Chaudhari Suresh H, Dobhal Rishabh, Kinhikar Rajesh A, Kadam Sudarshan S, Deshpande Deepak D
Department of Radiation Oncology, Apollo Hospitals, Navi Mumbai, Maharashtra, India.
Department of Radiation Oncology, Batra Hospital and Medical Research Centre, New Delhi, India.
J Med Phys. 2017 Jan-Mar;42(1):9-13. doi: 10.4103/jmp.JMP_114_16.
Advanced radiotherapy modalities such as stereotactic radiosurgery (SRS) and image-guided radiotherapy may employ very small beam apertures for accurate localized high dose to target. Accurate measurement of small radiation fields is a well-known challenge for many dosimeters. The purpose of this study was to measure total scatter factors for stereotactic cones with plastic scintillation detector and its comparison against diode detector and theoretical estimates. Measurements were performed on Novalis Tx linear accelerator for 6MV SRS beam with stereotactic cones of diameter 6 mm, 7.5 mm, 10 mm, 12.5 mm, and 15 mm. The advantage of plastic scintillator detector is in its energy dependence. The total scatter factor was measured in water at the depth of dose maximum. Total scatter factor with plastic scintillation detector was determined by normalizing the readings to field size of 10 cm × 10 cm. To overcome energy dependence of diode detector for the determination of scatter factor with diode detector, daisy chaining method was used. The plastic scintillator detector was calibrated against the ionization chamber, and the reproducibility in the measured doses was found to be within ± 1%. Total scatter factor measured with plastic scintillation detector was 0.728 ± 0.3, 0.783 ± 0.05, 0.866 ± 0.55, 0.885 ± 0.5, and 0.910 ± 0.06 for cone sizes of 6 mm, 7.5 mm, 10 mm, 12.5 mm, and 15 mm, respectively. Total scatter factor measured with diode detector was 0.733 ± 0.03, 0.782 ± 0.02, 0.834 ± 0.07, 0.854 ± 0.02, and 0.872 ± 0.02 for cone sizes of 6 mm, 7.5 mm, 10 mm, 12.5 mm, and 15 mm, respectively. The variation in the measurement of total scatter factor with published Monte Carlo data was found to be -1.3%, 1.9%, -0.4%, and 0.4% for cone sizes of 7.5 mm, 10 mm, 12.5 mm, and 15 mm, respectively. We conclude that total scatter factor measurements for stereotactic cones can be adequately carried out with a plastic scintillation detector. Our results show a high level of consistency within our data and compared well with published data.
立体定向放射外科(SRS)和图像引导放射治疗等先进的放射治疗方式可能会采用非常小的射野孔径,以便将高剂量精确地定位到靶区。对于许多剂量仪而言,精确测量小辐射野是一项众所周知的挑战。本研究的目的是使用塑料闪烁探测器测量立体定向锥形射野的总散射因子,并将其与二极管探测器及理论估计值进行比较。在Novalis Tx直线加速器上,使用直径为6毫米、7.5毫米、10毫米、12.5毫米和15毫米的立体定向锥形射野,对6MV的SRS射束进行测量。塑料闪烁探测器的优势在于其能量依赖性。在剂量最大值深度的水中测量总散射因子。通过将读数归一化为10厘米×10厘米的射野尺寸,来确定塑料闪烁探测器的总散射因子。为克服二极管探测器在确定散射因子时的能量依赖性,采用了菊花链连接法。塑料闪烁探测器相对于电离室进行了校准,发现测量剂量的重复性在±1%以内。对于6毫米、7.5毫米、10毫米、12.5毫米和15毫米的锥形射野尺寸,使用塑料闪烁探测器测量的总散射因子分别为0.728±0.3、0.783±0.05、0.866±0.55、0.885±0.5和0.910±0.06。对于6毫米、7.5毫米、10毫米、12.5毫米和15毫米的锥形射野尺寸,使用二极管探测器测量的总散射因子分别为0.733±0.03、0.782±0.02、0.834±0.07、0.854±0.02和0.872±0.02。对于7.5毫米、10毫米、12.5毫米和15毫米的锥形射野尺寸,总散射因子测量值与已发表的蒙特卡罗数据的差异分别为-1.3%、1.9%、-0.4%和0.4%。我们得出结论,使用塑料闪烁探测器可以充分地进行立体定向锥形射野的总散射因子测量。我们的结果表明,我们的数据具有高度的一致性,并且与已发表的数据相比表现良好。