Comparison of recovery from potential mitotic abnormality in mitotically quiescent lens cells after X, neutron, and 56Fe irradiations

After exposure to various doses of 250 kVp X radiation, 0.85 Me V fission spectrum neutrons, or 600 MeV/A iron (Fe) particles, mitotically quiescent rat lens cells showed no visible evidence of radiation injury. However, following the mitogenic stimulus of wounding, mitotic abnormalities became evident when responding cells entered mitosis. Latent damage and recovery therefrom were monitored at 3, 7, 14, and 28 days after irradiation. Following doses of 1 to 10 Gy of X radiation, the recovery rate, indicated by a decrease in abnormalities with time, was proportional to dose, and the dose-effect slope decreased exponentially with time. Virtually no recovery occurred during the 28 days after 1.25 to 2.25 Gy of fission neutron radiation. After doses of 0.5 to 3.0 Gy of Fe particles, an increased expression of mitotic damage or recovery than recovery occurred. As a consequence of the differing patterns in time for expression of damage or recovery following X rays and the high-LET radiations, the relative biological effectiveness (RBE) increased from 3.6 to 16 for neutrons and from 2 to 10 for Fe particles over the 28-day observation period.     

Sequential exposures of mammalian cells to low- and high-LET radiations. II. As a function of cell-cycle stages

The synergistic effects of low- and high-LET radiations were further studied with partially synchronized Chinese hamster V79 cells. Principally, nearly monoenergetic 425 MeV/u neon ions and 570 MeV/u argon ions produced near the Bragg peak were employed as the high-LET radiations and 225 kVp X rays as the low-LET counterpart. It was found that the killing effect due to damage interaction after sequential irradiations with the particle beam and X rays varies throughout the cell cycle. The greatest effect was observed in late-S phase which was most resistant to either of the radiations. The effect was quantitatively less in the G1/S border and in G2. Effects on pure mitotic cells have not been investigated in this study. For all cell stages studied, a dose of high-LET particles modified the shape of the X-ray survival curve in a way similar to the modification predicted by an appropriately selected X-ray dose. This finding suggests that the mechanism for the synergistic effects is similar to that operating for sequential treatments with X rays alone. Experiments with an S population, either incubated at 37 degrees C or room temperature between fractionation of high- and low-LET radiation treatments further verified that the damage involved is a repairable type. At a certain fractionation interval (6 to 8 h) following a dose of high-LET treatment, initially asynchronous cells were found to be very sensitive to X-irradiation. It is noteworthy that the net killing measured at this "radiosensitive window" was as effective as the killing observed by "immediately" sequential treatments with the same doses of high- and low-LET radiations. Such a time window also existed when the order of the treatment sequence was reversed except that the time of occurrence was earlier and the window was broader. This sensitization effect may be explained by radiation-induced G2 arrest together with an increase of radiosensitivity as the previously irradiated cells progress into S phase. Radiotherapy strategies using combined high-LET and low-LET radiations for rapidly proliferative tumors are presented.     

Cell killing and chromatid damage in primary human bronchial epithelial cells irradiated with accelerated 56Fe ions

We examined cell killing and chromatid damage in primary human bronchial epithelial cells irradiated with high-energy 56Fe ions. Cells were irradiated with graded doses of 56Fe ions (1 GeV/nucleon) accelerated with the Alternating Gradient Synchrotron at Brookhaven National Laboratory. The survival curves for cells plated 1 h after irradiation (immediate plating) showed little or no shoulder. However, the survival curves for cells plated 24 h after irradiation (delayed plating) had a small initial shoulder. The RBE for 56Fe ions compared to 137Cs gamma rays was 1.99 for immediate plating and 2.73 for delayed plating at the D10. The repair ratio (delayed plating/immediate plating) was 1.67 for 137Cs gamma rays and 1.22 for 56Fe ions. The dose-response curves for initially measured and residual chromatid fragments detected by the Calyculin A-mediated premature chromosome condensation technique showed a linear response. The results indicated that the induction frequency for initially measured fragments was the same for 137Cs gamma rays and 56Fe ions. On the other hand, approximately 85% of the fragments induced by 137Cs gamma rays had rejoined after 24 h of postirradiation incubation; the corresponding amount for 56Fe ions was 37%. Furthermore, the frequency of chromatid exchanges induced by gamma rays measured 24 h after irradiation was higher than that induced by 56Fe ions. No difference in the amount of chromatid damage induced by the two types of radiations was detected when assayed 1 h after irradiation. The results suggest that high-energy 56Fe ions induce a higher frequency of complex, unrepairable damage at both the cellular and chromosomal levels than 137Cs gamma rays in the target cells for radiation-induced lung cancers.     

