium bromide in TAE buffer and room temperature. The gel images were acquired and analysed in the same way as described for PFGE (Belyaev and Harms-Ringdahl 2002). Treatment with CPT and VP-16 Cells were exposed to different concentrations of CPT or VP-16 (Sigma). Drugs were dissolved in dimethyl sulfoxide (DMSO). Final concentration of DMSO in cell cultures during treatment was 0.5%. Control cells were incubated at the same time with same concentration of DMSO. Immunostaining and foci analysis Anti-53BP1 antibody was kindly provided by Dr T. Halazonetis, The Wistar Institute, University of Pennsylvania, Philadelphia, USA. The antibody recognizes the C-terminal domain of the protein. The immunostaining was performed according to Shultz et al. (2000) with some modifications. Cytospin preparations were fixed in 4% paraformaldehyde at room temperature for 10 min, washed once with PBS, permeabilized with 0.2% Triton X100 for 5 min at room temperature, washed three times for 5 min, stained with primary antibody for 1 h, followed by three washes in PBS, incubated with secondary goat anti-mouse IgG (H + L) antibody conjugated with fluorescein isothiocyanate (FITC) or Texas red, washed three times and mounted with 80% glycerol solution in PBS containing 2.5% 1,4diazabicyclo[2.2.2]octane. Bisbenzimide (Hoechst 33258) was added at a concentration of 0.4 mg ml – 1 to the secondary antibody for DNA staining. The images were recorded on a DAS microscope Leitz DM RB with a Hamamatsu dual mode cooled CCD 129 camera C4880. In each version of experiment, 30 cells were analysed from each of three to five randomly selected fields of vision. Statistical analysis The data from at least three identical experiments with cells from different donors were statistically analysed using Kolmogorov – Smirnov test. Most data did not fulfil the normal distribution and were further analysed by the Mann – Whitney U-test, the Wilcoxon matched pairs signed rank test or regression analysis. Results were considered as significantly different at p 5 0.05. Results Morphological changes during radiation-induced apoptosis were analysed by staining with acridine orange and propidium iodide (Figure 1a). No statistically significant changes in morphology were observed at 4 h after irradiation (Figure 1a). The dose dependence after 48 and 72 h were characterized by an initial steep increase in the number of apoptotic cells up to a dose of 2 – 3 Gy followed by a plateau up to 15 Gy. The same dose dependence with saturation at 2 – 3 Gy was observed at later stage of apoptosis 96 h after irradiation (data not shown). After 24 h, a slight increase was seen from 5 to 10 Gy but not as steep as in the beginning of dose – response. It has previously been shown that the AVTD peaks correlate with condensation and fragmentation of chromatin during apoptosis in human lymphocytes (Belyaev et al. 2001). In particular, AVTD parameters declined with progression of apoptosis. These data were confirmed and extended in this study. The AVTD peaks, e.g. normalized maximum relative viscosity (NRV), correlated with the number of vital cells as measured with trypan blue assay from 48 h up to 168 h after irradiation (Figure 1b). An almost complete decline in the AVTD parameters was observed in correlation with cell death at very late stage of apoptosis, 168 h after irradiation with doses higher than 4 Gy (Figure 1b). We also studied the TP53 and BCL-2 protein levels in cell lysates by Western blot. Actin was used as an internal control. Variations in levels of actin were not more than 20% among all samples. A significant dose-dependent increase in the level of the TP53 protein was observed after irradiation (Figure 2a). Dose – response relations for TP53 induction were determined at 4, 24 and 48 h postirradiation (Figure 2b). These dose dependences had the same shape as those for morphological changes, i.e. an increase up to 2 Gy followed by a plateau region between the doses 3 and 15 Gy. In replicated 130 J. Torudd et al. Figure 2. (a) Typical Western blots showing induction of TP53 protein at 4 and 24 h after irradiation of human G0 lymphocytes. Actin was used as an internal control. (b) Quantifications of Western blots obtained following 4 h (&), 