Dosimetric evaluation of a glass dosimeter for proton beam measurements

被引:24
作者
Rah, Jeong-Eun [2 ]
Oh, Do Hoon [2 ]
Shin, Dongho [3 ]
Kim, Dae-Hyun [4 ]
Ji, Young Hoon [5 ]
Kim, Jong Won [2 ]
Park, Sung Yong [1 ]
机构
[1] McLaren Canc Inst, Proton Therapy Ctr, Flint, MI USA
[2] Kwandong Univ, Coll Med, Myongji Hosp, Dept Radiat Oncol, Kangnung, South Korea
[3] Natl Canc Ctr, Proton Therapy Ctr, Seoul, South Korea
[4] Catholic Univ Korea, Dept Biomed Engn, Seoul, South Korea
[5] Korea Inst Radiol & Med Sci, Taejon, South Korea
关键词
Glass dosimeter; Proton beam; TLD; GEANT 4 Monte-Carlo simulation; PHOTON; RADIOTHERAPY; ELECTRON; DETECTOR;
D O I
10.1016/j.apradiso.2012.04.007
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
Purpose: The GD-301 radiophotoluminescent glass dosimeter system has recently become commercially available. The purpose of this study was to investigate the dosimetric characteristics (reproducibility, linearity, dose rate, fading, angular dependence, and depth-dose distribution) of this system for clinical dosimetry in a high-energy proton beam and to compare it with lithium fluoride TLD-100. Materials and methods: The depth-dose distribution measured with the glass dosimeter was compared to those from GEANT4 Monte-Carlo simulation. All measurements were performed in a proton beam (IBA Proton Therapy System-Proteus 235) at the National Cancer Center in Korea. Dosimeters were irradiated in a water phantom using a stair-shaped holder specially designed for this study. Maximum height was 100 mm with 1 mm steps in each of ten-tiers. Results: Reproducibility in the 200 MeV proton beam was within 1.5% for the glass dosimeter, and within 1.7% for TLD-chip responses. The glass dosimeter signal was linear as a function of applied dose in the range of 1-10 Gy. The dose rate dependence of both dosimeters was within 1.5%. The fading effect of the glass dosimeter was found to be within 1.6% for 6 months. Angular dependence of the glass dosimeter was measured to be approximately 1.3% for angles that were 80 degrees from the beam axis using a cylindrical phantom. Depth-dose distributions in the non-modulated and modulated proton beams obtained with the glass dosimeter were estimated to be within 3.0% lower than those measured with the ionization chamber and simulation model using GEANT4 code. The Bragg peak depths determined from the ionization chamber, the glass dosimeter and GEANT4 simulation were 84.8 mm, 84.2 mm and 85.0 mm, respectively. For the modulated proton beam, the SOBP width between the 90% proximal and the distal dose levels as obtained from the glass dosimeter was 48.1 mm. The SOBP width measured with the ionization chamber was 52.2 mm. Conclusions: Measurements comparing the glass dosimeter and TLD-100 dosimetric characteristics demonstrated the suitability of use of the glass dosimeter for dose measurement in high-energy proton beam therapy. (c) 2012 Elsevier Ltd. All rights reserved.
引用
收藏
页码:1616 / 1623
页数:8
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