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Radiation-Induced Chromosome Aberrations in Saccharomyces cerevisiae : Influence of DNA Repair Pathways
Anna A. Friedla,b, Markus Kiechlea, Barbara Fellerhoffa, and Friederike Eckardt-Schuppaa GSF-Forschungszentrum für Umwelt und Gesundheit, Institut für Strahlenbiologie, 85758 Oberschleißheim, Germany,
b Strahlenbiologisches Institut, Ludwig-Maximilians-Universität, 80336 München, Germany
Corresponding author: Anna A. Friedl, Institut für Strahlenbiologie, GSF-Forschungszentrum, Postfach 1129, D-85758 Oberschleißheim, Germany, friedl{at}gsf.de (E-mail).
Communicating editor: F. WINSTON
| ABSTRACT |
|---|
Radiation-induced chromosome aberrations, particularly exchange-type aberrations, are thought to result from misrepair of DNA double-strand breaks. The relationship between individual pathways of break repair and aberration formation is not clear. By electrophoretic karyotyping of single-cell clones derived from irradiated cells, we have analyzed the induction of stable aberrations in haploid yeast cells mutated for the RAD52 gene, the RAD54 gene, the HDF1(=YKU70) gene, or combinations thereof. We found low and comparable frequencies of aberrational events in wildtype and hdf1 mutants, and assume that in these strains most of the survivors descended from cells that were in G2 phase during irradiation and therefore able to repair breaks by homologous recombination between sister chromatids. In the rad52 and the rad54 strains, enhanced formation of aberrations, mostly exchange-type aberrations, was detected, demonstrating the misrepair activity of a rejoining mechanism other than homologous recombination. No aberration was found in the rad52 hdf1 double mutant, and the frequency in the rad54 hdf1 mutant was very low. Hence, misrepair resulting in exchange-type aberrations depends largely on the presence of Hdf1, a component of the nonhomologous end-joining pathway in yeast.
STRUCTURAL chromosomal aberrations are an important consequence of ionizing radiation in eukaryotic cells, and may cause mitotic cell death and neoplastic cell transformation. In the earliest days of radiation biology, a model was already established saying that the generation of exchange-type aberrations requires breakage of chromosomes and reunion of the "wrong" ends (for review see ![]()
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Three different pathways of DSB repair/rejoining have been observed both in Saccharomyces cerevisiae and mammalian cells: (1) homologous recombination associated with gene conversion events (![]()
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The similarity between end products of DSB repair/rejoining in S. cerevisiae and mammalian cells suggests an evolutionary conservation of DSB processing pathways. The relative importance and efficiency of these pathways, however, seem to differ in yeast and mammalian cells. In S. cerevisiae, homologous recombination is the predominant mechanism (reviewed by ![]()
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Probably all of these pathways have the potential of causing exchange-type aberrations: Ectopic homologous recombination results in exchange-type aberrations if associated with a crossover ( ![]()
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Because knowledge about repair proteins and their roles in the various mechanisms of DSB processing in mammalian cells is still limited, here we started to analyze the relationship between individual pathways of DSB processing and induction of chromosomal aberrations in the yeast S. cerevisiae. In this yeast, classical cytological techniques cannot be used because of insufficient chromatin condensation (![]()
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We have analyzed yeast strains mutated for the genes RAD52, RAD54, and HDF1. It is well established that rad52 mutant cells cannot repair DSB via homologous recombination. SSA seems independent of RAD52 within large arrays of tandemly repeated sequences (![]()
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Here, we show that electrophoretic karyotyping is a suitable means for detection of stable, untargeted, radiation-induced, chromosomal alterations. Analysis of the patterns of chromosomal bands in aberrant clones suggests that aberration types are similar to those obtained in irradiated mammalian cells. The yield of aberrations in haploid wild-type and hdf1 mutant cells after irradiation in stationary growth phase is low, presumably because most survivors descended from cells that were in G2 phase at the time of irradiation. In rad52 and rad54 mutants, the yield was strongly enhanced, demonstrating the misrepair capacity of DSB repair pathways other than homologous recombination. In rad52 hdf1 and rad54 hdf1 double mutants, the yield in alterations was very low, showing that the Hdf1-mediated NHEJ pathway is very prone to result in misrepair.
