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Cell killing and division delay in asynchronous and synchronized HeLa cells irradiated with alpha particles or X rays.

HeLa cells irradiated with a single or two split doses of alpha particles or X rays were observed with time-lapse photography or examined for their colony-forming ability. The cell cycle-dependent variation of cell killing and division delay were compared in synchronous and asynchronous cell populations. Cellular damage by alpha particles was manifested in the form of cessation of division, or death, rather than partial division which was predominant for X irradiation. Furthermore, an increased number of interrupted divisions leading to death following split doses correlated with the lack of production of reparable damage from alpha particles. As to the cell cycle-dependent variation of radiosensitivity, a somewhat different pattern was noted with alpha particles, especially for division delay. The pattern of cell killing with alpha particles was similar to that found with X rays, in that high sensitivity was noted at or close to mitosis, while a resistant peak remained at late S but not in early G1. The pattern of division delay was similar for X rays and alpha particles during G2-M, with a maximum delay at mid G2 and no delay past the transition point, but differed during G1-S. During this period, division delay increased with cell age, whereas it showed a broad peak at G1-S boundary and a trough at late S for X rays. There was a reverse correlation between division delay and cell killing except for G2-M in the case of X rays. However, such was not the case for alpha particles.

Alpha Particles↗

The oncogenic transforming potential of the passage of single alpha particles through mammalian cell nuclei.

Domestic, low-level exposure to radon gas is considered a major environmental lung-cancer hazard involving DNA damage to bronchial cells by alpha particles from radon progeny. At domestic exposure levels, the relevant bronchial cells are very rarely traversed by more than one alpha particle, whereas at higher radon levels-at which epidemiological studies in uranium miners allow lung-cancer risks to be quantified with reasonable precision-these bronchial cells are frequently exposed to multiple alpha-particle traversals. Measuring the oncogenic transforming effects of exactly one alpha particle without the confounding effects of multiple traversals has hitherto been unfeasible, resulting in uncertainty in extrapolations of risk from high to domestic radon levels. A technique to assess the effects of single alpha particles uses a charged-particle microbeam, which irradiates individual cells or cell nuclei with predefined exact numbers of particles. Although previously too slow to assess the relevant small oncogenic risks, recent improvements in throughput now permit microbeam irradiation of large cell numbers, allowing the first oncogenic risk measurements for the traversal of exactly one alpha particle through a cell nucleus. Given positive controls to ensure that the dosimetry and biological controls were comparable, the measured oncogenicity from exactly one alpha particle was significantly lower than for a Poisson-distributed mean of one alpha particle, implying that cells traversed by multiple alpha particles contribute most of the risk. If this result applies generally, extrapolation from high-level radon risks (involving cellular traversal by multiple alpha particles) may overestimate low-level (involving only single alpha particles) radon risks.

Alpha Particles↗

Alpha-particle energy loss measurement of microgram depositions of biomolecules.

A commercially available alpha-particle spectrometer and 210Po alpha-particle source were used to determine the mass of microgram quantities of biomolecules. Samples were deposited in microliter volumes on thin silicon nitride windows and dried. The energy loss of the alpha-particles after traversing the sample was converted to a mass using tabulated alpha-particle stopping powers. The measurement was absolute, independent of biomolecule species, and no standards were needed for quantitation. The method has a dynamic range of 0.1-100 microg for deposits of diameter 1-2 mm. The precision varies from approximately 20% at 100 ng to a few percent at 5-100 microg. The silicon nitride windows allow multimodal analysis of the same quantified sample, including PIXE probing of elemental abundances, molecular identification by mass spectrometry, and isotopic quantitation of interactions. The method was used with accelerator mass spectrometry to quantify specific activities of microgram quantities of 14C-labeled proteins.

Alpha Particles↗

Unfolding of polonium distribution in depth of irradiated lead-bismuth eutectic from alpha-particle pulse-height distribution.

