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.     

A polymer, random walk model for the size-distribution of large DNA fragments after high linear energy transfer radiation

DNA double-strand breaks (DSBs) produced by densely ionizing radiation are not located randomly in the genome: recent data indicate DSB clustering along chromosomes. Stochastic DSB clustering at large scales, from >100 Mbp down to <0.01 Mbp, is modeled using computer simulations and analytic equations. A random-walk, coarse-grained polymer model for chromatin is combined with a simple track structure model in Monte Carlo software called DNAbreak and is applied to data on alpha-particle irradiation of V-79 cells. The chromatin model neglects molecular details but systematically incorporates an increase in average spatial separation between two DNA loci as the number of base-pairs between the loci increases. Fragment-size distributions obtained using DNAbreak match data on large fragments about as well as distributions previously obtained with a less mechanistic approach. Dose-response relations, linear at small doses of high linear energy transfer (LET) radiation, are obtained. They are found to be non-linear when the dose becomes so large that there is a significant probability of overlapping or close juxtaposition, along one chromosome, for different DSB clusters from different tracks. The non-linearity is more evident for large fragments than for small. The DNAbreak results furnish an example of the RLC (randomly located clusters) analytic formalism, which generalizes the broken-stick fragment-size distribution of the random-breakage model that is often applied to low-LET data. Received: 19 July 1999 / Accepted in revised form: 10 December 1999     

DNA damage in non-proliferating cells subjected to ionizing irradiation at high or low dose rates

Ionizing radiation damage to the genome of a non-cycling mammalian cell is analyzed using continuous time Markov chains. Immediate damage induced by the radiation is modeled as a batch Poisson arrival process of DNA double strand breaks (DSBs). Different kinds of radiation, for example gamma rays or alpha particles, have different batch probabilities. Enzymatic modulation of the immediate damage is modeled as a Markov process similar to the processes described by the master equation of stochastic chemical kinetics. An illustrative example is the restitution/complete exchange model, which postulates that radiation induced DSBs can subsequently either undergo enzymatically mediated repair (restitution) or can participate pairwise in chromosome exchanges, some of which make irremediable lesions such as dicentric chromosome aberrations. One may have rapid irradiation followed by enzymatic DSB processing or have prolonged irradiation with both DSB arrival and enzymatic DSB processing continuing throughout the irradiation period. A complete solution of the Markov chain is known for the case that the exchange rate constant is negligible so that no irremediable chromosome lesions are produced and DSBs are the only damage to the genome. Using PDEs for generating functions, a perturbation calculation is made assuming the exchange rate constant is small compared to the repair rate constant. Some non-perturbative results applicable to very prolonged irradiation are also obtained using matrix methods: Perron-Frobenius theory, variational methods and numerical approximations of eigenvalues. Applications to experimental results on expected values, variances and statistical distributions of DNA lesions are briefly outlined.Continuous time Markov chain models are the most systematic of those current radiation damage models which treat DSB-DSB interactions within the cell nucleus as homogeneous (e.g. ignore diffusion limitations). They contain most other homogeneous models as special cases, limiting cases or approximations. However, applying the continuous time Markov chain models to studying spatial dependence of DSB interactions, which is generally believed to be very important in some situations, presents difficulties.     

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.     

DNA damage caused by ionizing radiation.

A survey is given of continuous-time Markov chain models for ionizing radiation damage to the genome of mammalian cells. In such models, immediate damage induced by the radiation is regarded as a batch-Poisson arrival process of DNA double-strand breaks (DSBs). Enzymatic modification of the immediate damage is modeled as a Markov process similar to those described by the master equation of stochastic chemical kinetics. An illustrative example is the restitution/complete-exchange model. The model postulates that, after being induced by radiation, DSBs subsequently either undergo enzymatically mediated restitution (repair) or participate pairwise in chromosome exchanges. Some of the exchanges make irremediable lesions such as dicentric chromosome aberrations. One may have rapid irradiation followed by enzymatic DSB processing or have prolonged irradiation with both DSB arrival and enzymatic DSB processing continuing throughout the irradiation period. Methods for analyzing the Markov chains include using an approximate model for expected values, the discrete-time Markov chain embedded at transitions, partial differential equations for generating functions, normal perturbation theory, singular perturbation theory with scaling, numerical computations, and certain matrix methods that combine Perron-Frobenius theory with variational estimates. Applications to experimental results on expected values, variances, and statistical distributions of DNA lesions are briefly outlined. Continuous-time Markov chains are the most systematic of those radiation damage models that treat DSB-DSB interactions within the cell nucleus as homogeneous (e.g., ignore diffusion limitations). They contain virtually all other relevant homogeneous models and semiempirical summaries as special cases, limiting cases, or approximations. However, the Markov models do not seem to be well suited for studying spatial dependence of DSB interactions, which is known to be important in some situations.     

