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The nature of mutants induced by ionising radiation in cultured hamster cells. III. Molecular characterization of HPRT-deficient mutants induced by gamma-rays or alpha-particles showing that the majority have deletions of all or part of the hprt gene.

DNA from 58 independent HPRT-deficient mutants of V79 hamster cells induced by ionising radiation was analysed by Southern blot hybridization to a full-length hamster hprt cDNA. About half of the gamma-ray-induced mutants (20/43) were apparently total gene deletions, because they lacked all functional hprt gene sequences hybridizing to the cDNA probe. Another 10 mutants showed various partial deletions and/or rearrangements of the hprt gene. The remaining 13 mutants showed no detectable change in comparison to the structure of the normal gene, which correlated well with previous characterization of these mutants indicating that most carry point mutations in the hprt gene. However, it is probable that some of these point mutations occurred spontaneously rather than being radiation-induced. A smaller number of alpha-particle induced mutants gave similar results: out of a total of 15 mutants, 6 appeared to be total gene deletions, 5 had partial deletions and/or rearrangements, and 4 had no detectable changes. Thus, 70% or more of radiation-induced HPRT-deficient mutants arise through large genetic changes, especially deletions of all or part of the hprt gene. This result is to be contrasted with data published previously by ourselves and others indicating that the majority of spontaneous and ethyl methanesulphonate-induced mutations of hprt and similar genes arise by point mutation.

Alpha Particles↗

Formation of ionization clusters in nanometric structures of propane-based tissue-equivalent gas or liquid water by electrons and alpha-particles.

Despite the importance of ionization yield formation in sub-cellular structures a few nanometres in size, with regard to radiation damage our present knowledge in this respect is almost exclusively based on Monte Carlo simulations which in turn are based on cross section sets for water vapour or liquid water. Experimental data, although urgently needed, are still missing because the direct measurement of ionization yields in sub-cellular structures or, at least, in nanometric volumes of liquid water, is not yet possible. The best feasible way to overcome this problem of measurement at present, is the use of highly sophisticated counters filled with gases at low operating pressure to simulate target volumes a few nanometres in diameter at unit density. An indispensable prerequisite of the reliability of such measurements is, however, a check of the equivalence of the ionization yield produced in a specified target gas and the yield to be expected in liquid water or biological material. For this purpose, the ionization yield formation by electrons and alpha-particles in liquid water was simulated using the Monte Carlo method and compared with that produced in propane-based tissue-equivalent gas (composition by volume 55% C3H8, 39.6% CO2, 5.4% N2). After a short summary of the most important physical aspects of ionization cluster formation, new results are presented and discussed from the point of view of radiation physics and radiation biology.

Alpha Particles↗

Alpha-particle radiotherapy with 211At-labeled monodisperse polymer particles, 211At-labeled IgG proteins, and free 211At in a murine intraperitoneal tumor model.

Four different chemical forms of the alpha-particle emitting radionuclide 211At were injected intraperitoneally in mice inoculated intraperitoneally 30 hr in advance with 10(6) cells of the K13 murine hybridoma cell line. The different 211At forms were (a) free 211At, (b) 211At-labeled TP-3 nonspecific monoclonal antibody (211At-TP-3), (c) 211At-labeled human IgG kappa (211At-hIgG kappa), and (d) 211At-labeled monodisperse polymer particles (211At-MDPP). A significantly prolonged survival (P < 0.05) was observed with injected doses down to 7 kBq for the 211At-MDPP, and down to 25 kBq for 211At-hIgG kappa. There were no significant differences in survival between 211At-MDPP, 211At-hIgG kappa, and 211At-TP-3 at the dose level of 200 kBq. The group receiving 250 kBq free 211At per animal had a shorter survival than the three other forms at 200 kBq. The groups treated with 500, 200, and 65 kBq 211At-MDPP had a similar survival. The group given the highest dose of 211At-hIgG kappa (275 kBq) had the highest fraction (50%) of long-term survivors of all groups. Biodistribution measurements and total body scintigrams in mice without tumor revealed that the free 211At was distributed all over the body within 10 min after injection while at 2 hr a high fraction of the 211At-TP-3 and 211At-hIgG kappa was still present intraperitoneally. In conclusion this study indicates that 211At-labeled MDPP and 211At-labeled IgG's may be efficient tools for treatment of intraperitoneal superficial tumor cells and malignant ascites.

Animals↗

DNA-lesion and cell death by alpha-particles and nitrogen ions.