The alpha-particle pulse-height distribution measured from irradiated LBE is determined from the polonium distribution in it. The unfolding of vertical polonium distribution in irradiated LBE ingot is performed with the unfolding code UFOQ. The code uses quadratic programming to consider the constraint that polonium distribution does not have negative values. The response function defined as normalized alpha-particle pulse-height distributions caused by alpha-particles emitted from polonium in surface region, which is divided vertically to thin layers, of LBE ingot is calculated by Monte Carlo method. The polonium distribution around surface of irradiated LBE ingot is obtained clearly with the response function calculated for the surface region divided narrowly. Also, the polonium distribution in deeper layer of the surface region is obtained consistently with the response function calculated for the surface region divided widely.

Journal Article↗

Absorbed fractions for alpha-particles in tissues of trabecular bone: considerations of marrow cellularity within the ICRP reference male.

UNLABELLED: Alpha-particles are of current interest in radionuclide therapy due to their short range and high rates of energy transfer to target tissues. Published values of alpha-particle absorbed fraction phi in the skeletal tissues, as needed for patient-specific dosimetry under the MIRD schema, do not generally account for its variation with particle energy or skeletal site. Furthermore, variations in alpha-particle absorbed fraction with marrow cellularity have yet to be fully considered. METHODS: In this study, a 3-dimensional (3D) chord-based radiation transport model (or 3D-CBIST) is presented, which combines (a) chord-based techniques for tracking alpha-particles across bone trabeculae, endosteum, and marrow cavities and (b) a spatial model of the marrow tissues that explicitly considers the presence of marrow adipocytes. Chord-length distributions are taken from a 44-y male subject (ICRP [International Commission on Radiological Protection] Reference Male) and are identical to those used currently for clinical dose estimates for beta-particle emitters. RESULTS: Values of phi(active marrow<--active marrow) given by the 3D-CBIST model are shown to be considerably lower than phi = 1.0 assumed under the ICRP Publication 30 and 2003 Eckerman bone models. For example, values of absorbed fraction for the self-dose to active bone marrow in the ribs, cervical vertebra, and parietal bone are 0.81, 0.80, and 0.55 for 6-MeV alpha-particles and are 0.74, 0.72, and 0.43 for 9-MeV alpha-particles, where each is evaluated at ICRP reference cellularities in the 3D-CBIST model (72%, 72%, and 42%, respectively, at age 25 y). CONCLUSION: Improvements in patient-specific dosimetry of skeletal tissues require explicit consideration of not only changes in target mass with variable patient marrow cellularity (i.e., active marrow) but also corresponding changes in values of the absorbed fraction. The data given in this study provide a more-firm basis for application of the MIRD schema to patient-specific dosimetry for newly developing therapies using alpha-particle emitters.

Adult↗

Targeted alpha particle immunotherapy for myeloid leukemia.

Unlike beta particle-emitting isotopes, alpha emitters can selectively kill individual cancer cells with a single atomic decay. HuM195, a humanized anti-CD33 monoclonal antibody, specifically targets myeloid leukemia cells and has activity against minimal disease. When labeled with the beta-emitters (131)I and (90)Y, HuM195 can eliminate large leukemic burdens in patients, but it produces prolonged myelosuppression requiring hematopoietic stem cell transplantation at high doses. To enhance the potency of native HuM195 yet avoid the nonspecific cytotoxicity of beta-emitting constructs, the alpha-emitting isotope (213)Bi was conjugated to HuM195. Eighteen patients with relapsed and refractory acute myelogenous leukemia or chronic myelomonocytic leukemia were treated with 10.36 to 37.0 MBq/kg (213)Bi-HuM195. No significant extramedullary toxicity was seen. All 17 evaluable patients developed myelosuppression, with a median time to recovery of 22 days. Nearly all the (213)Bi-HuM195 rapidly localized to and was retained in areas of leukemic involvement, including the bone marrow, liver, and spleen. Absorbed dose ratios between these sites and the whole body were 1000-fold greater than those seen with beta-emitting constructs in this antigen system and patient population. Fourteen (93%) of 15 evaluable patients had reductions in circulating blasts, and 14 (78%) of 18 patients had reductions in the percentage of bone marrow blasts. This study demonstrates the safety, feasibility, and antileukemic effects of (213)Bi-HuM195, and it is the first proof-of-concept for systemic targeted alpha particle immunotherapy in humans.

Alpha Particles↗

Electret ion chambers for estimating alpha particle energy.