24 h (.) and 48 h (~) post-irradiation. Figure 1. (a) Dose dependence for G0 human lymphocytes with characteristic apoptotic morphological changes as measured with fluorescence microscopy at different times after irradiation with 137 Cs g-rays: 4 h (&), 24 h (.), 48 h (~) and 72 h (~). Mean of at least three experiments and standard deviations are shown here and in other figures. (b) Condensation and fragmentation of chromatin during apoptosis as measured by AVTD 48 h (&), 72 h (*), and 168 h (~) after irradiation and cell viability as measured with trypan blue assay 48 h (&), 72 h (.), and 168 h (~) postirradiation. experiments, TP53 induction was rather stable 24 – 48 h post-irradiation. No statistically significant changes in the BCL-2 protein levels were found (data not shown). The fragmentation of DNA in apoptotic cells was measured with the alkaline comet assay 24 and 48 h after irradiation. No significant difference between control and irradiated samples were observed 24 h after irradiation. The effect of irradiation becomes significant 48 h after irradiation. The dose dependence had a plateau with saturation at 2 Gy (Figure 3). Apoptotic fragmentation was also studied by PFGE. Significant fragmentation of DNA below 50 kb was observed in apoptotic cells at 24 h (Figure 4), 48, 72 and 96 h after irradiation (data not shown). In Figure 5, a typical DNA ladder obtained 96 h after irradiation using conventional agarose gel electrophoresis along with quantification is shown. The dose – responses for DNA fragmentation as measured with different techniques and at all time points showed saturation above 3 Gy. Relaxation of DNA-loops was observed immediately after irradiation as indicated by the significant increase in the AVTD peaks. The dose dependence had a sigmoid shape with a plateau at doses above 2 – 3 Gy (Figure 6a). For neutral comets, the saturation of dose dependence was similar as for AVTD (Figure 6b). The longest comet tails we observed in neutral comets were around 325 mm. This length corresponds to approximately 1 Mb of DNA or 2 Mb loops, assuming 3 bp per nm. Since neutral comets showed similar dose – response as AVTD we assume that the saturation in dose – response observed with these two methods is primarily due to cellular DNAloop organization and not to saturation in DNA damage. Dose – response in human lymphocytes 131 Figure 3. Dose dependence for apoptotic cells with extensively fragmented DNA as measured with alkaline comet assay 48 h after irradiation. Note that the fraction of apoptotic cells with extensively fragmented DNA is much lower than the fraction of cells with morphological changes (10 versus 60%), showing that extensive fragmentation is a later event in the apoptotic process. Figure 4. Typical PFGE, protocol A, showing induction of apoptotic fragmentation below 50 kb. Samples were prepared 4 and 24 h after irradiation of human G0 lymphocytes. Markers: M1 is Lambda digest DNA, 8 – 48.5 kb; M2 is Lambda ladder DNA, 48.5 – 1000 kb. To compare further the dose dependence for initial DNA damage and apoptosis, the alkaline comet assay and PFGE were used. The cells were irradiated on ice in agarose blocks and lysed immediately after irradiation. Almost linear dose dependence was seen with the alkaline comet assay (Figure 6c). There was no sign of saturation at 2 Gy. This damage was almost repaired during 2 h after irradiation (Figure 6d). Induction of DSB was analysed by PFGE and a dose-dependent increase of high-molecular weight fragmentation of DNA was observed (Figure 7). These DSB were repaired within 3 – 6 h after irradiation and no DNA fragments above 5.7 Mb were observed 24 h after irradiation (not shown). Interestingly, significant correlations between dose dependence for apoptosis and DNA-loop relaxation were also found following treatment of cells with either CPT or VP-16. In preliminary experiments, we used different concentrations of Figure 5. (a) Typical DNA ladder obtained 96 h after irradiation with conventional agarose gel electrophoresis. Marker (M) is 1 kb plus DNA ladder, 100 – 12000 bp. (b) IOD of laddering was measured in the area within the 100 and 700 kb marker. CPT and VP-16, and measured AVTD in cell lysates after different