Relative biological effectiveness of tritium oxide based on nucleic acid metabolic indices

Relative biological effectiveness (RBE) of tritium oxide, as compared to gamma-rays (137Cs), with regard to LD50/30 is 2,32 +/- 0,69 for rats. The RBE coefficients for tritium oxide are obtained with regard to some indices of nucleic acid metabolism in the thymus and spleen during the dose formation (0-14 days). The RBE of tritium oxide increases with a decrease in radiation dose as determined according to the concentration and content of DNA per organ and activity of thymus DNAases.     

Relative biological effectiveness and dose rate effect of tritiated water on chromosomes in human lymphocytes and bone marrow cells

Tritriated water (HTO) is a major toxic effluent from the nuclear power industry, that is released into the environment in large quantities. The low dose radiation effect and dose rate effect of HTO on human lymphocytes and bone marrow cells have not been well studied. The present study was therefore undertaken to investigate the HTO dose-response relationship for chromosomal aberrations in human lymphocytes and bone marrow cells at low in vitro radiation doses ranging from 0.1 to 1 Gy. Lymphocytes (G₀ stage) and bone marrow cells were incubated for 10–150 min with HTO at a dose rate of 2cGy/min (555 MBq/ml). The relative biological effectiveness (RBE) of HTO was calculated with respect to ₆₀Co γ-rays for the induction of dicentric and centric ring chromosomes at low radiation doses. The RBE value for HTO β-rays relative to ⁶⁰Co γ-rays was 2.7 for lymphocytes and 3.1 for chromatid aberrations in bone marrow cells. Lymphocytes were also chronically exposed to HTO for 6.7–80 h at dose rates of 0.5 cGy/min (138.5 MBq/ml) and 0.02 cGy/min (5.6 MBq/ml). There was a 71.5% decrease in the yield of dicentrics and centric rings at the dose rate of 0.02 cGy/min, indicating a clear dose rate effect of HTO. The RBE value for HTO relative to ¹³⁷Cs γ-rays was 2.0 at a dose rate of 0.02 cGy/min, suggesting that low HTO dose rates produce no increase of the RBE values and that the values may be constant between 2 and 3 within these dose rates. These results should prove useful in assessment of the health risk for humans exposed to low levels of HTO.     

Chromosome damage induced by decay of 3H and 125I incorporated into DNA of Chinese hamster cells

The present study was undertaken to compare the frequency of chromatid-type aberrations in Chinese hamster cells with previous results on accumulation of unrepaired DNA-strand breaks after incorporation of 3H-TdR or 125IUdR into DNA. A linear-quadratic function was fitted by the weighted-least-square method to the data on yield of chromatid aberrations at different dpm values. Based on a significant linear response at low doses, RBE for 125I in relation to 3H was calculated for (i) chromatid breaks (17 +/- 6), (ii) the sum of isochromatid breaks and chromatid exchanges (21 +/- 9), and (iii) the total number of chromatid aberrations (18 +/- 5). Analogously, the RBE for accumulation of DNA-strand breaks was determined (13 +/- 6). Our results are consistent with the assumption that chromosomal aberrations mainly originate from unrepaired DNA-strand breaks.     

Comparison of the biological effects of tritium oxide and gamma radiation based on changes in the mass of the rat thymus gland

RBE of tritium oxide (cumulative doses from 0.33 to 14.7 Gy), in comparison with gamma-radiation, amounted to 2-3 as estimated by the thymus mass. As determined by the rate of injury and repair, the RBE values decreased from 4 to 1.4 with dose increasing, and from 6.5 to 1.3, by the periods of half-decrease and half-recovery of the organ mass. The 2-3-fold variations in the RBE values for various parameters of the organ mass changes were registered at low doses, whereas within the range of median and high doses under study, the differences were insignificant.     

