Modifying effect of deep hypoxia on neutron-irradiated mice

Deep hypoxia was shown to influence the survival of animals, the state of the small intestine mucosa and the haemopoietic system. DMF (LD50/30) was 2.49 and 1.66 with X- and neutron radiation, respectively. As to haemopoietic stem cells X-irradiated in vivo, D0 was 0.96 +/- 0.04 Gy (control) and 2.82 +/- 0.14 Gy (anoxia). With neutron irradiation, D0 was 0.44 +/- 0.01 Gy and 0.8 +/- 0.03 for the control and experimental animals respectively.     

Survival of erythroid burst-forming units and erythroid colony-forming units in canine bone marrow cells exposed in vitro to 1 MeV neutron radiation or X rays

Conditioned media (CM) from allogeneic stimulated cultures of light density cells (less than 1.08 g/cm3) from the peripheral blood of normal dogs were used to stimulate the growth of erythroid burst-forming units (BFU-E) in bone marrow from normal dogs. Maximum numbers of BFU-E were obtained when 5% (vol/vol) 3 X CM and 2 U/ml erythropoietin were added to plasma clot cultures of bone marrow cells. In addition, the radiation sensitivity (D0 value) was determined for CFU-E and for BFU-E in bone marrow cells exposed in vitro to 1 MeV fission neutron radiation or 250 kVp X rays. BFU-E were more sensitive than CFU-E to the lethal effects of both types of radiation. For bone marrow cells exposed to 1 MeV neutron radiation, the D0 for CFU-E was 0.27 +/- 0.01 Gy, and the D0 for BFU-E was 0.16 +/- 0.03 Gy. D0 values for CFU-E and BFU-E were, respectively, 0.61 +/- 0.05 Gy and 0.26 +/- 0.09 Gy for cells exposed to X rays. The neutron RBE values for the culture conditions described were 2.3 +/- 0.01 for CFU-E and 1.6 +/- 0.40 for BFU-E.     

Depression of p53-independent Akt survival signals in human oral cancer cells bearing mutated p53 gene after exposure to high-LET radiation

Although mutations and deletions in the p53 tumor suppressor gene lead to resistance to low linear energy transfer (LET) radiation, high-LET radiation efficiently induces cell lethality and apoptosis regardless of the p53 gene status in cancer cells. Recently, it has been suggested that the induction of p53-independent apoptosis takes place through the activation of Caspase-9 which results in the cleavage of Caspase-3 and poly (ADP-ribose) polymerase (PARP). This study was designed to examine if high-LET radiation depresses serine/threonine protein kinase B (PKB, also known as Akt) and Akt-related proteins. Human gingival cancer cells (Ca9-22 cells) harboring a mutated p53 (mp53) gene were irradiated with 2 Gy of X-rays or Fe-ion beams. The cellular contents of Akt-related proteins participating in cell survival signaling were analyzed with Western Blotting 1, 2, 3 and 6h after irradiation. Cell cycle distributions after irradiation were assayed with flow cytometric analysis. Akt-related protein levels decreased when cells were irradiated with high-LET radiation. High-LET radiation increased G(2)/M phase arrests and suppressed the progression of the cell cycle much more efficiently when compared to low-LET radiation. These results suggest that high-LET radiation enhances apoptosis through the activation of Caspase-3 and Caspase-9, and suppresses cell growth by suppressing Akt-related signaling, even in mp53 bearing cancer cells.     

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.     

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.     

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.     

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.     

The paradoxical nature of DNA damage and cell death induced by 125I decay.