durations of treatment, 10 min to 2 h. For both drugs, DNA-loop relaxation were saturated after 1 h of treatment. CPT induced complete relaxation of DNA-loops as measured with AVTD technique at the dose 10 mg ml – 1 (Figure 8a). At the same dose, saturation in apoptosis was observed as measured with morphological analysis (Figure 8b), apoptotic DNA fragmentation (Figure 8c), and TP53 induction (Figure 8d). Dose – responses for VP-16-induced DNA-loop relaxation and apoptosis as measured by DNA fragmentation, morphological changes and viability reached saturation at 100 mg ml – 1 (data are not shown). As shown in Figure 8e and Table I there was a fairly linear correlation between relaxation and apoptosis for three different agents. VP-16 that induces DSB is more efficient than grays that induced mainly SSB with some DSB and 132 J. Torudd et al. Figure 6. Dose dependence of normalized maximal relative viscosity measured with AVTD in lysates of irradiated cells (a) and tail moment in neutral (b) and alkaline (c) comets. Human lymphocytes were irradiated with 137Cs g-rays at 10.6 Gy min – 1 on ice and lysed immediately after irradiation. (d) Vast majority of SSB were repaired 2 h post-irradiation as measured with alkaline comets. Figure 7. Radiation-induced DSB analysed by the PFGE, Protocol C. Cells were irradiated on ice in agarose blocks and lysed immediately after irradiation. Marker (M) is S. pombe chromosomal DNA. g-rays is more efficient than CPT that induces SSB. The slope was steeper for VP-16 compared with CPT and g-rays, indicating that loop relaxation is not the only determinant for apoptosis. To analyse DSB-related foci we used immunostaining with anti-53BP1 antibody (Schultz et al. 2000). Human lymphocytes were irradiated with 3 Gy g-rays and immunostaining was performed 15, 30 min, 4 and 24 h after irradiation. 53BP1 foci formation was maximal 15 – 30 min after irradiation (Figure 9). At this time after irradiation, we observed approximately 10 foci/Gy/cell. This value corresponded to published data (Schultz et al. 2000). Afterwards, foci disappeared and only 9 + 4 foci/cell were seen 4 h after irradiation with 3 Gy. However, even 24 h after irradiation, a dosedependent number of foci were detected at the doses of 0.5 – 10 Gy (Figure 10a). These foci were observed in both apoptotic cells and cells displaying no morphological hallmarks of apoptosis. Approximately 1.4 foci/Gy/cell was seen in the cells 24 h after irradiation, this corresponds to 14% of the foci observed 15 min after irradiation. However, this value is preliminary as we have not performed a full analysis of the time kinetics for foci formation. In addition, the primary foci were very small in size as compared with the residual Dose – response in human lymphocytes 133 Figure 8. Dose – response for CPT-induced DNA-loop relaxation (a) and apoptosis (b – d) as measured in human lymphocytes 24 h (&) and 48 h (.) after treatment with CPT. Means and SD are shown from two to four experiments with different donors. (a) Cells were lysed 1 h after beginning of treatment with CPT and dose dependence for NRV was measured with the AVTD method. (b) Cells were scored for apoptotic changes. (c) Apoptotic DNA fragmentation was analysed by PFGE, protocol B. (d) The Western blot shown is representative of induction of TP53 by CPT in one of four experiments. (e) Apoptosis as determined by morphology in dependence on relative relaxation as determined by AVTD for VP-16 (&, solid line), g-rays (~, short dash) and CPT (., dash). Relative relaxation was determined as the relaxation at a certain dose relative to the background relaxation. foci, observed 24 h after irradiation. Thereby, the number of primary foci might be underestimated. The number of residual foci constitutes about 3.5% of primary DSB, assuming that g-rays induce 40 DSB/Gy/cell. In Figure 10b, the probability for one or more residual foci per cell at different doses 134 J. Torudd et al. Table I. Slopes, intercepts regression and coefficients for the lines plotted in Figure 8e. The significance of the slopes and the dependence of apoptosis on loop relaxation relative to g-rays are also shown. g-rays VP-16 CPT Slope and intercept R2 Significance (p) Slope relative to