Electret ion chambers (EICs) are inexpensive, lightweight, robust, commercially available, passive, charge-integrating devices for measuring different radiations. At Florida International University's Hemispheric Center for Environmental Technology (FIU-HCET), EIC performance was evaluated with the goal of providing the U.S. Department of Energy (DOE) with a low-cost, low-risk means of alpha contamination monitoring using an existing commercial technology. During this evaluation, sensitivity of electrets in 960-mL hemispherical ion chamber (radius: 7.6 cm) was observed to increase with alpha particle energy because alpha particles expended their entire energy in the chamber volume. This observation prompted us to explore another EIC application: estimation of alpha particle energy. Correlation between electret mid-point voltage, alpha particle energy, and response was developed for the 960-mL EIC and was used to determine energy of an unknown source. The response (change in voltage per disintegration) is the ratio of the change of voltage per unit time and alpha particle activity. Since an EIC measures only the change in voltage per minute, to determine the alpha particle energy, the source activity should be accurately determined by another method.

Alpha Particles↗

The average number of alpha-particle hits to the cell nucleus required to eradicate a tumour cell population.

Alpha-particle emitters are currently being considered for the treatment of micrometastatic disease. Based on in vitro studies, it has been speculated that only a few alpha-particle hits to the cell nucleus are considered lethal. However, such estimates do not consider the stochastic variations in the number of alpha-particle hits, energy deposited, or in the cell survival process itself. Using a tumour control probability (TCP) model for alpha-particle emitters, we derive an estimate of the average number of hits to the cell nucleus required to provide a high probability of eradicating a tumour cell population. In simulation studies, our results demonstrate that the average number of hits required to achieve a 90% TCP for 10(4) clonogenic cells ranges from 18 to 108. Those cells that have large cell nuclei, high radiosensitivities and alpha-particle emissions occurring primarily in the nuclei tended to require more hits. As the clinical implementation of alpha-particle emitters is considered, this type of analysis may be useful in interpreting clinical results and in designing treatment strategies to achieve a favourable therapeutic outcome.

Alpha Particles↗

Analysis of radiation risk from alpha particle component of solar particle events.

The solar particle events (SPE) will contain a primary alpha particle component, representing a possible increase in the potential risk to astronauts during an SPE over the often studied proton component. We discuss the physical interactions of alpha particles important in describing the transport of these particles through spacecraft and body shielding. Models of light ion reactions are presented and their effects on energy and linear energy transfer (LET) spectra in shielding discussed. We present predictions of particle spectra, dose, and dose equivalent in organs of interest for SPE spectra typical of those occurring in recent solar cycles. The large events of solar cycle 19 are found to have substantial increase in biological risk from alpha particles, including a large increase in secondary neutron production from alpha particle breakup.

Alpha Particles↗

Cellular dose conversion factors for alpha-particle--emitting radionuclides of interest in radionuclide therapy.

UNLABELLED: alpha-Particle--emitting radionuclides are of increasing interest in radionuclide therapy. The decay scheme of alpha-emitting radionuclides typically includes a chain of unstable progeny. It is generally assumed that alpha-particle emission by the parent radionuclide will break the chemical bond with its carrier molecule and that the resulting daughter atom will no longer be associated with the carrier molecule. If the daughter is very short lived, it will not have enough time to be carried any significant distance from the site of parent decay and a cellular, absorbed dose estimate must consider the energy deposited by the daughter as well as the parent. Depending on the site of parent decay and the expected removal rate of daughter atoms from this site, the contribution of emissions from longer-lived daughters may also be warranted. In this study, dose conversion factors (DCFs) for cellular dimensions that incorporate the fate of daughter radionuclides were derived for (225)Ac, (213)Bi, (211)At, and (223)Ra, the alpha-particle--emitting radionuclides of interest in radionuclide therapy. METHODS: The dose contribution of daughter radionuclides at the site of parent decay was made dependent on a cutoff time parameter, which was used to estimate the fraction of daughter decays expected at the site of parent decay. Previously tabulated S values (cell-surface to nucleus and cell-surface to cell) for each daughter in the decay scheme were scaled by this fraction and a sum over all daughters was performed to yield a cutoff time--dependent set of corresponding DCF values for each radionuclide. RESULTS: DCF values for the absorbed dose to the nuclear or cellular volume from cell-surface decays are presented as a function of the cutoff time for 4 different cellular and nuclear dimensions. CONCLUSION: In contrast to the cellular S values that account only for parent decay, the DCF values provided in this study make it possible to easily include the contribution of daughter decays in cellular alpha-particle emitter dose calculations.

