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PubMed2006

Increased complexity of radiation-induced chromosome aberrations consistent with a mechanism of sequential formation.

Complex chromosome aberrations (any exchange involving three or more breaks in two or more chromosomes) are effectively induced in peripheral blood lymphocytes (PBL) after exposure to low doses (mostly single particles) of densely ionising high-linear energy transfer (LET) alpha-particle radiation. The complexity, when observed by multiplex fluorescence in situ hybridisation (m-FISH), shows that commonly four but up to eight different chromosomes can be involved in each rearrangement. Given the territorial organisation of chromosomes in interphase and that only a very small fraction of the nucleus is irradiated by each alpha-particle traversal, the aim of this study is to address how aberrations of such complexity can be formed. To do this, we applied theoretical "cycle" analyses using m-FISH paint detail of PBL in their first cell division after exposure to high-LET alpha-particles. In brief, "cycle" analysis deconstructs the aberration "observed" by m-FISH to make predictions as to how it could have been formed in interphase. We propose from this that individual high-LET alpha-particle-induced complex aberrations may be formed by the misrepair of damaged chromatin in single physical "sites" within the nucleus, where each "site" is consistent with an "area" corresponding to the interface of two to three different chromosome territories. Limited migration of damaged chromatin is "allowed" within this "area". Complex aberrations of increased size, reflecting the path of alpha-particle nuclear intersection, are formed through the sequential linking of these individual sites by the involvement of common chromosomes.

Cell Cycle↗

PubMed1998

Rejoining and misrejoining of radiation-induced chromatin breaks. IV. Charged particles.

We have recently reported the kinetics of chromosome rejoining and exchange formation in human lymphocytes exposed to gamma rays using the techniques of fluorescence in situ hybridization (FISH) and premature chromosome condensation (PCC). In this paper, we have extended previous measurements to cells exposed to charged particles. Our goal was to determine differences in chromatin break rejoining and misrejoining after exposure to low- and high-linear energy transfer (LET) radiation. Cells were irradiated with hydrogen, neon, carbon or iron ions in the LET range 0.3-140 keV/microm and were incubated at 37 degrees C for various times after exposure. Little difference was observed in the yield of early prematurely condensed chromosome breaks for the different ions. The kinetics of break rejoining was exponential for all ions and had similar time constants, but the residual level of unrejoined breaks after prolonged incubation was higher for high-LET radiation. The kinetics of exchange formation was also similar for the different ions, but the yield of chromosome interchanges measured soon after exposure was higher for high-LET particles, suggesting that a higher fraction of DNA breaks are misrejoined quickly. On the other hand, the rate of formation of complete exchanges was slightly lower for densely ionizing radiation. The ratios between the yields of different types of aberrations observed at 10 h postirradiation in prematurely condensed chromosome preparations were dependent on LET. We found significant differences between the yields of aberrations measured in interphase (after repair) and metaphase for densely ionizing radiation. This difference might be caused by prolonged mitotic delay and/or interphase death. Overall, the results point out significant differences between low- and high-LET radiation for the formation of chromosome aberrations.

Animals↗

PubMed1998

The effects of delta rays on the number of particle-track traversals per cell in laboratory and space exposures.

It is a common practice to estimate the number of particle-track traversals per cell or cell nucleus as the product of the ion's linear energy transfer (LET) and cell area. This practice ignores the effects of track width due to the lateral extension of delta rays. We make estimates of the number of particle-track traversals per cell, which includes the effects of delta rays using radial cutoffs in the ionization density about an ion's track of 1 mGy and 1 cGy. Calculations for laboratory and space radiation exposures are discussed, and show that the LET approximation provides a large underestimate of the actual number of particle-track traversals per cell from high-charge and energy (HZE) ions. In light of the current interest in the mechanisms of radiation action, including signal transduction and cytoplasmic damage, these results should be of interest for radiobiology studies with HZE ions.

