Scanning force microscopy studies of X-ray-induced double-strand breaks in plasmid DNA

We present an analysis of X-ray-induced damage in ΦX174 plasmid DNA, applying doses between D = 250 and 1,500 Gy. To analyse this damage in detail, the distribution of plasmid fragments after irradiation have been determined by scanning force microscopy. The results show that even for the lowest dose of D = 250 Gy, a significant amount of double-strand breaks are observed. For increasing dose, the percentage of small fragments increases and is accompanied by a shortening of the average fragment length from < L> = 1,400 nm for a dose of D = 250 Gy to < L> = 1,080 nm after irradiation with D = 1,500 Gy. The most crucial parameter, the average number of double-strand breaks per broken plasmid (<DSB_b> ) has been determined for the first time for the applied doses. The results show that the average number of DSBs per broken plasmid <DSB_b> increases almost linearly from a value of <DSB_b> = 1.3 after irradiation with D = 250 Gy to <DSB_b> = 1.7 after exposure to D = 1,500 Gy. The presented results show that the amount of DSBs induced by X-ray radiation in plasmid DNA can be calculated with high accuracy by means of scanning force microscopy, providing relevant information regarding the interaction of X-rays with DNA molecules.

Relative biological effectiveness of accumulated 125IdU and 125I-estrogen decays in estrogen receptor-expressing MCF-7 human breast cancer cells

The therapeutic potential for delivering a cytotoxic dose of radiation (using the decay of Auger-electron emitters) to the cell nucleus of cancer cells that express estrogen receptors (ERs) by radiolabeled estrogen was investigated in the ER-expressing human breast cancer cell line, MCF-7. The radiolabeled estrogen/ER complex irradiates the cell nucleus by binding specific DNA sequences called estrogen response elements (EREs). Cell clonogenicity and induction of DNA double-strand breaks (DSBs) by gamma radiation or accumulation of (125)I-iododeoxyuridine ((125)IdU) or E-17alpha[(125)I]iodovinyl-11betamethoxyestradiol ((125)IVME2) decays were determined. MCF-7 cells were efficiently killed by accumulation of (125)IdU (D(0) = 30 decays per cell) and (125)IVME2 decays (D(0) = 28 decays per cell). DNA DSBs were induced by the accumulation of (125)IdU (approximately 3750 decays per cell required to reduce the mean value of the elution profile to 50%) or (125)IVME2 decays (approximately 465 decays per cell required to reduce the mean value to 50%). For survival of MCF-7 cells after gamma irradiation, the D(0) was 1 Gy, and approximately 65 Gy was required to reduce the mean value to 50% for induction of DSBs. The RBE values for cell killing and induction of DSBs by (125)IVME2 relative to gamma radiation were 4.8 and 18.8, respectively. The RBE values for cell killing and induction of DSBs by (125)IdU relative to gamma radiation were 4.5 and 2.3, respectively. Cell killing in a manner similar to that induced by high-LET radiation and the high RBE for induction of DSBs by (125)IVME2 in the ER-expressing MCF-7 cells provide a biological rationale for the use of Auger electron-emitting radionuclides covalently bound to estrogen to deliver a cytotoxic dose of radiation to ER-positive cancers.     

Asymmetric field inversion gel electrophoresis: a new method for detecting DNA double-strand breaks in mammalian cells

A new method is described for detecting DNA double-strand breaks (DSBs) that utilizes asymmetric field inversion gel electrophoresis (AFIGE). DNA purified from cells in agarose plugs is subjected to AFIGE and DNA breakage quantitated by the fraction of DNA released from the plug. To test the specificity of the method for DNA DSBs, purified DNA in agarose plugs was treated for increasing times with restriction endonuclease, XhoI. After an initial time period, the fraction of DNA released increased in direct proportion to time. This correlates with the expected response for a randomly broken DNA molecule. In contrast, treatment with the single-strand breaking agent, hydrogen peroxide, over a 1000-fold range produced no release of DNA from the plug. Thus the assay appears to be specific for DNA DSBs and was used to measure DNA breaks induced by gamma radiation. Purified DNA, irradiated in agarose plugs, exhibited a log-linear dose response up to doses that release greater than 90% DNA from the plug. When live cells were irradiated in agarose, a similar linear dose response was observed up to 40 Gy and a significant signal as low as 2.5 Gy. Also in live cells, a threefold lower percentage of DNA was released from the plug over the same dose range. However, less DNA per gray is released at doses above 40 Gy and may reflect a crosslinking effect produced by the irradiation of DNA in live cells. DNA which was "pulse-labeled" was used to test the effect of DNA replication on the ability of AFIGE to detect DNA DSBs. Replicating DNA irradiated in the cell or after purification exhibited a reduced rate of release from the plug per dose of irradiation. Overall, the above results indicate that AFIGE is a sensitive method for detecting DSBs in DNA.     

