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PubMed2001

Radiation risk to low fluences of alpha particles may be greater than we thought.

Based principally on the cancer incidence found in survivors of the atomic bombs dropped in Hiroshima and Nagasaki, the International Commission on Radiation Protection (ICRP) and the United States National Council on Radiation Protection and Measurements (NCRP) have recommended that estimates of cancer risk for low dose exposure be extrapolated from higher doses by using a linear, no-threshold model. This recommendation is based on the dogma that the DNA of the nucleus is the main target for radiation-induced genotoxicity and, as fewer cells are directly damaged, the deleterious effects of radiation proportionally decline. In this paper, we used a precision microbeam to target an exact fraction (either 100% or < or =20%) of the cells in a confluent population and irradiated their nuclei with exactly one alpha particle each. We found that the frequencies of induced mutations and chromosomal changes in populations where some known fractions of nuclei were hit are consistent with non-hit cells contributing significantly to the response. In fact, irradiation of 10% of a confluent mammalian cell population with a single alpha particle per cell results in a mutant yield similar to that observed when all of the cells in the population are irradiated. This effect was significantly eliminated in cells pretreated with a 1 mM dose of octanol, which inhibits gap junction-mediated intercellular communication, or in cells carrying a dominant negative connexin 43 vector. The data imply that the relevant target for radiation mutagenesis is larger than an individual cell and suggest a need to reconsider the validity of the linear extrapolation in making risk estimates for low dose, high linear-energy-transfer (LET) radiation exposure.

Alpha Particles↗

PubMed1988

Central nervous system radiation syndrome in mice from preferential 10B(n, alpha)7Li irradiation of brain vasculature.

Ionizing radiations were directed at the heads of anesthetized mice in doses that evoked the acute central nervous system (CNS) radiation syndrome. Irradiations were done using either a predominantly thermal neutron field at a nuclear reactor after intraperitoneal injection of 10B-enriched boric acid or 250-kilovolt-peak x-rays with and without previous intraperitoneal injection of equivalent unenriched boric acid. Since 10B concentrations were approximately equal to 3-fold higher in blood than in cerebral parenchyma during the reactor irradiations, more radiation from alpha and 7Li particles was absorbed by brain endothelial cells than by brain parenchymal cells. Comparison of the LD50 dose for CNS radiation lethality from the reactor experiments with the LD50 dose from the x-ray experiments gives results compatible with morphologic evidence that endothelial cell damage is a major determinant of acute lethality from the CNS radiation syndrome. It was also observed that boric acid is a low linear energy transfer radiation-enhancement agent in vivo.

Animals↗

PubMed1989

Labeling monoclonal antibodies and F(ab')2 fragments with the alpha-particle-emitting nuclide astatine-211: preservation of immunoreactivity and in vivo localizing capacity.

alpha-Particles such as those emitted by 211At may be advantageous for radioimmunotherapy since they are radiation of high linear energy transfer, depositing high energy over a short distance. Here we describe a strategy for labeling monoclonal antibodies and F(ab')2 fragments with 211At by means of the bifunctional reagent N-succinimidyl 3-(trimethylstannyl)benzoate. An intact antibody, 81C6, and the F(ab')2 fragment of Me1-14 (both reactive with human gliomas) were labeled with 211At in high yield and with a specific activity of up to 4 mCi/mg in a time frame compatible with the 7.2-hr half-life of 211At. Quantitative in vivo binding assays demonstrated that radioastatination was accomplished with maintenance of high specific binding and affinity. Comparison of the biodistribution of 211At-labeled Me1-14 F(ab')2 to that of a nonspecific antibody fragment labeled with 211At and 131I in athymic mice bearing D-54 MG human glioma xenografts demonstrated selective and specific targeting of 211At-labeled antibody in this human tumor model.

Animals↗

PubMed1997

Mutagenic effects of a single and an exact number of alpha particles in mammalian cells.

