PubMed · 13463674
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C FELDMAN. 1957. Bilayer bichromatic cathode screen.. https://doi.org/10.1364/josa.47.000790
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The properties of several directly polarized radioluminescent light (RL) sources are described. The RL sources are composed of a [small beta]-particle-emitting (90)Sr radioisotope coupled to polarization-oriented light-emitting plastic scintillators. The polarization of the scintillator molecules was achieved through a mechanical stress applied to the polymer matrix. The emission stability of the RL sources is described. It was found that the degree of polarization of light emitted by the sources varied from zero to 26%, depending on the matrix and scintillating material. The RL source with the highest degree of polarization was constructed from polystyrene and anthracene.
A radioactive ion beam like 9C serves as a double radiation source and may be useful in cancer treatment, where the essential irradiation comes from the external beam itself and the extra one is due to the low-energy particles emitted internally during the decay of 9C. Based on the microdosimetric specific energy spectrum in cell nuclei, a model to evaluate the biological effect induced by the internally emitted particles from a beta-delayed particle decay beam has been developed. In this paper, using this model the additional contributions to the cell-killing effect due to the emitted particles from stopping 9C ions were incorporated in the design of spread-out Bragg peaks (SOBP) for radioactive 9C beams. For this purpose, a simulated annealing algorithm was employed to optimize the superposing weighting fractions of all monoenergetic beams so that a uniform cell survival level could be realized across the SOBP within an acceptable deviation of 5%. SOBPs with different widths and at different cell survival levels were designed for both therapeutic 9C and 12C beams for comparison. The potential use of the 9C beam in radiotherapy compared to the 12C beam, which is commonly adopted in the practices of current heavy-ion therapy, is shown systematically in terms of the distributions of biological effective dose and cell survival along the beam penetration.
Electron backscattering is a prominent secondary effect in beta dosimetry, and is closely correlated with factors such as the geometries of the source and the scattering material, as well as the composition of the scattering material. Previous results were varied depending on the experimental setup and detector resolution, and were generally performed for monoenergetic electron beams, which makes direct application of these factors to beta sources difficult. In this work, backscattering factors were calculated with MCNP 4C for selected beta sources currently in use (32P and 90Sr/90Y) as well as for sources of potential therapeutic use (45Ca, 142Pr and 185W). Specifically, the calculations used beta spectra generated by the SADDE MOD2 code. The factors were calculated as a function of the distance from the interface between water and scatterers. The scatterers include source surroundings, source supporting materials and contrast agents commonly used for imaging purposes in brachytherapy. The results were fit by a simple function for future incorporation into a dose point kernel code. Due to the high-Z material content (iodine, Z = 53) in the contrast agent, a significant dose backscatter was observed near the water interface. Different cross-section algorithms in the MCNP code (inherent and ITS 3.0) affect the factor calculations. The results generated by the ITS 3.0 algorithm closely matched the EGS4 calculations for 32P. The dependence of backscatter factors on log(Z + 1) (Baily 1980 Med. Phys. 7514-9) was observed for all the beta sources with a high correlation coefficient, R (> 0.95). The overall results indicate that the backscattering effect is significant at short distances from the surface of the interface between water and the scattering material. This model can also aid in choosing a source support or mixing materials for beta brachytherapy sources.