Chromatin perturbations during the DNA damage response in higher eukaryotes

The DNA damage response is a widely used term that encompasses all signaling initiated at DNA lesions and damaged replication forks as it extends to orchestrate DNA repair, cell cycle checkpoints, cell death and senescence. ATM, an apical DNA damage signaling kinase, is virtually instantaneously activated following the introduction of DNA double-strand breaks (DSBs). The MRE11-RAD50-NBS1 (MRN) complex, which has a catalytic role in DNA repair, and the KAT5 (Tip60) acetyltransferase are required for maximal ATM kinase activation in cells exposed to low doses of ionizing radiation. The sensing of DNA lesions occurs within a highly complex and heterogeneous chromatin environment. Chromatin decondensation and histone eviction at DSBs may be permissive for KAT5 binding to H3K9me3 and H3K36me3, ATM kinase acetylation and activation. Furthermore, chromatin perturbation may be a prerequisite for most DNA repair. Nucleosome disassembly during DNA repair was first reported in the 1970s by Smerdon and colleagues when nucleosome rearrangement was noted during the process of nucleotide excision repair of UV-induced DNA damage in human cells. Recently, the multi-functional protein nucleolin was identified as the relevant histone chaperone required for partial nucleosome disruption at DBSs, the recruitment of repair enzymes and for DNA repair. Notably, ATM kinase is activated by chromatin perturbations induced by a variety of treatments that do not directly cause DSBs, including treatment with histone deacetylase inhibitors. Central to the mechanisms that activate ATR, the second apical DNA damage signaling kinase, outside of a stalled and collapsed replication fork in S-phase, is chromatin decondensation and histone eviction associated with DNA end resection at DSBs. Thus, a stress that is common to both ATM and ATR kinase activation is chromatin perturbations, and we argue that chromatin perturbations are both sufficient and required for induction of the DNA damage response.     

Use of a Recombination Reporter Insert To Define Meiotic Recombination Domains on Chromosome III of Saccharomyces cerevisiae

In Saccharomyces cerevisiae, meiotic recombination is initiated by DNA double-strand breaks (DSBs). DSBs usually occur in intergenic regions that display nuclease hypersensitivity in digests of chromatin. DSBs are distributed nonuniformly across chromosomes; on chromosome III, DSBs are concentrated in two "hot" regions, one in each chromosome arm. DSBs occur rarely in regions within about 40 kb of each telomere and in an 80-kb region in the center of the chromosome, just to the right of the centromere. We used recombination reporter inserts containing arg4 mutant alleles to show that the "cold" properties of the central DSB-deficient region are imposed on DNA inserted in the region. Cold region inserts display DSB and recombination frequencies that are substantially less than those seen with similar inserts in flanking hot regions. This occurs without apparent change in chromatin structure, as the same pattern and level of DNase I hypersensitivity is seen in chromatin of hot and cold region inserts. These data are consistent with the suggestion that features of higher-order chromosome structure or chromosome dynamics act in a target sequence-independent manner to control where recombination events initiate during meiosis.     

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.     

Induction by H2O2 of DNA and interphase chromosome damage in plateau-phase Chinese hamster ovary cells.