Charged-particle mutagenesis. 1. Cytotoxic and mutagenic effects of high-LET charged iron particles on human skin fibroblasts.

Cytotoxic and mutagenic effects of high-LET charged iron (56Fe) particles were measured quantitatively using primary cultures of human skin fibroblasts. Argon and lanthanum particles and gamma rays were used in comparative studies. The span of LETs selected was from 150 keV/microns (330 MeV/u) to 920 keV/microns (600 MeV/u). Mutations were scored at the hypoxanthine guanine phosphoribosyl transferase (HPRT) locus using 6-thio-guanine (6-TG) for selection. Exposure to these high-LET charged particles resulted in exponential survival curves. Mutation induction, however, was fitted by the linear model. The relative biological effectiveness (RBE) for cell killing ranged from 3.7 to 1.3, while that for mutation induction ranged from 5.7 to 0.5. Both the RBE for cell killing and the RBE for mutagenesis decreased with increasing LET over the range of 1.50 to 920 keV/microns. The inactivation cross section (sigma i) and the action cross section for mutation induction (sigma m) ranged from 32.9 to 92.0 microns2 and 1.45 to 5.56 X 10(-3) microns2; the maximum values were obtained by 56Fe with an LET of 200 keV/microns. The mutagenicity (sigma m/sigma i) ranged from 2.05 to 7.99 X 10(-5) with an inverse relationship to LET.     

The effectiveness of monoenergetic neutrons at 565 keV in producing dicentric chromosomes in human lymphocytes at low doses

The induction of dicentric chromosomes in human lymphocytes from one individual irradiated in vitro with monoenergetic neutrons at 565 keV was examined to provide additional data for an improved evaluation of neutrons with respect to radiation risk in radioprotection. The resulting linear dose-response relationship obtained (0.813 +/- 0.052 dicentrics per cell per gray) over the dose range of 0.0213-0.167 Gy is consistent with published results obtained for irradiation with neutrons from different sources and with different spectra at energies lower than 1000 keV. Comparing this value to previously published "average" dose-response curves obtained by different laboratories for (60)Co gamma rays and orthovoltage X rays resulted in maximum RBEs (RBE(m)) of about 37 +/- 8 and 16 +/- 4, respectively. However, when our neutron data were matched to low-LET dose responses that were constructed several years earlier for lymphocytes from the same individual, higher values of RBE(m) resulted: 76.0 +/- 29.5 for (60)Co gamma rays and 54.2 +/- 18.4 for (137)Cs gamma rays; differentially filtered 220 kV X rays produced values of RBE(m) between 20.3 +/- 2.0 or 37.0 +/- 7. 1. The results highlight the dependence of RBE(m) on the choice of low-LET reference radiation and raise the possibility that differential individual response to low-LET radiations may need to be examined more fully in this context.     

Chromosomal instability and delayed apoptosis in long-term T-lymphocyte cultures irradiated with carbon ions and x rays

In this study, we examined genomic instability induced by 250 kV X rays and 100 MeV/nucleon carbon ions in long-term lymphocyte cultures from two healthy donors. Two biological end points, delayed apoptosis and chromosomal instability, were studied in descendants of cells irradiated with three different doses of the particular radiation up to 22 population doublings. The delayed apoptosis showed no clear dependence on radiation dose, culture time or radiation quality. A persistent significant increase in the rate of apoptosis up to 36 days after X irradiation was observed for a dose of 4 Gy in donor 1 only. For both donors and radiations, de novo aberration yields were significantly increased in comparison to control values up to day 36. For both radiations, chromosome-type aberrations were seen more frequently than chromatid-type aberrations in both donors up to 22 days postirradiation. In both donors, carbon ions were more effective than X rays with respect to the induction of chromosome instability. A dose of 0.25 Gy of carbon ions corresponding to 1.4 ion traversals per cell nucleus was effective in the induction of instability in our cell system.     

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.     