Chinese hamster ovary cells were synchronized at the G1/S-phase boundary of the cell cycle and pulse-labeled for 10 min with 125I-iododeoxyuridine 30 min after entering the S phase. Cell samples were harvested for freezing and 125I-decay accumulation at intervals ranging from 15 to 480 min after termination of labeling. The survival data showed a marked shift from cell killing characteristic of low-LET radiation to that more characteristic of killing by high-LET radiation with increasing intervals between DNA pulse-labeling and decay accumulation. Cells harvested and frozen within 1 h after pulse-labeling yielded a low-LET radiation survival response with a pronounced shoulder and a large D0 of up to 0.9 Gy. With longer chase periods the shoulder and the D0 decreased progressively, and cells harvested 5 h after pulse-labeling or later exhibited a high-LET survival response (D0: 0.13 Gy). Two interpretations for these findings are discussed. (1) If DNA is the sole target for radiation death, the results indicate that DNA maturation increases radiation damage to DNA or reduces damage repair. (2) If radiation cell death involves damage to higher-order structures in the cell nucleus, the findings suggest that newly replicated DNA is not attached to these structures during the initial low-LET period, but 125I starts to induce high-LET radiation effects as labeled DNA segments become associated with the target structure(s). On balance, or data favor the latter interpretation.     

The generation and characterization of a radiation-resistant model system to study radioresistance in human breast cancer cells.

To systematically study the selection of radioresistant cells in clinically advanced breast cancer, a model system was generated by treating MDA-MB231 breast cancer cells with fractionated gamma radiation. A clonogenic assay of the surviving cell populations showed that 2-6 Gy per fraction resulted in a rapid selection of radioresistant populations, within three to five fractions. Irradiation with additional fractions after this initial increase did not increase the radioresistance of the surviving population significantly. Doses of 0.5 and 8 Gy per fraction were not effective in selecting radioresistant cells. To further determine the cause of the changes in radiosensitivity, 15 clones were isolated from the cell populations treated with 40 or 60 Gy with 2 or 4 Gy per fraction, respectively, and were analyzed for radiosensitivity. The average D(10) for these clones was 6.75 +/- 0.36 Gy, which was higher than that for the parental cell population (D(10) = 6.0 +/- 0.2 Gy). The operation of cell cycle checkpoints and the doubling time were similar for both the nonirradiated parental population and the isolated radioresistant subclones. In contrast, a decrease in the apoptotic potential was correlated (r = 0.7, P < 0.01) with increased survival after irradiation, suggesting that apoptosis is an important factor in determining radioresistance under our experimental conditions. We also isolated several subclones from the nonirradiated parental cell population and analyzed them to determine their radiosensitivity after fractionated irradiation. Ten fractions of 4 Gy (40 Gy in total) did not result in a significant increase in the radioresistance of these subclones compared to the irradiated cell populations. The possible mechanisms of the increased radioresistance after fractionated irradiation are discussed.     

Chromatin decondensed by acetylation shows an elevated radiation response

V-79 Chinese hamster lung fibroblasts exposed to 5 mM n-sodium butyrate were irradiated with 60Co gamma rays and cell survival was determined by the cell colony assay. In a separate set of experiments the acetylated chromatin obtained from these cells was irradiated and the change of molecular weight of the DNA was evaluated by alkaline sucrose density centrifugation. At a survival level of 10(-2) to 10(-4) cells exposed to butyrate were found to be 1.3-1.4 times more radiosensitive than control cells. Exposure of isolated chromatin to 100 Gy of 60Co gamma irradiation generated 0.9 +/- 0.03 single-strand breaks (ssb) per 10 Gy per 10(8) Da and 2.0 +/- 0.3 ssb/10 Gy/10(8) Da for control and acetylated chromatin, respectively. The elevated radiation sensitivity of chromatin relaxed by acetylation is in good agreement with previous results on chromatin expanded by histone H1 depletion [Heussen et al., Radiat. Res. 110, 84-94 (1987)]. Packing and accessibility of DNA in chromatin appear to be major factors which influence the radiation sensitivity. The intrinsic radiation sensitivity of chromatin in various packing states is discussed in light of the variation of radiation sensitivity of whole cells in the cell cycle which incorporates repair.     

The effect of He-Ne laser radiation on the survival of HeLa cells subjected to ionizing radiation]

A monolayer of HeLa cells, at the stationary phase of growth, exposed to He-Ne laser radiation (632.8 nm; 100 J/m2) either 5 min or 60 min prior to gamma irradiation (0.1-10 Gy; 6.75 Gy/min), or 5 min after irradiation has been investigated. With a 5-min interval between irradiation sessions (both sequences) the survival curves are virtually the same as those for gamma-irradiated cells only. With He-Ne laser radiation delivered 60 min before gamma irradiation with doses exceeding 5 Gy, a fraction of radioresistant cells is identified whose D0 is almost twice as high as D0 of basic cell mass (3.6 and 1.7 Gy respectively. The survival curve becomes a two-component one. A hypothesis is proposed that He-Ne laser radiation activates, in some cells, the processes that promote the repair of radiation damages.     