Algorithms↗

Energy dependence of etch pit diameter in a CR-39 detector for alpha-particles with the energy from 1.29 to 5.48 MeV.

The characteristics for alpha-particle recording of CR-39 plastics was studied for practical use. Sample detectors were irradiated with alpha-particles at normal incident angle. The energy was varied from 1.29 to 5.48 MeV. Tracks of alpha-particles could sufficiently be recognized through the etch pit observation with 1 hour etching in 30% solution of NaOH at a temperature of 70 degrees C. The etch pit diameter decreased almost linearly with the energy of alpha-particles at the early stage of etching, which suggested the possibility of the estimation of alpha-particle energy. The energy resolution was evaluated from the FWHM of the measured distribution of etch pit diameters and found to be about 1.8 MeV for 1, 2 and 3 hour etching.

Alpha Particles↗

Alpha-particle-induced sister chromatid exchange in normal human lung fibroblasts: evidence for an extranuclear target.

We investigated the relationship between nuclear hits by alpha particles and the subsequent occurrence of sister chromatid exchanges (SCEs) in normal human diploid lung fibroblasts (HFL1). Cells were exposed to 238Pu alpha particles at doses ranging from 0.4-12.9 cGy and subsequently analyzed for SCEs. A significant increase in SCE frequency was observed even at the lowest dose examined. The extent of induction of SCEs in the HFL1 cells showed dose dependency in the very low dose range, i.e. 0.4-2.0 cGy. Thereafter, induction of SCEs was independent of dose. Based on measurements of the nuclear areas of the HFL1 cells in conjunction with target theory calculations, the lowest dose resulted in an approximately 8.6-fold increase in the percentage of cells showing excessive SCEs over the theoretically expected percentage of cells whose nuclei were calculated to be traversed by one or more alpha particles. The extent of the discrepancies between theoretically expected and experimentally observed frequencies of SCEs became progressively reduced with increasing radiation dose. We additionally determined that SCEs induced by the alpha particles have no significant dependency on the time of cell collection after exposure to a selected dose of alpha particles, thereby confirming that the differences between the theoretically predicted and observed SCE frequencies were not due to an artifact of the time of cell sampling for the SCE measurements. These results obtained with normal human cells are similar to those of other investigators who observed excessive SCEs in immortalized rodent cells beyond that which could be attributed exclusively to nuclear traversals by alpha particles. Such consistent findings point to the existence of an alternative, extranuclear target through which alpha particles cause DNA damage, as detected by SCE analysis. The existence of an extranuclear compartment as a target for alpha particles may have important implications for the susceptibility of lung cells to the DNA-damaging effects of alpha-particle exposure due to the inhalation of radon progeny.

Alpha Particles↗

Response of cultured human airway epithelial cells to X-rays and energetic alpha-particles.

Radon and its progeny, which emit alpha-particles during decay, may play an important role in inducing human lung cancer. To gain a better understanding of the biological effects of alpha-particles in human lung we studied the response of cultured human airway epithelial cells to X-rays and monoenergetic helium ions. Our experimental results indicated that the radiation response of primary cultures was similar to that for airway epithelial cells that were transformed with a plasmid containing an origin-defective SV40 virus. The RBE for cell inactivation determined by the ratio of D0 for X-rays to that for 8 MeV helium ions was 1.8-2.2. The cross-section for helium ions, calculated from the D0 value, was about 24 microm 2 for cells of the primary culture. This cross-section is significantly smaller than the average geometric nuclear area (approximately 180 microms 2), suggesting that an average of 7.5 alpha-particles (8 MeV helium ions) per cell nucleus are needed to induce a lethal lesion.

Alpha Particles↗

A new mechanism for DNA alterations induced by alpha particles such as those emitted by radon and radon progeny.