One of the main uncertainties in risk estimation for environmental radon exposure using lung cancer data from underground miners is the extrapolation from high- to low-dose exposure where multiple traversal is extremely rare. The biological effects of a single alpha particle are currently unknown. Using the recently available microbeam source at the Radiological Research Accelerator Facility at Columbia University, we examined the frequencies and molecular spectrum of S1- mutants induced in human-hamster hybrid (A(L)) cells by either a single or an exact number of alpha particles. Exponentially growing cells were stained briefly with a nontoxic concentration of Hoechst dye for image analysis, and the location of individual cells was computer-monitored. The nucleus of each cell was irradiated with either 1,2,4, or 8 alpha particles at a linear energy transfer of 90 keV/microm consistent with the energy spectrum of domestic radon exposure. Although single-particle traversal was only slightly cytotoxic to A(L) cells (survival fraction approximately 0.82), it was highly mutagenic, and the induced mutant fraction averaged 110 mutants per 10(5) survivors. In addition, both toxicity and mutant induction were dose-dependent. Multiplex PCR analysis of mutant DNA showed that the proportion of mutants with multilocus deletions increased with the number of particle traversals. These data provide direct evidence that a single a particle traversing a nucleus will have a high probability of resulting in a mutation and highlight the need for radiation protection at low doses.

Alpha Particles↗

PubMed2000

Clustered DNA damages induced in isolated DNA and in human cells by low doses of ionizing radiation.

Clustered DNA damages-two or more closely spaced damages (strand breaks, abasic sites, or oxidized bases) on opposing strands-are suspects as critical lesions producing lethal and mutagenic effects of ionizing radiation. However, as a result of the lack of methods for measuring damage clusters induced by ionizing radiation in genomic DNA, neither the frequencies of their production by physiological doses of radiation, nor their repairability, nor their biological effects are known. On the basis of methods that we developed for quantitating damages in large DNAs, we have devised and validated a way of measuring ionizing radiation-induced clustered lesions in genomic DNA, including DNA from human cells. DNA is treated with an endonuclease that induces a single-strand cleavage at an oxidized base or abasic site. If there are two closely spaced damages on opposing strands, such cleavage will reduce the size of the DNA on a nondenaturing gel. We show that ionizing radiation does induce clustered DNA damages containing abasic sites, oxidized purines, or oxidized pyrimidines. Further, the frequency of each of these cluster classes is comparable to that of frank double-strand breaks; among all complex damages induced by ionizing radiation, double-strand breaks are only about 20%, with other clustered damage constituting some 80%. We also show that even low doses (0.1-1 Gy) of high linear energy transfer ionizing radiation induce clustered damages in human cells.

Bacteriophage T7↗

PubMed2006

Radioimmunotherapy as non-myeloablative conditioning for allogeneic marrow transplantation.

Radioimmunotherapy (RIT) combines the advantages of specific immunotherapy with the cytotoxicity of radionuclides resulting in targeted radiation therapy. In the setting of allogeneic hematopoietic cell transplantation (HCT), RIT can be used to both target tumor cells and to suppress immunocompetent recipient cells. RIT with beta-emitters has been successfully used for further dose intensification of myeloablative conditioning regimens for HCT. Alpha-emitters with their short path length and high linear energy transfer bear certain advantages over beta-emitters if used to target hematopoietic cells. Using a canine model of non-myeloablative HCT, one could demonstrate that pre-transplant RIT with the alpha-emitter bismuth-213 (213Bi) coupled to anti-CD45 or anti-TCRalphabeta monoclonal antibodies (mAb) together with post-grafting immunosuppression with mycophenolate mofetil and cyclosporine can achieve stable engraftment and long-term mixed chimerism. The two mAbs may allow a tailored approach to RIT in non-myeloablative conditioning with 213Bi-anti-CD45 used for patients with hematologic malignancies and 213Bi-anti-TCRalphabeta for non-malignant diseases. Extensive studies of biodistribution, dose de-escalation and toxicity provide the basis for the conception of clinical trials using RIT for non-myeloablative HCT.

Animals↗

PubMed2001

Radiation-induced DNA damage and chromatin structure.