Cells↗

PubMed2005

Cellular and molecular effects for mutation induction in normal human cells irradiated with accelerated neon ions.

We investigated the linear energy transfer (LET) dependence of mutation induction on the hypoxanthine-guanine phosphoribosyl transferase (HPRT) locus in normal human fibroblast-like cells irradiated with accelerated neon-ion beams. The cells were irradiated with neon-ion beams at various LETs ranging from 63 to 335 keV/microm. Neon-ion beams were accelerated by the Riken Ring Cyclotron at the Institute of Physical and Chemical Research in Japan. Mutation induction at the HPRT locus was detected to measure 6-thioguanine-resistant clones. The mutation spectrum of the deletion pattern of exons of mutants was analyzed using the multiplex polymerase chain reaction (PCR). The dose-response curves increased steeply up to 0.5 Gy and leveled off or decreased between 0.5 and 1.0 Gy, compared to the response to (137)Cs gamma-rays. The mutation frequency increased up to 105 keV/microm and then there was a downward trend with increasing LET values. The deletion pattern of exons was non-specific. About 75-100% of the mutants produced using LETs ranging from 63 to 335 keV/mum showed all or partial deletions of exons, while among gamma-ray-induced mutants 30% showed no deletions, 30% partial deletions and 40% complete deletions. These results suggested that the dose-response curves of neon-ion-induced mutations were dependent upon LET values, but the deletion pattern of DNA was not.

Cell Line↗

PubMed2006

Chromosome breakpoint distribution of damage induced in peripheral blood lymphocytes by densely ionizing radiation.

PURPOSE: To assess the chromosomal breakpoint distribution in human peripheral blood lymphocytes (PBL) after exposure to a low dose of high linear energy transfer (LET) alpha-particles using the technique of multiplex fluorescence in situ hybridization (m-FISH). MATERIALS AND METHODS: Separated PBL were exposed in G0 to 0.5 Gy 238Pu alpha-particles, stimulated to divide and harvested approximately 48 - 50 hours after exposure. Metaphase cells were assayed by m-FISH and chromosome breaks identified. The observed distribution of breaks were then compared with expected distributions of breaks, calculated on the assumption that the distribution of breaks is random with regard to either chromosome volume or chromosome surface area. RESULTS: More breaks than expected were observed on chromosomes 2 and 11, however no particular region of either chromosome was identified as significantly contributing to this over-representation. The identification of hot or cold chromosome regions (pter,p,cen,q,qter) varied depending on whether the data were compared according to chromosome volume or surface area. CONCLUSIONS: A deviation from randomness in chromosome breakpoint distribution was observed, and this was greatest when data were compared according to the relative surface area of each individual chromosome (or region). The identification of breaks by m-FISH (i.e., more efficient observation of interchanges than intrachanges) and importance of territorial boundaries on interchange formation are thought to contribute to these differences. The significance of the observed non-random distribution of breaks on chromosomes 2 and 11 in relation to chromatin organization is unclear.

Alpha Particles↗

PubMedDate not supplied

Cancer risk in space due to radiation assessed by determining cell lethality and mutation frequencies of prokaryotes and a plasmid during the Second International Microgravity Laboratory (IML-2) Space Shuttle experiment.

We participated in a space experiment conducted during the 2nd International Microgravity Laboratory Mission (IML-2) project. The aim of our study was to investigate the effects of space radiation, i.e., high-LET (linear energy transfer) cosmic radiation, on living organisms in the 'Realtime Radiation Monitoring Device (RRMD)'. The biological samples, dried E. coli DNA repair-deficient mutant cells and shuttle vector plasmid pZl89 DNA, were prepared and placed in a biospecimen box sandwiched between 'Harzlas' plastic radiation detectors. This box was then loaded into the RRMD sensor unit in the Space Shuttle 'Columbia' and an identical box was left in the NASA John F. Kennedy Space Center (KSC) as a control. 'Columbia' (flight No. STS-65) was launched from KSC in Florida, USA on July 8, 1994. The mission duration was 14.75 days and after 'Columbia' returned to earth, we studied (i) the lethal and mutagenic effects of high-LET cosmic radiation on E. coli mutants and (ii) the relationship between high-LET cosmic radiation and the mutation frequency of pZ189 DNA. There were virtually no differences between the cell viabilities of the space and control samples of Escherichia coli KMBL3835 (wild-type), KY383 (lexA-), KY385 (recA-) and KY386 (uvrA-), nor between the mutation frequency ratios of the space and control E. coli mutant samples. Furthermore, the survival and mutation frequency of the supF gene of pZ189 DNA space samples did not differ from those of the control samples. We concluded there was no cancer risk during this Space Shuttle flight.

