The response of spermatogonia and spermatocytes of the Northern vole Microtus oeconomus to the induction of sex-chromosome nondisjunction, diploidy and chromosome breakage by X-rays and fast fission neutrons

Microtus males were exposed to different doses of 250 kV X-rays or fast fission neutrons of 1 MeV mean energy. Early (= round) spermatids were analyzed for the presence of extra sex chromosomes, diploidy and micronuclei at different time intervals corresponding with treated differentiating spermatogonia and spermatocytes. Induction of nondisjunction of sex chromosomes could not be detected. In contrast, induction of diploids by both types of radiation was statistically significant at all sampling times. Dose-effect relationships for most of the sampling times were linear and sometimes linear-quadratic concave upward or downward. There were pronounced stage-specific differences in sensitivity as reflected by differences in doubling doses that ranged from 4 to 22 cGy for X-rays and from 0.4 to 4 cGy for neutrons. Spermatocytes at pachytene were the most sensitive cells and proliferating spermatogonia the least sensitive ones. The relative biological effectiveness (RBE) of neutrons depended on the cell stage treated and fluctuated between 1.4 and 9.2. Evidence for radiation-induced chromosomal breakage events was obtained via detection of micronuclei. Induction of micronuclei by X-rays or neutrons was statistically significant at all spermatocyte stages tested. There was no effect in spermatogonia. With a few exceptions dose-effect relationships were linear. Differences in stage sensitivity were clearly present as evidenced by doubling dose which ranged from 5 to 29 cGy for X-rays and from 1 to 3 cGy for neutrons. RBE values varied from 5.2 to 12.7. Maximum sensitivity was detected in spermatocytes at diakinesis, MI and MII. Resting primary spermatocytes (G1 and S phase) were somewhat less sensitive and actively proliferating spermatogonia were the least sensitive cells. The pattern of stage sensitivity for induction of diploids was distinctly different from that for induction of chromosomal breakage.     

Lung tumour induction in mice after X-rays and neutrons

Dose-response curves were determined for pulmonary adenomas and adenocarcinomas in mice after single acute doses of 200 kVp X-rays and cyclotron neutrons (E = 7.5 MeV). A serial-killing experiment established that the radiation induces the tumours and does not merely accelerate the appearance of spontanoeus cancers [corrected]. The dose versus incidence (I) of tumours in male and female mice for X-ray doses between 0.25 and 7.5 Gy is 'bell-shaped' and best fitted with a purely quadratic induction and exponential inactivation terms, i.e. I = A + BD2e-alpha D. In contrast, the tumour dose-response after 0.1-4.0 Gy of neutrons is best fitted by I = A + BDe-alpha D and is steeply linear less than or equal to 1 Gy, peaks between 1 and 3 Gy and sharply declines at 4.0 Gy. The data for the female mice less than or equal to 1 Gy neutrons are best fitted to the square root of the dose. A major objective of the experiments was to derive neutron RBE values. Because of the differences between the X-ray (quadratic) and neutron (linear) curves, the RBEn will vary inversely with decreasing X-ray dose. The RBE values at 1 Gy of X-rays derived from the B coefficients in the above equations are 7.4 +/- 3.2 (male and female); 8.6 +/- 3.6 (female) and 4.7 +/- 1.8 (male). These are high values and imply even higher values at the doses of interest to radiation protection. If, however, one restricts the analysis to the initial, induction side of the response (less than or equal to 1 Gy neutrons, less than or equal to 3 Gy X-rays) then good linear fits are obtainable for both radiations and indicate neutron RBE values of 7.4 +/- 2.3 for female mice and 4.5 +/- 1.8 for males, and these are independent of dose level.     

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.     

The induction by ionizing radiation of chromosomal aberrations in rhesus monkey pre-meiotic germ cells: effects of dose rate and radiation quality

The induction of reciprocal translocations in rhesus monkey stem-cell spermatogonia was studied using multivalent analysis at metaphase of primary spermatocytes. Animals were exposed to 1 Gy gamma-rays at dose rates of 140 and 0.2 mGy/min or to 0.25 Gy acute 2 MeV neutrons. Reduction of the dose rate from 140 mGy/min to 0.2 mGy/min did not result in a lowering of the frequencies of recovered translocations of 0.43%. The neutron data indicated an RBE (neutrons vs. X-rays) of 2.1, which is clearly lower than the value of 4 obtained in the mouse. It is made plausible that in general mammalian species with high sensitivities for the cytotoxic effects of ionizing radiation, such as the rhesus monkey, will exhibit relatively high threshold dose rates below which no further reduction in aberration yield occurs, whereas in more resistant species, such as the mouse, the threshold dose rate will be at a very low level. Similarly, resistant species will show relatively high RBE values for neutron irradiation and sensitive species low ones.     