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

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

The cell cycle of spermatogonial colony forming stem cells in the CBA mouse after neutron irradiation

In the CBA mouse testis about 10% of the stem cell population is highly resistant to neutron irradiation (D0, 0.75 Gy). Following a dose of 1.50 Gy these cells rapidly increase their sensitivity towards a second neutron dose and progress fairly synchronously through their first post-irradiation cell cycle. From experiments in which neutron irradiation was combined with hydroxyurea it appeared that in this cycle the S-phase is less radiosensitive (D0, 0.43 Gy) than the other phases of the cell cycle (D0, 0.25 Gy). From experiments in which hydroxyurea was injected twice after irradiation the speed of inflow of cells in S and the duration of S and the cell cycle could be calculated. Between 32 and 36 hr after irradiation cells start to enter the S-phase at a speed of 30% of the population every 12 hr. At 60 hr 50% of the population has already passed the S-phase while 30% is still in S. The data point to a cell cycle time of about 36 hr, while the S-phase lasts 12 hr at the most.     

Fibroblasts from patients with inherited predisposition to retinoblastoma exhibit normal sensitivity to the mutagenic effects of ionizing radiation

Retinoblastoma (RB) is a cancer of the retina which characteristically occurs in early childhood. Bilateral RB is an inherited form of this disease. Such patients are at greatly increased risk of subsequently developing second tumors in mesenchymal tissue, especially in areas exposed to ionizing radiation therapy. Fibroblasts from bilateral RB patients have been reported to be more sensitive than normal fibroblasts to the cytotoxic effects of ionizing radiation. Because xeroderma pigmentosum patients have a hereditary predisposition to UV-induced cancer and the cells of such patients are abnormally sensitive to the cytotoxic and mutagenic effects of UV radiation, we compared fibroblasts from 6 bilateral RB patients and 3 normal individuals for their sensitivity to the mutagenic effects of cobalt 60, using resistance to 6-thioguanine (TG) as the genetic marker. The results showed no statistically significant difference between the two types of cell lines. The slope of the weighted least squares line representing the frequency of TG-resistant cells induced in the RB populations as a function of dose was 17 +/- 6 (S.E.)/10(6) cells/Gy with an intercept of 0.09 Gy; that for the normal cells was 17 +/- 7/10(6) cells/Gy with an intercept of 0.14 Gy. We also compared 8 bilateral RB cell lines and 9 age-matched normal cell lines for their sensitivity to the cytotoxic effect of 60Co, using survival of colony-forming ability. The cloning efficiency of the unirradiated RB cell lines ranged from 22% to 76% with an average of 52%; that of the normal cell lines from 21% to 89% with an average of 64%. The results showed the RB cells were somewhat more sensitive than the normal cells. The mean D0 for the RB cell lines ranged from 0.99 +/- 0.01 (S.E.) to 1.69 +/- 0.04 Gy with a weighted average of 1.44 +/- 0.08 Gy; that of the normal cell lines ranged from 1.42 +/- 0.17 to 2.24 +/- 0.10 Gy, with a weighted average of 1.79 +/- 0.11 Gy. The difference in means was estimated to be 0.34 +/- 0.14. The mean for the RB cell lines is statistically significantly lower than the mean for the normal cell lines, at a significance level ca. 1%.     

