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优化用于测量质子放射治疗过程中发射的瞬发伽马射线的三阶段康普顿相机。

Optimizing a three-stage Compton camera for measuring prompt gamma rays emitted during proton radiotherapy.

机构信息

Department of Radiation Physics, Unit 94, The University of Texas M D Anderson Cancer Center, 1515 Holcombe Blvd., Houston, TX 77030, USA.

出版信息

Phys Med Biol. 2010 Nov 21;55(22):6841-56. doi: 10.1088/0031-9155/55/22/015. Epub 2010 Nov 3.

Abstract

In this work, we investigate the use of a three-stage Compton camera to measure secondary prompt gamma rays emitted from patients treated with proton beam radiotherapy. The purpose of this study was (1) to develop an optimal three-stage Compton camera specifically designed to measure prompt gamma rays emitted from tissue and (2) to determine the feasibility of using this optimized Compton camera design to measure and image prompt gamma rays emitted during proton beam irradiation. The three-stage Compton camera was modeled in Geant4 as three high-purity germanium detector stages arranged in parallel-plane geometry. Initially, an isotropic gamma source ranging from 0 to 15 MeV was used to determine lateral width and thickness of the detector stages that provided the optimal detection efficiency. Then, the gamma source was replaced by a proton beam irradiating a tissue phantom to calculate the overall efficiency of the optimized camera for detecting emitted prompt gammas. The overall calculated efficiencies varied from ∼ 10(-6) to 10(-3) prompt gammas detected per proton incident on the tissue phantom for several variations of the optimal camera design studied. Based on the overall efficiency results, we believe it feasible that a three-stage Compton camera could detect a sufficient number of prompt gammas to allow measurement and imaging of prompt gamma emission during proton radiotherapy.

摘要

在这项工作中,我们研究了使用三阶段康普顿相机来测量接受质子束放射治疗的患者发出的次级瞬发伽马射线。本研究的目的是:(1) 开发一种专门设计用于测量组织中发出的瞬发伽马射线的最佳三阶段康普顿相机;(2) 确定使用这种优化的康普顿相机设计来测量和成像质子束辐照期间发出的瞬发伽马射线的可行性。三阶段康普顿相机在 Geant4 中建模为三个高纯锗探测器阶段,以平行平面几何排列。最初,使用各向同性伽马源,范围从 0 到 15 MeV,以确定提供最佳检测效率的探测器阶段的横向宽度和厚度。然后,用质子束照射组织模型来代替伽马源,以计算优化相机检测发射瞬发伽马的整体效率。对于所研究的几种最佳相机设计的变化,整体计算效率从每个入射到组织模型的质子检测到的约 10(-6)到 10(-3)个瞬发伽马不等。基于整体效率结果,我们认为三阶段康普顿相机有可能检测到足够数量的瞬发伽马射线,从而允许在质子放射治疗期间测量和成像瞬发伽马发射。

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