Biological effectiveness of fast neutrons with a mean energy of 22 MeV

Biological effectiveness of fast neutrons of a mean energy of 22 MeV obtained by the reaction d[50 MeV]----Be, measured by the death rate, was substantially lower than that of division spectrum neutrons of a mean energy of 1.2 MeV. LD50/30 of the division spectrum neutrons was within 2.57 +/- 0.07 Gy and that of 22 MeV fast neutrons 4.79 +/- 0.13 Gy. The RBE coefficient for the studied neutrons was 1.34 +/- 0.05 as estimated by LD50/30 and 1.5 +/- 0.1 as determined by D37 for a cell model of radiation affection.     

Relative biological efficiency of neutrons (2 MeV) and X-rays for mastocytoma cell division capacity]

The effects of 2 MeV neutrons were compared with those of 200 kV X-rays for the criterion of lethality in mastocytoma cells of ascites type. The cells prepared as suspension were exposed to the radiations in vitro under aerobic condition and transplanted in the abdominal cavity of mice. Their viability was estimated according to the growing speed of the excreted amount of urinary 5-HIAA in the host animal. The RBE varied between a value of 3.1 at the 10 per cent level of cell survival to 1.8 for the mean lethal dose (Do).     

The RBE of 0.85 MeV neutrons on guinea pig mortality

A comparative study was made of the death rate of guinea pigs after neutron (0.85 MeV) and 137Cs-gamma-radiation (0.66 MeV); LD50/30 were 1.58 and 3.44 Gy respectively. CRBE of neutrons was 2.2 as determined by median lethal dose values for guinea pigs.     

Flow cytometric analysis of the effects of 0.4 MeV fission neutrons on mouse spermatogenesis

(C57Bl/Cne X C3H/Cne)F1 male mice were irradiated with single acute doses of 0.4 MeV neutrons ranging from 0.05 to 2 Gy, and testis cell suspensions were prepared for cytometric analysis of the DNA content 2-70 days after irradiation. Various cell subpopulations could be identified in the control histogram including mature and immature spermatids, diploid spermatogonia and spermatocytes, tetraploid cells and cells in the S-phase. Variations in the relative proportions of different cell types were detected at each dose and time, reflecting lethal damage induced on specific spermatogenetic stages. The reduction of the number of elongated spermatids 28 days after irradiation was shown to be a particularly sensitive parameter for the cytometrical assessment of the radiosensitivity of differentiating gonia. A D0 value of 0.13 Gy was calculated and compared with data obtained after X-irradiation, using the same experimental protocol. In the latter case a biphasic curve was obtained over the dose range from 0.25 to 10 Gy, possibly reflecting the existence of some cell population heterogeneity. RBE values were estimated at different neutron doses relative to the radiosensitive component of the X-ray curve, and ranged from 3.3 to 4, in agreement with data in the literature. Genotoxic effects were monitored 7 days after irradiation by a dose-dependent increase of the coefficient of variation (CV) values of the round spermatid peak, reflecting the induction of numerical and structural chromosome aberrations, and 14 or 21 days after irradiation by the detection of diploid elongated spermatids, probably arising from a radiation-induced complete failure of the first or second meiotic division.     

Survival and proliferative activity of L-cells after irradiation with neutrons of different energies

With L-cells exposed to neutrons and X-rays the RBE of fission spectrum neutrons (1.2 MeV) was 2.8, and that of high-energy neutrons (22 MeV), 1.3. X-Irradiation with small doses (0.25 to 0.50 Gy) exerted a stimulatory effect on the growth and division of cells.     

The influence of hypoxia on the relative sensitivity of human tumor cells to 62.5 MeV (p-->Be) fast neutrons and 4 MeV photons

