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An assessment of the efficiency of methods for measurement of the computed tomography dose index (CTDI) for cone beam (CBCT) dosimetry by Monte Carlo simulation

机译:通过蒙特卡洛模拟评估锥形束(CBCT)剂量的计算机断层摄影剂量指数(CTDI)方法的效率评估

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The IEC has introduced a practical approach to overcome shortcomings of the CTDI100 for measurements on wide beams employed for cone beam (CBCT) scans. This study evaluated the efficiency of this approach (CTDIIEC) for different arrangements using Monte Carlo simulation techniques, and compared CTDIIEC to the efficiency of CTDI100 for CBCT. Monte Carlo EGSnrc/BEAMnrc and EGSnrc/DOSXYZnrc codes were used to simulate the kV imaging system mounted on a Varian TrueBeam linear accelerator. The Monte Carlo model was benchmarked against experimental measurements and good agreement shown. Standard PMMA head and body phantoms with lengths 150, 600, and 900 mm were simulated. Beam widths studied ranged from 20-300 mm, and four scanning protocols using two acquisition modes were utilized. The efficiency values were calculated at the centre (εc) and periphery (εp) of the phantoms and for the weighted CTDI (εw). The efficiency values for CTDI100 were approximately constant for beam widths 20-40 mm, where εc(CTDI100), ε(CTDI100), and εw(CTDI100) were 74.7 ± 0.6%, 84.6 ± 0.3%, and 80.9 ± 0.4%, for the head phantom and 59.7 ± 0.3%, 82.1 ± 0.3%, and 74.9 ± 0.3%, for the body phantom, respectively. When beam width increased beyond 40 mm, ε(CTDI100) values fell steadily reaching ~30% at a beam width of 300 mm. In contrast, the efficiency of the CTDIIECwas approximately constant over all beam widths, demonstrating its suitability for assessment of CBCT. εc(CTDIIEC), εp(CTDIIEC), and εw(CTDIIEC) were 76.1 ± 0.9%, 85.9 ± 1.0%, and 82.2 ± 0.9% for the head phantom and 60.6 ± 0.7%, 82.8 ± 0.8%, and 75.8 ± 0.7%, for the body phantom, respectively, within 2% of ε(CTDI100) values for narrower beam widths. CTDI100,w and CTDIIEC,w underestimate CTDI∞,w by ~55% and ~18% for the head phantom and by ~56% and ~24% for the body phantom, respectively, using a clinical beam width 198 mm. The CTDIIEC approach addresses the dependency of efficiency on beam width successfully and correction factors have been derived to allow calculation of CTDI∞.
机译:IEC引入了一种实用的方法来克服CTDI100在锥束(CBCT)扫描所使用的宽光束上进行测量的缺点。本研究使用蒙特卡洛模拟技术评估了这种方法(CTDIIEC)在不同布置下的效率,并将CTDIIEC与CBCT的CTDI100效率进行了比较。蒙特卡洛EGSnrc / BEAMnrc和EGSnrc / DOSXYZnrc代码用于模拟安装在Varian TrueBeam线性加速器上的kV成像系统。蒙特卡洛模型是根据实验测量结果和良好的一致性进行基准测试的。模拟了长度分别为150、600和900 mm的标准PMMA头部和身体模型。研究的光束宽度范围为20-300 mm,并使用了两种使用两种采集模式的扫描协议。在体模的中心(εc)和外围(εp)以及加权CTDI(εw)处计算效率值。对于20-40 mm的光束宽度,CTDI100的效率值大致恒定,其中εc(CTDI100),ε(CTDI100)和εw(CTDI100)分别为74.7±0.6%,84.6±0.3%和80.9±0.4%头部体模分别为59.7±0.3%,82.1±0.3%和74.9±0.3%。当光束宽度增加到40 mm以上时,在300 mm光束宽度下ε(CTDI100)值稳定下降至〜30%。相比之下,CTDIIEC的效率在所有光束宽度上都大致恒定,这表明其适用于CBCT评估。头部模型的εc(CTDIIEC),εp(CTDIIEC)和εw(CTDIIEC)分别为76.1±0.9%,85.9±1.0%和82.2±0.9%,以及60.6±0.7%,82.8±0.8%和75.8±0.7对于较窄的光束宽度,对于人体模型,分别在ε(CTDI100)值的2%以内。 CTDI100,w和CTDIIEC,w使用临床光束宽度198 mm分别低估了头模的CTDI∞,w〜55%和〜18%,以及体模的CTDI∞,w约低56%和〜24%。 CTDIIEC方法成功地解决了效率对光束宽度的依赖性,并推导了校正因子以允许计算CTDI∞。

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