Ohira Shingo, Isono Masaru, Ueda Yoshihiro, Hirata Takero, Ashida Reiko, Takahashi Hidenori, Miyazaki Masayoshi, Takashina Masaaki, Koizumi Masahiko, Teshima Teruki
1 Department of Radiation Oncology, Osaka Medical Center for Cancer and Cardiovascular Diseases, Osaka, Japan.
2 Department of Medical Physics and Engineering, Osaka University Graduate School of Medicine, Suita, Japan.
Br J Radiol. 2017 Apr;90(1072):20160815. doi: 10.1259/bjr.20160815. Epub 2017 Mar 3.
The volume of targets to which a high radiation dose can be delivered is limited for pancreatic radiotherapy. We assessed changes in movements of pancreatic tumours between simulation and treatment and determined compensatory margins.
For 23 patients, differences in implanted fiducial marker motion magnitude (MMM) and mean marker position (MMP) between four-dimensional CT and cone-beam CT were measured. Subsequently, residual uncertainty was simulated after no action level (NAL) and extended no action level (eNAL) protocols were adopted.
With no correction, respective 95th percentile of MMM were 4.5 mm, 6.2 mm and 16.0 mm and systematic (random) errors of MMP were 2.8 mm (3.3 mm), 3.2 mm (2.0 mm) and 5.9 mm (4.0 mm) in the left-right (L-R), anteroposterior (A-P) and superoinferior (S-I) directions, so that large margins were required (L-R, 10.5 mm; A-P, 11.7 mm; and S-I, 24.8 mm). NAL reduced systematic errors of MMP, but resultant margins remained large (L-R, 8.0 mm; A-P, 9.6 mm; and S-I, 18.1 mm). eNAL compensated for time trends and obtained minimal margins (L-R, 6.7 mm; A-P, 6.7 mm; and S-I, 15.2 mm).
Motion magnitude and position of pancreatic tumours during simulation are frequently not representative of that during treatment. eNAL compensated for systematic interfractional position change and would be a practical approach for improving targeting accuracy. Advances in knowledge: Considerably large margins, especially in the S-I direction, were required to compensate for intrafractional motion and interfractional position changes of the pancreatic tumour. An application of eNAL was an effective strategy to diminish these margins.
胰腺放疗中能够给予高辐射剂量的靶区体积有限。我们评估了模拟定位与治疗期间胰腺肿瘤运动的变化,并确定了补偿边界。
对23例患者,测量四维CT与锥形束CT之间植入的基准标记物运动幅度(MMM)和标记物平均位置(MMP)的差异。随后,在采用无行动水平(NAL)和扩展无行动水平(eNAL)方案后,模拟残余不确定性。
未进行校正时,在左右(L-R)、前后(A-P)和上下(S-I)方向上,MMM的第95百分位数分别为4.5毫米、6.2毫米和16.0毫米,MMP的系统误差(随机误差)分别为2.8毫米(3.3毫米)、3.2毫米(2.0毫米)和5.9毫米(4.0毫米),因此需要较大的边界(L-R为10.5毫米;A-P为11.7毫米;S-I为24.8毫米)。NAL减少了MMP的系统误差,但最终边界仍然很大(L-R为8.0毫米;A-P为9.6毫米;S-I为18.1毫米)。eNAL补偿了时间趋势并获得了最小边界(L-R为6.7毫米;A-P为6.7毫米;S-I为15.2毫米)。
模拟定位期间胰腺肿瘤的运动幅度和位置通常不能代表治疗期间的情况。eNAL补偿了分次间的系统位置变化,将是提高靶向准确性的一种实用方法。知识进展:需要相当大的边界,尤其是在S-I方向,以补偿胰腺肿瘤的分次内运动和分次间位置变化。应用eNAL是减小这些边界的有效策略。