When the natural logarithm of the surviving fraction is plotted against the dose of radiation, curves with shoulders at relatively high survival levels are obtained after gamma-rays. The curves were practically linear in case of HMV-I and HA-1 cells irradiated by charged particle beams. These cells were derived from human malignant melanoma and Chinese hamster cells, respectively. The amount of DNA single strand breaks (ssb) by gamma-rays or nitrogen-ions (LET=530KeV/micrometers) in HMV-I cells increases linearly with increment in dose, when the ssb is detected using the alkaline elution technique. There is no close relationship between the dose-response curve of the ssb and the dose-survival curves after gamma-rays or N-ions. The amount of DNA double strand breaks (dsb) by gamma-rays increases quadratically with increment of dose, in both HMV-I cells and HA-1 cells, when the dsb is detected using the neutral elution technique. The survival fraction for HA-1 cells is slightly higher than that for HMV-I cells, at the same dose, and the amount of dsb for HA-1 cells is considerably greater than that for HMV-I cells. These results suggest that the radiosensitivities to gamma-rays in different cell lines do not correspond to the number of DNA strand breaks. The amount of both non-repairable ssb and dsb also increases quadratically with increment of dose for gamma-rays and almost linearly with increment of dose for N-ions and alpha-particles (LET=36keV/micrometers for HA-1 cells and LET=77keV/micrometers for HMV-I cells). The dose-response curves for non-repairable dsb in case of these radiations seemed to mirror image the dose-survival curves for these radiations, in both cell lines. The number of non-repairable DNA strand breaks in the two cell lines, at the same level of survival was much the same. These results show the close relationship between the induction of non-repairable DNA strand breaks and cell killing.

Alpha Particles↗

Interaction of alpha particles with bronchial cells.

The alpha-activity on the bronchial airways has been calculated for 222Rn daughter exposures producing observable excess bronchogenic lung cancer in underground miners. The activity distribution of aerosol particles with attached 222Rn daughters on the bronchial tree is truly diffuse because of the short half-life of the daughters and the large number of particles in the ambient aerosol. From the bronchial airway activity and the minor epidemiology, it can be shown that it requires, on average, 4 X 10(9) stem cells in bronchial epithelium to be hit in order to produce an observed lung cancer. For very high 222Rn daughter exposures of miners, multiply hit cells are highly probable; yet the lung cancer response is lower per unit exposure at high exposures than for mining exposures--near those sustained in the environment probably due to stem cell death. A knowledge of the number of multiply hit cells in miners permits some infererences to be made about the effectiveness of particulate versus diffusely distributed alpha emitters in the lung, namely, that particulates should not be significantly more effective in lung cancer induction than a diffuse distribution.

Air Pollution, Radioactive↗

Standardisation of low-activity actinide solutions by alpha-particle counting at a defined solid angle.

In the frame of an IAEA co-ordinated research project 232U, 236Pu and 229Th tracers were standardised by alpha-particle counting at a defined solid angle. The aim of this project was to assign property values that are traceable to the International System of Units (SI). This article depicts the standardisation of the tracers, elaborating on problems related to low activity and interference from daughter nuclides. The activity concentrations of 232U, 236Pu and 229Th were found to be, respectively (734+/-4), (142.0+/-0.9) and (528.2+/-2.6) Bq g(-1), at reference date (1 January 2003).

Journal Article↗

Experimental detection of alpha-particles from the radioactive decay of natural bismuth.

The only naturally occurring isotope of bismuth, 209Bi, is commonly regarded as the heaviest stable isotope. But like most other heavy nuclei abundant in nature and characterized by an exceptionally long lifetime, it is metastable with respect to alpha-decay. However, the decay usually evades observation because the nuclear structure of 209Bi gives rise to an extremely low decay probability and, moreover, generates low-energy alpha-particles difficult to detect. Indeed, dedicated experiments attempting to record the alpha-decay of 209Bi in nuclear emulsions failed. However, scintillating bolometers operated at temperatures below 100 mK offer improved detection efficiency and sensitivity, whereas a broad palette of targets could be available. Here we report the successful use of this method for the unambiguous detection of 209Bi alpha-decay in bismuth germanate detectors cooled to 20 mK. We measure an energy release of 3,137 +/- 1 (statistical) +/- 2 (systematic) keV and a half-life of (1.9 +/- 0.2) x 10(19) yr, which are in agreement with expected values.

Journal Article↗

The biological effects of Auger electrons compared to alpha-particles and Li ions.