Evaluation of the relative biological effectiveness of a clinical epithermal neutron beam using dog brain

This investigation was designed to determine the relative biological effectiveness (RBE) of an epithermal neutron beam (FiR 1 beam) using the brains of dogs. The FiR 1 beam was developed for the treatment of patients with glioma using boron neutron capture therapy. Comparisons were made between the effects of whole-brain irradiation with epithermal neutrons and 6 MV photons. For irradiations with epithermal neutrons, three dose groups were used, 9.4 +/- 0.1, 10.2 +/- 0.1 and 11.5 +/- 0.2 Gy. These physical doses were given as a single exposure and are quoted at the 90% isodose. Four groups of five dogs were irradiated with single doses of 10, 12, 14 or 16 Gy of 6 MV photons to the 100% isodose. Different reference isodoses were used to obtain the most comparable dose distribution in the brain for the two different irradiation modalities. Sequential magnetic resonance images (MRI) were taken for 77-115 weeks after irradiation to detect changes in the brain. Dose-effect relationships were established for changes in the brain as detected either by MRI or by subsequent gross morphology and histology. The doses that caused a specified response in 50% of the animals (ED(50)) were calculated from these dose-effect curves for each end point, and these values were used to calculate the RBE values for the different end points. The RBE values for the FiR 1 beam, based on changes observed on MRI, were in the range 1.2-1.3. For microscopic and gross pathological lesions, the values were in the range 1.2-1.4. The corresponding RBE values for the MRI and pathological end points for the high-LET components (protons from nitrogen capture and recoil protons from fast neutrons) were in the ranges 3.5-4.0 and 3.4-4.4, respectively. This assumed a dose-rate reduction factor of 0.6 for the low-dose-rate gamma-ray component of this beam. Finally, a comparison was made between experimentally derived photon doses, for a specified end point, with calculated photon equivalent doses, which were obtained using the weighting factors for clinical studies on the epithermal neutron beam on the Brookhaven Medical Research Reactor (BNL) in New York. This indicated that the radiation-induced lesions seen in the present study were, on average, detected at a 12% lower photon dose than predicted by the use of the BNL clinical weighting factors. This indicates the need for caution in the extrapolation of results from one reactor-based epithermal neutron beam to another.     

Ex vivo determination of the effect of whole-body exposure to fast neutrons on murine spleen cell viability and apoptosis

The effects of high-linear energy transfer (LET) radiations on lymphoid tissues and lymphocytes are not well understood. As a first approach to delineate these effects, the present work was conducted to assess the effects of high-LET radiations on murine spleen cells ex vivo and in vitro. BALB/c mice were irradiated whole-body with 65 MeV neutrons or 15 MV X rays at doses ranging from 0.2 to 3 Gy. Spleens were removed 1 day postirradiation and weighed, and single cell suspensions were prepared and cultured for several days. Apoptosis occurring in vitro was determined at different times by flow cytometry analysis of cells labeled with propidium iodide. It was found that irradiation with fast neutrons reduced spleen weight and cellularity to a greater extent than photons. Considering the spleen cellularity as end point, the relative biological effectiveness (RBE) of fast neutrons was 2. However, for both modes of irradiation, apoptosis of recovered spleen cells in vitro increased as a function of dose and the duration of culture. The level of apoptosis occurring at various times postirradiation was found to be identical for high- and low-LET radiations. Taken together, these results suggest that external as well as cellular factors might differentially modulate the sensitivity of lymphocytes to fast neutrons and photons.     

The effect of 29 kV X rays on the dose response of chromosome aberrations in human lymphocytes

The induction of chromosome aberrations in human lymphocytes irradiated in vitro with X rays generated at a tube voltage of 29 kV was examined to assess the maximum low-dose RBE (RBE(M)) relative to higher-energy X rays or 60Co gamma rays. Since blood was taken from the same male donor whose blood had been used for previous irradiation experiments using widely varying photon energies, the greatest possible accuracy was available for such an estimation of the RBE(M), avoiding the interindividual variations in sensitivity or differences in methodology usually associated with interlaboratory comparisons. The magnitude of the linear coefficient alpha of the linear-quadratic dose-effect relationship obtained for the production of dicentric chromosomes by 29 kV X rays (alpha = 0.0655 +/- 0.0097 Gy(-1)) confirms earlier observations of a strong increase in alpha with decreasing photon energy. Relating this value to previously published values of alpha for the dose-effect curves for dicentrics obtained in our own laboratory, RBE(M) values of 1.6 +/- 0.3 in comparison with weakly filtered 220 kV X rays, 3.0 +/- 0.7 compared to heavily filtered 220 kV X rays, and 6.1 +/- 2.5 compared to 60Co gamma rays have been obtained. These data emphasize that the choice of the reference radiation is of fundamental importance for the RBE(M) obtained. A special survey of the RBE(M) values obtained by different investigators in the narrow quality range from about 30 to 350 kV X rays indicates that the present RBE is in fairly good agreement with previously published findings for the induction of chromosome aberrations or micronuclei in human lymphocytes but differs from recently published findings for neoplastic transformation in a human hybrid cell line.     