Cosmic Radiation↗

PubMed1999

Induction of DNA double-strand breaks by 1H and 4He lons in primary human skin fibroblasts in the LET range of 8 to 124 keV/microm.

Yields of DNA double-strand breaks were determined in primary human skin fibroblasts exposed to 1H and 4He ions at various linear energy transfers (LETs) and to 15 MeV electrons as the reference radiation. The values obtained for the relative biological effectiveness (RBE) were 2.03, 1.45 and 1.36 for 1H ions at LETs of 35, 23 and 7.9 keV/microm, respectively, and 1.2, 1.18, 1.38 and 1.31 for 4He ions at LETs of 124, 76, 35 and 27 keV/microm, respectively. The data were obtained using pulsed-field gel electrophoresis of DNA released from cells using the chromosomes of the yeast Saccharomyces cerevisiae as length markers and fitting the experimental mass distributions of fragmented DNA to those obtained by computer simulation of the random breakage of human chromosomes. The RBE values for induction of DSBs in mammalian cells cannot be fitted to a common RBE-LET relationship for electrons and 1H, 4He and light ions. Comparison of the RBEs for mammalian cells with the corresponding RBEs obtained for yeast cells shows similar RBEs of electrons for yeast and mammalian cells; however, for 4He and light ions in the LET range of 100 to 1000 keV/microm, the RBEs for yeast are significantly higher compared with mammalian cells. These characteristics of the RBE-LET relationships for yeast and mammalian cells are attributed to the fraction of small DNA fragments induced by particles when traversing the higher-order chromatin structures which are different to some extent in these two cell types.

DNA↗

PubMed1995

The quality of DNA double-strand breaks: a Monte Carlo simulation of the end-structure of strand breaks produced by protons and alpha particles.

The quality of DNA damage induced by protons and alpha-particles of various linear energy transfer (LET) was studied. The aim was to single out specific lesions in the DNA molecule that might lead to biological endpoints such as inactivation. A DNA model coupled with a track structure code (MOCA-15) were used to simulate the lesions induced on the two helixes. Four categories of DNA breaks were considered: single-strand breaks (ssb), blunt-ended double-strand breaks (dsb, with no or few overlapping bases), sticky-ended double-strand breaks (with cohesive free ends of many bases), and deletions (complex lesions which involve at least two dsb within a small number of base pairs). Calculations were carried out assuming various sets of parameters characterizing the production of these different DNA breaks. No large variations in the yields of ssb and blunt- or sticky-ended dsb were found in the LET range between 10 and 200 keV/mu m. On the other hand, the yield of deletions increases up to about 100 keV/mu m and seems to reach a plateau at higher LET values. In the LET interval from 30 to 60 keV/mu m, protons proved to be more efficient than alpha-particles in inducing deletions. The induction of these complex lesions is thus dependent not simply on LET but also on the characteristics of the track structure. Comparison with RBE values for cell killing shows that this special class of dsb might play an important role in radiation-induced cell inactivation.

Alpha Particles↗

PubMed1996

Absorbed dose measurements on LDEF and comparisons with predictions.