Relative biological effectiveness of high-energy iron ions for micronucleus formation at low doses

Dose-response curves for micronucleus (MN) formation were measured in Chinese hamster V79 and xrs6 (Ku80(-)) cells and in human mammary epithelial MCF10A cells in the dose range of 0.05-1 Gy. The Chinese hamster cells were exposed to 1 GeV/nucleon iron ions, 600 MeV/nucleon iron ions, and 300 MeV/nucleon iron ions (LETs of 151, 176 and 235 keV/microm, respectively) as well as with 320 kVp X rays as reference. Second-order polynomials were fitted to the induction curves, and the initial slopes (the alpha values) were used to calculate RBE. For the repair-proficient V79 cells, the RBE at these low doses increased with LET. The values obtained were 3.1 +/- 0.8 (LET = 151 keV/microm), 4.3 +/- 0.5 (LET = 176 keV/microm), and 5.7 +/- 0.6 (LET = 235 keV/microm), while the RBE was close to 1 for the repair-deficient xrs6 cells regardless of LET. For the MCF10A cells, the RBE was determined for 1 GeV/nucleon iron ions and was found to be 5.5 +/- 0.9, slightly higher than for V79 cells. To test the effect of shielding, the 1 GeV/nucleon iron-ion beam was intercepted by various thicknesses of high-density polyethylene plastic absorbers, which resulted in energy loss and fragmentation. It was found that the MN yield for V79 cells placed behind the absorbers decreased in proportion to the decrease in dose both before and after the iron-ion Bragg peak, indicating that RBE did not change significantly due to shielding except in the Bragg peak region. At the Bragg peak itself with an entrance dose of 0.5 Gy, where the LET is very high from stopping low-energy iron ions, the effectiveness for MN formation per unit dose was decreased compared to non-Bragg peak areas.     

Study of dose-rate effects of neutron radiation in a wild-type and a repair-deficient yeasts saccharomyces

We report here a comparative analysis of RBE for lethality of a single pulse (duration 65 micros) of fast neutron with ultra high dose rates (up to 6 x 10(6) Gy/s) and continuous neutron radiation (3.6 x 10(3) s) of the pulse reactor BARS-6. Three diploid strains, one haploid strain and three diploid repair-deficient strains (rad52-1/rad52-1; rad54/rad54; rad2/rad2) were used. The RBE values (D(0gamma)/1D(0n)) of a single pulse and continuous neutron irradiation were equal (1.7-1.8) with maximum RBE (4.1-3.1) in region of low doses (shoulder region). Haploid cells were found to be more (3 times) sensitive to both gamma-rays and neutrons than the wild type. There was no obvious decrease in the RBE of 1.9 in highly sensitive haploid cells as compared with highly resistant diploid cells. The repair-deficient strains (rad52-1/rad52-1; rad54/rad54) were more (up to 10 fold) sensitive to both neutrons and gamma-rays as compared with their parent line. The RBE values of 1.5-1.7 of neutrons for these mutants (independent by of the mode of irradiation) were found. The repair-deficient mutant rad2/rad2 had similar sensitivity as a wild type and a RBE value was 2.0. We have concluded that biological effectiveness of the neutrons of pulse reactor BARS-6 was independent of the dose-rate, differing up to 10(8) fold. The RBE didn't vary significantly with the capacity of cells to repair DNA damages.     

Heat shock at the germinal vesicle breakdown stage induces apoptosis in surrounding cumulus cells and reduces maturation rates of porcine oocytes in vitro

The objectives were to determine the effects of cumulus cells (CC) on porcine oocyte maturation in vitro (IVM) after heat shock (HS). Treated oocytes were cultured at 39 degrees C for 20h, followed by HS treatment (42 degrees C for 1h), and then matured in vitro for 23h. The CC were removed before maturation (H1), after HS (H2), or after maturation (H3). Control oocytes were continuously cultured under the same conditions and CC were similarly removed before maturation (C1), after 21h of IVM (C2), and after maturation (C3). Maturation rates were affected by HS (P<0.01) and by an interaction between HS and CC (P<0.01). A significant decrease in maturation rate only occurred when CC were not removed from cumulus oocyte complexes during IVM after HS (H3, 39.2+/-5.7% versus C3, 78.2+/-8.2%, P<0.01). Mature oocytes in all treatment groups were electrically activated and cultured for 8 d in NCSU23. Blastocyst rates in group H1 (7.2+/-3.5%) and C1 (6.3+/-3.1%) were lower than in other groups (H2, 21.4+/-4.4%, C2, 20.5+/-7.0%, H3, 23.1+/-2.0%, C3, 24.3+/-3.1%, P<0.05). Damaged DNA was detected in CC by a comet assay at 0h after HS (60.8+/-12.5% compared with 9.2+/-2.2% in control, P<0.05); in HS groups, both DNA damage (comet assay, 74.9+/-6.3% compared with 10.0+/-2.1% in control) and apoptosis (TUNEL assay, 21.6+/-1.6% compared with 5.6+/-0.6% in control) in CC were increased (P<0.05) at 44h of maturation. In conclusion, heat shock (42 degrees C for 1h) during IVM induced DNA damage and apoptosis of porcine CC; furthermore, apoptotic CC may contribute to maturation failure of oocytes in vitro.     

