Karaiskos P, Angelopoulos A, Pantelis E, Papagiannis P, Sakelliou L, Kouwenhoven E, Baltas D
Nuclear and Particle Physics Section, Department of Physics, University of Athens, Panepistimioupolis, Ilisia, 157 71 Athens, Greece.
Med Phys. 2003 Jan;30(1):9-16. doi: 10.1118/1.1524168.
A new microSelectron pulsed dose rate source has been designed, containing two active pellets instead of one inactive and one active pellet contained in the old design, to facilitate the incorporation of higher activity up to 74 GBq (2 Ci). In this work, Monte Carlo simulation is used to derive full dosimetric data following the AAPM TG-43 formalism, as well as the dose rate per unit air kerma strength data in Cartesian, "away and along" coordinates for both source designs. The calculated dose rate constant of the new PDR source design was found equal to lambda=(1.121 +/- 0.006) cGy h(-1) U(-1) compared to lambda = (1.124 +/- 0.006) cGy h(-1) U(-1) for the old design. Radial dose functions of the two sources calculated using the point source approximated geometry factors were found in close agreement (within 1%) except for radial distances under 2 mm. At polar angles close to the longitudinal source axis at the sources' distal end, the new design presents increased anisotropy (up to 10%) compared to the old one due to its longer active core. At polar angles close to the longitudinal source axis at the sources' drive wire end however, the old design presents increased anisotropy (up to 18%) due to attenuation of emitted photons through the inactive Ir pellet. These differences, also present in "away and along" dose rate results, necessitate the replacement of treatment planning input data for the new microSelectron pulsed dose rate source.
一种新型的微型Selectron脉冲剂量率源已被设计出来,它包含两个活性小球,而不是旧设计中的一个非活性小球和一个活性小球,以便能够纳入高达74 GBq(2 Ci)的更高活度。在这项工作中,采用蒙特卡罗模拟方法,依据美国医学物理师协会(AAPM)TG - 43形式主义推导完整的剂量学数据,以及两种源设计在笛卡尔坐标系、“远离和沿”坐标下每单位空气比释动能强度的剂量率数据。结果发现,新的PDR源设计的计算剂量率常数为λ = (1.121 ± 0.006) cGy h⁻¹ U⁻¹,而旧设计的为λ = (1.124 ± 0.006) cGy h⁻¹ U⁻¹。使用点源近似几何因子计算得到的两种源的径向剂量函数,除了在2 mm以下的径向距离外,结果非常接近(在1%以内)。在源的远端,靠近纵向源轴的极角处,由于新设计具有更长的活性芯,与旧设计相比呈现出更大的各向异性(高达10%)。然而,在源的驱动线端,靠近纵向源轴的极角处,由于发射的光子通过非活性铱小球的衰减,旧设计呈现出更大的各向异性(高达18%)。这些差异也体现在“远离和沿”剂量率结果中,因此需要为新型微型Selectron脉冲剂量率源替换治疗计划输入数据。