The radiation environment on LDEF was monitored by cumulative absorbed dose measurements made with TLDs at different locations and shielding depths. The TLDs were included in four experiments: A0015(a) Biostack, P0004 Seeds in Space and P0006 Linear Energy Transfer Spectrum Measurements at the trailing edge (west side) of the satellite; M0004 Fiber Optics Data Link at the leading edge (east side); and A0015(b) Biostack at the Earth side. The shielding depths varied between 0.48 and 15.4 g/cm2, Al equivalent. Both the directional dependence of trapped protons incident on the satellite and the shielding thickness were reflected in absorbed dose values. The trapped proton anisotropy was measured by TLDs at the east and west sides of LDEF. At the east side doses ranged from 2.10 to 2.58 Gy under shielding of 2.90 to 1.37 g/cm2 (M0004) while on the west side doses ranged from 2.66 to 6.48 Gy under shielding of 15.4 to 0.48 g/cm2 (P0006). The west side doses were more than a factor of two higher, where the vertical shielding thicknesses to space were equal. Other west side doses of 3.04 to 4.49 Gy under shielding of 11.7 to 3.85 g/cm2 (A0015(a)) and 2.91 to 6.64 Gy under shielding of 11.1 to 0.48 g/cm2 (P0004) generally agreed with the P0006 results. The Earth side doses of 2.41 to 3.93 Gy under shielding of 10.0 to 1.66 g cm2 (A0015(b)) were intermediate between the east side and west side doses. Calculations utilizing a model of trapped proton spectra were performed by Watts et al. (1993) and comparisons of dose measurement and calculations may be found in a companion paper (Armstrong et al., 1996).

Aluminum↗

PubMed1992

An analysis of particle track effects on solid mammalian tissues.

Relative biological effectiveness (RBE) and quality factor (Q) at extreme values of linear energy transfer (LET) have been determined on the basis of experiments with single-cell systems and specific tissue responses. In typical single-cell systems, each heavy particle (Ar or Fe) passes through a single cell or no cell. In experiments on animal tissues, however, each heavy particle passes through several cells, and the LET can exceed 200 keV micrometers-1 in every cell. In most laboratory animal tissue systems, however, only a small portion of the hit cells are capable of expressing the end-point being measured, such as cell killing, mutation or carcinogenesis. The following question was therefore addressed: do RBEs and Q factors derived from single-cell experiments properly account for the damage at high LET when multiple cells are hit by HZE tracks? A review is offered in which measured radiation effects and known tissue properties are combined to estimate on the one hand, the number of cells at risk, p3n, per track, where n is the number of cells per track based on tissue and organ geometry, and p3 is the probability that a cell in the track is capable of expressing the experimental end-point. On the other hand, the tissue and single-cell responses are compared by determining the ratio RBE in tissue/RBE in corresponding single cells. Experimental data from the literature indicate that tissue RBEs at very high LET (Fe and Ar ions) are higher than corresponding single-cell RBEs, especially in tissues in which p3n is high.

Animals↗

PubMed2000

Immediate localized CDKN1A (p21) radiation response after damage produced by heavy-ion tracks.

Using confocal microscopy on immunofluorescence-stained cells, we have investigated the response of CDKN1A (p21), one of the key proteins involved in the DNA damage response pathway, after irradiation with accelerated lead or chromium ions. Each traversal of an accelerated ion leads to the formation of a single, bright focus of the CDKN1A protein in the nuclei of human fibroblasts within 2 min after irradiation at 4 degrees C. This immediate, localized CDKN1A response is specific for particle irradiation with a high linear energy transfer (LET), whereas X irradiation, after a period of induction, yields a diffusely spread pattern, in line with the differences in the microscopic dose deposition pattern of both radiation types. The particle-induced CDKN1A foci persist for several hours until they become diffuse and vanish. These findings suggest that CDKN1A accumulates at the sites of primary DNA damage, possibly mediated by the interaction with proteins involved in DNA repair. Here, for the first time, an immediate biological response confined to the radial extension of low-energy particle tracks ( approximately 1 micrometer) is directly visualized and correlated to ion traversals. This indicates that particle irradiation represents an ideal tool to study the processing of biological damage induced in defined subnuclear regions.