The present study reports the results of V-79 Chinese hamster cell survival studies in which Auger electron emission was stimulated in gadolinium (Gd) after thermal neutron capture. When a porphyrin that had previously been labeled with boron (10BOPP) was also labeled with Gd (Gd-10BOPP), the cells were incubated with Gd-10BOPP to assess the compound's ability to physiologically transport the Gd into the cell, and localize the Gd atoms in or near the cell's critical target, presumably the DNA. It was anticipated that Auger electron emission, stimulated during the 157Gd (n, gamma)158Gd interaction, would impart additional high LET damage to that observed from the alpha-particle and Li ion during the 10B(n, alpha) 7Li reaction. Following irradiation with thermal neutrons from the Brookhaven Medical Research Reactor, the effectiveness of the Auger electrons was determined by comparing the response of cells incubated with 10BOPP, where damage was imparted by the boron neutron capture (BNC) products, to that from Gd-10BOPP, with equal concentration of 10B in both solutions. An Auger effectiveness factor of approximately 2 was found for the Gd-10BOPP cells. The Auger effectiveness observed with Gd strongly suggested that the 10BOPP molecule physiologically transported the Gd3+ ion intracellularly where it probably bound to DNA. Others have reported that Gd3+ does, in fact, complex with DNA. While depositing less energy per interaction than the high LET BNC reaction by-products, Auger electron ionization was more effective.

Animals↗

N-succinimidyl 3-[211At]astato-4-guanidinomethylbenzoate: an acylation agent for labeling internalizing antibodies with alpha-particle emitting 211At.

The objective of this study was to develop a method for labeling internalizing monoclonal antibodies (mAbs) such as those reactive to the anti-epidermal growth factor receptor variant III (EGFRvIII) with the alpha-particle emitting radionuclide (211)At. Based on previous work utilizing the guanidine-containing acylation agent, N-succinimidyl 4-guanidinomethyl-3-[(131)I]iodobenzoate ([(131)I]SGMIB), we have now investigated the potential utility of its astato analogue for labeling the anti-EGFRvIII mAb L8A4. N-succinimidyl 3-[(211)At]astato-4-guanidinomethylbenzoate ([(211)At]SAGMB) in its Boc-protected form was prepared from a tin precursor in 61.7 +/- 13.1% radiochemical yield, in situ deprotected to [(211)At]SAGMB, which was coupled to L8A4 in 36.1 +/- 1.9% yield. Paired-label internalization assays demonstrated that tumor cell retention of radioactivity for L8A4 labeled using [(211)At]SAGMB was almost identical to L8A4 labeled using [(131)I]SGMIB, and 3-4-fold higher than for mAb radioiodinated using Iodogen. Paired-label biodistribution of L8A4 labeled using [(211)At]SAGMB and [(131)I]SGMIB in athymic mice hosting U87MGdeltaEGFR xenografts resulted in identical uptake of both (211)At and (131)I in tumor tissues over 24 h. Although higher levels of (211)At compared with (131)I were sometimes seen in tissues known to sequester free astatide, these (211)At/(131)I uptake ratios were considerably lower than those seen with other labeling methods. These results suggest that [(211)At]SAGMB may be a useful acylation agent for labeling internalizing mAbs with (211)At.

Acylation↗

The characteristics of a wire-plane corona streamer detector when an alpha-particle source is moved in a plane parallel to the cathode.

The operation characteristics of a wire-plane corona streamer detector (WPCSD) in open air were investigated for broad side irradiation. Investigations were made on the counting characteristics in relation to their dependence on various anode diameters and source-anode spacing. The onset voltages for the corona mode Vo as well as for the spark mode Vp were determined. For each wire diameter a streamer mode (Vp - Vo) was found. The sensitivity of the WPCSD was studied when a collimated beam of a-particles was moved parallel to the plane of the cathode from the anode-wire toward the cathode. In addition, the pulse height spectra of alpha-particles incident on the detector for different values of the anode voltage, Va, were determined and studied. A qualitative interpretation of the experimental data was given.

Journal Article↗

Autoradiography: technique for drastic reduction of exposure time to alpha particles.

High-speed, gross, alpha autoradiographs can be made if silver-activated zinc sulfide is used as an intensifier in conjunction with high-speed film. The intensifier is interposed between the sample and film. This technique requires about 1/1000 of the exposure time required with Kodak NTB plates. The gross autoradiographs have greater contrast but slightly less resolution than conventional plates.

Animals↗