DNA lesions induced by ionizing radiation in cells are clustered and not randomly distributed. For low linear energy transfer (LET) radiation this clustering occurs mainly on the small scales of DNA molecules and nucleosomes. For example, experimental evidence suggests that both strands of DNA on the nucleosomal surface can be damaged in single events and that this damage occurs with a 10-bp modulation because of protection by histones. For high LET radiation, clustering also occurs on a larger scale and depends on chromatin organization. A particularly significant clustering occurs when an ionizing particle traverses the 30 nm chromatin fiber with generation of heavily damaged DNA regions with an average size of about 2 kbp. On an even larger scale, high LET radiation can produce several DNA double-strand breaks in closer proximity than expected from randomness. It is suggested that this increases the probability of misrejoining of DNA ends and generation of lethal chromosome aberrations.

Chromatin↗

PubMed2001

Biologically optimized radiation therapy.

Advanced treatment optimization is possible using quantitative radiobiological dose response models. Although all present models are necessarily linked to a certain degree of uncertainty, this will only have a small influence on the relative shape of the resultant optimal dose distribution. However the exact dose level should perferably be determined clinically by dose escalation with the optimized dose plan as a control arm. It is shown that a large part of the biological effect of high linear energy transfer radiation is due to the spectrum of low-energy delta-electrons that can generate dense clusters of complex DNA damage. Such electrons are efficiently generated by low-energy photons or densely ionizing ion beams and to a considerably smaller degree by high-energy electrons, photons and protons. A new analytical expression is developed for the effective radiation resistance of heterogeneous tumors, making it possible to approximate the response of such tumors by the effective clonogen number N0,eff and the effective D0 value D0,eff. It is shown that a relatively small number of resistant tumor cells may well be sufficient to dominate the response of hypoxic or otherwise heterogeneous tumors. Finally, several examples are given of intensity-modulated dose distributions generated by multiple radiation modalities, the total effect of which is biologically optimized.

Cell Survival↗

PubMed2000

Inactivation of human normal and tumour cells irradiated with low energy protons.

PURPOSE: To analyse the cell inactivation frequencies induced by low energy protons in human cells with different sensitivity to photon radiation. MATERIALS AND METHODS: Four human cell lines with various sensitivities to photon irradiation were used: the SCC25 and SQ20B derived from human epithelium tumours of the tongue and larynx, respectively, and the normal lines M/10, derived from human mammary epithelium, and HF19 derived from a lung fibroblast. The cells were irradiated with y-rays and proton beams with linear energy transfer (LET) from 7 to 33 keV/microm. Clonogenic survival was assessed. RESULTS: Survival curves are reported for each cell line following irradiation with gamma-rays and with various proton LETs. The surviving fraction after 2 Gy of gamma-rays was 0.72 for SQ20B cells, and 0.28-0.35 for the other cell lines. The maximum LET proton effectiveness was generally greater than that of gamma-rays. In particular there was a marked increase in beam effectiveness with increasing LET for the most resistant cells (SQ20B) whose 2 Gy-survival varied from 0.72 with gamma-radiation down to 0.37 with 30 keV/microm protons. The relative biological effectiveness (RBE(2 Gy gamma)) with the 30 keV/microm beam, evaluated as the ratio of 2 Gy to the proton dose producing the same inactivation level as that given by 2 Gy of gamma-rays, was 3.2, 1.8, 1.3 and 0.8 for SQ20B, M/10, SCC25, and HF19, respectively. CONCLUSIONS: RBE for inactivation with high-LET protons increased with the cellular radioresistance to gamma-rays. The cell line with the greatest resistance to gamma-rays was the most responsive to the highest LET proton beam. A similar trend has also been found in studies reported in the literature with He, C, N ions with LET in the range 20-125 keV/microm on human tumour cell lines.

Cell Line↗

PubMed2000

DNA DSB induction and rejoining in V79 cells irradiated with light ions: a constant field gel electrophoresis study.

PURPOSE: To study the induction and the time-course of rejoining of DNA double strand breaks (DSB) in V79 cells irradiated with light ions with different linear energy transfer (LET). MATERIALS AND METHODS: V79 cells were irradiated in monolayer with monoenergetic proton, deuteron, helium-3 or helium-4 ion beams, each at two different energy values. Gamma rays were used as reference radiation. DSB have been measured by constant field gel electrophoresis (CFGE). RESULTS: The initial yield depended little on the particle type and LET. The amount of DSB left unrejoined for up to 2 h incubation time could be roughly described by a decreasing exponential function with a final plateau, although more complex functions cannot be excluded. Radiation quality had little effect on the rejoining rate but affected the plateau. The amount of residual DSB after 2 h was higher for densely than for sparsely ionizing radiation, and for the same particle was dependent on LET. The corresponding RBE ranged from 1.8 to 6.0. CONCLUSIONS: The results support the hypothesis that complex, less reparable DSB are induced in higher proportion by light ions with respect to gamma-rays and that, for the same ion, increasing LET leads to an increase in this proportion.