The radioenhancement of two human head and neck squamous cell carcinomas by 2'-2' difluorodeoxycytidine (gemcitabine; dFdC) is mediated by an increase in radiation-induced residual chromosome aberrations but not residual DNA DSBs

PURPOSE: The present study aimed at investigating if 2'-2' difluorodeoxycytidine (dFdC) radioenhancement was mediated by an effect on induction and/or repair of radiation-induced DNA DSBs and chromosome aberrations in cells with different intrinsic radiosensitivity. METHODS: Confluent human head and neck squamous cell carcinoma cell lines designated SCC61 and SQD9 were treated with 5 microM dFdC for 3 or 24 h prior to irradiation. DNA DSBs induction and repair were analyzed by PFGE. Radiation-induced chromosome aberrations were examined with a FISH technique. RESULTS: In both cell lines, dFdC did not modify radiation-induced DNA DSBs in a dose range between 0 and 40 Gy. After a single dose of 40 Gy, dFdC affected neither the kinetic of repair nor the residual amount of DNA DSBs up to 4 h after irradiation. Whereas dFdC did not increase the induction of chromosome aberrations, after a single dose of 5 Gy, the percentage of aberrant cells and the number of aberrations per aberrant cells were significantly higher in combination with dFdC. CONCLUSION: Our data suggest that under experimental conditions yielding substantial radioenhancement, dFdC decreases the repair of genomic lesions inducing secondary chromosome breaks but has no effect on DNA DSBs repair as measured by PFGE.     

Pulsed-dose-rate and low-dose-rate brachytherapy: comparison of sparing effects in cells of a radiosensitive and a radioresistant cell line

Pulsed-dose-rate regimens are an attractive alternative to continuous low-dose-rate brachytherapy. However, apart from data obtained from modeling, only a few in vitro results are available for comparing the biological effectiveness of both modalities. Cells of two human cell lines with survival fractions of 80% (RT112) and 10% (HX142) after a single dose of 2 Gy and with different halftimes for split-dose recovery and low-dose recovery were used. The cells were irradiated with a continuous low dose rate (80 cGy per hour) or with pulsed dose rate. Two different pulsed dose rates were tested: 4.25 Gy/h and 63 Gy/h. The effects of dose per pulse and the length of the interval between the pulses were investigated while keeping the overall treatment time constant. Survival after low-dose-rate irradiation was indistinguishable from that after pulses of 4.25 Gy/h in cells of both cell lines. Survival decreased with increasing dose per pulse. When the dose rate during the pulses was increased, survival decreased even further. This effect was most pronounced for the radiosensitive HX142 cells. In clinical pulsed-dose-rate brachytherapy, iridium sources move stepwise through the implant and deliver pulses at a high dose rate locally. These high-dose-rate pulses produce greater biological effectiveness compared to continuous low dose rate; this should be taken into account.     

Induction by gamma irradiation of double-strand breaks of Escherichia coli chromosomes and their role in cell lethality

Viscoelastometric measurements of DNA from gamma-irradiated bacteria were used to identify the induction of double-strand breaks ( DSBs ) in the chromosome of Escherichia coli. It is shown by means of inhibitors of repair endonucleases and different repair mutants that most DSBs in DNA of E. coli, gamma-irradiated in buffer, arise from enzymatic incision of primary gamma-damages; therefore, previous conclusions regarding DSB repair must be reconsidered. Based on these results, much of the reparable damage is single-strand breaks, and this damage can initiate formation of gaps and ultimately, when repair is insufficient, generation of enzymatically caused DSBs . After extensive repair, the first residual DSB in the E. coli chromosome is generated at approximately 160 Gray (Gy), which corresponds to the D37 dose. We propose that DSBs induced directly by gamma-irradiation are not repaired in wild-type strains. In a recently isolated gamma-resistant strain, E. coli Gamr444 , the dose required for observation of DSB after postirradiation incubation is 1,000 Gy, which corresponds to the D37 of the strain. The resistance is proposed to be due to an ability to repair genuine DSBs .     

