Melhus Christopher S, Rivard Mark J
Department of Radiation Oncology, Tufts University School of Medicine, Boston, Massachusetts 02111, USA.
Med Phys. 2006 Jun;33(6):1729-37. doi: 10.1118/1.2199987.
Underlying characteristics in brachytherapy dosimetry parameters for medical radionuclides 137Cs, 125I, 192Ir, 103Pd, and 169Yb were examined using Monte Carlo methods. Sources were modeled as unencapsulated point or line sources in liquid water to negate variations due to materials and construction. Importance of phantom size, mode of radiation transport physics--i.e., photon transport only or coupled photon:electron transport, phantom material, volume averaging, and Monte Carlo tally type were studied. For noninfinite media, g(r) was found to degrade as r approached R, the phantom radius. MCNP5 results were in agreement with those published using GEANT4. Brachytherapy dosimetry parameters calculated using coupled photon:electron radiation transport simulations did not differ significantly from those using photon transport only. Dose distributions from low-energy photon-emitting radionuclides 125I and 103Pd were sensitive to phantom material by upto a factor of 1.4 and 2.0, respectively, between tissue-equivalent materials and water at r =9 cm. In comparison, high-energy photons from 137Cs, 192Ir, and 169Yb demonstrated +/- 5% differences in dose distributions between water and tissue substitutes at r=20 cm. Similarly, volume-averaging effects were found to be more significant for low-energy radionuclides. When modeling line sources with L < or = 0.5 cm, the two-dimensional anisotropy function was largely within +/- 0.5% of unity for 137Cs, 125I, and 192Ir. However, an energy and geometry effect was noted for 103Pd and 169Yb, with Pd-103F(0.5,0 degrees)=l.05 and yb-169F(0.5,0 degrees)=0.98 for L=0.5 cm. Simulations of monoenergetic photons for L=0.5 cm produced energy-dependent variations in F(r, theta) having a maximum value at 10 keV, minimum at 50 keV, and approximately 1.0 for higher-energy photons up to 750 keV. Both the F6 cell heating and *F4 track-length estimators were employed to determine brachytherapy dosimetry parameters. F6 was found to be necessary for g(r), while both tallies provided equivalent results for F(r, theta).
使用蒙特卡罗方法研究了医用放射性核素137Cs、125I、192Ir、103Pd和169Yb近距离放射治疗剂量学参数的潜在特征。将源建模为液态水中的无封装点源或线源,以消除由于材料和结构引起的变化。研究了体模尺寸、辐射传输物理模式(即仅光子传输或光子与电子耦合传输)、体模材料、体积平均以及蒙特卡罗计数类型的重要性。对于非无限介质,发现当r接近体模半径R时,g(r)会降低。MCNP5的结果与使用GEANT4公布的结果一致。使用光子与电子耦合辐射传输模拟计算的近距离放射治疗剂量学参数与仅使用光子传输计算的参数没有显著差异。在r = 9 cm时,低能光子发射放射性核素125I和103Pd的剂量分布对体模材料敏感,在组织等效材料和水之间的差异分别高达1.4倍和2.0倍。相比之下,137Cs、192Ir和169Yb的高能光子在r = 20 cm时,水和组织替代物之间的剂量分布差异为±5%。同样,体积平均效应对于低能放射性核素更为显著。当对线源进行建模且线源长度L≤0.5 cm时,对于137Cs、125I和192Ir,二维各向异性函数在很大程度上在±0.5%的单位范围内。然而,对于103Pd和169Yb,注意到了能量和几何效应,对于L = 0.5 cm,103Pd的F(0.5,0°)=1.05,169Yb的F(0.5,0°)=0.98。对于L = 0.5 cm的单能光子模拟产生了F(r,θ)中与能量相关的变化,在10 keV时具有最大值,在50 keV时具有最小值,对于高达750 keV的更高能量光子约为1.0。F6细胞加热和*F4径迹长度估计器都被用于确定近距离放射治疗剂量学参数。发现F6对于g(r)是必要的,而两种计数方法对于F(r,θ)提供了等效的结果。