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Clinical radiation therapy measurements with a new commercial synthetic single crystal diamond detector

机译:使用新型商用合成单晶金刚石探测器进行临床放射治疗测量

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摘要

A commercial version of a synthetic single crystal diamond detector (SCDD) in a Schottky diode configuration was recently released as the new type 60019 microDiamond detector (PTW‐Freiburg, Germany). In this study we investigate the dosimetric properties of this detector to independently confirm that findings from the developing group of the SCDDs still hold true for the commercial version of the SCDDs. We further explore if the use of the microDiamond detector can be expanded to high‐energy photon beams of up to 15 MV and to large field measurements. Measurements were performed with an Elekta Synergy linear accelerator delivering 6, 10, and 15 MV X‐rays, as well as 6, 9, 12, 15, and 20 MeV electron beams. The dependence of the microdiamond detector response on absorbed dose after connecting the detector was investigated. Furthermore, the dark current of the diamond detector was observed after irradiation. Results are compared to similar results from measurements with a diamond detector type 60003. Energy dependency was investigated, as well. Photon depth‐dose curves were measured for field sizes 3×3,10×10, and 30×30cm2. PDDs were measured with the Semiflex type 31010 detector, microLion type 31018 detector, P Diode type 60016, SRS Diode type 60018, and the microDiamond type 60019 detector (all PTW‐Freiburg). Photon profiles were measured at a depth of 10 cm. Electron depth‐dose curves normalized to the dose maximum were measured with the 14×14cm2 electron cone. PDDs were measured with a Markus chamber type 23343, an E Diode type 60017 and the microDiamond type 60019 detector (all PTW‐Freiburg). Profiles were measured with the E Diode and microDiamond at half of D90,D90,D70, and D50 depths and for electron cone sizes of 6×6cm2, 14×14cm2, and 20×20cm2. Within a tolerance of 0.5% detector response of the investigated detector was stable without any preirradiation. After preirradition with approximately 250 cGy the detector response was stable within 0.1%. A dark current after irradiation was not observed. The microDiamond detector shows no energy dependence in high energy photon or electron dosimetry. Electron PDD measurements with the E Diode and microDiamond are in good agreement. However, compared to E Diode measurements, dose values in the bremsstrahlungs region are about 0.5% lower when measured with the microDiamond detector. Markus detector measurements agree with E Diode measurements in the bremsstrahlungs region. For depths larger than dmax, depth‐dose curves of photon beams measured with the microDiamond detector are in close agreement to those measured with the microLion detector for small fields and with those measured with a Semiflex 0.125 cc ionization chamber for large fields. Differences are in the range of 0.25% and less. For profile measurements, microDiamond detector measurements agree well with microLion and P Diode measurements in the high‐dose region of the profile and the penumbra region. For areas outside the open field, P Diode measurements are about 0.5%–1.0% higher than microDiamond and microLion measurements. Thus it becomes evident that the investigated diamond detector (type 60019) is suitable for a wide range of applications in high‐energy photon and electron dosimetry and is interesting for relative, as well as absolute, dosimetry.PACS numbers: 00.06, 80.87
机译:肖特基二极管配置的合成单晶金刚石探测器(SCDD)的商业版本最近作为新型60019微型金刚石探测器(德国PTW‐Freiburg)发布。在这项研究中,我们调查了此检测器的剂量学特性,以独立确认来自SCDD开发组的发现对于SCDD的商业版本仍然成立。我们进一步探讨了microDiamond检测器的用途是否可以扩展到高达15 MV的高能光子束和大视野测量。使用Elekta Synergy线性加速器进行测量,可提供6、10和15 MV X射线以及6、9、12、15和20 MeV电子束。在连接检测器后,研究了微金刚石检测器响应对吸收剂量的依赖性。另外,照射后观察到金刚石检测器的暗电流。将结果与使用60003型钻石探测器的测量结果进行了比较。还研究了能量依赖性。测量了光子深度剂量曲线的场大小 3 × 3 10 × 10 30 × 30 cm 2 。 PDD使用Semiflex 31010型检测器,microLion 31018型检测器,P Diode 60016型,SRS Diode 60018型和microDiamond 60019型检测器(均为PTW-Freiburg)进行测量。在10 cm的深度测量光子轮廓。使用 14 × 14 cm 2 电子锥。 PDD使用Markus腔室类型23343,E Diode类型60017和microDiamond类型60019检测器(均为PTW-Freiburg)进行测量。使用E Diode和microDiamond在的一半处测量轮廓 D 90 D 90 D 70 D 50 深度和 6 × 6 cm 2 14 × 14 cm 2 20 × 20 < msup> cm 2 。在0.5%的检测误差范围内,所研究的检测器的响应是稳定的,没有任何预辐射。预照射约250 cGy后,检测器响应稳定在0.1%以内。照射后未观察到暗电流。 microDiamond检测器在高能光子或电子剂量测定中显示无能量依赖性。使用E二极管和microDiamond进行电子PDD测量非常吻合。但是,与E Diode测量相比,用microDiamond检测器测量时,在ms致辐射区域的剂量值要低约0.5%。 Markus检测器的测量值与the致辐射区中的E Diode测量值一致。对于大于 d max ,使用microDiamond检测器测量的光子束的深度剂量曲线与使用microLion检测器测量的光子束的深度剂量曲线非常接近场,以及使用Semiflex 0.125 cc电离室测量的场。差异在0.25%以内。对于轮廓测量,在轮廓的高剂量区域和半影区域中,microDiamond检测器测量与microLion和P二极管测量非常吻合。对于开阔地带以外的区域,P二极管的测量值比microDiamond和microLion测量值高约0.5%–1.0%。因此,很明显,所研究的金刚石检测器(60019型)适用于高能光子和电子剂量学的广泛应用,并且对于相对和绝对剂量学都很有趣.PACS编号:00.06,80.87

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