Fast neutrons have been used in the clinical radiation therapy of tumors largely because of experimental evidence that their cytotoxic effects are much less dependent on oxygen levels than those of low-LET photons. The potential therapeutic advantage of fast neutrons based on hypoxia alone can be calculated as the "hypoxic gain factor", which is the ratio of the OERs for the fast-neutron compared to the photon beams. The hypoxic gain factor that is generally anticipated based on studies with established mammalian cell lines is about 1.6. However, surprisingly few studies have examined the influence of hypoxia on the fast-neutron radiosensitivity of human tumor cells of different histological types. For this reason, we have determined the OERs of five human tumor cell lines exposed to 62.5 MeV (p-->Be) cyclotron-generated fast neutrons or 4 MeV photons from a clinical linear accelerator. The OERs for four chemotherapy-naive cell lines, HT29/5, Hep2, HeLa and RT112, were invariably greater for photons than for neutrons, but all of these values were lower than expected on the basis of the previous literature. Despite their low OERs, these cell lines showed hypoxic gain factors that were within the range of 1.31-1.63, indicating that such effects cannot entirely explain the disappointing clinical results obtained with fast neutrons. In contrast, comparison of the surviving fractions at clinically relevant doses (1.6 Gy of neutrons and 2.0 Gy of photons) for these four tumor cell lines suggested that little benefit should result from neutron treatment. Only the cisplatin-resistant OAW42-CP line showed a significant hypoxic gain factor by this method of analysis. We conclude that, at the dose fractions used in clinical radiation therapy, there may not be a radiobiological precedent for higher local control rates after fast-neutron irradiation of hypoxic tumor cells.     

The use of 'top-up' experiments to investigate the effect of very small doses per fraction in mouse skin

The partial tolerance type of 'top-up' experiment has been investigated to determine the resolution of this approach for studying the damage to mouse skin from very small doses of X-rays and neutrons. The effect of 20 fractions, each as small as 0.10 Gy of X-rays or of 0.05 Gy of neutrons, can be detected if 3 MeV neutrons are used as the 'top-up' reference radiation. This capability results from the almost linear underlying dose-response curve and highly reproducible dose-effect relationship for the low energy neutrons. The data fit the linear quadratic model of dose fractionation for X-rays down to fractional doses of 0.75 Gy, but at lower doses there is a trend towards an increase in the skin radiosensitivity. Modelling shows that this might be consistent with a sub-population of the cells showing an exceptional radiosensitivity, and a replenishment of this subpopulation occurring in the 8 h between small dose fractions. More experiments are needed at very low doses in order to confirm this hypothesis for skin and for other tissues.     

The r.b.e. of different energy neutrons as measured by the heamatopoietic spleen-colony technique.

The spleen-colony technique has been used for determining the relative biological effectiveness (r.b.e.) for several energies of neutron radiation. Donor mice were exposed for fission and accelerator-generated neutrons at a variety of doses and energies. Immediately after exposure, donor bone-marrow was removed from the hind legs, and standard amounts were injected intravenously into lethally X-irradiated recipients. After 7 days the recipients spleens were evaluated for surface colonies. Dose-response curves were obtained for each type of radiation and the Do was determined. The neutron r.b.e. values from the Do compared with 250kVp X-rays were: reactor 1.58, 252Cf 1:59, and accelerator varied from 2.85 at 1.0 Mev to 0.85 at 13.4 MeV.     

Relative biological effectiveness of gamma-neutron irradiation with neutron energy of 0.9 MeV

Relative biological effectiveness (RBE) of gamma-neutron radiation with neutron energy of 0.9 MeV was estimated with a reference to rat death. It was shown that RBE of gamma-neutron radiation (the share of neutrons was 67% as related to dose) at LD33/30 and LD100/30 was 2, and RBE of 0.9 MeV neutrons, in experiments with mixed radiation, was 3.1 and 2.86 at LD33/30 and LD100/30, respectively. The value of a maximum dose at which death was not registered during 30 days, was 1 Gy with gamma-neutron radiation and 4 Gy with X-radiation.     

Induction of chromosome aberrations and cell killing in Syrian hamster fibroblasts by gamma-rays, X-rays and fast neutrons

Chromosome aberrations were scored in BHK21 C13 Syrian hamster fibroblasts, exposed to 60Co gamma-rays, 250 kV X-rays, 15 MeV neutrons or neutrons of mean energy 2.1 MeV produced from the 9Be(d,n)10B reaction. The cells were irradiated in stationary phase, where they are concentrated in the G1 phase of the cell cycle. Within experimental uncertainty there was no detectable difference between the responses to 60Co gamma-rays and to 250kV X-rays. The r.b.e. for the production of dicentrics, based on the 'one-hit' component of response, was (5 +/- 2) for the 15 MeV neutrons and (12 +/- 5) for the 2.1 MeV neutrons. For each radiation, a graph of the proportion of cells without a dicentric, centric ring or acentric fragment corresponded closely to the survival curve for stationary-phase cells obtained in the same experiment.     

Relative biological effectiveness of x-rays and fast neutrons in inducing translocations in mouse spermatogonia

The dose-response relationships for inducing translocations in the spermatogonia of mice were studied, and they were compared for 200 kVp X-rays and 2 MeV fast neutrons. The dose response for fast neutrons was markedly convex; more precisely, the response obtained was linear in the dose range from 24 to 94 rad with a regression coefficient of 11.36·10^?4, but decreased for a further increase in dose up to 267 rad. On the other hand, that for X-rays showed a linear dose-response relationship from 48 to 672 rad with a regression coefficient of 2.69·10^?4. The relative biological effectiveness for inducing translocations in the spermatogonia of mice was compared for the linear parts of the dose response in both types of radiation, and the relative biological effectiveness (RBE) value was 4.22.     