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

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

Radiosensitivity of human bone marrow granulocyte-macrophage progenitor cells and stromal colony-forming cells: effect of dose rate

Study of the radiation biology of human bone marrow hematopoietic cells has been difficult since unseparated bone marrow cell preparations also contain other nonhematopoietic stromal cells. We tested the clonogenic survival after 0.05 or 2 Gy/min X irradiation using as target cells either fresh human bone marrow or nonadherent hematopoietic cells separated from stromal cells by the method of long-term bone marrow culture (LTBMC). Sequential nonadherent cell populations removed from LTBMC were enriched for hematopoietic progenitors forming granulocyte-macrophage colony-forming unit culture (GM-CFUc) that form colonies at Day 7, termed GM-CFUc7, or Day 14 termed GM-CFUc14. The results demonstrated no effect of dose rate on the D0 or n of fresh marrow GM-CFUc (colonies greater than or equal to 50 cells) after plating in a source of their obligatory growth factor, colony-stimulating factor (CSF) (GM-CFUc7 irradiated at 2 Gy/min, D0 = 1.02 +/- 0.05, n = 1.59 +/- 0.21; at 0.05 Gy/min, D0 = 1.07 +/- 0.03, n = 1.50 +/- 0.04; GM-CFUc14 at 2 Gy/min, D0 = 1.13 +/- 0.03, n = 1.43 +/- 0.03; at 0.05 Gy/min, D0 = 1.16 +/- 0.04, n = 1.34 +/- 0.05). There was a decrease in the radiosensitivity of GM-CFUc7 and GM-CFUc14 derived from nonadherent cells of long-term bone marrow cultures compared to fresh marrow that was observed at both dose rates. In contrast, adherent stromal cells irradiated at low compared to high dose rate showed a significantly greater radioresistance (Day 19 colonies of greater than or equal to 50 cells; at 2 Gy/min, D0 = 0.99 Gy, n = 1.03; at 0.05 Gy/min D0 = 1.46 Gy, n = 2.00). These data provide strong evidence for a difference in the radiosensitivity of human marrow hematopoietic progenitor compared to adherent stromal cells.     

Impact of a 1.5 T magnetic field on DNA damage in MRI-guided HDR brachytherapy

PurposeSome studies have suggested that the presence of a static magnetic field (SMF) during irradiation alters biological damage. Since MRI-guided radiotherapy is becoming increasingly common, we constructed a DNA-based detector to assess the effect of a 1.5 T SMF on DNA damage during high dose rate (HDR) brachytherapy irradiation.MethodsBlock phantoms containing a small cavity for the placement of plasmid DNA (pBR322) samples were 3-D printed with biocompatible tissue equivalent material. The phantom was CT scanned and an HDR brachytherapy treatment plan was designed to deliver 20 Gy and 30 Gy doses to the DNA samples in the presence and absence of a 1.5 T SMF. Relative yields of single- and double-strand breaks (SSBs and DSBs, respectively) were computed from gel electrophoresis images of the DNA band intensities and averaged over sample sizes ranging from 12 to 30. Radiation dose was also measured in the presence and absence of the 1.5 T SMF using GafChromic™ EBT3 film placed in the coronal, sagittal, and axial planes.ResultsThe average yield of DNA with SSBs and DSBs in the presence and absence of the SMF showed no statistically significant differences (all p ≥ 0.17). Differences in the net optical densities of the EBT3 films for each plane were within experimental uncertainty, suggesting no dose difference in the presence and absence of the SMF.ConclusionsHDR irradiation in the presence of the 1.5 T SMF did not alter dose deposition to the DNA cavity nor change SSB and DSB DNA damage.     