Animals↗

PubMed2001

Low-dose hypersensitivity of V79 cells under exposure to gamma-rays and 4He ions of different energies: survival and chromosome aberrations.

PURPOSE: To examine the low-dose sensitivity of V79 cells under exposure to gamma-rays and 4He ions of different energies. MATERIALS AND METHODS: Cell survival and cytogenetic analysis using the Giemsa technique were studied following irradiation to doses of 0-3 Gy at the INFN-LNL facilities. RESULTS: Low-dose hyper-radiosensitivity (HRS) of V79 was demonstrated after irradiation with gamma-rays and alpha-particles of various linear energy transfers (LET) (58.9, 79.3 and 101.7 keV microm(-1)). Cytogenetic analysis showed an LET dependence of aberrations at a dose of 1Gy; the frequency of chromatid fragments appeared to vary with the number of alpha-particles traversing the cell nucleus. The results of both studies fit together to give a better understanding of so-called 'induced radioresistance' phenomenon. CONCLUSIONS: The mechanism of induced cellular radioresistance appears to be initiated after a certain amount of energy is deposited in the cell nucleus. This amount depends on both radiation quality and the number of particles traversing the cell.

Animals↗

PubMed2002

Rejoining of double-stranded DNA-fragments studied in different size-intervals.

PURPOSE: To measure rejoining of radiation-induced doublestranded DNA-fragments of different sizes and to evaluate the effects of size-resolution in the analysis of rejoining. MATERIAL AND METHODS: Normal human fibroblasts (GM5758) were irradiated with photons or accelerated nitrogen ions (linear energy transfer, LET = 125 keV microm(-1)) and incubated for repair for 0-22 h. Double-stranded DNA-fragments from the irradiated cells were separated by pulsed-field gel electrophoresis in the range approximately 5 kbp to 5.7 Mbp. RESULTS: For cells irradiated with high LET nitrogen ions, there was an increase in the fast half-time from approximately 5 min for fragments < 400 kbp to 10 min when all fragments < 5.7 Mbp were measured. Further, the fraction of fragments rejoined by the slow-rejoining phase increased significantly for increased threshold sizes. The fraction of unrejoined fragments after 22 h and the half-time for the slow-rejoining phase remained constant for all threshold sizes. For cells irradiated with lower doses of low LET radiation the rejoining was shifted towards a slower kinetics when fragments up to 10 Mbp were excluded in the analysis. CONCLUSION: DNA exclusion-size and resolution may affect the estimates of DNA double-strand break rejoining. Using a low-resolution technique that does not detect small fragments will result in an underestimation, or even disappearance of the fast-rejoining phase. This is due to substantial rejoining of fragments taking place before the fragments are of sufficient size to be monitored.

Cell Line↗

PubMed2002

Quantification of radiation induced DNA double-strand breaks in human fibroblasts by PFGE: testing the applicability of random breakage models.