Chromosome aberration analysis and the influence of mitotic delay after simulated partial-body exposure with high doses of sparsely and densely ionising radiation

The influence of high doses of sparsely and densely ionising radiation on the yield of aberrant human peripheral lymphocytes in simulated partial-body exposures was studied by investigating radiation-induced chromosome aberration frequencies, namely dicentric and centric ring chromosomes. Peripheral blood samples from two volunteers were irradiated with high doses of 200 kV X-rays or neutrons with a mean energy of <E _n>=2.1 MeV and partial-body exposure was simulated by mixing irradiated and non-irradiated blood from the same two donors in proportions of 25, 50, and 75%. Lymphocytes were cultured and first-division metaphase cells were collected after culture times of 48, 56, and 72 h. A significant underrepresentation of dicentric and centric ring chromosomes was observed at the three highest doses of X-rays between the different culture times for nearly all proportions. After neutron irradiation, some significant differences were observed at all doses and all culture times, without however, revealing any systematic pattern. The distribution of dicentric and ring chromosomes showed overdispersion for both radiation types. After simulated partial-body exposures with 200 kV X-rays and <E _n>=2.1 MeV neutrons, strong mitotic delays could be observed, which depended on both the irradiated volume and the applied dose: the smaller the irradiated volume and the higher the dose, the higher was the selective advantage of non-irradiated cells. For the purpose of biological dosimetry after partial body exposure, an extension of the lymphocyte culture time is suggested at least for doses ≥3.0 Gy of 200 kV X-rays and ≥0.5 Gy of <E _n>=2.1 MeV neutrons in order to prevent a systematic underestimation of cytogenetic damage.     

Effect of low doses of 14 MeV neutrons on polymers

The structural modifications of polymers irradiated with 14 MeV neutrons were studied. Two elastomers, a polypropylene-type polymer and poly(ethylene oxide) were exposed to low doses of fast neutrons in the range of 0.3-14 Gy. The radiation damages were observed at the molecular scale by infrared spectroscopy. The morphological changes were investigated by steric exclusion chromatography, insoluble fraction measurements, differential scanning calorimetry and X-ray diffraction. It was found that neutrons provoked oxidation processes accompanied by modifications in the polymer architecture, including chain scissions, crosslinking reactions and changes in the crystallinity. Moreover, the conventional antioxidants were shown to be inefficient in inhibiting the aging of the polymers. These results also suggest that the radiation damages could be used successfully for dosimetry applications using an easily implementable protocol.     

Oncogenic transformation by fractionated doses of neutrons

Oncogenic transformation was assayed after C3H 10T1/2 cells were irradiated with monoenergetic neutrons; cells were exposed to 0.23-, 0.35-, 0.45-, 5.9-, and 13.7-MeV neutrons given singly or in five equal fractions over 8 h. At the biologically effective neutron energy of 0.45 MeV, enhancement of transformation was evident with some small fractionated doses (below 1 Gy). When transformation was examined as a function of neutron energy at 0.5 Gy, enhancement was seen for cells exposed to three of the five energies (0.35, 0.45, and 5.9 MeV). Enhancement was greatest for cells irradiated with 5.9-MeV neutrons. Of the neutron energies examined, 5.9-MeV neutrons had the lowest dose-averaged lineal energy and linear energy transfer. This suggests that enhancement of transformation by fractionated low doses of neutrons may be radiation-quality dependent.     

Effect of negative pions,relative to 140 kV - 29 MeV photons and 20 MeV electrons,on proliferation of Ehrlich ascites carcinoma cells

Summary The effect of negative pions (peak and plateau), photons (140 kV and 29 MeV), and 20 MeV electrons on the proliferative capacity of Ehrlich ascites carcinoma cells was investigated. Proliferative survival curves plotted for the modalities employed are presented. Under the experimental conditions used, the peak pions were more effective than plateau pions by a factor of about 1.4. For 50% survival, 140 kV X-rays had the same effect as peak pions but the latter was more effective (factor 1.2) at 10% survival level. When 140 kV X-rays were taken as the standard, following are the RBE values calculated at 50% survival level: plateau pions -0.73; peak pions -about 1.0; 29 MeV photons -0.73 and 20 MeV electrons -0.6. The results obtained are compared with those reported on other tumor systems and biological test objects.