Dose-response relationship for the induction of structural chromosome aberrations in human spermatozoa after in vitro exposure to tritium beta-rays

The effects of tritium (HTO) beta-rays on human sperm chromosomes were studied using our interspecific in vitro fertilization system between human spermatozoa and zona-free hamster oocytes. Semen samples were treated with media containing 1.53-24.3 mCi/ml HTO for about 80 min. 1290 spermatozoa from the controls and 1842 spermatozoa from the irradiated groups were karyotyped. The incidence of spermatozoa with structural chromosome aberrations increased linearly with increasing dosage. Breakage-type aberrations occurred far more frequently than exchange-type. Chromosome-type aberrations appeared far more frequently than chromatid-type. All of these types of aberrations showed linear dose-dependent increases. The RBE values of HTO beta-rays relative to X-rays were calculated for the above-mentioned 5 indices, respectively. Their RBE values ranged from 1.89 to 3.00 when the absorbed dose was estimated to be the minimum, whereas the values ranged between 1.04 and 1.65 when the absorbed dose was estimated to be the maximum.     

Mechanism of the radiation effect at the level of the supramolecular structures of eukaryotic DNA

The methods of viscosimetry and light scattering were used to study the radiosensitivity of the supramolecular DNA (SM DNA) structure in vivo. Irreversible lesions were found in SM DNA 2 min after gamma-irradiation of rats with a dose of 10 Gy. They were associated with the damage to the RNA-lipoprotein component (a linker) and with the dissociation of SM DNA to fragments of different molecular weight, that is, 109 +/- 25 X 10(6), 51 +/- 15 X 10(6), and 47 +/- 21 X 10(6) D for liver, spleen, and thymus, respectively, which correlated with the radiosensitivity of these organs.     

MAGE-3 DNA疫苗的构建及其免疫效果的观察

通过RT PCR方法扩增MAGE 3cDNA ,以pcDNA3 1+为载体 ,构建重组表达质粒pcDNA3 1 MAGE 3。重组质粒用脂质体转染鼠B16细胞 ,经RT PCR、细胞免疫染色及免疫印迹法鉴定转化细胞中MAGE 3的表达。以 10 0 μg质粒剂量肌肉注射接种小鼠 ,间隔 10天 ,共 3次 ,以空载体和PBS为对照。结果 ,重组质粒免疫的小鼠 ,其脾淋巴细胞对MAGE 3阳性靶细胞的杀伤活性为 51 0 8± 7 41% ,与空载体组 (8 44± 1 89% )及PBS组 (5 76± 1 75% )相比 ,差异有显著性 (P <0 0 1) ,而对MAGE 3阴性靶细胞的杀伤活性分别为 8 2 1± 1 65% ,7 68± 1 56%和 5 13±1 42 % ,其差异无显著性 ;MAGE 3DNA疫苗组免疫血清 1∶15稀释时能检测到抗MAGE 3抗体 ,脾细胞培养上清中Th1类细胞因子IFN γ、IL 2水平明显升高 ,外周血中CD4+、CD8+T细胞也提高 ,小鼠肿瘤的生长速度明显减慢 ,与对照组相比 ,差异显著 (P <0 0 1)。说明MAGE 3重组质粒免疫小鼠可以诱导小鼠产生特异性的体液和细胞免疫应答     