g-rays y = 23.0x – 15.3 y = 35.5x – 21.6 y = 19.9x – 19.0 0.9078 0.8972 0.8682 5 0.02 5 0.01 5 0.001 1 1.54 0.86 Figure 9. Formation of 53BP1 foci 15 min after irradiation of human lymphocytes with 3 Gy and residual 53BP1 foci 24 h after irradiation, as analysed by immunostaining with antibody against 53BP1. have been calculated using Poisson statistics. Note that the 3 Gy dose results in at least one residual foci per cell. Discussion A large number of highly conserved genes have been shown to control the apoptotic process. One of the most important triggering mechanisms is mediated by the TP53 protein. The induction of this protein has been shown during apoptosis in human resting lymphocytes (Seki et al. 1994). Seki et al. found that TP53 is induced by irradiation with 0.5 – 15 Gy. Saturation in dose dependence of TP53 induction has been observed at 2 – 4 Gy, 4 h post-irradiation. In our experiments, dose dependence for TP53 induction saturated above 3 Gy at 4, 24 and 48 h after irradiation. Therefore, our data confirmed and extended the findings of Seki et al. (1994). No changes in the level of BCL-2 have been observed (Seki et al. 1994). In agreement with these data, we did not observe any changes in the BCL-2 levels either (not shown). TP53 is typically induced transiently in most cell types in response to ionizing radiation. Permanently induced level of TP53 in G0 human lymphocytes may be accounted for a rather stable organization of DNA loops in these cells. The data may suggest that during the stage of radiation-induced relaxed chromatin in G0 human lymphocytes, TP53 binds to chromatin and subsequent condensation of chromatin results in a stabilization of bound TP53 (Torudd et al. 2000). This study illuminates dose dependence of radiation-induced apoptosis as measured with several end-points in resting lymphocytes. The dose dependences for apoptotic morphological changes, DNA fragmentation, trypan blue uptake and TP53 expression saturated above 2 – 3 Gy at different times after irradiation. Others have observed similar shapes of dose dependence for apoptosis in different types of lymphocytes as measured with various techniques (Hedges and Hornsey 1978, Filippovich et al. 1982, Sorokina et al. 1992, Warenius and Down 1995, Vral et al. 1998). The dose dependence for induction of apoptotic cells was measured by Vral et al. (1998) 24, 48 and 72 h after g-irradiation of G0 human lymphocytes. Dose – response was characterized by an initial steep increase below 1 Gy, with a flattening at higher doses towards 5 Gy. In the same dose range, 1 – 5 Gy, a similar dose – response was also obtained for morphological apoptotic changes in our previous study (Belyaev et al. 2001). Here, we extended the dose range, used several techniques and analysed apoptosis at several time points starting with 4 h up to several days following irradiation. Note that the fraction of apoptotic cells with extensively fragmented DNA (Figure 3) is much lower than the fraction of cells with morphological changes (Figure 1), showing that extensive fragmentation is a later event in the apoptotic process. In general, at all time points, clear saturation in dose – responses was observed indicating that saturation in dose – response is not a peculiarity of a specific time point or specific end- Dose – response in human lymphocytes Figure 10. Dose – response for residual 53BP1 foci analysed 24 h after irradiation (a) and for the probability to have one or more residual foci per cell (b). Foci were scored in irradiated lymphocytes as described in the Materials and methods. In each experiment, 30 cells were analysed from each of three to five randomly selected fields of vision. Means of three experiments with cells from different donors and standard deviations are shown. The probability was calculated from the Poisson distribution of residual foci among the cells. point but a rather general trend of radiationinduced apoptosis in human lymphocytes. Note, that the increment of dose was 1 Gy in this paper and slight differences in the dose for saturation were observed between different time- and endpoints. The presented data may be interpreted as showing saturation in the range of 2 – 3 Gy. The role of membrane damage