The response of ataxia-telangiectasia lymphoblastoid cells to neutron irradiation

The response of control and ataxia-telangiectasia (A-T) cells to increasing doses of high-linear-energy-transfer (LET) ionizing radiation (neutrons) was compared. Ataxia-telangiectasia cells were markedly more sensitive to neutron irradiation than were control cells. The D0 value for the two A-T cell lines was 0.4 Gy while the value for controls was approximately 1.4 Gy. Fast neutrons were considerably more effective than gamma rays in inducing cell death in both cell types, but the sensitivity factor remained approximately the same as with gamma rays. A minimal depression of DNA synthesis was observed in ataxia-telangiectasia cells after neutron irradiation, similar to that reported previously after gamma irradiation. The extent of inhibition was not significantly greater in control cells, contrary to that seen with gamma rays. In time-course experiments a significant difference in degree of inhibition of DNA synthesis was observed between the cell types. Low doses of fast neutrons induced a G2-phase delay in both cell types, but the degree and extent of this delay was greater in ataxia-telangiectasia cells as observed previously with low-LET radiation.     

The effects of graded doses of 1 MeV fission neutrons or X rays on the murine hematopoietic stroma.

The acute radiosensitivity in vivo of the murine hematopoietic stroma for 1 MeV fission neutrons or 300 kVp X rays was determined. Two different assays were used: (1) an in vitro clonogenic assay for fibroblast precursor cells (CFU-F) and (2) subcutaneous grafting of femora or spleens. The number of stem cells (CFU-S) or precursor cells (CFU-C), which repopulated the subcutaneous implants, was used to measure the ability of the stroma to support hemopoiesis. The CFU-F were the most radiosensitive, and the survival curves after neutron and X irradiation were characterized by D0 values of 0.75 and 2.45 Gy, respectively. For regeneration of CFU-S and CFU-C in subcutaneously implanted femora, D0 values of 0.92 and 0.84 Gy after neutron irradiation and 2.78 and 2.61 Gy after X irradiation were found. The regeneration of CFU-S and CFU-C in subcutaneously implanted spleens was highly radioresistant as evidenced by D0 values of 2.29 and 1.49 Gy for survival curves obtained after neutron irradiation, and D0 values of 6.34 and 4.85 Gy after X irradiation. The fission-neutron RBE for all the cell populations was close to 3 and varied from 2.77 to 3.28. The higher RBE values observed for stromal cells, compared to the RBE of 2.1 reported previously for hemopoietic stem cells, indicate that stromal cells are relatively more sensitive than hemopoietic cells to neutron irradiation.     

The role of Bcl-X(S) in radiation sensitivity

Bcl-X(S) is a pro-apoptosis member of the Bcl2 family that has been shown to induce cell death and enhance chemosensitivity. We have investigated the effect of Bcl-X(S) overexpression on radiation sensitivity. Using a tetracycline-repressible system, we found that removal of tetracycline for 16 h induced Bcl-X(S) and reduced the surviving fraction of NIH 3T3 cells to 25%. However, radiation sensitivity was not significantly affected by Bcl-X(S) expression; the mean inactivation doses for Bcl-X(S) repressed and Bcl-X(S) induced cells were 2.7 +/- 0.3 and 2.3 +/- 0.1 Gy, respectively. We conclude that Bcl-X(S) induces cell death without affecting radiation sensitivity. These results suggest that mitochondrial pathways to apoptosis may not have a significant role in survival after irradiation.     

The radiosensitivity of kidney colony-forming cells: a short-term assay in situ in the mouse

A short-term colony assay for renal tubule epithelium has been developed. Uranyl nitrate (UN) is a heavy metal nephrotoxin that induces acute tubule necrosis followed by a large compensatory increase in the rate of cell proliferation in the nephron. UN was used to precipitate latent damage following renal irradiation. Using a subcapsular colony count at 14 days after unilateral irradiation, a single-dose cell survival curve was obtained with a D0 of 4.2 +/- 0.3 Gy. High-dose irradiation of an exteriorized kidney resulted in a survival curve which was biphasic, with a plateau in survival between 18 and 40 Gy. Subtraction of this plateau level from all the survival data gave D0 values of 2.5 +/- 0.2 Gy (data analyzed between 7.5 and 16 Gy) or 2.0 +/- 0.2 Gy (over range 12-16 Gy). The D0 value obtained at 20 months after bilateral (or unilateral) kidney irradiation, without the use of UN, was 2.9 +/- 1.1 Gy (over range 10-14 Gy).     

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.