Induction and processing of oxidative clustered DNA lesions in 56Fe-ion-irradiated human monocytes

Space and cosmic radiation is characterized by energetic heavy ions of high linear energy transfer (LET). Although both low- and high-LET radiations can create oxidative clustered DNA lesions and double-strand breaks (DSBs), the local complexity of oxidative clustered DNA lesions tends to increase with increasing LET. We irradiated 28SC human monocytes with doses from 0-10 Gy of (56)Fe ions (1.046 GeV/ nucleon, LET = 148 keV/microm) and determined the induction and processing of prompt DSBs and oxidative clustered DNA lesions using pulsed-field gel electrophoresis (PFGE) and Number Average Length Analysis (NALA). The (56)Fe ions produced decreased yields of DSBs (10.9 DSB Gy(-1) Gbp(-1)) and clusters (1 DSB: approximately 0.8 Fpg clusters: approximately 0.7 Endo III clusters: approximately 0.5 Endo IV clusters) compared to previous results with (137)Cs gamma rays. The difference in the relative biological effectiveness (RBE) of the measured and predicted DSB yields may be due to the formation of spatially correlated DSBs (regionally multiply damaged sites) which result in small DNA fragments that are difficult to detect with the PFGE assay. The processing data suggest enhanced difficulty compared with gamma rays in the processing of DSBs but not clusters. At the same time, apoptosis is increased compared to that seen with gamma rays. The enhanced levels of apoptosis observed after exposure to (56)Fe ions may be due to the elimination of cells carrying high levels of persistent DNA clusters that are removed only by cell death and/or "splitting" during DNA replication.     

Induction of chromosome aberrations in G0 human lymphocytes by low doses of ionizing radiations of different quality

Human peripheral blood lymphocytes from two donors were exposed to low doses (0.05 to 2.0 Gy) of gamma rays, X rays, or fast neutrons of different energies. Chromosome aberrations were analyzed in metaphase of first-division cells after a culture time of 45-46 hr. At this time, less than 5% of the cells were found in second division. Different dose-response relationships were fitted to the data by using a maximum likelihood method; best fits for radiation-induced dicentric aberrations were obtained with the linear-quadratic law for all radiations. The linear component of this equation predominated, however, for neutrons in the range of doses studied, and the frequency of dicentrics induced by d(16)+Be neutrons up to 1.0 Gy could also be described by a linear relationship. The relative biological efficiency (RBE) of X rays and d(16)+Be, d(33)+Be, and d(50)+Be neutrons compared to 60Co gamma rays in the low dose range was calculated from the dose-effect relationships for the dicentrics produced. The RBE increased with decreasing neutron dose and with decreasing neutron energy from d(50)+Be to d(16)-+Be neutrons. The limiting RBE at low doses (RBEo) was calculated to be about 1.5 for X rays and 14.0, 6.2, and 4.7 for the d(16)+Be, d(33)+Be, and d(50)+Be neutrons, respectively.     

PLD repair in rat rhabdomyosarcoma tumor cells irradiated in vivo and in vitro with high-LET and low-LET radiation