Cells, Cultured↗

PubMed1997

Neon heavy charged particle radiotherapy of glioblastoma of the brain.

PURPOSE: High-linear energy transfer (LET) radiation beams have potential applications in the treatment of glioblastoma, but have not yet demonstrated significant improvement in results. However, some patients have had local control of glioblastoma with high-LET irradiations such as neutrons and heavy charged particles. METHODS AND MATERIALS: In this collaborative study, 15 patients were entered into a randomized protocol comparing two dose levels of 20 and 25 Gy in 4 weeks of neon ion irradiation. This trial was intended to determine the optimal neon dose in terms of survival and effects of radiation. RESULTS: Fourteen patients were evaluable with no significant differences in median survival (13 and 14 months; p = NS) or median time to failure (7 and 9 months; p = NS) between the two dose arms. Three patients died of nontumor-related causes, of whom one (who died 19 months posttreatment) had autopsy confirmation of no tumor on pathological exam. The other two patients had stable magnetic resonance imaging scans at 6 and 22 months posttreatment. CONCLUSION: Although the results did not demonstrate the optimal high-LET dose level, there is an intriguing effect in that two patients had control of glioblastoma until death at 19 and 22 months. This suggests that better conformation of the high-LET dose to the tumor with neutron capture therapy or dynamic conformal heavy charged particle therapy might control glioblastoma while minimizing brain damage from radiation.

Adult↗

PubMed2003

Remote afterloading for neutron brachytherapy using californium-252.

BACKGROUND: Despite a pronounced technical process attained in radiotherapy of malignant neoplasms, no remarkable improvement in the treatment results has been achieved. The reason for this stagnation is the interaction between tumor cell and photon radiation. Tumor resistance against photon bombardment can be broken down by applying high linear energy transfer (LET) radiation-based treatment. The discovery of californium-252 ((252)Cf) nuclide, a source of gamma neutron radiation, established a precondition for using neutrons in tumor brachytherapy. The design of a remote afterloading device using (252)Cf sources remains an unsolved problem. MATERIAL AND METHODS: The afterloading device has been designed as a stationary radiator which is composed of three mutually interconnected units: 1. the control and drive unit consisting of a control computer and a motor-driven bowden system carrying the (252)Cf source; 2. the source which is housed in a watertight concrete vessel-storage strong room, situated in the ground at a depth of 25 cm beneath the patient's bed; 3. the afterloading application module installed in the irradiation room. RESULTS: Remote afterloading allows simple, inexpensive and highly efficient radiation protection and work safety for the operating personnel. The sources may be moved arbitrarily during treatment with a position accuracy of 0.5-1.0 mm within a distance of 520 cm from the source storage position in the strong room to the application position. Both afterloading systems' unused indexer outputs are protected electronically and mechanically against any unintentional movement of the source outside the application tubes. CONCLUSION: The technologic concept of the present automatic afterloading device for neutron brachytherapy represents a possible option from the range of conceivable design variants, which - while minimizing technologic and economic requirements - provides the operating personnel with optimum protection and work safety, thus extending the applicability of high LET radiation-based treatment methods in clinical practice.

Brachytherapy↗

PubMed2001

High-LET radiation induces apoptosis in lymphoblastoid cell lines derived from atazia-telangiectasia patients.

