Pujades-Claumarchirant Ma Carmen, Granero Domingo, Perez-Calatayud Jose, Ballester Facundo, Melhus Christopher, Rivard Mark
Physics Section, Department of Radiation Oncology, La Fe University Hospital, Valencia, Spain.
Department of Radiation Oncology, ERESA, Hospital General Universitario, Valencia, Spain.
J Contemp Brachytherapy. 2010 Mar;2(1):28-32. doi: 10.5114/jcb.2010.13715. Epub 2010 Apr 1.
The aim of this work was to determine dose distributions for high-energy brachytherapy sources at spatial locations not included in the radial dose function () and 2D anisotropy function (,) table entries for radial distance and polar angle . The objectives of this study are as follows: 1) to evaluate interpolation methods in order to accurately derive () and (,) from the reported data; 2) to determine the minimum number of entries in () and (,) that allow reproduction of dose distributions with sufficient accuracy.
Four high-energy photon-emitting brachytherapy sources were studied: Co model Co0.A86, Cs model CSM-3, Ir model Ir2.A85-2, and Yb hypothetical model. The mesh used for was: 0.25, 0.5, 0.75, 1, 1.5, 2-8 (integer steps) and 10 cm. Four different angular steps were evaluated for (,): 1°, 2°, 5° and 10°. Linear-linear and logarithmic-linear interpolation was evaluated for (). Linear-linear interpolation was used to obtain (,) with resolution of 0.05 cm and 1°. Results were compared with values obtained from the Monte Carlo (MC) calculations for the four sources with the same grid.
Linear interpolation of () provided differences ≤ 0.5% compared to MC for all four sources. Bilinear interpolation of (,) using 1° and 2° angular steps resulted in agreement ≤ 0.5% with MC for Co, Ir, and Yb, while Cs agreement was ≤ 1.5% for < 15°.
The radial mesh studied was adequate for interpolating () for high-energy brachytherapy sources, and was similar to commonly found examples in the published literature. For (,) close to the source longitudinal-axis, polar angle step sizes of 1°-2° were sufficient to provide 2% accuracy for all sources.
本研究的目的是确定高能近距离放射治疗源在径向剂量函数()和二维各向异性函数(,)表格中未包含的径向距离和极角的空间位置处的剂量分布。本研究的目标如下:1)评估插值方法,以便从报告的数据中准确推导()和(,);2)确定()和(,)中能够以足够精度再现剂量分布的最少条目数。
研究了四种高能光子发射近距离放射治疗源:钴模型Co0.A86、铯模型CSM-3、铱模型Ir2.A85-2和镱假设模型。用于的网格为:0.25、0.5、0.75、1、1.5、2 - 8(整数步长)和10厘米。对(,)评估了四种不同的角度步长:1°、2°、5°和10°。对()评估了线性 - 线性和对数 - 线性插值。使用线性 - 线性插值以0.05厘米和1°的分辨率获得(,)。将结果与使用相同网格对四种源进行蒙特卡罗(MC)计算得到的值进行比较。
对于所有四种源,()的线性插值与MC相比差异≤0.5%。使用1°和2°角度步长对(,)进行双线性插值,对于钴、铱和镱,与MC的一致性≤0.5%,而对于铯,当<15°时一致性≤1.5%。
所研究的径向网格足以对高能近距离放射治疗源的()进行插值,并且与已发表文献中常见的示例相似。对于靠近源纵轴的(,),1° - 2°的极角步长足以对所有源提供2%的精度。