HZE radiation effects for hereditary renal carcinomas.

Eker rat known as a model of hereditary renal carcinoma (RC) is an example of Mendelian dominantly inherited predisposition to a specific cancer in experimental animals. We investigate the effects of simulated space radiation on carcinogenesis using HIMAC. We estimated RBE from the Eker rats exposed to the heavy-ions, C (290 MeV/u) and Fe (500 MeV/u) ions, comparing to the effects of X-ray irradiation. Pregnant rats were exposed to C and Fe ions and X-rays with a single dose of 1 Gy, 2 Gy, 3 Gy on day 19 of gestation. The offspring were sacrificed at 8 weeks of age. We evaluated organ weights and tumor genesis. The weights of thymus, lung, liver, spleen were found to be no difference from the control at 1 Gy irradiation but 50% decrease at 3 Gy irradiation. We found in the irradiated animal that kidney, brain and testis were very sensitive organs of which the weight decreased to approximately 80% at 1 Gy and to 40% at 3 Gy irradiations. Based on the dose-response relationship of the radiation-induced carcinoma, averaged RBE ware calculated to be 1.1 for C-ion, 1.6 for Fe-ion.     

Relative cataractogenic effects of X rays, fission-spectrum neutrons, and 56Fe particles: a comparison with mitotic effects

The eyes of Sprague-Dawley rats were irradiated with doses of 2.5-10 Gy 250-kVp X rays, 1.25-2.25 Gy fission-spectrum neutrons (approximately 0.85 MeV), or 0.1-2.0 Gy 600-MeV/A 56Fe particles. Lens opacifications were evaluated for 51-61 weeks following X and neutron irradiations and for 87 weeks following X and 56Fe-particle irradiations. Average stage of opacification was determined relative to time after irradiation, and the time required for 50% of the irradiated lenses to achieve various stages (T50) was determined as a function of radiation dose. Data from two experiments were combined in dose-effect curves as T50 experimental values taken as percentages of the respective T50 control values (T50-% control). Simple exponential curves best describe dose responsiveness for both high-LET radiations. For X rays, a shallow dose-effect relationship (shoulder) up to 4.5 Gy was followed at higher doses by a steeper exponential dose-effect relationship. As a consequence, RBE values for the high-LET radiations are dose dependent. Dose-effect curves for cataracts were compared to those for mitotic abnormalities observed when quiescent lens epithelial cells were stimulated mechanically to proliferate at various intervals after irradiation. Neutrons were about 1.6-1.8 times more effective than 56Fe particles for inducing both cataracts and mitotic abnormalities. For stage 1 and 2 cataracts, the X-ray Dq was 10-fold greater and the D0 was similar to those for mitotic abnormalities initially expressed after irradiation.     

Irradiations of rabbit myofibrils with an ultraviolet microbeam. I. Effects of ultraviolet light on the myofibril components necessary for contraction

Glycerinated rabbit psoas myofibrils, F-actin, and myofibril ghosts were irradiated with ultraviolet light (UV) to investigate how UV blocks myofibril contraction. Myofibril contraction is most sensitive to 270- and 290-nm wavelength light. We irradiated I and A bands separately with 270- and 290-nm wavelength light using a UV microbeam and constructed dose-response curves for blocking sarcomere contraction. For both wavelengths, irradiations of A bands required less energy per area to block contraction than did irradiations of I bands, suggesting that the primary effects of both 270- and 290-nm wavelength light in stopping myofibril contraction are on myosin. We investigated whether the primary effect of UV in blocking I-band contraction is the depolymerization of actin by comparing the relative sensitivities of I-band contraction, F-actin depolymerization, and thin filament depolymerization to 270- and 290-nm light. We also compared the dose of UV required to depolymerize F-actin in solution with the dose needed to block I-band contraction and the dose required to alter thin filament structure in myofibril ghosts. The results confirm that UV blocks I-band contraction by depolymerizing actin. We discuss how the results might be relevant to the hypothesis that an actomyosin-based system is involved in chromosome movement.     