PURPOSE: To investigate and compare the propensity of Epstein-Barr virus (EBV)-transformed lymphoblastoid cell lines (LCL), derived from ataxia-telangiectasia (A-T) patients and from unaffected healthy individuals (controls), to undergo apoptosis after exposure to high-linear energy transfer (LET) radiation. MATERIALS AND METHODS: Four A-T (ARO, BMA, CSA and RJO) and two control (JAC and KKB3) LCL were exposed to doses of up to 4Gy of accelerated nitrogen ions (32-45 MeV/u, 8-12Gy/min). For comparative purposes X-ray irradiation (1.36 Gy/min) was also performed. The induction of apoptosis was studied 0-48 h after irradiation with the use of two methods: (1) monitoring of high molecular weight (HMW) DNA fragments by field inversion pulse gel electrophoresis (FIGE); and (2) morphological characterization ofapoptotic cells after fluorescent staining. In parallel, cell-cycle distribution, monitored by DNA flow cytometry, as well as measurements of p53/p21(WAF1) protein levels by Western blots, were investigated in these cells. RESULTS: High-LET radiation-induced apoptosis and G2/M-arrest in both A-T and control LCL. No significant increase in the amount of p53/p21(WAF1) proteins preceded apoptosis in control or in A-T LCL after high-LET irradiation. However, low-LET radiation did induce significant enhanced levels of p53 proteins in control but not in A-T LCL. CONCLUSIONS: LCL from both A-T homozygous and unaffected healthy individuals undergo apoptosis without accumulation of p53/p21(WAF1) proteins after exposure to high-LET radiation. In contrast, low-LET radiation induces apoptosis and significantly increases levels of p53 protein in control but not in A-T LCL.

Apoptosis↗

PubMed1999

RBE-LET relationships of high-LET radiations in Drosophila mutations.

The relative biological effectiveness (RBE) of 252Cf neutrons and synchrotron-generated high-energy charged particles for mutation induction was evaluated as a function of linear energy transfer (LET), using the loss of heterozygosity for wing-hair mutations and the reversion of the mutant white-ivory eye-color in Drosophila melanogaster. Loss of heterozygosity for wing-hair mutations results predominantly from mitotic crossing over induced in wing anlage cells of larvae, while the reverse mutation of eye-color is due to an intragenic structural change (2.96 kb-DNA excision) in the white locus on the X-chromosome. The measurements were performed in a combined mutation assay system so that induced mutant wing-hair clones as well as revertant eye-color clone can be detected simultaneously in the same individual. Larvae were irradiated at the age of 3 days post oviposition with 252Cf neutrons, carbon beam or neon beam. For the neutron irradiation, the RBE values for wing-hair mutations were larger than that for eye-color mutation by about 7 fold. The RBE of carbon ions for producing the wing-hair mutations increased with increase in LET. The estimated RBE values were found to be in the range 2 to 6.5 for the wing-hair. For neon beam irradiation, the RBE values for wing-hair mutations peak near 150 keV/micron and decrease with further increase in LET. On the other hand, the RBE values for the induction of the eye-color mutation are nearly unity in 252Cf neutrons and both ions throughout the LET range irradiated. We discuss the relationships between the initial DNA damage and LET in considering the mechanism of somatic mutation induction.

Animals↗

PubMed2002

Passive dosimetry aboard the Mir Orbital Station: internal measurements.

Passive radiation dosimeters were exposed aboard the Mir Orbital Station over a substantial portion of the solar cycle in order to measure the change in dose and dose equivalent rates as a function of time. During solar minimum, simultaneous measurements of the radiation environment throughout the habitable volume of the Mir were made using passive dosimeters in order to investigate the effect of localized shielding on dose and dose equivalent. The passive dosimeters consisted of a combination of thermoluminescent detectors to measure absorbed dose and CR-39 PNTDs to measure the linear energy transfer (LET) spectrum from charged particles of LET infinity H2O > or = 5 keV/micrometers. Results from the two detector types were then combined to yield mean total dose rate, mean dose equivalent rate, and average quality factor. Contrary to expectations, both dose and dose equivalent rates measured during May-October 1991 near solar maximum were higher than similar measurements carried out in 1996-1997 during solar minimum. The elevated dose and dose equivalent rates measured in 1991 were probably due to a combination of intense solar activity, including a large solar particle event on 9 June 1991, and the temporary trapped radiation belt created in the slot region by the solar particle event and ensuing magnetic storm of 24 March 1991. During solar minimum, mean dose and dose equivalent rates were found to vary by factors of 1.55 and 1.37, respectively, between different locations through the interior of Mir. More heavily shielded locations tended to yield lower total dose and dose equivalent rates, but higher average quality factor than did more lightly shielding locations. However, other factors such as changes in the immediate shielding environment surrounding a given detector location, changes in the orientation of the Mir relative to its velocity vector, and changes in the altitude of the station also contributed to the variation. Proton and neutron-induced target fragment secondaries, not primary galactic cosmic rays, were found to dominate the LET spectrum above 100 keV/micrometers. This indicates that in low earth orbit, trapped protons in the South Atlantic Anomaly are responsible for the major fraction of the total dose equivalent.