| MATERIALS AND METHODS |
|---|
Strain construction:
The strains used in this study are listed in Table 1. Deletion/disruption of HDF1 and RAD52 to create strains SX46A hdf1
, SX46A rad52
, SX46A rad52
hdf1
, and the respective derivatives of strain WS8105-1C have been described (![]()
|
To delete the entire RAD54 open reading frame, we applied a PCR-based gene disruption method (![]()
::kanMX fragment kindly provided by W.-D. HEYER (J. SCHMUCKLI-MAUER and W.-D. HEYER, unpublished results). With this method, transformants are selected by growth on YPD containing 200 mg/liter of geneticin (GIBCO BRL, Gaithersburg, MD). Because strain SX46A turned out resistant to geneticin at concentrations up to 800 mg/liter, we were forced to use strain WS8105-1C for constructing a rad54 and a rad54 hdf1 mutant. Correct transplacement was verified in each case by Southern hybridization and phenotypic tests (sensitivity towards ionizing irradiation and temperature sensitivity).
Irradiation:
Cells were grown in liquid YPD medium for 4 days to stationary growth phase, washed, and resuspended in potassium phosphate buffer. The cell suspension was aerated with O2 30 min before and during irradiation. Cells were irradiated on ice in a 60Co source (Atomic Energy of Canada, Ltd., Kanata, Ontario, Canada). Appropriate dilutions of irradiated and control samples were plated on YPD and incubated for 4 days (RAD52 strains) or 6 days (rad52 strains) at 30°. For determination of radiosensitivity, three plates per dose point were counted.
Clonal expansion of surviving cells:
Single colonies derived from cells surviving irradiation or controls were picked and restreaked on YPD in ordered arrays. After further incubation for 4 days, the clones were transferred to 10 ml liquid Y PD medium and grown for 4 days under shaking. Two milliters of the cell suspensions were then used to generate frozen stocks, and the remainders were used to prepare genomic DNA.
Preparation of genomic yeast DNA and electrophoretic separation in pulsed-field gels:
Preparation of genomic DNA of individual clones by the agarose plug method and PFGE using the CHEF DRII system (Bio-Rad, Richmond, CA) were performed as described (![]()
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Visualization of electrophoretic karyotypes and image analysis:
After electrophoresis, gels were stained with ethidium bromide and recorded by a CCD camera as described (![]()
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Determination of chromosomal lengths:
The lengths of the chromosomal molecules of the parental strains SX46A and WS8105-1C were determined by comparing their electrophoretic mobility in CHEF gels with that of
-phage concatemeres and yeast strains YNN295 and BK0, as described (![]()
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1600 kb. The lengths of longer molecules were estimated according to their migration behavior in ZIFE gels.