The mechanism(s) by which alpha (alpha) particles like those emitted from inhaled radon and radon progeny cause their carcinogenic effects in the lung remains unclear. Although direct nuclear traversals by alpha-particles may be involved in mediating these outcomes, increasing evidence indicates that a particles can cause alterations in DNA in the absence of direct hits to cell nuclei. Using the occurrence of excessive sister chromatid exchanges (SCE) as an index of DNA damage in human lung fibroblasts, we investigated the hypothesis that alpha-particles may induce DNA damage through the generation of extracellular factors. We have found that a relatively low dose of alpha-particles can result in the generation of extracellular factors, which, upon transfer to unexposed normal human cells, can cause excessive SCE to an extent equivalent to that observed when the cells are directly irradiated with the same irradiation dose. A short-lived, SCE-inducing factor(s) is generated in alpha-irradiated culture medium containing serum in the absence of cells. A more persistent SCE-inducing factor(s), which can survive freeze-thaw and is heat labile is produced by fibroblasts after exposure to the alpha-particles. These results indicate that the initiating target for alpha-particle-induced genetic changes can be larger than a cell's nucleus or even a whole cell. How transmissible factors like those observed here in vitro may extend to the in vivo condition in the context of a-particle-induced carcinogenesis in the respiratory tract remains to be determined.

Air Pollutants, Radioactive↗

Induction of micronuclei in a rat alveolar epithelial cell line by alpha particle irradiation.

Dose-response relationships for the induction of micronuclei were characterised in the rat alveolar epithelial cell line (SV40T2) exposed to either alpha particles(241Am: 3.2 MeV, 128 keV.micron-1, 0.093 Gy.min-1 at the cell-Mylar interface) or X rays (200 kVp, 1 Gy.min-1). The frequency of micronucleus formation was 1.6-3.0% for unirradiated subjects but increased for irradiated ones in a dose-dependent manner. A linear relationship between the dose and the micronucleus formation was observed until 1 Gy for alpha particles and 4 Gy for X rays. The linear slope for alpha particles was 28.5% per Gy and the relative biological effectiveness (RBE) was 4.3, as calculated from the slopes. The slope for alpha particles was dependent on the energy of the alpha particles. These results indicate that the micronucleus assay is available for biodosimetry of alpha particle irradiation in the rat alveolar epithelial cells, although consideration should be given to the range of the linearity and the LET of alpha particles.

Alpha Particles↗

A comparative study of rejoining of DNA double-strand breaks in yeast irradiated with 3.5 MeV alpha-particles or with 30 MeV electrons.

Yeast cells were irradiated with 3.5 MeV alpha-particles and 30 MeV electrons, as reference radiation. The kinetics of DNA double-strand break (dsb) rejoining during incubation of cells under non-growth conditions (PLDR conditions) were measured using the neutral sedimentation technique. A monophasic kinetic was found after irradiation of cells with alpha-particles, with a dose-independent t1/2 value of about 13 h. The kinetics of rejoining of dsb induced by 30 MeV electrons was found to be biphasic, with dose-independent t1/2 values of 3.8 h for the initial and of about 11 h for the slow component. The fraction of the slow component was, however, dose-dependent. These kinetics were measured for both types of radiation at doses yielding high surviving fractions (5% up to 100%). Dsb are induced linearly with dose of both radiations. The RBE value of alpha-particles was found to be 2.5 for initial dsb. The RBE of alpha-particles increased as a consequence of dsb rejoining. This increase in RBE value suggests that DSB may be primary lesions for chromosome aberrations, cellular inactivation and oncogenic transformation of mammalian cells which all exhibit high RBE values of alpha-particles.

Alpha Particles↗

[Rapid recovery in diploid yeast cells irradiated sequentially with fast electrons and alpha particles].

In the present work, fast repair after combined irradiation by fast electrons and alpha particles was studied in diploid yeast cells Saccharomyces cerevisiae of wild-type XS 800 and its radiosensitive mutant XS 1898. It was shown, that the fast repair significantly contribute to detected survival of the wild-type cells, while this repair is absent in XS 1898 mutant cells. An efficiency of the fast repair under combined irradiation (electrons + alpha particles), assessed on DMF of alpha particles, is lower, than that under irradiation by electrons and alpha particles separately.

Alpha Particles↗