Nanoscale analysis of clustered DNA damage after high-LET irradiation by quantitative electron microscopy – The heavy burden to repair

Low- and high-linear energy transfer (LET) ionising radiation are effective cancer therapies, but produce structurally different forms of DNA damage. Isolated DNA damage is repaired efficiently; however, clustered lesions may be more difficult to repair, and are considered as significant biological endpoints. We investigated the formation and repair of DNA double-strand breaks (DSBs) and clustered lesions in human fibroblasts after exposure to sparsely (low-LET; delivered by photons) and densely (high-LET; delivered by carbon ions) ionising radiation. DNA repair factors (pKu70, 53BP1, γH2AX, and pXRCC1) were detected using immunogold-labelling and electron microscopy, and spatiotemporal DNA damage patterns were analysed within the nuclear ultrastructure at the nanoscale level. By labelling activated Ku-heterodimers (pKu70) the number of DSBs was determined in electron-lucent euchromatin and electron-dense heterochromatin. Directly after low-LET exposure (5 min post-irradiation), single pKu70 dimers, which reflect isolated DSBs, were randomly distributed throughout the entire nucleus with a linear dose correlation up to 30 Gy. Most euchromatic DSBs were sensed and repaired within 40 min, whereas heterochromatic DSBs were processed with slower kinetics. Essentially all DNA lesions induced by low-LET irradiation were efficiently rejoined within 24 h post-irradiation. High-LET irradiation caused localised energy deposition within the particle tracks, and generated highly clustered DNA lesions with multiple DSBs in close proximity. The dimensions of these clustered lesions along the particle trajectories depended on the chromatin packing density, with huge DSB clusters predominantly localised in condensed heterochromatin. High-LET irradiation-induced clearly higher DSB yields than low-LET irradiation, with up to ∼500 DSBs per μm³ track volume, and large fractions of these heterochromatic DSBs remained unrepaired. Hence, the spacing and quantity of DSBs in clustered lesions influence DNA repair efficiency, and may determine the radiobiological outcome.     

No detectable misrejoining in double-minute chromosomes.

Pulsed-field gel electrophoresis combined with Southern hybridization and rare-cutting restriction endonuclease digestion has been used recently to quantify misrejoining of DNA double-strand breaks (DSBs) resulting from exposure to ionizing radiation. Measurements are made 24 h after a high dose of radiation. These studies have suggested that a large fraction of DSBs are misrejoined to result in gross rearrangements. In the experiments described here, we show that elimination of broken DNA also eliminates "misrejoined" DNA. Mouse cells resistant to high levels of methotrexate by virtue of 100-fold amplification of the dyhydrofolate reductase (Dhfr) gene were treated with 50 and 100 Gy of ionizing radiation. The cells were allowed to repair the damage for 24 h. After the repair period, the cells were immobilized in agarose. Aliquots of each sample were pre-electrophoresed to remove linear DNA molecules smaller than 6 Mbp resulting from apoptosis or necrosis. The samples repairing damage from 50 or 100 Gy that did not receive the pre-electrophoresis showed high levels of label in a region of the lane that could be due to misrejoining DNA molecules. However, when the DNA from cells undergoing apoptosis or necrosis was removed from these samples, the levels of "misrejoined" DNA were reduced to levels far below those of unirradiated controls. These results suggest that other radiation-induced effects present 24 h after irradiation with 50 or 100 Gy are more significant than misrejoining for altering hybridization to regions of the lane outside the specific bands. Measurements of misrejoining using PFGE, rare-cutting restriction endonucleases, and Southern hybridization are likely to be compromised by nonspecific hybridization to broken and difficult-to-digest DNA resulting from apoptosis or necrosis.     

Repair of radiation-induced heat-labile sites is independent of DNA-PKcs, XRCC1 and PARP

