Robinson D, Scrimger J W, Field G C, Fallone B G
Department of Medical Physics, Cross Cancer Institute, Edmonton, Alberta, Canada.
Med Phys. 2000 Oct;27(10):2380-4. doi: 10.1118/1.1308281.
Tomotherapy presents an evolutionary modality that holds forth the promise of better dose conformation to tumor volumes with a concomitant reduction in radiation-induced damage to surrounding normal structures. This delivery technique also presents a new set of radiation protection challenges that impact upon the design of the shielding vault required to house such a unit. A formalism is presented to determine the requisite amounts of shielding for both the primary beam and leakage radiation associated with a generic tomotherapy unit. A comparison is made with the shielding requirements for a conventional linear accelerator operated in a standard manner. Substantial differences in the amount of both primary and secondary shielding are indicated. A tomotherapy primary beam shield is both reduced in width by a factor of almost 10 and increased in thickness by more than a tenth value layer in comparison to a conventional accelerator. Furthermore, the secondary shielding requirements are enhanced by more than two tenth value layers with respect to conventional shielding demands.
断层放射治疗是一种具有革命性的治疗方式,有望更好地使剂量与肿瘤体积相匹配,同时减少对周围正常组织的辐射损伤。这种放疗技术也带来了一系列新的辐射防护挑战,影响着容纳该设备所需屏蔽室的设计。本文提出了一种形式主义方法,以确定与通用断层放射治疗设备相关的原射线束和泄漏辐射所需的屏蔽量。并与以标准方式运行的传统直线加速器的屏蔽要求进行了比较。结果表明,原屏蔽和二次屏蔽的量存在显著差异。与传统加速器相比,断层放射治疗的原射线束屏蔽宽度几乎缩小了10倍,厚度增加了超过十分之一半价层。此外,二次屏蔽要求比传统屏蔽要求增加了两个以上的半价层。