A proof of principle experiment for microbeam radiation therapy at the Munich compact light source

Microbeam radiation therapy (MRT), a preclinical form of spatially fractionated radiotherapy, uses an array of microbeams of hard synchrotron X-ray radiation. Recently, compact synchrotron X-ray sources got more attention as they provide essential prerequisites for the translation of MRT into clinics while overcoming the limited access to synchrotron facilities. At the Munich compact light source (MuCLS), one of these novel compact X-ray facilities, a proof of principle experiment was conducted applying MRT to a xenograft tumor mouse model. First, subcutaneous tumors derived from the established squamous carcinoma cell line FaDu were irradiated at a conventional X-ray tube using broadbeam geometry to determine a suitable dose range for the tumor growth delay. For irradiations at the MuCLS, FaDu tumors were irradiated with broadbeam and microbeam irradiation at integral doses of either 3 Gy or 5 Gy and tumor growth delay was measured. Microbeams had a width of 50 µm and a center-to-center distance of 350 µm with peak doses of either 21 Gy or 35 Gy. A dose rate of up to 5 Gy/min was delivered to the tumor. Both doses and modalities delayed the tumor growth compared to a sham-irradiated tumor. The irradiated area and microbeam pattern were verified by staining of the DNA double-strand break marker γH2AX. This study demonstrates for the first time that MRT can be successfully performed in vivo at compact inverse Compton sources.     

Adaptive response in different mitotic cycles after irradiation

The frequency of cells with chromosome aberrations and the number of aberrations per cell have been studied by metaphase analysis in the nonirradiated progeny of irradiated human blood lymphocytes. DNA fragmentation (DNA double-stranded breaks) has been investigated by DNA comet assay. To study the adaptive response (AR), PHA-stimulated lymphocytes were irradiated by the adaptive dose (0.05 Gy) in 24 h and by challenge dose (1 Gy) in 48 h after stimulation. The first through fourth mitoses were identified by 5-bromodeoxyuridine. It was found that the frequency of chromosome aberrations and double-strand breaks were increased in all mitotic cycles after the challenge irradiation. In most individuals, the adaptive response is induced by adaptive and challenge irradiations in the first and the second mitotic cycles (48 and 72 h after stimulation, respectively); however, it is absent in the third and the fourth mitoses. In the first mitosis (1Gy in 48 h after stimulation), only chromatid aberrations are observed; chromosome aberrations were registered in subsequent mitoses. DNA comet assay showed that the adaptive response was obvious at 48–72 h, but not 96 h, after stimulation. It can be concluded that the nonirradiated progeny of irradiated lymphocytes have genomic instability. The adaptive response is manifested up to the third mitosis and is explained by the decreasing number of chromatid and chromosome aberrations and DNA fragmentation. We suppose that double-stranded DNA breaks may be damage signals for the induction of adaptive response.     

RBE of the MIT epithermal neutron beam for crypt cell regeneration in mice

The RBE of the new MIT fission converter epithermal neutron capture therapy (NCT) beam has been determined using intestinal crypt regeneration in mice as the reference biological system. Female BALB/c mice were positioned separately at depths of 2.5 and 9.7 cm in a Lucite phantom where the measured total absorbed dose rates were 0.45 and 0.17 Gy/ min, respectively, and irradiated to the whole body with no boron present. The gamma-ray (low-LET) contributions to the total absorbed dose (low- + high-LET dose components) were 77% (2.5 cm) and 90% (9.7 cm), respectively. Control irradiations were performed with the same batch of animals using 6 MV photons at a dose rate of 0.83 Gy/min as the reference radiation. The data were consistent with there being a single RBE for each NCT beam relative to the reference 6 MV photon beam. Fitting the data according to the LQ model, the RBEs of the NCT beams were estimated as 1.50 +/- 0.04 and 1.03 +/- 0.03 at depths of 2.5 and 9.7 cm, respectively. An alternative parameterization of the LQ model considering the proportion of the high- and low-LET dose components yielded RBE values at a survival level corresponding to 20 crypts (16.7%) of 5.2 +/- 0.6 and 4.0 +/- 0.7 for the high-LET component (neutrons) at 2.5 and 9.7 cm, respectively. The two estimates are significantly different (P = 0.016). There was also some evidence to suggest that the shapes of the curves do differ somewhat for the different radiation sources. These discrepancies could be ascribed to differences in the mechanism of action, to dose-rate effects, or, more likely, to differential sampling of a more complex dose-response relationship.     