Ionizing radiation induces a variety of different DNA lesions; in addition to the most critical DNA damage, the DSB, numerous base alterations, SSBs and other modifications of the DNA double-helix are formed. When several non-DSB lesions are clustered within a short distance along DNA, or close to a DSB, they may interfere with the repair of DSBs and affect the measurement of DSB induction and repair. We have shown previously that a substantial fraction of DSBs measured by pulsed-field gel electrophoresis (PFGE) are in fact due to heat-labile sites within clustered lesions, thus reflecting an artifact of preparation of genomic DNA at elevated temperature. To further characterize the influence of heat-labile sites on DSB induction and repair, cells of four human cell lines (GM5758, GM7166, M059K, U-1810) with apparently normal DSB rejoining were tested for biphasic rejoining after gamma irradiation. When heat-released DSBs were excluded from the measurements, the fraction of fast rejoining decreased to less than 50% of the total. However, the half-times of the fast (t(1/2) = 7-8 min) and slow (t(1/2) = 2.5 h) DSB rejoining were not changed significantly. At t = 0, the heat-released DSBs accounted for almost 40% of the DSBs, corresponding to 10 extra DSBs per cell per Gy in the initial DSB yield. These heat-released DSBs were repaired within 60-90 min in all cells tested, including M059K cells treated with wortmannin and DNA-PKcs-defective M059J cells. Furthermore, cells lacking XRCC1 or poly(ADP-ribose) polymerase 1 (PARP1) rejoined both total DSBs and heat-released DSBs similarly to normal cells. In summary, the presence of heat-labile sites has a substantial impact on DSB induction and DSB rejoining rates measured by pulsed-field gel electrophoresis, and heat-labile sites repair is independent of DNA-PKcs, XRCC1 and PARP.     

Increased repair of gamma-induced DNA double-strand breaks at lower dose-rate in CHO cells

DNA double-strand breaks (DSBs) are highly cell damaging. We asked whether for a given dose a longer irradiation time would be advantageous for the repair of DSBs. Varying the gamma-irradiation dose and its delivery time (0.05 Gy/min low dose-rate (LDR) compared with 3.5 Gy/min high dose-rate), confluent Chinese hamster ovary cells (CHO-K1) and Ku80 mutant cells (xrs-6) deficient in nonhomologous end-joining (NHEJ) were irradiated in agarose plugs at room temperature using a cesium-137 gamma-ray source. We used pulsed-field gel electrophoresis (PFGE) to measure DSBs in terms of the fraction of activity released (FAR). At LDR, one third of DSBs were repaired in CHO-K1 but not in xrs-6 cells, indicating the involvement of NHEJ in the repair of gamma-induced DSBs at a prolonged irradiation incubation time. To improve DSB measurements, we introduced in our PFGE protocol an antioxidant at the cell lysis step, thus avoiding free-radical side reactions on DNA and spurious DSBs. Addition of the metal chelator deferoxamine (DFO) decreased more efficiently the basal DSB level than did reduced glutathione (GSH), showing that measuring DSBs in the absence of DFO reduces precision and underestimates the role of NHEJ in the dose-rate effect on DSB yield.     

Induction and rejoining of large DNA fragments after ion irradiation.

Radiation-induced DNA double-strand breaks (DSBs) were analyzed by separating large DNA fragments by pulsed-field gel electrophoresis. Human U-343MG glioma and K562 erythroleukemia cells were irradiated with 60Co gamma rays or nitrogen ions with high linear energy transfer (125 keV/microm). By comparing the fraction of DNA released into the gel below different size thresholds, corresponding to megabase-pair-sized DNA fragments, the relative effectiveness of the nitrogen ions was found to be dependent on both dose and the threshold size used in the evaluation. This dose dependence was most evident for the smallest threshold (6 Mbp) and was due to a linear dose response for release of the fragments for the ions compared to the curvilinear response for the gamma rays. The two curves intersected, and the relative yield of fragments (nitrogen ions/gamma rays) decreased from more than 3 below 1.5 Gy to 0.8 at 30 Gy. For the larger sizes (6-10.5 Mbp), the relative yield was constant at around 0.7. Thus the ion-induced fragments were shifted to smaller sizes compared to the 60Co gamma rays, and the data for nitrogen ions could not be fitted to random fragment distributions at doses < or =20 Gy. From these results, we conclude that a substantial fraction of the DSBs induced by heavy ions were nonrandomly distributed, correlated with DSBs within a region of < or =2 Mbp. After a dose of 20 Gy, the rejoining curves for ion-induced DSBs were different for each fragment size, resulting in different levels of unrejoined breaks after 6 h.     