has been considered in induction of apoptosis (Harms-Ringdahl et al. 1996) but no direct proof has been obtained so far for low linear energy transfer (LET) radiation. Radiation-induced apoptosis is commonly believed to be due to DNA damage. The results presented herein suggest that sufficient amount of DNA damage is produced by the dose of 2 – 3 Gy in 135 human lymphocytes to trigger radiation-induced apoptosis in all cells. There is a notion that slowly repaired or unrepaired DSB, as measured 24 h after irradiation, may correlate with clonogenic survival (Dikomey and Brammer 2000). However, no data are available to correlate residual DSB with radiation-induced apoptosis in lymphocytes. In this study, 53BP1 foci that presumably co-localize to radiation-induced DSB in different cell types were analysed (Schultz et al. 2000). According to the data obtained, one or more residual foci is induced by doses of 2 – 3 Gy in each cell. DSB in residual foci may hypothetically represent a sufficient event for triggering of apoptosis. The majority of DSB are repaired within few hours post-irradiation. Localization of DSB in specific areas of chromatin or complexity of DSB may be important constrains for the efficiency of the DSB repair. In particular, two or more DSB might be involved in formation of residual foci. Such breaks may take longer time to be repaired and could result in triggering of apoptotic signal transduction because of the failure to repair DSB. Other radiation-induced foci may contain only one, or less complex DSB, which may be subjected to fast repair and therefore do not signal for apoptosis. Residual foci constituted approximately 3.5% of all radiation-induced foci, assuming that g-rays induce 40 DSB(foci)/Gy/cell. These foci may be located to some specific structures of chromatin or DNA sequences such as nuclear matrix DNA or a specific fraction of DNA that constitute a minor part of the genomic DNA. In a recent investigation, Xray-induced 53BP1 foci retained at nuclear foci after detergent extraction of cells showing that foci localize in the detergent-insoluble fraction of chromatin (Iwabuchi et al. 2003). Release of the 53BP1 from the detergent-insoluble fraction coincided in time with the extensive 53BP1 focus dispersion (Iwabuchi et al. 2003). Residual 53BP1 foci remained even upon extraction of proteins with a standard high saltdetergent protocol for nuclear matrix preparation (Markova et al. 2003). These data may indicate a preferential localization of 53BP1 residual foci in the nuclear matrix. The comet assay and halo assay have directly confirmed that the increase in AVTD reflected relaxation of DNA-loops and that AVTD decrease was caused by chromatin condensation (Belyaev et al. 1999, Belyaev et al. 2001). Here, dose – responses of DNA damage was analysed by the AVTD technique and comet assay immediately after irradiation. We found similar dose – responses with saturation at 2 – 3 Gy using both techniques. Razin and co-workers have described the protocol for excision of DNA loops by topoisomerase II- 136 J. Torudd et al. mediated DNA cleavage at matrix attachment sites (Razin et al. 1995). The cleavage of DNA into fragments of approximately 2 Mb was observed in human resting lymphocytes using this protocol in combination with PFGE (Iarovaia et al. 1995) (Belyaev et al, unpublished). Assuming an average loop size of 2 Mb and the length of diploid genome being 6 6 109 base pairs, the genome of human lymphocytes will consist of approximately 3000 such DNA loops. As 1 Gy g-rays induces around 1000 SSB per genome (Ward 1988), most DNA-loops will be relaxed at the dose of 2 – 3 Gy. The first data showing plateau in dose – response as measured by neutral comet assay was described by inventors of this assay, Östling and Johanson (1984). Dose – response was measured for L517Y-S cells in the dose range up to 4 Gy and saturation was observed at 2 – 3 Gy. We used similar technique for cell lysis as these authors and our data are comparable. According to Östling and Johanson, DNAloops are stretched out during neutral comet assay and increases in comet lengths are observed because of this stretching. At higher doses, DNA fragmentation contributes stronger to increase of comet