The response of primary keratinocytes and fibroblasts from cancer patients to multiple low-dose irradiations

In our previous study, using the micronucleus (MN) assay, a hyper-radiosensitivity (HRS)-like phenomenon was observed after single low doses for fibroblasts from two and keratinocytes from four of the 40 patients studied. In this paper, we report the response of primary keratinocytes from 23 and fibroblasts from 21 of these cancer patients to multiple low-dose irradiations and answer the question regarding whether the patients with an HRS-like response after single low doses also demonstrate chromosomal hypersensitivity after multiple low doses. The cells were irradiated with three doses of 0.25 Gy separated by 4-h intervals, and MN induction was compared with that after the same total dose given as a single fraction of 0.75 Gy. Similarly, the effect of three doses of 0.5 Gy was compared with that of a single dose of 1.5 Gy. For fibroblasts from two and keratinocytes from four patients who demonstrated a single-dose HRS-like response, a significant inverse effect of fractionation (greater MN induction after three doses of 0.25 Gy than after a single dose of 0.75 Gy) was observed, which suggests a repeated hypersensitive response after each dose of 0.25 Gy. Such an effect was not seen for the cells from 19 patients who were single-dose HRS-like negative. In conclusion, an inverse fractionation effect for MN induction that was observed in fibroblasts from two and keratinocytes from four patients after three doses of 0.25 Gy (but not 3 x 0.5 Gy) reflects the chromosomal hyper-radiosensitivity seen in the same patients in response to single low doses.     

Dose-response curves and tolerance doses for late functional changes in the normal rat brain after stereotactic radiosurgery evaluated by magnetic resonance imaging: influence of end points and follow-up time

Late reaction of normal tissue is still a limiting factor in radiotherapy and radiosurgery of patients with brain tumors. Few quantitative data in terms of dose-response curves are available. In the present study, 99 animals were irradiated stereotactically at the right frontal lobe using a linear accelerator and single doses between 26 and 50 Gy. The diameter of the spherical dose distribution was 4.7 mm (80% isodose). Dose-response curves for late changes in the normal brain at 20 months were measured using T1- and T2-weighted magnetic resonance imaging (MRI). The dependence of the dose-response curves on the follow-up time and the definition of the biological end point were determined. Tolerance doses were calculated at several effect probability levels and times after irradiation. The MRI changes were found to be dependent on dose and progressive in time. At 20 months, the tolerance doses at a 50% effect probability level were 39.6 +/- 1.0 Gy and 42.4 +/- 1.4 Gy for changes in T1- and T2-weighted images, respectively. These dose-response curves can be used for further quantitative investigations on the influence of various treatment parameters, such as the application of charged particles, radiopharmaceuticals or the variation of tissue oxygenation.     

Radiosensitivity and Biological Effects of Gamma and X-Rays on Germination and Seedling Vigour of Three Coffea arabica Varieties

Effects of gamma and X-ray treatments were studied on three varieties of Coffea arabica (Kent, Mundo Novo and Geisha) to determine their radiosensitivity and relative biological effects. The coffee varieties seeds were subjected to 0, 50, 100, 150, 200 and 400 Gy of gamma and X-rays from Cobalt 60 (⁶⁰Co) source irradiation. The irradiated seeds were pre-germinated in Petri dishes placed in a germination chamber, whilst some were sown in the greenhouse for germination studies. Data were collected on germination date and rate, root and hypocotyl length to determine the relative biological effectiveness of treatments and the optimum dose. The results showed varieties responding differently to the irradiations and doses. There was a decrease in germination with increasing doses of the irradiation. The X-ray-treated seeds had less germination percentage and seedling vigour measured at 28 days after treatment compared to the gamma-irradiated seeds. The irradiation effects on germination suggest that lower doses of X-rays give the same Relative Biological Effects as higher gamma doses for both growth chamber and greenhouse germination for Geisha at LD₅₀, where the effects were similar for the two irradiations. Whereas 50–100 Gy stimulated germination and seedling vigour, 150 Gy adversely affected germination and no germination occurred at 200–400 Gy. The study concluded that all the coffee varieties evaluated are sensitive to gamma and X-ray irradiation in terms of germination, seedling vigour and biological effects with an optimum dose of 50–100 Gy. Therefore, both gamma and X-rays could be utilized in a future mutational breeding programme for coffee seedlings.