Dose-rate effect on the induction of HPRT mutants in human G0 lymphocytes exposed in vitro to gamma radiation

The influence of dose rate on expression time, cell survival and mutant frequency at the hypoxanthine-guanine phosphoribosyltransferase (HPRT) locus was evaluated in human G(0) peripheral blood lymphocytes exposed in vitro to gamma rays at low (0.0014 Gy/min) and high (0.85 Gy/min) dose rates. A cloning assay performed on different days of postirradiation incubation indicated an 8-day maximum expression period for the induction of HPRT mutants at both high and low dose rates. Cell survival increased markedly with decreasing dose rate, yielding D(0) values of 3.04 Gy and 1.3 Gy at low and high dose rates, respectively. The D(0) of 3.04 Gy obtained at low dose rate could be attributed to the repair of sublethal DNA damage taking place during prolonged exposure to low-LET radiation. Regression analysis of the mutant frequency yielded slopes of 12.35 x 10(-6) and 3.66 x 10(-6) mutants per gray at high and low dose rate, respectively. A dose and dose-rate effectiveness factor of 3.4 indicated a marked dose-rate effect on the induced HPRT mutant frequency. The results indicate that information obtained from in vitro measurements of dose-rate effects in human G(0) lymphocytes may be a useful parameter for risk estimation in radiation protection.     

Cell death (apoptosis) in mouse intestine after continuous irradiation with gamma rays and with beta rays from tritiated water

Apoptosis is a pattern of cell death involving nuclear pycnosis, cytoplasmic condensation, and karyorrhexis. Apoptosis induced by continuous irradiation with gamma rays (externally given by a 137Cs source) or with beta rays (from tritiated water injected ip) was quantified in the crypts of two portions of mouse bowel, the small intestine and descending colon. The time-course change in the incidence of apoptosis after each type of radiation could be explained on the basis of the innate circadian rhythm of the cells susceptible to apoptotic death and of the excretion of tritiated water (HTO) from the body. For 6-h continuous gamma irradiation at various dose rates (0.6-480 mGy/h) and for 6 h after injection of HTO of various radioactivities (0.15-150 GBq per kg body wt), the relationships between dose and incidence of apoptosis were obtained. Survival curves were then constructed from the curves for dose vs incidence of apoptosis. For the calculation of the absorbed dose from HTO, the water content both of the mouse body and of the cells was assumed to be 70%. One megabecquerel of HTO per mouse (i.e., 40 MBq/kg body wt) gave a dose rate of 0.131 mGy/h. The mean lethal doses (D0) were calculated for gamma rays and HTO, and relative biological effectiveness values of HTO relative to gamma rays were obtained. The D0 values for continuous irradiation with gamma rays were 210 mGy for small intestine and 380 mGy for descending colon, and the respective values for HTO were 130 and 280 mGy, indicating the high radiosensitivity of target cells for apoptotic death. The relative biological effectiveness of HTO relative to 137Cs gamma rays for cell killing in both the small intestine and the descending colon in the mouse was 1.4-2.1.     

The effect of graded doses of fission neutrons or X rays on the lymphoid compartment of the thymus in mice

Young adult CBA/H mice were exposed to graded doses of whole-body irradiation with either fast fission neutrons or 300 kVp X rays at center-line dose rates of 0.1 and 0.3 Gy/min, respectively. Dose-response curves were determined at Days 2 and 5 after irradiation for the total thymic cell survival and for the survival of thymocytes defined by monoclonal anti-Thy-1, -Lyt-1, -Lyt-2, and -T-200 antibodies as measured by flow cytofluorometric analysis. Cell dose-response curves of thymocytes show, 2 days after irradiation, a two-component curve with a radiosensitive part and a part refractory to irradiation. The radiosensitive part of the dose survival curve of the Lyt-2+ cells, i.e., mainly cortical cells, has a D0 value of about 0.26 and 0.60 Gy for neutrons and X rays, respectively, whereas that of the other cell types has corresponding D0 values of about 0.30 and 0.70 Gy. The radiorefractory part of the dose-response curves cannot be detected beyond 5 days after irradiation. At that time, the Lyt-2+ cells are again most radiosensitive with a D0 value of 0.37 and 0.99 Gy for neutrons and X rays, respectively. The other measured cell types have corresponding D0 values of about 0.47 Gy. The fission neutron RBE values for the reduction in the thymocyte populations defined by either monoclonal anti-Thy-1, -Lyt-1, -Lyt-2, or -T-200 antibodies to 1.0% vary from 2.6 to 2.8. Furthermore, the estimated D0 values of the Thy-1-, T-200- intrathymic precursor cells which repopulate the thymus during the bone marrow independent phase of the biphasic thymus regeneration after whole-body irradiation are 0.64-0.79 Gy for fission neutrons and 1.32-1.55 Gy for X rays.     

