Material efficiency studies for a Compton camera designed to measure characteristic prompt gamma rays emitted during proton beam radiotherapy

被引:38
|
作者
Robertson, Daniel [1 ,2 ]
Polf, Jerimy C. [1 ]
Peterson, Steve W. [3 ]
Gillin, Michael T. [1 ,2 ]
Beddar, Sam [1 ,2 ]
机构
[1] Univ Texas MD Anderson Canc Ctr, Dept Radiat Phys, Unit 94, Houston, TX 77030 USA
[2] Univ Texas Houston, Grad Sch Biomed Sci Houston, Houston, TX 77030 USA
[3] Univ Cape Town, Dept Phys, ZA-7701 Rondebosch, South Africa
来源
PHYSICS IN MEDICINE AND BIOLOGY | 2011年 / 56卷 / 10期
关键词
THERAPY; SYSTEM; IRRADIATION; EQUIVALENT; EMISSION; CARBON; FIELD;
D O I
10.1088/0031-9155/56/10/010
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
Prompt gamma rays emitted from biological tissues during proton irradiation carry dosimetric and spectroscopic information that can assist with treatment verification and provide an indication of the biological response of the irradiated tissues. Compton cameras are capable of determining the origin and energy of gamma rays. However, prompt gamma monitoring during proton therapy requires new Compton camera designs that perform well at the high gamma energies produced when tissues are bombarded with therapeutic protons. In this study we optimize the materials and geometry of a three-stage Compton camera for prompt gamma detection and calculate the theoretical efficiency of such a detector. The materials evaluated in this study include germanium, bismuth germanate (BGO), NaI, xenon, silicon and lanthanum bromide (LaBr(3)). For each material, the dimensions of each detector stage were optimized to produce the maximum number of relevant interactions. These results were used to predict the efficiency of various multi-material cameras. The theoretical detection efficiencies of the most promising multi-material cameras were then calculated for the photons emitted from a tissue-equivalent phantom irradiated by therapeutic proton beams ranging from 50 to 250 MeV. The optimized detector stages had a lateral extent of 10 x 10 cm(2) with the thickness of the initial two stages dependent on the detector material. The thickness of the third stage was fixed at 10 cm regardless of material. The most efficient single-material cameras were composed of germanium (3 cm) and BGO (2.5 cm). These cameras exhibited efficiencies of 1.15 x 10(-4) and 9.58 x 10(-5) per incident proton, respectively. The most efficient multi-material camera design consisted of two initial stages of germanium (3 cm) and a final stage of BGO, resulting in a theoretical efficiency of 1.26 x 10(-4) per incident proton.
引用
收藏
页码:3047 / 3059
页数:13
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