lengths as compared with the stretching of DNA-loops and this increase is usually used for the analysis of DSB (Banath et al. 1998). It is attractive to hypothesize that relaxation of DNA-loops initiate execution of apoptosis in lymphocytes, facilitating the binding of proteins such as TP53 to DNA, chromatin or nuclear matrix. This hypothesis is supported by recent data that TP53 binds to nuclear matrix in apoptotic cells of different types including human lymphocytes (Belyaev et al. 2001, Jiang et al. 2001). The induction of apoptosis at low doses in some cells does not contradict this hypothesis. Indeed, some DNA loops containing genes that are related to induction of apoptosis, will be relaxed by chance even at low doses. At the dose that relax all loops, 100% induction of apoptosis was observed. The data obtained here with VP-16 and CPT support this hypothesis. Despite of different causes resulting in DNA-loop relaxation after treatment with CPT and VP-16, SSB or DSB, respectively, a correlation between apoptosis and DNA-loop relaxation was observed. The slope for the correlation was steeper for VP-16 as compared with CPT and g-rays, indicating that loop relaxation is not the only determinant for apoptosis (Table I). The slopes were within a factor of 2, which is quite close for three agents with such different mechanisms of action. VP-16 that induces DSB is more efficient than g-rays that induced mainly SSB with some DSB and grays are more efficient than CPT that induces SSB. For most endpoints, however, DSB is much more efficient than SSB while in these experiments the difference was a mere 1.8 times. However, VP-16 and CPT do not induce direct breaks but protein associated breaks which may explain the small difference between the two compounds. The correlations between dose – responses for apoptosis, residual foci and DNA-loop relaxation do not prove that these events are causally related. Thus, additional data are needed to verify possible causality. Cells with different radiosensitivities such as subpopulations of lymphocytes may be further studied to elaborate this hypothesis. Recent results (Bakkenist and Kastan 2003) suggest that ionizing radiation can induce changes in chromatin structure that activate Ataxia telangiectasia mutated (ATM) kinase. ATM in turn phosphorylates TP53. Perhaps this is one of the biochemical links between chromatin relaxation, apoptosis and residual foci. Acknowledgements The authors are grateful to Dr T. Halazonetis for antibodies to 53BP1, Professor M. Harms-Ringdahl for valuable discussions and for reading manuscript. The Swedish Radiation Protection Institute, the Swedish National Board for Laboratory Animals and the Swedish Council for Working Life and Social Research supported this study. References Bakkenist CJ, Kastan MB. 2003. DNA damage activates ATM through intermolecular autophosphorylation and dimer dissociation. Nature 421: 499 – 506. Banath JP, Fushiki M, Olive PL. 1998. Rejoining of DNA singleand double-strand breaks in human white blood cells exposed to ionizing radiation. International Journal of Radiation Biology 73: 649 – 660. Belyaev IY, Czene S, Harms-Ringdahl M. 2001. Changes in chromatin conformation during radiation-induced apoptosis in human lymphocytes. Radiation Research 156: 355 – 364. Belyaev IY, Eriksson S, Nygren J, Torudd J, Harms-Ringdahl M. 1999. Effects of ethidium bromide on DNA loop organisation in human lymphocytes measured by anomalous viscosity time dependence and single cell gel electrophoresis. Biochimica et Biophysica Acta 1428: 348 – 356. Belyaev IY, Torudd J, Protopopova M, Nygren J, Eriksson S, Chovanec M, Selivanova G, Harms-Ringdahl M. 2002. Radiation-induced apoptosis in human lymphocytes: possible relationship to unrepaired DNA double strand breaks and DNA-loop organisation. In: Boniver J, De Saint-Georges L, Humblet C, Maisin JR, editors. 