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Radiographic film dosimetry of proton beams for depth‐dose constancy check and beam profile measurement

机译:质子束的射线照相底片剂量学,用于深度剂量稳定性检查和束轮廓测量

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Radiographic film dosimetry suffers from its energy dependence in proton dosimetry. This study sought to develop a method of measuring proton beams by the film and to evaluate film response to proton beams for the constancy check of depth dose (DD). It also evaluated the film for profile measurements. To achieve this goal, from DDs measured by film and ion chamber (IC), calibration factors (ratios of dose measured by IC to film responses) as a function of depth in a phantom were obtained. These factors imply variable slopes (with proton energy and depth) of linear characteristic curves that relate film response to dose. We derived a calibration method that enables utilization of the factors for acquisition of dose from film density measured at later dates by adapting to a potentially altered processor condition. To test this model, the characteristic curve was obtained by using EDR2 film and in-phantom film dosimetry in parallel with a 149.65 MeV proton beam, using the method. An additional validation of the model was performed by concurrent film and IC measurement perpendicular to the beam at various depths. Beam profile measurements by the film were also evaluated at the center of beam modulation. In order to interpret and ascertain the film dosimetry, Monte Carlos simulation of the beam was performed, calculating the proton fluence spectrum along depths and off-axis distances. By multiplying respective stopping powers to the spectrum, doses to film and water were calculated. The ratio of film dose to water dose was evaluated. Results are as follows. The characteristic curve proved the assumed linearity. The measured DD approached that of IC, but near the end of the spread-out Bragg peak (SOBP), a spurious peak was observed due to the mismatch of distal edge between the calibration and measurement films. The width of SOBP and the proximal edge were both reproducible within a maximum of 5 mm; the distal edge was reproducible within 1 mm. At 5 cm depth, the dose was reproducible within 10%. These large discrepancies were identified to have been contributed by film processor uncertainty across a layer of film and the misalignment of film edge to the frontal phantom surface. The deviations could drop from 5 to 2 mm in SOBP and from 10% to 4.5% at 5 cm depth in a well-controlled processor condition (i.e., warm up). In addition to the validation of the calibration method done by the DD measurements, the concurrent film and IC measurement independently validated the model by showing the constancy of depth-dependent calibration factors. For profile measurement, the film showed good agreement with ion chamber measurement. In agreement with the experimental findings, computationally obtained ratio of film dose to water dose assisted understanding of the trend of the film response by revealing relatively large and small variances of the response for DD and beam profile measurements, respectively. Conclusions are as follows. For proton beams, radiographic film proved to offer accurate beam profile measurements. The adaptive calibration method proposed in this study was validated. Using the method, film dosimetry could offer reasonably accurate DD constancy checks, when provided with a well-controlled processor condition. Although the processor warming up can promote a uniform processing across a single layer of the film, the processing remains as a challenge.PACS number: 87
机译:射线照相胶片剂量测定法在质子剂量测定法中具有能量依赖性。这项研究试图开发一种通过胶片测量质子束的方法,并评估胶片对质子束的响应,以进行深度剂量(DD)的稳定性检查。它还评估了胶片的轮廓测量。为了实现该目标,从通过膜和离子室(IC)测量的DDs中获得了作为幻像深度的函数的校准因子(通过IC测量的剂量与膜响应的比率)。这些因素意味着线性特征曲线的变化斜率(具有质子能量和深度)将膜响应与剂量相关联。我们推导了一种校准方法,该方法可以适应以后可能改变的加工条件,从而利用从以后测得的胶片密度中获取剂量的因素。为了测试该模型,使用EDR2膜和幻影膜剂量与149.65 MeV质子束平行,获得了特性曲线。通过同时在不同深度垂直于光束进行膜和IC测量,对模型进行了额外的验证。薄膜的光束轮廓测量也在光束调制的中心进行了评估。为了解释和确定薄膜剂量,对光束进行了蒙特卡洛斯模拟,计算了沿深度和离轴距离的质子注量谱。通过将各自的截止功率乘以光谱,可以计算出薄膜和水的剂量。评价膜剂量与水剂量的比率。结果如下。特性曲线证明了假定的线性。测得的DD接近IC的DD,但在展开的Bragg峰(SOBP)的末端附近,由于校准膜和测量膜之间的远端边缘不匹配,观察到了一个伪峰。 SOBP的宽度和近端边缘均可以在最大5 mm内再现。远端边缘可在1毫米内再现。在5厘米深处,剂量可重现10%以内。这些较大的差异被认为是由于胶片冲洗机在整个胶片层上的不确定性以及胶片边缘与正面幻影表面的未对准造成的。在良好控制的处理器条件下(即预热),SOBP的偏差可能从5毫米降至2毫米,而在5厘米深度处可能从10%降至4.5%。除了通过DD测量对校准方法进行验证之外,同时进行的胶片和IC测量通过显示深度相关的校准因子的恒定性来独立验证模型。对于轮廓测量,该膜与离子室测量显示出良好的一致性。与实验结果一致,通过计算得出的胶片剂量与水剂量的比值,通过揭示分别用于DD和光束轮廓测量的响应的相对较大和较小方差,有助于理解胶片响应的趋势。结论如下。对于质子束,射线照相胶片被证明可以提供准确的束轮廓测量。验证了本研究中提出的自适应校准方法。使用该方法,如果提供了良好控制的处理器条件,则薄膜剂量测定可以提供相当准确的DD常数检查。尽管冲洗机的预热可以促进胶片单层的均匀冲洗,但是冲洗仍然是一个挑战。PACS编号:87

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