Results are reported of studies to measure the extent of recovery of potentially lethal damage (PLD) in rat rhabdomyosarcoma tumor cells after irradiation both in vivo and in vitro with either high-LET or low-LET radiation. Stationary-phase cultures were found to exhibit repair of PLD following irradiation in vitro either with low-LET X rays or with high-LET neon ions in the extended-peak ionization region. Following a 9-Gy dose of 225-kVp X rays or a 3.5-Gy dose of peak neon ions, both of which reduced the initial cell survival to 6-8%, the maximum PLD recovery factors were 3.4 and 1.6, respectively. In contrast, the standard tumor excision assay procedure failed to reveal any recovery from PLD in tumors irradiated in situ with either X rays or peak neon ions. PLD repair by the in vivo tumor cells could be observed, however, when the excision assay procedure was altered by the addition of a known PLD repair inhibitor beta-arabinofuranosyladenine (beta-ara-A). When a noncytotoxic 50 microM concentration of beta-ara-A was added to the excised tumor cells immediately following a 14.5-Gy in situ dose of X rays, cell survival in the inhibitor-treated cells was lower than in the untreated cells (0.018 compared to 0.056), resulting in a PLD repair inhibition factor of 3.1. Delaying the addition of beta-ara-A for 1, 2, or 3 h following tumor excision reduced the PLD repair inhibition factor to 1.6, 1.5, and 0.9, respectively. Following tumor irradiation in situ with neon ions in the extended-peak ionization region (median LET = 145 keV/micron), less PLD repair was observed than after X irradiation. For 5.8 Gy of peak neon ions, the PLD repair inhibition factors were 2.1, 1.5, 1.3, and 1.1 at 0, 1, 2, and 3 h, respectively. We interpret the absence of measurable PLD repair using the standard tumor excision assay procedure as resulting from undetectable repair occurring during the long interval (about 2 h) required for the cell dissociation and plating procedures. We conclude that at least for our tumor system, PLD repair does occur after irradiation of tumors in situ, even though it is not detectable using the standard tumor excision assay procedure. Thus a failure to measure such repair by this assay in a given tumor system does not necessarily mean the cells are incapable of PLD repair.     

Accelerated heavy particles and the lens. III. Cataract enhancement by dose fractionation

For a number of biological end points it has been shown that, in contrast to low linear energy transfer (LET) radiation, dose fractionation of high-LET radiation does not result in a reduction in overall effectiveness. Studies were conducted to determine the effect of fractionating the exposures to heavy ion doses on the development of cataracts. Rat eyes were exposed to single doses of 1, 5, and 25 cGy of 570 MeV/amu40Ar ions and to 2, 4, and 10 Gy of 250 kVp X rays. These were compared to unirradiated controls and eyes which were exposed to the same total dose delivered in four fractions over 12 h. While in all cases fractionation of the exposure to X rays produced significant reduction in cataractogenic potential, fractionating doses of 40Ar ions caused a dose- and stage-dependent enhancement in the development of cataracts.     

Dose-response curves for late functional changes in the normal rat brain after single carbon-on doses evaluated by magnetic resonance imaging: influence of follow-up time and calculation of relative biological effectiveness

This study investigated late effects in the brain after irradiation with carbon ions using a rat model. Thirty-six animals were irradiated stereotactically at the right frontal lobe using an extended Bragg peak with maximum doses between 15.2 and 29.2 Gy. Dose-response curves for late changes in the normal brain were measured using T1- and T2-weighted magnetic resonance imaging (MRI). Tolerance doses were calculated at several effect probability levels and times after irradiation. The MRI changes were progressive in time up to 17 months and remained stationary after that time. At 20 months the tolerance doses at the 50% effect probability level were 20.3 +/- 2.0 Gy and 22.6 +/- 2.0 Gy for changes in T1- and T2-weighted MRI, respectively. The relative biological effectiveness (RBE) was calculated on the basis of a previous animal study with photons. Using tolerance doses at the 50% effect probability level, RBE values of 1.95 +/- 0.20 and 1.88 +/- 0.18 were obtained for T1- and T2-weighted MRI. A comparison with data in the literature for the spinal cord yielded good agreement, indicating that the RBE values for single-dose irradiations of the brain and the spinal cord are the same within the experimental uncertainty.     

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.     