     

Induction of external abnormalities in offspring of male mice irradiated with 252Cf neutron.

To assess the genetic effects of fission neutron, the induction of external malformations was studied in F1 fetuses after F0 male mice were irradiated. Male mice of the ICR:MCH strain were irradiated with 252Cf neutron at doses of 0.238, 0.475, 0.95 and 1.9 Gy. They were mated with non-irradiated female mice at 71-120 days after the irradiation. Pregnant females were autopsied on day 18 of gestation and their fetuses were examined for deaths and external abnormalities. No increases of pre- and post-implantation losses were noted at any dose. External abnormalities were observed at rates of 1.40% in the 0.238 Gy, 2.23% in the 0.475 Gy, 3.36% in the 0.95 Gy and 3.26% in the 1.9 Gy groups; the rate in the control group was 1.65%. The dose-response curve was linear up to 0.95 Gy, and then flattened out; the induction rate of external abnormalities was 2.7 x 10(-4)/gamete/cGy based on the linear regression. These results indicated that fission neutron effectively induces external abnormalities in F1 fetuses after spermatogonial irradiation.     

Breast cancer risk after radiotherapy in infancy: a pooled analysis of two Swedish cohorts of 17,202 infants.

The incidence of breast cancer was studied in a cohort of 17,202 women irradiated for skin hemangioma in infancy at the Radiumhemmet, Stockholm, or the Sahlgrenska University Hospital, Gothenburg. A major part of the cohort had been treated with radium-226 applicators, and the mean absorbed dose to the breasts was 0.29 Gy (range <0.01-35.8 Gy). Two hundred forty-five breast cancers were diagnosed in the cohort during the period 1958-1993, and the standardized incidence ratio (SIR) was 1.20 (95% CI 1.06-1.36). Different dose-response models were tested, and a linear model gave the best fit. Neither age at exposure, breast dose rate, ovarian dose nor time since exposure had any statistically significant modifying effect, and breast dose was the only determinant of risk. The excess relative risk per gray (ERR/Gy) was 0.35 (95% CI 0.18-0.59), which is lower than in most other studies.     

Effects of irradiation on the lip mucosa in the mice as a function of rate. Comparison with the effect of fractionation

We have investigated the effect of single doses delivered at various dose rates on the mouse lip mucosa biological system. The dose rates were: 642, 76.8, 14.1, 2.9 and 1.5 Gy/h. The incidence of desquamation in the different groups of mice was used for constructing dose effect curves. The dose leading to desquamation in 50% of the animals (ED50) was obtained by probit analysis. These ED50 were 16.5, 16.7, 19, 30.2 and 33.5 Gy for the respective dose rates. Fractionated irradiations have also been performed in the same biological system (separately published), and we have therefore been able to compare the fractionated and low dose rate irradiations. The recently published model of Dale was used for this comparison. With that mathematical approach a alpha/beta value of 7.4 Gy and a half time of repair of sublethal damage of 47 minutes have been derived. These results compare well with others from the literature on biological systems with similar characteristics (rapidly proliferating systems).     