PURPOSE: To assess the applicability of methods of quantification of double-strand breaks (DSB) based on the random breakage paradigm, measuring yield and distribution of DSB induced by varying radiation quality. MATERIAL AND METHODS: 240 kVp X-rays and (238)Pu alpha-particles were used to induce DSB in AG01522B primary human fibroblasts. DNA molecular weight distributions were resolved by means of three pulsed-field gel-electrophoresis (PFGE) protocols, which, when combined together, allowed separation and quantification of double-stranded fragments between 5.7 Mbp and 12 kbp. Several analytical methods quantified the DSB yields. RESULTS: Data showed significant differences in the fragmentation patterns according to radiation quality. For both X-rays and alpha-particles, it was observed that the shape of the fragmentation profiles deviates from the prediction of a random breakage mechanism. This is in contrast to other studies where sparsely ionizing radiations appeared to distribute breaks uniformly throughout the genome. Deviations from random breakage were more evident after high linear energy transfer (LET) radiation, which showed an excess of breaks <1 Mbp and a deficit in the production of fragments >1 Mbp, a value that could be dose-dependent. CONCLUSIONS: Current methods of DNA fragmentation analysis after induction of DSB may lead to contradictory conclusions on both DSB yields and distributions. This study showed that the application of different DSB quantification methods, derived from random breakage or supported by its concepts, resulted in different radiation biological effectivenesses (RBE) for the induction of DSB, depending on how these methods were employed. To compare experimental results from different laboratories, care should be taken to provide as many details as possible about the application of methods of quantification of DNA damage. For all the methods used, total DSB yields resulted in RBE less than those for mutation induction or reproductive cell death, suggesting that total DSB yields only gave a limited indication of the severity of the inflicted damage. Production of correlated breaks on the chromatin loop structures by single particle-track traversals may explain the deviations observed between experimental data and the predictions of the random breakage paradigm.

Alpha Particles↗

PubMed2002

Response of mammalian cell lines that undergo necrosis after ionizing irradiation to DNA-incorporated tritium and iodine-125 decays: implications for models of radiation action.

PURPOSE: To test the validity of enzymatic DNA repair-based models of ionizing radiation-induced mammalian cell killing. MATERIALS AND METHODS: Sensitivity to ionizing radiation-induced killing was determined by clonogenic survival assay. RESULTS: A panel of seven cell lines that have apparently normal enzymatic DNA repair capability and die predominantly by necrosis were shown to have marked differences in their sensitivity to killing by gamma- or X-irradiation. Despite such differences, the pseudo-diploid cell lines CHO, V79, and Vero (when corrected for differences in cell cycle distribution) and normal mouse embryo fibroblasts all had comparable D(o) values for killing by DNA-incorporated (125)I that were in the range of 57-66 decays; whilst the near-tetraploid or-triploid B16-F1, RUC-2 and SQ-20B cell lines had D(o) values of around 130 (125)I decays. The sensitivity of these cell lines to killing by DNA-incorporated (3)H decays was similarly related to ploidy. CONCLUSIONS: Differences in sensitivity to killing by DNA-incorporated (3)H or (125)I decays between the cell lines tested were primarily related to differences in ploidy and, second, to differences in cell cycle distribution or nuclear volume. The data do not support suggestions that generalized variability in an hypothetical aspect of enzymatic DNA repair can explain differences in sensitivity to killing by external-beam, low-linear energy transfer ionizing radiation.

Animals↗

PubMed2002

Modelling radiation-induced chromosome aberrations.

PURPOSE: To review the data and models on the induction of chromosomal aberrations by a single acute dose of radiation, then critically to assess progress that has been made so far to make a judgement about prospects for increased understanding. MATERIALS AND METHODS: Drawing upon many years of personal experience, a consistent set of data on the radiation-induced dicentric yield in human lymphocytes was produced. Other data concerning the production of complex rearrangements and the time-course of the appearance of dicentrics has also been reviewed. Three basic models have been reviewed and compared with respect to their ability to predict the judged dose-effect relationships as well as the time-course and complexity of the aberration production. CONCLUSIONS: None of the three basic models alone can explain adequately all of the available data. A combination of the models has succeeded to a greater extent, but there is still no complete agreement. The major reason for the discrepancy between the measured yield curves and their predictions lies in the variation of the quadratic term in the dose-response relationship with increasing linear energy transfer. Further experimental work is required to resolve this.

Animals↗

PubMed2005

Correlation between mitotic delay and aberration burden, and their role for the analysis of chromosomal damage.