Eccentric strain at long muscle length evokes the repeated bout effect

The repeated bout effect (RBE) is a phenomenon characterized by less delayed onset muscle soreness (DOMS) and torque deficit after the second of 2 separate eccentric exercise bouts. Previous investigators have reported that shifting of optimum angle after an initial bout of eccentric exercise mediates the RBE. We hypothesized that an RBE for elbow extensor exercise occurs after an initial bout performed at long (starting position of 50 degrees to an end position of 130 degrees) but not short (starting position of 0 degrees to an end position of 80 degrees) muscle length because strain at long length evokes a shifting of the optimum angle to a longer length. Untrained women performed an initial bout at either long or short length (n = 9 per group) followed 1 week later by a repeated bout (RB) through the full ROM (0-130 degrees). Extensor torque and optimum angle was evaluated before, immediately after, and 2 days after each bout. A mechanical transducer depressed on the triceps brachii quantified DOMS. Torque deficits were 3% and 7% after exercise at short vs. long length, respectively. Two days after the RB, torque deficit was 8% and 1% for those previously exercising at short vs. long length (group x bout, p < 0.05). Greater DOMS (N) was observed after exercise at long (16 +/- 3) vs. short (23 +/- 2) length; whereas greater DOMS occurred for the short-length (17 +/- 2) vs. long (26 +/- 3) group after the RB (group x bout, p < 0.05). Optimum angle shifted to a longer length after exercise at long (+10 +/- 4 degrees) vs. short (+1 +/- 3 degrees) length (group x bout, p < 0.05). After the RB, those exercising previously at short length experienced a shift of +15 +/- 4 degrees (main effect, p < 0.05). The findings of this study indicate that the repetitive strain at long but not short muscle length evokes both immediate and sustained shifts in optimum angle to longer lengths, and that this shifting mediates (r(2) = 0.71) the RBE.     

Influence of ultrafractionation on the effect of whole body uniform irradiation with protons of 1000 MeV energy

In experiments with rats a study was made of the radiobiological influence of a pulse frequency (45.9 and 4.5 c-1) of a 1000 MeV proton beam. The estimates of metabolic parameters of the peripheral blood and spleen 24 h and the survival rate during 60 days following irradiation have demonstrated the increase in the biological effectiveness of the proton beam with decreasing pulse frequency. As to 60Co-gamma-radiation, RBE of protons was 1.10 +/- 0.04 at the pulse frequency of 9 c-1 and 0.98 +/- 0.03 at 45 c-1 as determined by the probit-logarithm dose method.     

Responses of synchronous L5178Y S/S cells to heavy ions and their significance for radiobiological theory

Synchronous suspensions of the radiosensitive S/S variant of the L5178Y murine leukaemic lymphoblast at different positions in the cell cycle were exposed aerobically to segments of heavy-ion beams (20Ne, 28Si, 40Ar, 56Fe and 93Nb) in the Bragg plateau regions of energy deposition. The incident energies of the ion beams were in the range of 460 +/- 95 MeV u-1, and the calculated values of linear energy transfer (LET infinity) for the primary nuclei in the irradiated samples were 33 +/- 3, 60 +/- 3, 95 +/- 5, 213 +/- 21 and 478 +/- 36 keV microns-1, respectively; 280 kVp X-rays were used as the baseline radiation. Generally, the maxima or inflections in relations between relative biological effectiveness (RBE) and LET infinity were dependent upon the cycle position at which the cells were irradiated. Certain of those relations were influenced by post-irradiation hypothermia. Irradiation in the cell cycle at mid-G1 to mid-G1 + 3 h, henceforth called G1 to G1 + 3 h, resulted in survival curves that were close approximations to simple exponential functions. As the LET infinity was increased, the RBE did not exceed 1.0, and by 478 keV microns-1 it had fallen to 0.39. Although similar behaviour has been reported for inactivation of proteins and certain viruses by ionizing radiations, so far the response of the S/S variant is unique for mammalian cells. The slope of the survival curve for X-photons (D0: 0.27 Gy) is reduced in G1 to G1 + 3 h by post-irradiation incubation at hypothermic temperatures and reaches a minimum (Do: 0.51 Gy) at 25 degrees C. As the LET infinity was increased, however, the extent of hypothermic recovery was reduced progressively and essentially was eliminated at 478 keV microns-1. At the cycle position where the peak of radioresistance to X-photons occurs for S/S cells, G1 + 8 h, increases in LET infinity elicited only small increases in RBE (at 10% survival), until a maximum was reached around 200 keV microns-1. At 478 keV microns-1, what little remained of the variation in response through the cell cycle could be attributed to secondary radiations (delta rays) and smaller nuclei produced by fragmentation of the primary ions.     