Southern hybridization with chromosome-specific probes:
For the identification of altered chromosomes in case of ambiguity, Southern hybridizations were performed using centromere- or gene-specific probes. Chromosomal DNA separated by PFGE was UV nicked, denatured in 0.5 M NaOH/1.5 M NaCl (30 min), and transferred onto nylon membrane (Qiagen, Chatsworth, CA) by capillary transfer using the same buffer. Prehybridization and hybridization were carried out according to the membrane manufacturer's directions. DNA probes were generated by plasmid digestion with appropriate enzymes and gel purification of the desired fragments according to standard methods (![]()
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| RESULTS |
|---|
Construction of strains:
The aim of this work was to investigate the influence of mutational inactivation of various DSB repair pathways on the generation of radiation-induced chromosomal aberrations. Homologous recombination between sister chromatids or homologous chromosomes is a very efficient and largely error-free DSB repair mechanism in yeast. To be able to detect the influence of minor repair pathways and to obtain a reasonable quantity of aberrational misrepair events, we investigated the induction of aberrations in haploid cells irradiated in highly stationary growth phase (G0 cells). Furthermore, pilot experiments confirmed the observation (![]()
Repair-competent haploid G1 or G0 phase cells are incapable of DSB repair by homologous recombination using a homologous chromosome or sister chromatid as donor of information, but they can use ectopically located donors of information or alternative pathways of DSB repair other than homologous recombination. Cells mutated for RAD52 are not able to perform any kind of homologous recombination; furthermore, they show reduced ability for SSA. Inactivation of HDF1 affects NHEJ. Hence, in a rad52 hdf1 double mutant, all kinds of DSB repair/rejoining mechanisms known so far are completely or largely blocked. We observed a high degree of secondary DNA degradation during postirradiation incubation in rad52 hdf1 double mutants that is evident neither in the single mutants nor in a rad54 hdf1 double mutant (unpublished results), suggesting that one of two proteins, Rad52 or Hdf1, has to be present to protect broken ends against degradation. To be able to differentiate between effects caused by inactivation of homologous recombination, and those caused by enhanced DNA degradation, we included a rad54 mutant in our studies. The reduction of homologous recombination in rad54 mutants is not as complete as in rad52 mutants, but it is stronger than in any other mutant of the RAD52 epistasis group. Furthermore, rad54 mutants differ from rad52 mutants in that they are able to perform SSA.
In a first set of experiments, wild-type strain SX46A and its rad52, hdf1, and rad52 hdf1 mutant derivatives were investigated. Construction of these strains has been described in detail (![]()
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Radiosensitivity of the tested strains:
The radiosensitivity of strain SX46A and its rad52, hdf1, and rad52 hdf1 derivatives have been described (![]()
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200 Gy is equally pronounced. The rad54 and rad54 hdf1 mutants behave like rad52 and rad52 hdf1 mutants, respectively, only at doses up to
200 Gy; at higher doses, they are more resistant. This suggests that in rad54 mutants, some residual G2-specific repair takes place, albeit at a low level, and supports the notion that RAD54 is not indispensable for some low level of homologous recombination. A higher resistance of the rad54 mutant, as compared to the rad52 mutant, would be expected over the whole dose range if the ability to perform SSA had a clear impact on radiation sensitivity. The data obtained here suggest that this is not the case.
|
Detection of altered karyotypes:
Colonies arising from haploid cells that had survived irradiation and from unirradiated controls were picked randomly and expanded to obtain sufficient DNA for electrophoretic karyotyping by PFGE. Alterations in the localization of chromosomal bands or in relative band intensity are indicative of structural or numerical chromosomal aberrations. Examples of electrophoretic karyotypes in aberrant clones are shown in Figure 2. In these samples, which were all derived from strain SX46A rad52
, complete loss of chromosomal bands and appearance of new bands are clearly evident on the photographic image. Aberrational events that lead to alterations in the relative intensity of bands, however, are difficult to detect by eye because of the nonlinear response of photographic films (![]()
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To unambiguously detect karyotypic alterations, we use a simulation procedure that was developed earlier for the measurement of the frequency of DSB in yeast cells (![]()
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Examples for DNA profiles thus obtained are given in Figure 3A, showing the observed profiles of normal SX46A rad52
cells, as well as the aberrant derivatives SXrad52/350/21 and SXrad52/350/17 as solid lines. The respective simulated profiles are given as dashed lines. A good agreement between observed and computed profiles is seen for the control sample, whereas deviations are clearly evident in the samples of the aberrant clones. In clone SXrad52/350/21, the band corresponding to chromosome X (790 kb) is missing, and the double band corresponding to chromosomes XIII and XVI (1000 kb) exhibits a strongly decreased intensity. Simultaneously, two new bands whose localization correspond to the molecular lengths of 650 and 1050 kb, respectively, appear. In clone SXrad52/350/17, the band representing chromosome VI (300 kb) is absent, while the intensity of the 260-kb band is enhanced.