The induction by H2O2 of DNA breaks, DNA double-strand breaks (DSBs), and interphase chromatin damage and their relationship to cytotoxicity were studied in plateau-phase Chinese hamster ovary (CHO) cells. Damage in interphase chromatin was assayed by means of premature chromosome condensation (PCC); DNA DSBs were assayed by nondenaturing filter elution (pH 9.6), and DNA breaks by hydroxyapatite chromatography. Cells were treated with H2O2 in suspension at 0 degrees C for 30 min and treatment was terminated by the addition of catalase. Concentrations of H2O2 lower than 1 mM were not cytotoxic, whereas concentrations of 40 and 60 mM reduced cell survival to 0.1 and 0.004, respectively. An induction of DNA breaks that was dependent on H2O2 concentration was observed at low H2O2 concentrations that reached a maximum at approximately 1 mM; at higher H2O2 concentrations induction of DNA breaks either remained unchanged or decreased. Damage at the chromosome level was not evenly distributed among the cells, when compared to that expected based on a Poisson distribution. Three categories of cells were identified after exposure to H2O2: cells with intact, control-like chromosomes, cells showing chromosome fragmentation similar to that observed in cells exposed to ionizing radiation, and cells showing a loss in the ability of their chromatin to condense into chromosomes under the PCC reaction. The fraction of cells with fragmented chromosomes, as well as the number of excess chromosomes per cell, showed a dose response similar to that of DNA DSBs, reaching a maximum at 1 mM and decreasing at higher concentrations. The results indicate that induction of DNA and chromosome damage by H2O2 follows a complex dependence probably resulting from a depletion of reducing equivalents in the vicinity of the DNA. Reducing equivalents are required to recycle the transition metal ions that are needed to maintain a Fenton-type reaction. The absence of cell killing at H2O2 concentrations that yielded the maximum amount of DNA and chromosome damage suggests that this damage is nonlethal and repairable. It is suggested that lethal DNA and chromosome damage is induced at higher concentrations of H2O2 where cell killing is observed by an unidentified mechanism.     

Spermatocyte responses in vitro to induced DNA damage

Spermatocytes normally sustain many meiotically induced double-strand DNA breaks (DSBs) early in meiotic prophase; in autosomal chromatin, these are repaired by initiation of meiotic homologous-recombination processes. Little is known about how spermatocytes respond to environmentally induced DNA damage after recombination-related DSBs have been repaired. The experiments described here tested the hypothesis that, even though actively completing meiotic recombination, pachytene spermatocytes cultured in the absence of testicular somatic cells initiate appropriate chromatin remodeling and cell-cycle responses to environmentally induced DNA damage. Two DNA-damaging agents were employed for in vitro treatment of pachytene spermatocytes: gamma-irradiation and etoposide, a topoisomerase II (TOP2) inhibitor that results in persistent unligated DSBs. Chromatin modifications associated with DSBs were monitored after exposure by labeling surface-spread chromatin with antibodies against RAD51 (which recognizes DSBs) and the phosphorylated variant of histone H2AFX (herein designated by its commonly used symbol, H2AX), gammaH2AX (which modifies chromatin associated with DSBs). Both gammaH2AX and RAD51 were rapidly recruited to irradiation- or etoposide-damaged chromatin. These chromatin modifications imply that spermatocytes recruit active DNA damage responses, even after recombination is substantially completed. Furthermore, irradiation-induced DNA damage inhibited okadaic acid-induced progression of spermatocytes from meiotic prophase to metaphase I (MI), implying efficacy of DNA damage checkpoint mechanisms. Apoptotic responses of spermatocytes with DNA damage differed, with an increase in frequency of early apoptotic spermatocytes after etoposide treatment, but not following irradiation. Taken together, these results demonstrate modification of pachytene spermatocyte chromatin and inhibition of meiotic progress after DNA damage by mechanisms that may ensure gametic genetic integrity.     

