Phantom size in brachytherapy source dosimetric studies

An important point to consider in a brachytherapy dosimetry study is the phantom size involved in calculations or experimental measurements. As pointed out by Williamson [Med. Phys. 18, 776–786 (1991)] this topic has a relevant influence on final dosimetric results. Presently, one-dimensional (1-D)...

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Veröffentlicht in:Medical physics (Lancaster) 2004-07, Vol.31 (7), p.2075-2081
Hauptverfasser: Pérez-Calatayud, J., Granero, D., Ballester, F.
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Sprache:eng
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Zusammenfassung:An important point to consider in a brachytherapy dosimetry study is the phantom size involved in calculations or experimental measurements. As pointed out by Williamson [Med. Phys. 18, 776–786 (1991)] this topic has a relevant influence on final dosimetric results. Presently, one-dimensional (1-D) algorithms and newly-developed 3-D correction algorithms are based on physics data that are obtained under full scatter conditions, i.e., assumed infinite phantom size. One can then assume that reference dose distributions in source dosimetry for photon brachytherapy should use an unbounded phantom size rather than phantom-like dimensions. Our aim in this paper is to study the effect of phantom size on brachytherapy for radionuclide 137 Cs , 192 Ir , 125 I and 103 Pd , mainly used for clinical purposes. Using the GEANT4 Monte Carlo code, we can ascertain effects on derived dosimetry parameters and functions to establish a distance dependent difference due to the absence of full scatter conditions. We have found that for 137 Cs and 192 Ir , a spherical phantom with a 40 cm radius is the equivalent of an unbounded phantom up to a distance of 20 cm from the source, as this size ensures full scatter conditions at this distance. For 125 I and 103 Pd , the required radius for the spherical phantom in order to ensure full scatter conditions at 10 cm from the source is R=15  cm . A simple expression based on fits of the dose distributions for various phantom sizes has been developed for 137 Cs and 192 Ir in order to compare the dose rate distributions published for different phantom sizes. Using these relations it is possible to obtain radial dose functions for unbounded medium from bounded phantom ones.
ISSN:0094-2405
2473-4209
DOI:10.1118/1.1759826