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These examples show that by using the simulation approach, not only complete loss or gain of new bands are easy to detect, but increases or decreases in band intensity are also easy to detect. On the basis of the observed alterations, a guess about the karyotype, i.e., lengths of individual chromosomal molecules and their relative frequencies, in the aberrant clone is made, and the validity of the karyotype is then checked by comparing the observed profiles to theoretical profiles that were computed on the basis of the new karyotype. Examples for derivatives SXrad52/350/21 and SXrad52/350/17 are shown in Figure 3B. For clone SXrad52/350/21, it was assumed that the parental chromosome X and one of the two 1000-kb chromosomes (XIII or XVI) were lost, leaving a single band at the position of the former 1000-kb double band, and that two aberrant chromosomes with lengths of 650 and 1050 kb, respectively, were generated. For clone SXrad52/350/17, it was assumed that the parental chromosome VI was lost, while a new aberrant chromosome comigrated with chromosome I, thus yielding a band of double intensity at the position corresponding to 260 kb. These assumptions led to a good agreement between observed (solid lines) and computed profiles (dashed lines).
Spontaneous karyotypic alterations:
We analyzed the frequency of aberrant karyotypes after irradiation with various doses in three independent experiments for the strains SX46A, SX46A rad52
, SX46A hdf1
, and SX46A rad52
hdf1
, two experiments for WS8105-1C hdf1
, and one experiment each for WS8105-1C, WS8105-1C rad54
, and WS8105-1C rad54
hdf1
. In each irradiation experiment, we checked 1020 clones derived from unirradiated control cells. In all strains tested, large variations (up to ~1000 kb) in the length of chromosome XII (normal length 2200 kb) in subclones derived from both irradiated and unirradiated cells were observed (data not shown). This chromosome bears a large rDNA cluster, which is known for extensive mitotic length alterations (![]()
, chromosome VII (normal length 1135 kb) is ~50 kb longer than in the other strains of the SX46A series, and exhibits variations in length between individual clones in the range of
100 kb (data not shown). Since this band did not hybridize with a probe for 18S rDNA (data not shown), its instability seems to not be caused by a transmission of rDNA sequences. We decided that even extensive length alterations of these unstable chromosomes should not be regarded as induced chromosome aberrations unless they are accompanied by further karyotypic alterations.
In one of three independent experiments with strain SX46A hdf1
, the same type of alteration (lengthening of chromosomes XIV and XIII) was observed in one unirradiated subclone and two irradiated subclones (Table 2). These alterations were not regarded as radiation induced.
|
In the experiment with strain WS8105-1C rad54
, the same type of alteration (a putative translocation between VI and XI) was detected in three irradiated subclones, hinting at a spontaneous event that took place before irradiation, during cultivation of the cells. Again, these alterations were not regarded as radiation induced.
Frequency of radiation-induced karyotypic alterations:
Colonies arising from cells that survived irradiation were picked without any bias. Therefore, the frequency of aberrant karyotypes detected reflects the radiation-induced frequency of aberrational events. The results are given in Table 2. In irradiated samples of wild-type strains, karyotypic alterations were detected at a low frequency (three out of 167 clones of irradiated cells analyzed in total in SX46A, and one out of 80 clones in WS8105-1C). In the rad52 mutant (derived from SX46A) and the rad54 mutant (derived from WS8105-1C), the frequency of aberrational clones was substantially increased (14 out of 181 and five out of 40, respectively). We assume that this difference in aberration yield reflects the difference in the use of repair pathways: In the wild type, the majority of clones surviving doses of
200 Gy probably originated from cells that were in the G2 phase at the time of irradiation. These cells were able to repair DSB by homologous recombination between sister chromatids, a highly efficient process (![]()
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HDF1 is one of the few genes known so far to be involved in illegitimate end joining. The yield of karyotypic alterations in hdf1 mutants (derived from SX46A and WS8105-1C) was low (two out of 106 and one out of 124, respectively) and comparable to the yield observed in wild-type cells.
