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192Ir 剂量学中 TLD 校准方法的比较。

Comparison of TLD calibration methods for 192Ir dosimetry.

机构信息

Dept. Physical Sciences, Peter MacCallum Cancer Centre, Melbourne, Australia.

出版信息

J Appl Clin Med Phys. 2013 Jan 7;14(1):4037. doi: 10.1120/jacmp.v14i1.4037.

DOI:10.1120/jacmp.v14i1.4037
PMID:23318392
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5714053/
Abstract

For the purpose of dose measurement using a high-dose rate (192)Ir source, four methods of thermoluminescent dosimeter (TLD) calibration were investigated. Three of the four calibration methods used the (192)Ir source. Dwell times were calculated to deliver 1 Gy to the TLDs irradiated either in air or water. Dwell time calculations were confirmed by direct measurement using an ionization chamber. The fourth method of calibration used 6 MV photons from a medical linear accelerator, and an energy correction factor was applied to account for the difference in sensitivity of the TLDs in (192)Ir and 6 MV. The results of the four TLD calibration methods are presented in terms of the results of a brachytherapy audit where seven Australian centers irradiated three sets of TLDs in a water phantom. The results were in agreement within estimated uncertainties when the TLDs were calibrated with the (192)Ir source. Calibrating TLDs in a phantom similar to that used for the audit proved to be the most practical method and provided the greatest confidence in measured dose. When calibrated using 6 MV photons, the TLD results were consistently higher than the (192)Ir-calibrated TLDs, suggesting this method does not fully correct for the response of the TLDs when irradiated in the audit phantom.

摘要

为了使用高剂量率(192)Ir 源进行剂量测量,研究了四种热释光剂量计(TLD)校准方法。这四种校准方法中的三种使用了(192)Ir 源。通过 dwell time 计算,将 1 Gy 的剂量递送至在空气中或水中辐照的 TLD。通过使用电离室进行直接测量,验证了 dwell time 计算。第四种校准方法使用了来自医用直线加速器的 6 MV 光子,并应用能量校正因子来考虑 TLD 在(192)Ir 和 6 MV 中的灵敏度差异。将这四种 TLD 校准方法的结果呈现为七个澳大利亚中心在水模体中辐照三组 TLD 的近距离治疗审核的结果。当使用(192)Ir 源对 TLD 进行校准时,结果在估计的不确定度内一致。在类似于审核中使用的水模体中校准 TLD 被证明是最实用的方法,并为测量剂量提供了最大的信心。当使用 6 MV 光子进行校准时,TLD 的结果始终高于(192)Ir 校准的 TLD,这表明该方法不能完全校正 TLD 在审核水模体中辐照时的响应。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/c330c6eae68e/ACM2-14-258-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/466943302b49/ACM2-14-258-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/23f89a40e483/ACM2-14-258-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/c330c6eae68e/ACM2-14-258-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/466943302b49/ACM2-14-258-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/23f89a40e483/ACM2-14-258-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/eca7/5714053/c330c6eae68e/ACM2-14-258-g003.jpg

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本文引用的文献

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2
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3
Comparison of 192Ir air kerma calibration coefficients derived at ARPANSA using the interpolation method and at the National Physical Laboratory using a direct measurement.
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对澳大利亚辐射防护与核安全局使用插值法得出的192铱空气比释动能校准系数与英国国家物理实验室使用直接测量法得出的校准系数进行比较。
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