DNA double-strand breaks: linking gene expression to chromosome morphology and mobility

Ionizing radiation can lead to DNA double-strand breaks (DSBs) which belong to the most dangerous forms of damage to the DNA. Cells possess elaborate repair mechanisms and react in a complex manner to the emergence of DSBs. Experiments have shown that gene expression levels in irradiated cells are changed, and thousands of radiation-responsive genes have been identified. On the other hand, recent studies have shown that gene expression is tightly connected to the three-dimensional organization of the genome. In this work, we analyzed the chromatin organization in the cell nuclei before and after exposure to ionizing radiation with an expression-dependent folding model. Our results indicate that the alteration of the chromosome organization on the scale of a complete chromosome is rather limited despite the expression level change of a large number of genes. We further modelled breaks within sub-compartments of the model chromosomes and showed that entropic changes caused by a break lead to increased mobility of the break sites and help to locate break ends further to the periphery of the sub-compartments. We conclude that the changes in the chromatin structure after irradiation are limited to local scales and demonstrate the importance of entropy for the behaviour of break ends.     

Radiation breakage of DNA: a model based on random-walk chromatin structure

Monte Carlo computer software, called DNAbreak, has recently been developed to analyze observed non-random clustering of DNA double strand breaks in chromatin after exposure to densely ionizing radiation. The software models coarse-grained configurations of chromatin and radiation tracks, small-scale details being suppressed in order to obtain statistical results for larger scales, up to the size of a whole chromosome. We here give an analytic counterpart of the numerical model, useful for benchmarks, for elucidating the numerical results, for analyzing the assumptions of a more general but less mechanistic “randomly-located-clusters” formalism, and, potentially, for speeding up the calculations. The equations characterize multi-track DNA fragment-size distributions in terms of one-track action; an important step in extrapolating high-dose laboratory results to the much lower doses of main interest in environmental or occupational risk estimation. The approach can utilize the experimental information on DNA fragment-size distributions to draw inferences about large-scale chromatin geometry during cell-cycle interphase. Received: 2 March 2000 / Revised version: 2 February 2001 / Published online: 21 August 2001     

Deciphering the chromatin landscape induced around DNA double strand breaks

DNA double strand breaks (DSBs) are among the most deleterious forms of lesions and deciphering the details of the chromatin landscape induced around DSBs represents a great challenge for molecular biologists.

Chromatin Immunoprecipitation, followed by microarray hybridisation (ChIP-chip) or high-throughput sequencing (ChIP-seq), are powerful techniques that provide high-resolution maps of protein-genome interactions. However, applying these techniques to study chromatin changes induced around DSBs was previously hindered due to a lack of suitable DSB induction techniques.

We have recently developed an experimental system utilizing a restriction enzyme fused to a modified oestrogen receptor ligand binding domain (AsiSI-ER), which generates multiple, sequence-specific and unambiguously positioned DSBs across the genome upon induction with 4-hydroxytamoxifen (4OHT) ¹. Cell lines expressing this construct represent a powerful tool to study specific chromatin changes during DSB repair, enabling high-resolution profiling of DNA repair complexes and chromatin modifications induced around DSBs. Using this system, we have recently produced the first map of gH2AX, a DSB-induced chromatin modification, on two human chromosomes and have investigated its spreading properties ¹. Here we provide additional data characterizing the cell lines, present a genome-wide profile of gH2AX obtained by ChIP-seq, and discuss the potential of our system towards investigations of previously uncharacterized aspects of DSB repair.     

Chromatin stiffening underlies enhanced locus mobility after DNA damage in budding yeast

DNA double‐strand breaks (DSBs) induce a cellular response that involves histone modifications and chromatin remodeling at the damaged site and increases chromosome dynamics both locally at the damaged site and globally in the nucleus. In parallel, it has become clear that the spatial organization and dynamics of chromosomes can be largely explained by the statistical properties of tethered, but randomly moving, polymer chains, characterized mainly by their rigidity and compaction. How these properties of chromatin are affected during DNA damage remains, however, unclear. Here, we use live cell microscopy to track chromatin loci and measure distances between loci on yeast chromosome IV in thousands of cells, in the presence or absence of genotoxic stress. We confirm that DSBs result in enhanced chromatin subdiffusion and show that intrachromosomal distances increase with DNA damage all along the chromosome. Our data can be explained by an increase in chromatin rigidity, but not by chromatin decondensation or centromeric untethering only. We provide evidence that chromatin stiffening is mediated in part by histone H2A phosphorylation. Our results support a genome‐wide stiffening of the chromatin fiber as a consequence of DNA damage and as a novel mechanism underlying increased chromatin mobility.     