Exposure to heavy ion radiation induces persistent oxidative stress in mouse intestine

Ionizing radiation-induced oxidative stress is attributed to generation of reactive oxygen species (ROS) due to radiolysis of water molecules and is short lived. Persistent oxidative stress has also been observed after radiation exposure and is implicated in the late effects of radiation. The goal of this study was to determine if long-term oxidative stress in freshly isolated mouse intestinal epithelial cells (IEC) is dependent on radiation quality at a dose relevant to fractionated radiotherapy. Mice (C57BL/6J; 6 to 8 weeks; female) were irradiated with 2 Gy of γ-rays, a low-linear energy transfer (LET) radiation, and intestinal tissues and IEC were collected 1 year after radiation exposure. Intracellular ROS, mitochondrial function, and antioxidant activity in IEC were studied by flow cytometry and biochemical assays. Oxidative DNA damage, cell death, and mitogenic activity in IEC were assessed by immunohistochemistry. Effects of γ radiation were compared to (56)Fe radiation (iso-toxic dose: 1.6 Gy; energy: 1000 MeV/nucleon; LET: 148 keV/μm), we used as representative of high-LET radiation, since it's one of the important sources of high Z and high energy (HZE) radiation in cosmic rays. Radiation quality affected the level of persistent oxidative stress with higher elevation of intracellular ROS and mitochondrial superoxide in high-LET (56)Fe radiation compared to unirradiated controls and γ radiation. NADPH oxidase activity, mitochondrial membrane damage, and loss of mitochondrial membrane potential were greater in (56)Fe-irradiated mice. Compared to γ radiation oxidative DNA damage was higher, cell death ratio was unchanged, and mitotic activity was increased after (56)Fe radiation. Taken together our results indicate that long-term functional dysregulation of mitochondria and increased NADPH oxidase activity are major contributing factors towards heavy ion radiation-induced persistent oxidative stress in IEC with potential for neoplastic transformation.     

The combined effects of dietary supplements and low-dose-rate high-LET radiation on mice in vivo

The purpose of this study was to investigate the combined actions of food supplements and lowdose-rate high-LET radiation on radiosensitivity, induction of the adaptive response, and tumor growth in SHK mice in vivo. The animals were irradiated with 0.11 Gy (0.005 Gy/day) of low-dose-rate high-LET radiation behind the concrete shield of a 70 GeV proton accelerator (Protvino, Moscow oblast). Four groups of the mice were fed with selected products (soy meat, buckwheat, lettuce leaves, and a drug based on cod-liver oil) during the entire irradiation period (22 days). The results of the study indicate that the mice with diets containing soy meat, buckwheat, and lettuce leaves in contrast to those fed with a diet containing cod-liver oil had reduced sensitivity to X-radiation at a dose rate of 1.5 Gy and a significant slowdown in the growth of the Ehrlich carcinoma. The combined effect of high-LET radiation and the food supplements mentioned above (except for the cod-liver oil) reduced the sensitivity of the mice to the irradiation at a dose rate of 1.5 Gy, induced the adaptive response, and caused a decrease in the growth rate of the Ehrlich carcinoma in contrast to the mice that were only irradiated with high-LET radiation.     

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.     

The role of radiation quality in the stimulation of intercellular induction of apoptosis in transformed cells at very low doses

An important stage in tumorigenesis is the ability of precancerous cells to escape natural anticancer signals. Apoptosis can be selectively induced in transformed cells by neighboring normal cells through cytokine and ROS/RNS signaling. The intercellular induction of apoptosis in transformed cells has previously been found to be enhanced after exposure of the normal cells to very low doses of both low- and high-LET ionizing radiation. Low-LET ultrasoft X rays with a range of irradiation masks were used to vary both the dose to the cells and the percentage of normal cells irradiated. The results obtained were compared with those after α-particle irradiation. The intercellular induction of apoptosis in nonirradiated src-transformed 208Fsrc3 cells observed after exposure of normal 208F cells to ultrasoft X rays was similar to that observed for γ rays. Intercellular induction of apoptosis was stimulated by irradiation of greater than 1% of the nontransformed 208F cells and increased with the fraction of cells irradiated. A maximal response was observed when ～10-12% of the cells were irradiated, which gave a similar response to 100% irradiated cells. Between 1% and 10%, high-LET α particles were more effective than low-LET ultrasoft X rays in stimulating intercellular induction of apoptosis for a given fraction of cells irradiated. Scavenger experiments show that the increase in intercellular induction of apoptosis results from NO(?) and peroxidase signaling mediated by TGF-β. In the absence of radiation, intercellular induction of apoptosis was also stimulated by TGF-β treatment of the nontransformed 208F cells prior to coculture; however, no additional increase in intercellular induction of apoptosis was observed if these cells were also irradiated. These data suggest that the TGF-β-mediated ROS/RNS production reaches a maximum at low doses or fluences of particles, leading to a plateau in radiation-stimulated intercellular induction of apoptosis at higher doses.