Combination of the hdf1 mutation with inactivation of RAD52 or RAD54 abrogates the increased formation of karyotypic alterations seen in the rad52 and rad54 single mutants, indicating that the generation of aberrations in these mutants depends largely on HDF1. In the rad52 hdf1 double mutant (derived from SX46A), no aberrant clone was detected among a total of 179 analyzed clones; in the rad54 hdf1 double mutant (derived from WS8105-1C), one out of 80 clones bore a karyotypic alteration.
Characterization of aberration events:
To learn more about the formation of radiation-induced chromosomal aberrations in yeast, we started to characterize the radiation-induced aberrations found in samples with altered karyotypes. It was, however, not our intention to exactly elucidate the type of aberrational event in all clones because this would require detailed hybridization studies with a panel of probes for each chromosome.
In all aberrant clones, the chromosomal length and identity of altered bands was recorded. In case a chromosome that normally migrates in a double band with another chromosome was involved, the identity of the altered band was determined by hybridization with chromosome-specific DNA probes. The lengths of molecules migrating in newly arisen bands were determined using calibration curves for the relation between molecular length and migration distance, which were based on the positions of bands corresponding to chromosomes with known length. Descriptions of the karyotypes of all altered clones are given in Table 3 and Table 4.
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A typical stable outcome of misrepair events is a translocation. Translocations are expected to lead to loss of two (or more) parental bands and the simultaneous appearance of the same number of new bands. Furthermore, the sum of the lengths of the chromosomal molecules in the lost and new bands should be equal. We found a total of 14 aberrants that follow these criteria (Table 3). In 11 of these, two chromosomes were involved; in two aberrants (WS/500/64 and SXrad52/500/12), four chromosomes exhibited length alterations, and in one aberrant (SXrad52/500/77), three bands were altered. In most of the samples, the molecular lengths seem to not be exactly conserved, but the differences were on the order of a low percentage and may be explained by uncertainties in the determination of molecular lengths, especially when large chromosomes were involved. As expected, in all cases further analyzed by hybridization with probes for lost bands, the signal was found at the position of one of the new bands (data not shown).
One major drawback of the system is caused by the mitotically unstable chromosomes (XII and VII) because it is difficult to prove their involvement in exchange-type aberrations on the basis of length alterations. We observed seven clones exhibiting a length alteration in one band only, which was not clearly compensated by a length alteration in chromosome XII (or the likewise unstable chromosome VII in strain SX46A hdf1
). These aberrants (included in Table 4) may represent either true deletions or insertions, or translocations involving the unstable chromosomes. Further hybridization studies will be required to elucidate the type of event in these clones.
Also listed in Table 4 are two clones (SX/200/M4 and WSrad54_hdf1/500/21) that lack the band representing chromosome III. Assuming that these clones might carry a circularized chromsome III (which cannot enter the gel), we
-irradiated the cells of these clones to linearize the circle, prepared the genomic DNA directly after irradiation, and separated it by PFGE. Now, hybridization with a probe for CENIII gave a signal at a position corresponding to ~310 kb, agreeing well with the expected length if circularization occurred by fusion of the partially homologous regions HML and HMR (![]()
In one case (clone SXrad52/500/19), an obviously dicentric chromosome was formed: in this clone, the bands corresponding to chromosomes II (855 kb) and XV (1135 kb) were missing, and one new band of ~2000 kb was observed. This band gave a signal after hybridization with both probes for chromosomes II and XV (data not shown).