The aim was to investigate further the relationship between radiation-induced mitotic delay and the expression of chromosome damage in V79 cells. Recently published data on the time-course of chromosome aberrations in V79 first-cycle metaphases after exposure to 10.4 MeV u(-1) Ar ions (LET = 1226 keV microm(-1)) were supplemented and reanalysed. A statistical analysis of the distribution of aberrations among cells was performed. Furthermore, cells were grouped into subpopulations carrying 0, 1 -2, 3-4, 5- 6 and 7 or more aberrations. Then, based on the mitotic index, the flux of each subgroup through the first mitosis was determined and the average entrance time to mitosis was estimated. For comparison, the flux of aberrant V79 cells generated by X-irradiation was analysed. Analysis of the Ar ion data revealed that the flux of each subpopulation through the first mitosis is strongly affected by its aberration burden, i.e. a positive correlation between the mitotic delay and the number of aberrations carried by a cell was observed. The distribution of aberrations among cells could be well described by Neyman-type A statistics; the corresponding fit parameters also reflect the damage-dependent mitotic delay. Interestingly, comparison of the flux of Ar ion and X-ray-irradiated V79 cells through mitosis revealed (1) that a direct correlation exists between the number of aberrations carried by a cell and its average entrance time to mitosis, and (2) that this effect is independent of the linear energy transfer. The role of these observations for radiation cytogenetics is discussed.

Animals↗

PubMed2004

Aspects of the geographical variations of naturally occurring 210Pb/210Po in permanent teeth of juveniles in the UK.

PURPOSE: To study geographical variations in the level of naturally occurring 210Pb-supported 210Po in permanent teeth of juveniles in the UK. MATERIALS AND METHODS: Permanent teeth extracted from 278 juveniles for orthodontic purposes were obtained from 48 counties in the UK. 210Po activity concentration was measured on the outer enamel surface using TASTRAK alpha-particle-sensitive plastic track detectors. RESULTS: Geometric mean +/- SE activity concentrations in teeth from urban, suburban and rural areas, excluding the high radon area of Devon, were 8.41 + 0.25/-0.24, 7.76 + 0.37/-0.35 and 7.20 +0.49/-0.46 Bq kg(-1), respectively. Overall, there was no significant association between alpha-activity on the outer enamel surface of permanent teeth and proximity to the major UK motorways. However, when the data were considered with respect to the prevailing south-westerly wind on the western side of the UK, a statistically significant association with respect to donors living downwind (on the easterly side) of the motorways was found. This effect was greater for sections of the M5 and M6 motorways that traverse urban areas. 210Po levels in teeth were also associated with domestic radon concentration. This effect was comparable with that from traffic and urban pollution. CONCLUSIONS: Higher levels of 210Pb-supported 210Po are seen in permanent teeth of juveniles near sources of increased exposure in the UK. Inhalation uptake is an important pathway of exposure, especially with respect to domestic radon exposure. The results might be important in assessing integrated exposure to 210Po in the skeleton and consequent high linear energy transfer dose to bone marrow.

Adolescent↗

PubMed2004

Distribution of breakpoints and fragment sizes in human chromosome 5 after heavy-ion bombardment.

PURPOSE: To measure the location of heavy ion-induced residual breakpoints in human chromosome 5 and the size distribution of chromosome fragments involved in inter- or intrachromosomal exchanges. MATERIALS AND METHODS: Human peripheral blood lymphocytes were exposed to 4 Gy accelerated 56Fe (iron) ions (500 MeV per nucleon (MeV n(-1)), linear energy transfer=200 keV microm(-1)). Cells were then stimulated to grow in vitro for 48 h, and chromosomes were prematurely condensed by calyculin A. Chromosome 5 was painted using high-resolution multicolour banding. The location of the observed residual breakpoints and the size of all chromosome 5 fragments involved in structural aberrations were measured using dedicated image analysis software. RESULTS: Mapping of 283 breakpoints revealed a slight deviation from randomness, with an excess of breakpoints clustered in two small bands and an under representation of breaks at the telomeric end in the q-arm. Breakpoints per unit length were similar in p- and q-arms. The distribution of chromosome fragments has a maximum for very small fragments (< 10% of the chromosome size), indicating a severe fragmentation of chromosome 5 after heavy-ion bombardment. Only fragments < 40% of the chromosome size were involved in intrachromosomal exchanges (interstitial deletions or inversions), whereas fragments up to 75% of the whole chromosome 5 were found in interchromosomal exchanges. CONCLUSIONS: Residual breakpoints after exposure to high-energy iron ions were not distributed randomly along chromosome 5, although the p- and q-arms displayed similar radiosensitivity. Large fragments are either restituted or misrejoined to other chromosome ends, whereas small intrachromosomal fragments can produce either inter- or intrachromosomal exchanges.

Chromosome Breakage↗