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Monte Carlo calculations of the dose distribution around a commercial gynecologic tandem applicator.商业妇科串联施源器周围剂量分布的蒙特卡罗计算
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2
Monte Carlo dosimetry of 60Co HDR brachytherapy sources.60钴高剂量率近距离放射治疗源的蒙特卡罗剂量测定法。
Med Phys. 2003 Apr;30(4):712-21. doi: 10.1118/1.1563662.
3
Optimization of a 90Sr/90Y radiation source train stepping for intravascular brachytherapy.用于血管内近距离放射治疗的90锶/90钇放射源序列步进优化
Med Phys. 2002 Dec;29(12):2891-6. doi: 10.1118/1.1524169.
4
Dosimetry of source stepping for intravascular brachytherapy.血管内近距离治疗源步进的剂量测定
Cardiovasc Radiat Med. 2001 Jul-Sep;2(3):165-72. doi: 10.1016/s1522-1865(01)00082-8.
5
Transit dose of an Ir-192 high dose rate brachytherapy stepping source.铱-192高剂量率近距离治疗步进源的传输剂量。
Phys Med Biol. 2001 Feb;46(2):323-31. doi: 10.1088/0031-9155/46/2/304.
6
Dose rate calculations around 192Ir brachytherapy sources using a Sievert integration model.使用西弗积分模型进行192铱近距离治疗源周围的剂量率计算。
Phys Med Biol. 2000 Feb;45(2):383-98. doi: 10.1088/0031-9155/45/2/309.
7
Dose errors in the near field of an HDR brachytherapy stepping source.高剂量率近距离治疗步进源近场中的剂量误差
Phys Med Biol. 1999 Feb;44(2):357-63. doi: 10.1088/0031-9155/44/2/005.
8
Experimental and Monte Carlo dosimetry of the Henschke applicator for high dose-rate 192Ir remote afterloading.用于高剂量率192铱远程后装的亨施克施源器的实验和蒙特卡罗剂量测定法
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9
Monte Carlo aided dosimetry of the microselectron pulsed and high dose-rate 192Ir sources.蒙特卡洛辅助的微型电子脉冲及高剂量率192铱源剂量测定法。
Med Phys. 1995 Jun;22(6):809-19. doi: 10.1118/1.597483.

基于矩阵移位技术的GZP6(60)钴步进源蒙特卡罗剂量计算

Monte Carlo dose calculation of GZP6 (60)Co stepping source based on a matrix shift technique.

作者信息

Toossi Mohammad Taghi Bahreyni, Abdollahi Malihe, Ghorbani Mahdi

机构信息

Medical Physics Research Center, Medical Physics Department, Faculty of Medicine, Mashhad University of Medical Sciences, Mashhad, Iran.

出版信息

Rep Pract Oncol Radiother. 2010 Dec 21;16(1):10-3. doi: 10.1016/j.rpor.2010.11.005. eCollection 2010.

DOI:10.1016/j.rpor.2010.11.005
PMID:24376950
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3863268/
Abstract

BACKGROUND

As a routine method for stepping source simulation, a Monte Carlo program is run according to the number of steps and then the summation of dose from each run is taken to obtain total dose distribution. This method is time consuming.

AIM

As an alternative method, a matrix shift based technique was applied to simulate a stepping source for brachytherapy.

MATERIALS AND METHODS

The stepping source of GZP6 brachytherapy unit was simulated. In a matrix shift method, it is assumed that a radiation source is stationary and instead the data matrix is shifted based on the number of steps. In this study, by running MCNPX program for one point and calculation of the dose matrix using the matrix shift method, the isodose curves for the esophageal cancer tumor lengths of 4 and 6 cm were obtained and compared with the isodose curves obtained by running MCNPX programs in each step position separately (15 and 23 steps for esophageal cancer tumor lengths of 4 and 6 cm, respectively).

RESULTS

The difference between the two dose matrixes for the stepping and matrix shift methods based on the average dose differences are 3.85 × 10(-4) Gy and 5.19 × 10(-4) Gy for treatment length of 4 cm and 6 cm, respectively. Dose differences are insignificant and these two methods are equally valid.

CONCLUSIONS

The matrix shift method presented in this study can be used for calculation of dose distribution for a brachytherapy stepping source as a quicker tool compared to other routine Monte Carlo based methods.

摘要

背景

作为步进源模拟的常规方法,根据步数运行蒙特卡罗程序,然后对每次运行的剂量求和以获得总剂量分布。这种方法很耗时。

目的

作为一种替代方法,应用基于矩阵移位的技术来模拟近距离放射治疗的步进源。

材料与方法

模拟了GZP6近距离放射治疗装置的步进源。在矩阵移位方法中,假设辐射源是固定的,而是根据步数移动数据矩阵。在本研究中,通过针对一个点运行MCNPX程序并使用矩阵移位方法计算剂量矩阵,获得了4厘米和6厘米食管癌肿瘤长度的等剂量曲线,并与分别在每个步位运行MCNPX程序获得的等剂量曲线进行比较(4厘米和6厘米食管癌肿瘤长度分别为15步和23步)。

结果

基于平均剂量差异,步进法和矩阵移位法的两个剂量矩阵之间的差异,对于4厘米和6厘米的治疗长度分别为3.85×10⁻⁴戈瑞和5.19×10⁻⁴戈瑞。剂量差异不显著,这两种方法同样有效。

结论

本研究中提出的矩阵移位方法可用于计算近距离放射治疗步进源的剂量分布,作为一种比其他基于蒙特卡罗的常规方法更快的工具。