Clone SXrad52/500/26 showed a puzzling phenotype: Bands of three chromosomes (I, V, and XII, representing a total of 3050 kb) were missing in the karyotype, and only two new bands (460 and 1135 kb) could be detected. If a three-way interchange had taken place in this clone, a further band of ~1450 kb would be expected, which was not present. It remains to be tested whether the missing genetic material is present in a circularized chromosome.
Doubling of the relative intensity of a band, presumably indicative for a disomy, was detected in clone SX/500/18 (855 kb). A special alteration is given by clone SXrad52/200/24: here, the intensity of the 830-kb band was increased by 50% only, but a band of 660 kb also arose, but this band had only half of the stochiometric intensity.
| DISCUSSION |
|---|
FASULLO and colleagues (![]()
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Electrophoretic karyotyping allows the detection of those structural aberrations that lead to altered chromosome lengths. We estimate the limit of detection of length alterations in CHEF gels to be ~10 kb, except for the two longest chromosomes, where the limit is higher. Translocations, deletions, and insertions that result in smaller length alterations will escape detection, as will inversions.
It should be emphasized that electrophoretic karyotyping requires clonal expansion of cells, thus only aberration types that do not prevent colony formation will be obtained. Hence, the distribution of observed aberration types will differ from that observed cytogenetically in irradiated mammalian cells, where aberrations are usually scored in the first metaphase after irradiation or in scarcely dividing lymphocytes. Although a thorough elucidation of aberration types was not intended here, the observed alterations in the banding pattern allow for some conclusions about the type of the underlying aberrational event.
The simplest type of a structural interchange aberration is an exchange between two chromosomes that results in a reciprocal translocation or a dicentric chromosome plus an acentric fragment (for a recent survey on aberration types see ![]()
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In mammalian cells, it has been observed repeatedly that the frequency with which certain chromosomes are involved in translocations is not proportional to their molecular lengths, e.g., ![]()
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Structural interchange reactions can also produce dicentric chromosomes plus acentric fragments. Chromosomes with two functional centromeres as well as acentric fragments are considered unstable. In one clone (SXrad52/500/19), however, we found a putative dicentric. The apparent mitotic stability of this chromosome may be explained by mutational inactivation or loss of one of the centromeric sequences, as has already been described for yeast ( ![]()
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Besides being associated with asymmetrical interchange reactions, acentric fragments can also result from intrachromosomal rearrangements (interstitial deletion) or simply from failure to rejoin a break (terminal deletion). Because of the remarkable compactness of the yeast genome (![]()
In a similar manner, an increase in length in one chromosome species can be explained by an interchange with chromosome XII (or chromosome VII in case of strain SX46A hdf1
). Alternatively, it may be explained by insertion of unknown genetic material (see below).
In mammalian cells, circularized chromosomes are often observed after DSB induction. They are considered mitotically unstable because sister chromatid exchange can interlock the chromatids and lead to proliferative cell death. In S. cerevisiae, however, spontaneous circularization of chromosome III by recombination between the HML and HMR loci has been described (![]()
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Besides structural chromosome aberrations, numerical aberrations have also been observed after irradiation in mammalian cells, showing that ionizing radiation has clastogenic as well as aneugenic activity (![]()
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In conclusion, the banding patterns observed in clones of irradiated yeast cells can easily be explained, assuming that aberration types are similar to those frequently observed in mammalian cells, suggesting that similar mechanisms took place.