Atlantic Ocean↗

PubMed2003

Mechanisms of suppression of neoplastic transformation in vitro by low doses of low LET radiation.

Suppression of neoplastic transformation of HeLa x skin fibroblast human hybrid cells in vitro following low doses of low linear energy transfer radiation has been reported previously. The present study represents an exploration of two hypothesized mechanisms that may underlie this observed suppression. These are the up-regulation of reduced glutathione (GSH), a known antioxidant, and induction of DNA repair activity. The hybrid cells were found to have a high endogenous level of GSH and no induction following low doses of 60 kVp X-rays was observed. Buthionine sulfoximine (BSO), a GSH biosynthesis inhibitor, completely suppressed GSH levels in both unirradiated and irradiated cells. Furthermore, there was no significant impact of BSO-induced suppression of GSH on the neoplastic transformation frequency of either unirradiated or low dose irradiated cells indicating that glutathione levels play no role in the low dose suppression of transformation frequency. To assess the possible role of DNA repair in the low dose suppression of transformation the effect of 3-aminobenzamide (3-AB), a poly-ADP-ribose polymerase (PARP) inhibitor was examined. In these experiments, there was no significant effect of 3-AB on the transformation frequency at a dose of Cs-137 gamma rays of 0.5 cGy, however, at a dose of 5 cGy there was a significant increase (P < 0.05) in the transformation frequency in the presence of 3-AB. These findings suggest that the influence of DNA repair on the low dose suppression of transformation is significant at a dose of 5 cGy, but not at the lower dose of 0.5 cGy.

Antioxidants↗

PubMed2006

Acute effects of iron-particle radiation on immunity. Part II: Leukocyte activation, cytokines and adhesion.

The effects of high-linear energy transfer (LET) radiation on immune function have not been clearly established. The major goal of this study was to evaluate leukocyte responses after whole-body exposure to high-LET radiation. C57BL/6 mice were exposed to 0, 0.5, 2 and 3 Gy (56)Fe(26+) particles (1055 MeV/nucleon, 148.2 keV/microm) and killed humanely 4 days after exposure. Spontaneous synthesis of DNA in blood and spleen cells was increased significantly in groups receiving either 2 or 3 Gy (P < 0.001). In contrast, a significant depression in the response of T lymphocytes to phytohemagglutinin (PHA) and concanavalin A (ConA) was noted (P < 0.005); the response to lipopolysaccharide (LPS), a B-cell mitogen, was similar among groups. A cytometric bead array assay revealed that the level of tumor necrosis factor alpha (Tnfa) secreted by splenocytes increased significantly with increasing (56)Fe-particle dose (P < 0.05); interferon gamma, interleukin2 (Il2), Il4 and Il5 were unaffected. Flow cytometry analysis showed that 2 and 3 Gy markedly reduced splenic mononuclear cells expressing the activation markers CD25 and CD71, both with and without the T-cell marker CD3 (P < 0.05); proportions also varied significantly. Similar patterns were noted in mononuclear and granular cells with adhesion markers CD11b and, to a lesser extent, CD54 (P < 0.05). The results show that a single, acute exposure to high-LET radiation induced changes that can profoundly alter leukocyte functions. The implications of the data are discussed in relation to low-LET radiation, altered gravity, and space flight.

Animals↗