Chromosome aberrations induced by tritiated water or 60Co gamma-rays at early pronuclear stage in mouse eggs

The induction of chromosome aberrations in mouse eggs by exposure to HTO beta-particles and 60Co gamma-rays at the early pronuclear stage was examined at the first-cleavage metaphase by using an in vitro fertilization technique. Eggs at the pronuclear stage were exposed to beta-particles in a chemically defined medium containing tritiated water (HTO) for 2 h at 3-5 h after insemination. Other eggs at the same stage were exposed to gamma-rays from 60Co during the same period. The dose-response relationships for frequencies of chromosome aberrations per egg were fitted to a linear-quadratic model for HTO beta-particles, and to a linear model for 60Co gamma-rays. The chromosome aberrations were mainly chromosome-type, and the majority of all aberrations were fragments. RBE values of HTO beta-particles relative to 60Co gamma-rays and acute X-rays, which were estimated from the ratio of the linear regression coefficients over 0.05-Gy range, were 2.0 and 1.6, respectively.     

Prolonged lymphopenia, lymphoid depletion, and hypoprolactinemia in children with nosocomial sepsis and multiple organ failure

Lymphopenia and lymphoid depletion occur in adults dying of sepsis. Prolactin increases Bcl-2 expression, suppresses stress-induced lymphocyte apoptosis, and improves survival from experimental sepsis. We hypothesized that prolonged lymphopenia, lymphoid depletion, and hypoprolactinemia occur in children dying with sepsis and multiple organ failure (MOF). Fifty-eight critically ill children with and 55 without MOF admitted to a university hospital pediatric intensive care unit were enrolled in a prospective, longitudinal, observational clinical study. Prolactin levels and absolute lymphocyte count were measured on days 1, 3, 7, 14, and 21. Lymph node, thymus, and spleen autopsy specimens were examined for lymphoid depletion, with immunohistochemical staining for CD4, CD20, and CD21 and for lymphoid apoptosis. Prolonged lymphopenia (absolute lymphocyte count < 1000 for >7 days) occurred only in children with MOF (29 vs 0%, p < 0.05) and was associated independently with nosocomial infection (odds ratio (OR), 5.5, 95% confidence interval (CI), 1.7-17, p < 0.05), death (OR, 6.8, 95% CI, 1.3-34, p < 0.05), and splenic and lymph node hypocellularity (OR, 42, 95% CI, 3.7-473, p < 0.05). Lymphocyte apoptosis and ante/postmortem infection were observed only in children with lymphoid depletion. Prolonged hypoprolactinemia (>7 days) was more common in children with MOF (17 vs 2%, p < 0.05) and was associated independently with prolonged lymphopenia (OR, 8.3, 95% CI, 2.1-33, p < 0.05) and lymphoid depletion (OR, 12.2, 95% CI, 2.2-65, p < 0.05). Prolonged lymphopenia and apoptosis-associated depletion of lymphoid organs play a role in nosocomial sepsis-related death in critically ill children. Prolonged hypoprolactinemia is a previously unrecognized risk factor for this syndrome.     

Thermodynamics and kinetics of the cleavage of DNA catalyzed by bleomycin A5.