Preimplantation growth delay and micronucleus formation after in vivo exposure of mouse zygotes to fast neutrons.

Mouse zygotes were irradiated with fast neutrons (0.06 to 1.00 Gy) 1 h after conception and examined at various intervals (24 to 100 h after conception) for embryonic development and micronucleus formation. The frequency of micronuclei per cell increased linearly with dose in 2-cell embryos observed at 24 h after conception and in 4-cell and 8-cell embryos at 48 h after conception. Compared with X rays, the relative biological effectiveness of neutrons for the induction of micronuclei per embryo was 2.5 at 24 h after conception and 3.5 at 48 h after conception. Neutron-induced micronucleus formation was accompanied by morphological growth delay and a significant decrease in the number of cells in the embryos. An inverse relationship was found between the number of cells in embryos and the number of micronuclei when observed at 48 h after conception following irradiation with 0.12 to 1.00 Gy and at 78 h after conception following exposure to 0.50 Gy. The effect of neutron irradiation on embryonic development was likely to be mediated by cell death, as suggested by a significantly increased dead cell index in blastocysts following irradiation of zygotes.     

The relative biological effectiveness of low doses of 14 MeV neutrons in steady-state murine spermatogenesis as determined by flow cytometry

The relative biological effectiveness of 14 MeV neutrons in the low-dose range < or =1 Gy has been determined in differentiating and differentiated spermatogonia. Male NMRI mice were exposed to single doses of 2 cGy to 3 Gy of (60)Co gamma rays or neutrons. The ratios of testicular S-phase cells, 4c primary spermatocytes, and elongated spermatids were quantified by DNA flow cytometry 2 to 70 days after irradiation and were found to decrease. Histological samples and testis weight were analyzed in parallel. Doses of 2-5 cGy neutrons and 10-50 cGy gamma rays significantly (P<0.05) decreased the proportions of S-phase cells, spermatocytes and elongated spermatids at 4, 14 and 28 days postirradiation. For S-phase cells, the biphasic shape of the cell survival curves was described with a D(50) of 5 cGy neutrons. The D(50) for (60)Co gamma rays and the relative biological effectiveness could not be determined. The relative biological effectiveness of neutrons at 50% reductions of testis weight, primary spermatocytes, and elongated spermatids were 2.5, 10.0 and 6.1, respectively. This in vivo assay is interesting because of its sensitivity at dose ranges that are relevant for exposures in the environment, the workplace and radiotherapy.     

γ射线对人淋巴细胞cx43和ANLN基因转录表达的影响

目的研究γ射线对人外周血淋巴细胞cx43和ANLN基因转录表达的影响。方法对数生长期的淋巴细胞,分别给予1、2、3、4、5、6 Gy的^60Coγ射线照射,照射后12h,以及2Gy照射后4、8、12、24、36、48、72h,分别提取总RNA,反转录成cDNA。利用实时荧光定量PCR技术,检测各组cx43和ANLN基因表达改变。结果人外周血淋巴细胞cx43 mRNA表达水平在2Gy照射后4、8、12h明显增高,分别为对照组（未照射组）的6．74、9．06、7．22倍（P〈0．05）;24～72h,其表达水平与对照组相比没有明显变化。1、2、3、4、5、6Gy剂量照射后12h,cx43 mRNA表达水平显著增高（P〈0．05）。ANLN mRoNA表达水平在2Gy不同时间点及1～5Gy照射后12h,表达降低（P〈0．05）,6Gy照射后12h其表达开始升高,为对照组的6．08倍（P〈0．05）。结论γ射线照射2Gy不同时间点及不同剂量照射后12h,cx43基因表达上调,ANLN基因表达下调。1～3Gy剂量照射后12h,cx43 mRNA表达在此范围内有时间和剂量的依赖性。cx43可能会发展为核事故受照射人员的分子生物学剂量标记物。