32nd Annual Meeting of the European Society for Radiation Biology (ESRB). Liege: Eurogentec. p. 94. Belyaev IY, Torudd J, Tapper L, Harms-Ringdahl M. 2001. Chromatin remodeling, DNA fragmentation and induction of DNA double strand breaks in apoptotic cells. In: Conference on Cancer, Cancerfonden, Stockholm, Sweden. Dose – response in human lymphocytes Belyaev IY, Harms-Ringdahl M. 2002. A simple and sensitive pulsed field gel electrophoresis protocol to study 50 kb apoptotic DNA fragmentation in human lymphocytes. Radiatsionnaia Biologiia, Radioecologiia/Rossiiskaia Akademiia Nauk 42: 279 – 283. Brown JM, Wouters BG. 1999. Apoptosis, p53, and tumor cell sensitivity to anticancer agents. Cancer Research 59: 1391 – 1399. Czene S, Testa E, Nygren J, Belyaev I, Harms-Ringdahl M. 2002. DNA fragmentation and morphological changes in apoptotic human lymphocytes. Biochemical and Biophysical Research Communications 294: 872 – 878. Dikomey E, Brammer I. 2000. Relationship between cellular radiosensitivity and non-repaired double-strand breaks studied for different growth states, dose rates and plating conditions in a normal human fibroblast line. International Journal of Radiation Biology 76: 773 – 781. DiTullio RA Jr, Mochan TA, Venere M, Bartkova J, Sehested M, Bartek J, Halazonetis TD. 2002. 53BP1 functions in an ATMdependent checkpoint pathway that is constitutively activated in human cancer. Nature Cell Biology 4: 998 – 1002. Eastham AM, Atkinson J, West CM. 2001. Relationships between clonogenic cell survival, DNA damage and chromosomal radiosensitivity in nine human cervix carcinoma cell lines. International Journal of Radiation Biology 77: 295 – 302. Fernandez-Capetillo O, Chen HT, Celeste A, Ward I, Romanienko PJ, Morales JC, Naka K, Xia Z, Camerini-Otero RD, Motoyama N, Carpenter PB, Bonner WM, Chen J, Nussenzweig A. 2002. DNA damage-induced G2-M checkpoint activation by histone H2AX and 53BP1. Nature Cell Biology 4: 993 – 997. Filippovich IV, Sorokina NI, Soldatenkov VA, Romantzev EF. 1982. Supercoiled DNA repair in thymocyte fractions differing in radiosensitivity. International Journal of Radiation Biology and Related Studies in Physics, Chemistry, and Medicine 42: 31 – 44. Hara S, Nakashima S, Kiyono T, Sawada M, Yoshimura S, Iwama T, Banno Y, Shinoda J, Sakai N. 2004. p53-Independent ceramide formation in human glioma cells during gammaradiation-induced apoptosis. Cell Death and Differentiation, in press. Harms-Ringdahl M, Nicotera P, Radford IR. 1996. Radiation induced apoptosis. Mutation Research 366: 171 – 179. Hedges MJ, Hornsey S. 1978. The effect of X-rays and neutrons on lymphocyte death and transformation. International Journal of Radiation Biology and Related Studies in Physics, Chemistry, and Medicine 33: 291 – 300. Iarovaia OV, Lagarkova MA, Razin SV. 1995. The specificity of human lymphocyte nucleolar DNA long-range fragmentation by endogenous topoisomerase II and exogenous Bal 31 nuclease depends on cell proliferation status. Biochemistry 34: 4133 – 4138. Iwabuchi K, Basu BP, Kysela B, Kurihara T, Shibata M, Guan D, Cao Y, Hamada T, Imamura K, Jeggo PA, Date T, Doherty AJ. 2003. Potential role for 53BP1 in DNA end-joining repair through direct interaction with DNA. Journal of Biological Chemistry 278: 36487 – 36495. Jiang M, Axe T, Holgate R, Rubbi CP, Okorokov AL, Mee T, Milner J. 2001. p53 binds the nuclear matrix in normal cells: binding involves the proline-rich domain of p53 and increases following genotoxic stress. Oncogene 20: 5449 – 5458. Kao GD, McKenna WG, Guenther MG, Muschel RJ, Lazar MA, Yen TJ. 2003. Histone deacetylase 4 interacts with 53BP1 to mediate the DNA damage response. Journal of Cell Biology 160: 1017 – 1027. 137 Kern P, Keilholz L, Forster C, Seegenschmiedt MH, Sauer R, Herrmann M. 1999. In vitro apoptosis in peripheral blood mononuclear cells induced by low-dose radiotherapy displays a discontinuous dose-dependence. International Journal of Radiation Biology 75: 995 – 1003. Kingma PS, Osheroff N. 1998. The response of eukaryotic topoisomerases to DNA damage. Biochimica et Biophysica Acta 1400: 223 – 232. Klaude M, Eriksson S, Nygren J, Ahnstrom G. 1996. The comet assay: mechanisms and technical considerations. Mutation Research 363: 89 – 96. Li Z, Xia L, Lee LM, Khaletskiy A, Wang J, Wong JY, Li JJ. 2001. Effector genes altered in MCF-7 human breast cancer cells after exposure to fractionated ionizing radiation. Radiation Research 155: 543 – 553. Maniatis T, Fritsch EF, Sambrook J. 1982. Molecular cloning: A laboratory manual. New York: Cold Spring Harbor. Marini M, Musiani D, Sestili