Suitability of FISH painting techniques for the detection of partial-body irradiations for biological dosimetry

Peripheral blood was irradiated with 2, 3, 4 or 5 Gy of X rays and was mixed with nonirradiated blood at five different dilutions to simulate partial-body irradiations. Analysis by FISH was performed using whole-chromosome painting probes for chromosomes 1, 4 and 11 in combination with a pancentromeric probe. Chromosome aberrations affecting the painted fraction were classified according to the PAINT nomenclature; other unstable aberrations affecting the unpainted material were also recorded. To evaluate the suitability of painting for dose assessment in partial-body irradiations, the ability of the u test and a proposed s test to detect the expected overdispersion and the similarity between the real doses and the doses estimated using Dolphin's approach were considered. For short-term biodosimetry, compared with solid-stained dicentric analyses, the suitability of FISH painting techniques for the detection of partial-body exposures is reduced, because of the decrease in the frequency of aberrations detected by FISH and in the number of cells with two or more aberrations. For reconstruction of past doses, when only complete apparently simple translocations in cells free of unstable aberrations were considered, the detection of the overdispersion and the accuracy of dose estimations were dramatically reduced. In a partial-body exposure, as the original dose increased, the whole-body dose estimated a long time after irradiation would tend to be lower, and the difference from the original dose would tend to be greater.     

Tissue repair and repopulation in the tumor bed effect

These experiments were designed to study the kinetics and magnitude of cell repair and repopulation in tissues whose damage results in the tumor bed effect. The right hind thighs of mice were irradiated with single doses or two equal gamma-ray fractions. Interfraction intervals ranging from 30 min to 24 h (to measure the kinetics of repair from sublethal damage) and 6 and 12 weeks (to determine the extent of repopulation) were used. One day after the second radiation dose 5 X 10(5) FSA tumor cells were inoculated into the center of the irradiated field. Radiation dose-response curves were obtained by calculating the time required for tumors to reach 12 mm diameter. No recovery occurred within 6 h of the radiation delivery as measured by this assay. Some recovery, 3.2-4.6 Gy above a single radiation dose, occurred when the interval between two fractions was 24 h. With increasing interfraction intervals of 6 and 12 weeks further dose sparing occurred in the amount of 5.0-6.9 and 7.5-8.3 Gy, respectively. The data suggest that repopulation is the major contributor to the radiation dose-sparing recovery of stromal tissue and that some proliferative response may occur as early as 1 day after the first irradiation.     

Effect of preliminary adaptive irradiation on the concentration of lipid peroxidation products in blood serum and degradation of DNA in thymus of irradiated mice

The animals were irradiated within adaptive dose of 0.1 Gy and 5 hours later with a challenge dose of 2 Gy. The adaptive dose reduced the effects induced by the challenge dose of 2 Gy: the increased content of the products of lipid peroxidation reactive to thiobarbituric acid in blood serum, and the increased number of breaks in thymus DNA of irradiated mice.     

Out-of-field doses from secondary radiation produced in proton therapy and the associated risk of radiation-induced cancer from a brain tumor treatment

PurposeTo determine out-of-field doses produced in proton pencil beam scanning (PBS) therapy using Monte Carlo simulations and to estimate the associated risk of radiation-induced second cancer from a brain tumor treatment.MethodsSimulations of out-of-field absorbed doses were performed with MCNP6 and benchmarked against measurements with tissue-equivalent proportional counters (TEPC) for three irradiation setups: two irradiations of a water phantom using proton energies of 78–147 MeV and 177–223 MeV, and one brain tumor irradiation of a whole-body phantom. Out-of-field absorbed and equivalent doses to organs in a whole-body phantom following a brain tumor treatment were subsequently simulated and used to estimate the risk of radiation-induced cancer. Additionally, the contribution of absorbed dose originating from radiation produced in the nozzle was calculated from simulations.ResultsOut-of-field absorbed doses to the TEPC ranged from 0.4 to 135 µGy/Gy. The average deviation between simulations and measurements of the water phantom irradiations was about 17%. The absorbed dose contribution from radiation produced in the nozzle ranged between 0 and 70% of the total dose; the contribution was however small in absolute terms. The absorbed and equivalent doses to the organs ranged between 0.2 and 60 µGy/Gy and 0.5–151 µSv/Gy. The estimated lifetime risk of radiation-induced second cancer was approximately 0.01%.ConclusionsThe agreement of out-of-field absorbed doses between measurements and simulations was good given the sources of uncertainties. Calculations of out-of-field organ doses following a brain tumor treatment indicated that proton PBS therapy of brain tumors is associated with a low risk of radiation-induced cancer.     