Microcalorimetry and UV-vis spectroscopy were used to conduct thermodynamic and kinetic investigations of the scission of calf thymus DNA catalyzed by bleomycin A5 (BLM-A5) in the presence of ferrous ion and oxygen. The molar reaction enthalpy for the cleavage, the Michaelis-Menten constant for calf thymus DNA and the turnover number of BLM-A5 were calculated by a novel thermokinetic method for an enzyme-catalyzed reaction to be -577 +/- 19 kJ.mol-1, 20.4 +/- 3.8 microm and 2.28 +/- 0.49 x 10-2 s-1, respectively, at 37.0 degrees C. This DNA cleavage was a largely exothermic reaction. The catalytic efficiency of BLM-A5 is of the same order of magnitude as that of lysozyme but several orders of magnitude lower than those of TaqI restriction endonuclease, NaeI endonuclease and BamHI endonuclease. By comparing the molar enthalpy change for the cleavage of calf thymus DNA induced by BLM-A5 with those for the scission of calf thymus DNA mediated by adriamycin and by (1,10-phenanthroline)-copper, it was found that BLM-A5 possessed the highest DNA cleavage efficiency among these DNA-damaging agents. These results suggest that BLM-A5 is not as efficient as a DNA-cleaving enzyme although the cleavage of DNA by BLM-A5 follows Michaelis-Menten kinetics. Binding of BLM-A5 to calf thymus DNA is driven by a favorable entropy increase with a less favorable enthalpy decrease, in line with a partial intercalation mode involved in BLM-catalyzed breakage of DNA.     

Thermodynamic investigation of M-DNA: a novel metal ion-DNA complex

The thermodynamics of formation of a novel divalent metal ion-DNA complex known as M-DNA have been investigated using an ethidium bromide (EB) fluorescence assay, and with isothermal titration calorimetry. The process of M-DNA formation was observed from the EB assay to be strongly temperature-dependent. The binding of Zn(2+) to calf thymus (42% GC content) and Escherichia coli (50% GC content) DNA at pH 8.5 exhibited an endothermic cooperative binding process at Zn(2+) concentrations of approximately 0.1 mM, indicating an entropy driven process. This binding process is consistent with a site-specific binding interaction, similar in nature to Z-DNA formation; however, the interaction occurs at much lower metal ion concentrations. The enthalpy of M-DNA formation for calf thymus DNA was determined to be 10.5+/-0.7 and 9+/-2 kJ/mbp at DNA concentrations of 100 and 50 microg ml(-1), respectively. An enthalpy of 13+/-3 kJ/mbp was obtained for M-DNA formation for 50 microg ml(-1) E. coli DNA. No evidence of M-DNA formation was observed in either DNA at pH 7.5 with Zn(2+) or at either pH 7.5 or 8.5 with Mg(2+).     

Dependence of the yield of DNA double-strand breaks in Chinese hamster V79-4 cells on the photon energy of ultrasoft X rays

Induction of DNA DSBs by low-LET radiations reflects clustered damage produced predominantly by low-energy, secondary electron "track ends". Cell inactivation and induction of DSBs and their rejoining, assayed using pulsed-field gel electrophoresis, were determined in Chinese hamster V79-4 cells irradiated as a monolayer with characteristic carbon K-shell (CK) (0.28 keV), aluminum K-shell (AlK) (1.49 keV), and titanium K-shell (TiK) (4.55 keV) ultrasoft X rays under aerobic and anaerobic conditions. Relative to (60)Co gamma rays, the relative biological effectiveness (RBE) for cell inactivation at 10% survival and for induction of DSBs increases as the photon energy of the ultrasoft X rays decreases. The RBE values for cell inactivation and for induction of DSBs by CK ultrasoft X rays are 2.8 +/- 0.3 and 2.7 +/- 0.3, respectively, and by TiK ultrasoft X rays are 1.5 +/- 0.1 and 1.4 +/- 0.1, respectively. Oxygen enhancement ratios (OERs) of approximately 2 for cell inactivation and induction of DSBs by ultrasoft X rays are independent of the photon energy. The time scale for rejoining of DNA DSBs is similar for both ultrasoft X rays and 60Co gamma rays. From the size distribution of small DNA fragments down to 0.48 kbp, we concluded that DSBs are induced randomly by CK and AlK ultrasoft X rays. Therefore, ultrasoft X rays are more efficient per unit dose than gamma radiation at inducing DNA DSBs, the yield of which increases with decreasing photon energy.     

