Inaniwa Taku, Kanematsu Nobuyuki, Matsufuji Naruhiro, Kanai Tatsuaki, Shirai Toshiyuki, Noda Koji, Tsuji Hiroshi, Kamada Tadashi, Tsujii Hirohiko
Medical Physics Research Group, Research Center for Charged Particle Therapy, National Institute of Radiological Sciences, 4-9-1 Anagawa, Inage-ku, Chiba 263-8555, Japan.
Phys Med Biol. 2015 Apr 21;60(8):3271-86. doi: 10.1088/0031-9155/60/8/3271. Epub 2015 Mar 31.
At the National Institute of Radiological Sciences (NIRS), more than 8,000 patients have been treated for various tumors with carbon-ion (C-ion) radiotherapy in the past 20 years based on a radiobiologically defined clinical-dose system. Through clinical experience, including extensive dose escalation studies, optimum dose-fractionation protocols have been established for respective tumors, which may be considered as the standards in C-ion radiotherapy. Although the therapeutic appropriateness of the clinical-dose system has been widely demonstrated by clinical results, the system incorporates several oversimplifications such as dose-independent relative biological effectiveness (RBE), empirical nuclear fragmentation model, and use of dose-averaged linear energy transfer to represent the spectrum of particles. We took the opportunity to update the clinical-dose system at the time we started clinical treatment with pencil beam scanning, a new beam delivery method, in 2011. The requirements for the updated system were to correct the oversimplifications made in the original system, while harmonizing with the original system to maintain the established dose-fractionation protocols. In the updated system, the radiation quality of the therapeutic C-ion beam was derived with Monte Carlo simulations, and its biological effectiveness was predicted with a theoretical model. We selected the most used C-ion beam with αr = 0.764 Gy(-1) and β = 0.0615 Gy(-2) as reference radiation for RBE. The C-equivalent biological dose distribution is designed to allow the prescribed survival of tumor cells of the human salivary gland (HSG) in entire spread-out Bragg peak (SOBP) region, with consideration to the dose dependence of the RBE. This C-equivalent biological dose distribution is scaled to a clinical dose distribution to harmonize with our clinical experiences with C-ion radiotherapy. Treatment plans were made with the original and the updated clinical-dose systems, and both physical and clinical dose distributions were compared with regard to the prescribed dose level, beam energy, and SOBP width. Both systems provided uniform clinical dose distributions within the targets consistent with the prescriptions. The mean physical doses delivered to targets by the updated system agreed with the doses by the original system within ± 1.5% for all tested conditions. The updated system reflects the physical and biological characteristics of the therapeutic C-ion beam more accurately than the original system, while at the same time allowing the continued use of the dose-fractionation protocols established with the original system at NIRS.
在日本国立放射科学研究所(NIRS),过去20年里,基于放射生物学定义的临床剂量系统,已有8000多名患者接受了碳离子(C离子)放射治疗以治疗各种肿瘤。通过临床经验,包括广泛的剂量递增研究,已为各肿瘤建立了最佳剂量分割方案,这些方案可被视为C离子放射治疗的标准。尽管临床剂量系统的治疗适宜性已通过临床结果得到广泛证明,但该系统存在一些过度简化之处,如与剂量无关的相对生物效应(RBE)、经验性核碎裂模型以及使用剂量平均线能量转移来表示粒子谱。2011年,当我们开始使用笔形束扫描这种新的束流输送方法进行临床治疗时,我们借此机会更新了临床剂量系统。更新后的系统要求纠正原系统中的过度简化之处,同时与原系统协调一致,以维持已确立的剂量分割方案。在更新后的系统中,治疗用C离子束的辐射质量通过蒙特卡罗模拟得出,其生物效应通过理论模型进行预测。我们选择最常用的αr = 0.764 Gy(-1)且β = 0.0615 Gy(-2)的C离子束作为RBE的参考辐射。等效C生物剂量分布的设计旨在使人类唾液腺(HSG)肿瘤细胞在整个扩展布拉格峰(SOBP)区域达到规定的存活率,同时考虑RBE的剂量依赖性。这种等效C生物剂量分布按比例缩放到临床剂量分布,以与我们的C离子放射治疗临床经验相协调。使用原临床剂量系统和更新后的临床剂量系统制定治疗计划,并就规定剂量水平、束流能量和SOBP宽度比较了物理剂量分布和临床剂量分布。两个系统在靶区内均提供了与处方一致的均匀临床剂量分布。在所有测试条件下,更新后的系统输送到靶区的平均物理剂量与原系统的剂量在±1.5%范围内一致。更新后的系统比原系统更准确地反映了治疗用C离子束的物理和生物学特性;与此同时,它还允许继续使用NIRS原系统确立的剂量分割方案。