Mechanism of radiosensitization by halogenated pyrimidines: effect of BrdU on repair of DNA breaks, interphase chromatin breaks, and potentially lethal damage in plateau-phase CHO cells.

There is evidence suggesting that radiosensitization induced in mammalian cells by substitution in the DNA of thymidine with BrdU has a component that relies on inhibition of repair and/or fixation of radiation damage. Here, experiments designed to study the mechanism of this phenomenon are described. The effect of BrdU incorporation into DNA was studied on cellular repair capability, rejoining of interphase chromosome breaks, as well as induction and rejoining of DNA double- and single-stranded breaks (DSBs and SSBs) in plateau-phase CHO cells exposed to X rays. Repair of potentially lethal damage (PLD), as measured by delayed plating of plateau-phase cells, was used to assay cellular repair capacity. Rejoining of interphase chromosome breaks was assayed by means of premature chromosome condensation (PCC); induction and rejoining of DNA DSBs were assayed by pulsed-field gel electrophoresis and induction and rejoining of DNA SSBs by DNA unwinding. A decrease was observed in the rate of repair of PLD in cells grown in the presence of BrdU, the magnitude of which depended upon the degree of thymidine replacement. The relative increase in survival caused by PLD repair was larger in cells substituted with BrdU and led to a partial loss of the radiosensitizing effect compared to cells tested immediately after irradiation. A decrease was also observed in the rate of rejoining of interphase chromosome breaks as well as in the rate of rejoining of the slow component of DNA DSBs in cells substituted with BrdU. The time constants measured for the rejoining of the slow component of DNA DSBs and of interphase chromosome breaks were similar both in the presence and in the absence of BrdU, suggesting a correlation between this subset of DNA lesions and interphase chromosome breaks. It is proposed that a larger proportion of radiation-induced potentially lethal lesions becomes lethal in cells grown in the presence of BrdU. Potentially lethal lesions are fixed via interaction with processes associated with cell cycle progression in cells plated immediately after irradiation, but can be partly repaired in cells kept in the plateau-phase. It is hypothesized that fixation of PLD is caused by alterations in chromatin conformation that occur during normal progression of cells throughout the cell cycle.(ABSTRACT TRUNCATED AT 400 WORDS)     

Differentiated function and localisation of SPO11-1 and PRD3 on the chromosome axis during meiotic DSB formation in Arabidopsis thaliana

During meiosis, DNA double-strand breaks (DSBs) occur throughout the genome, a subset of which are repaired to form reciprocal crossovers between chromosomes. Crossovers are essential to ensure balanced chromosome segregation and to create new combinations of genetic variation. Meiotic DSBs are formed by a topoisomerase-VI-like complex, containing catalytic (e.g. SPO11) proteins and auxiliary (e.g. PRD3) proteins. Meiotic DSBs are formed in chromatin loops tethered to a linear chromosome axis, but the interrelationship between DSB-promoting factors and the axis is not fully understood. Here, we study the localisation of SPO11-1 and PRD3 during meiosis, and investigate their respective functions in relation to the chromosome axis. Using immunocytogenetics, we observed that the localisation of SPO11-1 overlaps relatively weakly with the chromosome axis and RAD51, a marker of meiotic DSBs, and that SPO11-1 recruitment to chromatin is genetically independent of the axis. In contrast, PRD3 localisation correlates more strongly with RAD51 and the chromosome axis. This indicates that PRD3 likely forms a functional link between SPO11-1 and the chromosome axis to promote meiotic DSB formation. We also uncovered a new function of SPO11-1 in the nucleation of the synaptonemal complex protein ZYP1. We demonstrate that chromosome co-alignment associated with ZYP1 deposition can occur in the absence of DSBs, and is dependent on SPO11-1, but not PRD3. Lastly, we show that the progression of meiosis is influenced by the presence of aberrant chromosomal connections, but not by the absence of DSBs or synapsis. Altogether, our study provides mechanistic insights into the control of meiotic DSB formation and reveals diverse functional interactions between SPO11-1, PRD3 and the chromosome axis.