Relative biological effectiveness of 144 keV neutrons in producing dicentric chromosomes in human lymphocytes compared with 60Co gamma rays under head-to-head conditions

The RBE for neutrons was assessed in a head-to-head experiment in which cultures of lymphocytes from the same male donor were irradiated simultaneously with 144 keV neutrons and with 60Co gamma rays as the reference radiation and evaluated using matched time, culture conditions, and the end point of chromosomal aberrations to avoid potential confounding factors that would influence the outcome of the experiment. In addition, the irradiation time was held constant at 2 h for the high-dose groups for both radiation types, which resulted in rather low dose rates. For the induction of dicentric chromosomes, the exposure to the 144 keV neutrons was found to be almost equally as effective (yield coefficient alpha(dic) = 0.786 +/- 0.066 dicentrics per cell per gray) as that found previously for irradiation with monoenergetic neutrons at 565 keV (alpha(dic) = 0.813 +/- 0.052 dicentrics per cell per gray) under comparable exposure and culture conditions (Radiat. Res. 154, 307-312, 2000). However, the values of the maximum low-dose RBE (RBE(m)) relative to 60Co gamma rays that were determined in the present and previous studies show an insignificant but conspicuous difference: 57.0 +/- 18.8 and 76.0 +/- 29.5, respectively. This difference is mainly due to the difference in the alpha(dic) value of the 60Co gamma rays, the reference radiation, which was 0.0138 +/- 0.0044 Gy(-1) in the present study and 0.0107 +/- 0.0041 Gy(-1) in the previous study. In the present experiment, irradiations with 144 keV neutrons and 60Co gamma rays were both performed at 21 degrees C, while in the earlier experiment irradiations with 565 keV neutrons were performed at 21 degrees C and the corresponding reference irradiation with gamma rays was performed at 37 degrees C. However, the temperature difference between 21 degrees C and 37 degrees C has a minor influence on the yield of chromosomal alterations and hence RBE values. The large cubic PMMA phantom that was used for the gamma irradiations in the present study results in a larger dose contribution from Compton-scattered photons compared to the mini-phantom used in the earlier experiments. The contribution of these scattered photons may explain the large value of alpha(dic) for gamma irradiation in the present study. These results indicate that the yield coefficient alpha(dic) for 144 keV neutrons is similar to the one for 565 keV neutrons, and that modification of the alpha(dic) value of the low-LET reference radiation, due to changes in the experimental conditions, can influence the RBE(m). Consequently, alpha(dic) values cannot be shared between cytogenetic laboratories for the purpose of assessment of RBM(m) without verification of the comparability of the experimental conditions.     

Relative biological effectiveness of fission neutrons for induction of micronucleus formation in mouse reticulocytes in vivo

Following whole-body irradiation of ICR mice with various doses of fission neutrons or X-rays, the frequency of micronuclei (MNs) in peripheral blood reticulocytes was measured at 12 h intervals beginning immediately after irradiation and ending at 72 h after irradiation. The resulting time-course curve of MN frequency had a clear peak 36 h after irradiation, irrespective of the type of radiation applied and the dose used. The MN frequency, averaged as the unweighted mean over the experimental time course, showed a linear increase with increasing dose of either fission neutrons or X-rays. The linear response to X-rays supports reported conclusion that induction of MN formation in reticulocytes is a dose-rate independent phenomenon. The relative biological effectiveness (RBE) of fission neutrons to X-rays for MN induction was estimated to be 1.9 +/- 0.3. This value is considerably lower than the RBE value of 4.6 +/- 0.5 reported for the same fission neutrons for induction of lymphocyte apoptosis in the thymus of ICR mice that represents dose-rate independent, one-track event. Based on these results, we propose that MNs increased in reticulocytes after irradiation mostly represent acentric fragments caused by single chromosome breaks, and that some confounding factor is operating in erythroblasts for the formation of aberrations from non-rejoining DNA double-strand breaks more severely after high-LET radiation than after low-LET radiation.