Radiation-induced chromosome aberrations were rarely detected in wild-type cells. We assume that the majority of colonies formed after irradiation originated from cells that were in the G2 phase during irradiation and thus able to repair breaks in an error-free manner by sister chromatid recombination. Although the low yield of aberrants obtained renders a statement on dose dependence difficult, no indication for an increase in the yield with dose is obvious. This suggests that the frequency of aberrants detected depends not only on the frequency of DSB, but also on the probability of G0 vs. G2 cells to survive irradiation. Out of four aberrants, we detected two bona fide translocations in wild-type cells. These may be explained by ectopic homologous recombination. Indeed, it has been shown with several kinds of model recombination substrates that induction of DSB leads to induced ectopic recombination (![]()
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In contrast to the wild type, in the rad52 mutant, the yield of aberrants was substantially higher. The majority of events detected seems to have arisen by interchromosomal reactions. As interchromosomal homologous recombination depends strongly on RAD52, these aberrations must have been caused by an alternative mechanism. In contrast to earlier findings (![]()
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By use of systems depending on the circularization of plasmids linearized in regions lacking homology to the yeast genome, it has been shown that the yeast Ku protein homologs Hdf1 and yKu80 (![]()
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In the rad54 hdf1 double mutant, one aberration, a circularized chromosome III, was detected, which was probably caused by a recombination between the partially homologous regions HML and HMR. The occurrence of alterations in the two hdf1 single mutant strains also shows that the HDF1-dependent pathway is not the only one leading to chromosomal alterations. Interestingly, all the aberrants obtained in unirradiated and irradiated samples of the two hdf1 mutant strains show enlargement of one or two chromosome species without apparent length compensation. One of these aberrant clones (SXhdf1/500/4) was repeatedly subcultivated, and single-cell subclones were karyotyped to check the length stability of the altered chromosome. We found that the length varies between the subclones (data not shown). Unstable enlargement of one chromosome (VII) is also a general feature of our strain SX46A hdf1
. Additionally, in a recent attempt to construct a hdf1
derivative of SX46A with normal karyotype, we surprisingly observed the same type of alteration in one of four candidates tested by PFGE. Taken together, these observations suggest that inactivation of HDF1 causes the insertion or amplification of (unstable) genetic material by some as yet unexplained mechanism. Therefore, we regard the chromosomal alterations found in the hdf1 mutants as being qualitatively different from those observed in the wild-type strains.
To our knowledge, this work is the first description of a decrease in the frequency of aberration induction by inactivation of one type of DSB repair, showing that functional repair mechanisms can be a prerequisite for aberration formation. In particular, we find that the yeast Ku70 homolog Hdf1 plays an important role in the generation of misrepair events. The products of the HDF1 and the yKU80 gene form a heterodimer that constitutes the major DNA end-binding activity in yeast (![]()
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No aberration data on Ku70-deficient mammalian cells have been reported so far. If one assumes that mammalian cells deficient for Ku70, Ku80, or DNA-PKcs behave similarly with respect to misrepair of DSB, however, our results obtained in yeast seem to contradict results obtained in mammalian cells in certain regards. For the Ku80-deficient hamster cell lines xrs-5, xrs-6, and XR-V15B, and for DNA-PKcs-deficient murine scid cells, an increase in the frequency of chromosomal aberrations after treatment with DSB-inducing agents has been reported. This increase seems largely attributable to terminally unrepaired breaks, but with regard to the formation of exchange-type events, conflicting data have been reported: after irradiation, an increase in the yield of exchange-type events as compared to wild-type cells was found in xrs-5 and xrs-6 cells (![]()
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| ACKNOWLEDGMENTS |
|---|
Part of this work was supported by the Commission of European Communities (grant FI4P-CT95-0010). We thank MARTIN KUPIEC and WOLFRAM SIEDE for valuable discussions, ULRIKE HAMM and TASSILO TIEMANN for expert technical assistance, and FRED AHNE, WOLF-DIETRICH HEYER, MARTIN KUPIEC, CORNELIA MORAWETZ, PETER PHILIPPSEN, and WOLFRAM SIEDE for plasmids and constructs.
Manuscript received September 8, 1997; Accepted for publication December 1, 1997.
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), WS8105-1C hdf1
), WS8105-1C rad54
), WS8105-1C rad52
), WS8105-1C rad54
), and WS8105-1C rad52
).





