Department of Radiation Physics, The University of Texas MD Anderson Cancer Center, Houston, Texas 77030 and The University of Texas Graduate School of Biomedical Sciences at Houston, Houston, Texas 77030.
Med Phys. 2013 Nov;40(11):112102. doi: 10.1118/1.4824915.
The aim of this work was to create a mailable phantom with measurement accuracy suitable for Radiological Physics Center (RPC) audits of high dose-rate (HDR) brachytherapy sources at institutions participating in National Cancer Institute-funded cooperative clinical trials. Optically stimulated luminescence dosimeters (OSLDs) were chosen as the dosimeter to be used with the phantom.
The authors designed and built an 8 × 8 × 10 cm(3) prototype phantom that had two slots capable of holding Al2O3:C OSLDs (nanoDots; Landauer, Glenwood, IL) and a single channel capable of accepting all (192)Ir HDR brachytherapy sources in current clinical use in the United States. The authors irradiated the phantom with Nucletron and Varian (192)Ir HDR sources in order to determine correction factors for linearity with dose and the combined effects of irradiation energy and phantom characteristics. The phantom was then sent to eight institutions which volunteered to perform trial remote audits.
The linearity correction factor was kL = (-9.43 × 10(-5) × dose) + 1.009, where dose is in cGy, which differed from that determined by the RPC for the same batch of dosimeters using (60)Co irradiation. Separate block correction factors were determined for current versions of both Nucletron and Varian (192)Ir HDR sources and these vendor-specific correction factors differed by almost 2.6%. For the Nucletron source, the correction factor was 1.026 [95% confidence interval (CI) = 1.023-1.028], and for the Varian source, it was 1.000 (95% CI = 0.995-1.005). Variations in lateral source positioning up to 0.8 mm and distal∕proximal source positioning up to 10 mm had minimal effect on dose measurement accuracy. The overall dose measurement uncertainty of the system was estimated to be 2.4% and 2.5% for the Nucletron and Varian sources, respectively (95% CI). This uncertainty was sufficient to establish a ± 5% acceptance criterion for source strength audits under a formal RPC audit program. Trial audits of four Nucletron sources and four Varian sources revealed an average RPC-to-institution dose ratio of 1.000 (standard deviation = 0.011).
The authors have created an OSLD-based (192)Ir HDR brachytherapy source remote audit tool which offers sufficient dose measurement accuracy to allow the RPC to establish a remote audit program with a ± 5% acceptance criterion. The feasibility of the system has been demonstrated with eight trial audits to date.
本研究旨在创建一种可邮寄的模体,其测量精度适合参加美国国立癌症研究所资助的合作临床试验的机构中的放射物理中心(RPC)对高剂量率(HDR)近距离放射治疗源的审核。作者选择光激励发光剂量计(OSLD)作为与模体一起使用的剂量计。
作者设计并制造了一个 8×8×10cm3 的原型模体,该模体有两个插槽,能够容纳 Al2O3:C OSLD(nanoDots;Landauer,Glenwood,IL)和一个能够容纳美国当前临床使用的所有(192)Ir HDR 近距离放射治疗源的单个通道。作者用 Nucletron 和 Varian(192)Ir HDR 源对该模体进行了辐照,以确定剂量线性度和辐照能量与模体特性综合影响的校正因子。然后,该模体被送到八家自愿进行远程试用审核的机构。
线性度校正因子为 kL=(-9.43×10(-5)×剂量)+1.009,其中剂量以 cGy 为单位,这与使用(60)Co 辐照时 RPC 为同一批剂量计确定的校正因子不同。为当前版本的 Nucletron 和 Varian(192)Ir HDR 源分别确定了单独的块校正因子,这些特定于供应商的校正因子相差近 2.6%。对于 Nucletron 源,校正因子为 1.026[95%置信区间(CI)=1.023-1.028],而对于 Varian 源,校正因子为 1.000(95%CI=0.995-1.005)。侧向源定位偏差高达 0.8mm 和远侧/近侧源定位偏差高达 10mm 对剂量测量精度的影响很小。该系统的总体剂量测量不确定度估计分别为 Nucletron 和 Varian 源的 2.4%和 2.5%(95%CI)。这一不确定度足以在正式的 RPC 审核程序下为源强度审核建立±5%的可接受标准。对四个 Nucletron 源和四个 Varian 源的试用审核显示,RPC 与机构之间的平均剂量比为 1.000(标准差=0.011)。
作者已经创建了一种基于 OSLD 的(192)Ir HDR 近距离放射治疗源远程审核工具,该工具具有足够的剂量测量精度,使 RPC 能够建立一个具有±5%可接受标准的远程审核程序。迄今为止,该系统的可行性已通过八项试用审核得到证明。