Single low doses of X rays inhibit the development of experimental tumor metastases and trigger the activities of NK cells in mice

There is evidence indicating that low-level exposures to low- LET radiation may inhibit the development of tumors, but the mechanism of this effect is virtually unknown. In the present study, BALB/c mice were irradiated with single doses of 0.1 or 0.2 Gy X rays and injected intravenously 2 h later with syngeneic L1 sarcoma cells. Compared to the values obtained for sham-irradiated control mice, the numbers of pulmonary tumor colonies were significantly reduced in the animals exposed to either 0.1 or 0.2 Gy X rays. Concurrently, a significant stimulation of NK cell-mediated cytotoxic activity was detected in splenocyte suspensions obtained from irradiated mice compared to sham-exposed mice. Intraperitoneal injection of the NK-suppressive anti-asialo GM1 antibody totally abrogated the tumor inhibitory effect of the exposures to 0.1 and 0.2 Gy X rays. These results indicate that single irradiations of mice with either 0.1 or 0.2 Gy X rays suppress the development of experimental tumor metastases primarily due to the stimulation of the cytolytic function of NK cells by radiation.     

Biodosimetry using micronucleus assay in acute partial body therapeutic irradiation

Biological dosimetry provides information on the absorbed dose and its distribution in the body for an early assessment of irradiation consequences in exposed individuals. In this study, an effort has been made to see the applicability of biological dosimetry using micronuclei assay for dose estimation in therapeutic irradiation of cancer patients in acute high dose partial body irradiation. Dose estimation in partial body irradiations was done on the basis of Dolphin's contaminated Poisson method, using the in vitro dose response calibration curve. The equivalent whole body dose and the dose to the irradiated part of the body were estimated to be 1.8 ± 0.1 Gy and 6.4 ± 0.3 Gy, respectively. The estimated percentage of irradiated blood and the fraction of cells exposed were 41.5 ± 1.6% and 10.4 ± 0.8%, respectively. The estimated fraction of irradiated cells was comparable with the actual volume of irradiation.     

Chromosomal aberrations induced by (12)C6+ ions and 60Co gamma-rays in mouse immature oocytes

The ovaries of Kun-Ming strain mice (3 weeks) were irradiated with different doses of (12)C6+ ion or (60)Co gamma-ray. Chromosomal aberrations were analyzed in metaphase II oocytes at 7 weeks after irradiation. The relative biological effectiveness (RBE) of (12)C6+ ion was calculated with respect to 60Co gamma-ray for the induction of chromosomal aberrations. The (12)C6+ ion and 60Co gamma-ray dose-response relationships for chromosomal aberrations were plotted by linear quadratic models. The data showed that there was a dose-related increase in frequency of chromosomal aberrations in all the treated groups compared to controls. The RBE values for (12)C6+ ions relative to 60Co gamma-rays were 2.49, 2.29, 1.57, 1.42 or 1.32 for the doses of 0.5, 1.0, 2.0, 4.0 or 6.0 Gy, respectively. Moreover, a different distribution of the various types of aberrations has been found for (12)C6+ ion and 60Co gamma-ray irradiations. The dose-response relationships for (12)C6+ ion and 60Co gamma-ray exhibited positive correlations. The results from the present study may be helpful for assessing genetic damage following exposure of immature oocytes to ionizing radiation.     

Autoradiographically detected impairment of RNA synthesis pattern in 8-16 cell bovine embryos after irradiation

Early preimplantation bovine embryos at 8- or 16-cell stage were analysed by [5-3H]uridine autoradiography for distribution of newly synthesized RNA after 60Co irradiation with a single dose of 1 Gy, 2 Gy or 4 Gy gamma rays, respectively. Embryos irradiated with a single dose of 1 Gy showed equally decreased synthesis of RNA in nucleoplasma as well as in nucleolus. In embryos irradiated with a single dose of 2 Gy or 4 Gy, RNA synthesis was decreased and localized mostly on the periphery of the nucleus; in both cases of irradiation, the nucleus center being without labelling. In most of embryos irradiated with a dose of 4 Gy, the nucleoli were not labelled, and an increasing occurrence appeared of various nucleus chromatin segregation forms, mainly as its marginalization.