P, Cantoni O. 1996. Apoptosis of human lymphocytes in the absence or presence of internucleosomal DNA cleavage. Biochemical and Biophysical Research Communication 229: 910 – 915. Markova E, Schultz N, Torudd J, Harms-Ringdahl M, Protopopova M, Selivanova G, Khakimov H, Belyaev I. 2003. Validation of novel DSB-co-localizing foci assay for radiosensitivity. In: 12th International Congress of Radiation Research. Brisbane: ICMS. p. 235. Ostling O, Johanson KJ. 1984. Microelectrophoretic study of radiation-induced DNA damages in individual mammalian cells. Biochemical and Biophysical Research Communication 123: 291 – 298. Paull TT, Rogakou EP, Yamazaki V, Kirchgessner CU, Gellert M, Bonner WM. 2000. A critical role for histone H2AX in recruitment of repair factors to nuclear foci after DNA damage. Current Biology 10: 886 – 895. Raff MC. 1992. Social controls on cell survival and cell death. Nature 356: 397 – 400. Rappold I, Iwabuchi K, Date T, Chen J. 2001. Tumor suppressor p53 binding protein 1 (53BP1) is involved in DNA damagesignaling pathways. Journal of Cell Biology 153: 613 – 620. Razin SV, Gromova II, Iarovaia OV. 1995. Specificity and functional significance of DNA interaction with the nuclear matrix: new approaches to clarify the old questions. International Review of Cytology 162B: 405 – 448. Rogakou EP, Boon C, Redon C, Bonner WM. 1999. Megabase chromatin domains involved in DNA double-strand breaks in vivo. Journal of Cell Biology 146: 905 – 916. Rothkamm K, Lobrich M. 2003. Evidence for a lack of DNA double-strand break repair in human cells exposed to very low x-ray doses. Proceedings of the National Academy of Sciences, USA 100: 5057 – 5062. Russell J, Wheldon TE, Stanton P. 1995. A radioresistant variant derived from a human neuroblastoma cell line is less prone to radiation-induced apoptosis. Cancer Research 55: 4915 – 4921. Schultz LB, Chehab NH, Malikzay A, Halazonetis TD. 2000. p53 binding protein 1 (53BP1) is an early participant in the cellular response to DNA double-strand breaks. Journal of Cell Biology 151: 1381 – 1390. Sedelnikova OA, Rogakou EP, Panyutin IG, Bonner WM. 2002. Quantitative detection of (125)IdU-induced DNA doublestrand breaks with gamma-H2AX antibody. Radiation Research 158: 486 – 492. 138 J. Torudd et al. Seki H, Kanegane H, Iwai K, Konno A, Ohta K, Yachie A, Taniguchi N, Miyawaki T. 1994. Ionizing radiation induces apoptotic cell death in human TcR-gamma/delta + T and natural killer cells without detectable p53 protein. European Journal of Immunology 24: 2914 – 2917. Shen Y, White E. 2001. p53-dependent apoptosis pathways. Advances in Cancer Research 82: 55 – 84. Sorokina NI, Pushkareva NB, Nikolsky AV, Denisenko MF, Filippovich IV. 1992. Accumulation of cAMP in gammairradiated thymocytes and internucleosomal DNA fragmentation. International Journal of Radiation Biology 62: 603 – 612. Story MD, Voehringer DW, Malone CG, Hobbs ML, Meyn RE. 1994. Radiation-induced apoptosis in sensitive and resistant cells isolated from a mouse lymphoma. International Journal of Radiation Biology 66: 659 – 668. Torudd J, Belyaev I, Czene S, Harms-Ringdahl M. 2000. Kinetics of p53 induction and DNA fragmentation during radiationinduced apoptosis in human lymphocytes. In: 30th Annual Meeting of the European Society for Radiation Biology (ESRB). Warsaw: BioMeriux. p. 54. Tounekti O, Kenani A, Foray N, Orlowski S, Mir LM. 2001. The ratio of single- to double-strand DNA breaks and their absolute values determine cell death pathway. British Journal of Cancer 84: 1272 – 1279. Vral A, Cornelissen M, Thierens H, Louagie H, Philippe J, Strijckmans K, De Ridder L. 1998. Apoptosis induced by fast neutrons versus 60Co gamma-rays in human peripheral blood lymphocytes. International Journal of Radiation Biology 73: 289 – 295. Ward JF. 1988. DNA damage produced by ionizing radiation in mammalian cells: identities, mechanisms of formation, and reparability. Progress in Nucleic Acid Research and Molecular Biology 35, 95 – 125. Warenius HM, Down JD. 1995. RBE of fast neutrons for apoptosis in mouse thymocytes. International Journal of Radiation Biology 68: 625 – 629. Wyllie AH. 1995. The genetic regulation of apoptosis. Current Opinion in Genetics and Development 5, 97 – 104.